ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
Excerpts
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
This expansion of $f(a + h)$ is known as **’s Series**.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
A point at which the tangent to a curve has contact of the second order is called a **of inflexion**.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
if there is to be a maximum or minimum the first derivative which does not vanish must be an even derivative, and there will be a maximum if it is negative, a minimum if it is positive.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
The formula $f(x + h) = f(x) + hf'(x + \theta_{1}h)$ is not true if $f(x) = 1/x$ and $x < 0 < x + h$.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
The fact is of course that *$\dd x/\dd r$ and $\dd r/\dd x$ are not formed upon the same hypothesis as to the variation of $P$.*
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
Thus if $u = x + y + z$, $x$, $y$, and $z$ being the independent variables, then $\dd u/\dd x = 1$. But if we regard $u$ as a function of the variables $x$, $x + y = \eta$, and $x + y + z = \zeta$, so that $u = \zeta$, then $\dd u/\dd x = 0$.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
We have up to the present attributed no meaning of any kind to the symbol $dy$ standing by itself. We now agree to *define* $dy$ by the equation
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
The advantages of the ‘differential’ notation are in reality of a purely technical character.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
The number _a^b f(x) dx is called a **integral**; $a$ and $b$ are called its **and upper limits**; $f(x)$ is called the **of integration** or ****; and the interval $\DPmod{(a, b)}{[a, b]}$ the **of integration**.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
The distinction between the definite and the indefinite integral is merely one of point of view.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
And when we are considering a ‘definite integral’ we are not as a rule concerned with any possible variation of the limits.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
which is the formula for the transformation of a definite integral by ****.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
The reader must not suppose, however, that these new notations imply any essential novelty of idea: ‘partial differentiation’ with respect to $x$ is exactly the same process as ordinary differentiation, the only novelty lying in the presence in $f$ of a second variable $y$ independent of $x$.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
But the reader must be careful to impress on his mind that the notion of the partial derivative of a function of several variables is only determinate when *all* the independent variables are specified.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
Suppose for example that $y = 1 - x$ and $f(x, y) = x + y$. Then $D_{x}f(x, 1 - x) = D_{x}1 = 0$, but $D_{x}f(x, y) = 1$.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
The symbol $dy/dx$ thus acquires a double meaning; but there is no inconvenience in this, since (6) is true whichever meaning we choose.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
This is sometimes expressed by saying that $dy$ is the *principal part* of $\delta y$ when $\delta x$ is small, just as we might say that $ax$ is the ‘principal part’ of $ax + bx^{2}$ when $x$ is small.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
Thus *the formula which expresses $dz$ in terms of $dx$ and $dy$ is the same whether the variables $x$ and $y$ are independent or not*. This remark is of great importance in applications.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
But nothing which we know so far provides us with a direct definition of the area of a figure bounded by curved lines. We shall now show how to give a definition of $F(x)$ which will enable us to *prove* its existence.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
We define the area of $PpqQ$ as being *the common limit of $s$ and $S$, that is to say $J$*.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
The reader should be careful to guard himself against supposing that the continuity of all the derivatives of $f(x)$ is a sufficient condition for the validity of Taylor’s series. A direct discussion of the behaviour of $R_{n}$ is always essential.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
In view of the great importance of this theorem we shall give at the end of this chapter another proof, not essentially distinct from that given above, but different in form and depending on the method of integration by parts.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
Apply this process to the equation $x^{2} = 2$, taking $\xi = 3/2$ as the first approximation. [We find $h = -1/12$, $\xi + h = 17/12 = 1.417\dots$, which is quite a good approximation, in spite of the roughness of the first. If now we repeat the process, taking $\xi = 17/12$, we obtain $\xi + h = 577/408 = 1.414\MS215\dots$, which is correct to $5$ places of decimals.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
It is evident that the degree of smallness of $QR$ may be taken as a kind of measure of the *closeness of the contact* of the curves.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
In order that there should be a maximum or a minimum this expression must be of constant sign for all sufficiently small values of $h$, positive or negative. This evidently requires that $n$ should be even.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
Two curves are said to *intersect* (or *cut*) at a point if the point lies on each of them. They are said to *touch* at the point if they have the same tangent at the point.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
But a difficulty arises if $-1 < x < 0$, since $1 + \theta_{n}x < 1$ and $(1 + \theta_{n}x)^{m-n} > 1$ if $n > m$; knowing only that $0 < \theta_{n} < 1$, we cannot be assured that $1 + \theta_{n}x$ is not quite small and $(1 + \theta _{n}x)^{m-n}$ quite large.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
The circle which has contact of the second order with the curve at the point $(\xi, \eta)$ is called the **of curvature**, and its radius the **of curvature**.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
As it is not always practicable actually to determine the form of $F(x)$, it is convenient to have a formula which represents the area $PpqQ$ and contains no explicit reference to $F(x)$.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
But when we are considering ‘indefinite integrals’ or ‘integral functions’ we are usually thinking of *a relation between two functions*, in virtue of which one is the derivative of the other.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
The whole difficulty lies in the question, *what is the $x$ which occurs in $\cos x$ and $\sin x$*? To answer this question, we must define the measure of an angle, and we are now in a position to do so.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
It has however, for our present purpose, a fatal defect; for we have not proved that the arc of a curve, even of a circle, possesses a length.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
We must therefore found our definition on the notion not of length but of *area*. We define the measure of the angle $AOP$ as *twice the area of the sector $AOP$ of the unit circle*.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
This follows from (7). For we can take $H$ to be the least and $K$ the greatest value of $f(x)$ in $\DPmod{(a, b)}{[a, b]}$. Then the integral is equal to $\eta(b - a)$, where $\eta$ lies between $H$ and $K$. But, since $f(x)$ is continuous, there must be a value of $\xi$ for which $f(\xi) = \eta$ ([§]100).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
That the value of a definite integral may sometimes be found without a knowledge of the integral function is only to be expected, for the fact that we cannot determine the general form of a function $F(x)$ in no way precludes the possibility that we may be able to determine the difference $F(b) - F(a)$ between two of its particular values.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
It will be remembered that the difficulty in using Lagrange’s form, in % [examples:lvi]Ex. lvi%. 2, arose in connection with negative values of $x$.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
We define the integral of a complex function $f(x) = \DPtypo{\psi}{\phi}(x) + i\psi(x)$ of the real variable $x$, between the limits $a$ and $b$, by the equations
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
This inequality may be deduced without difficulty from the definitions of [§§]156 and 157.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
In these circumstances $u$ is called a *homogeneous function of degree $n$* in the variables $x$, $y$, $z$, ….
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
This result is known as **’s Theorem** on homogeneous functions.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
Two functions $u$ and $v$ are said to be *dependent* or *independent* according as they are or are not connected by such a relation as (1).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
This condition is therefore *necessary* for the existence of a relation such as (1).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
This rule, which gives a very good approximation, is known as **’s Rule**.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
It should be observed that if $\phi(x)$ is any cubic polynomial then $\phi^{(4)}(x) = 0$, and Simpson’s Rule is exact.
Equations
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\lim \frac{QR}{h^{n}} = \frac{1}{n!}\{\phi^{(n)}(\xi) - f^{(n)}(\xi)\}When the first n-1 derivatives of the two curves agree at xi, the gap QR is of order n, with coefficient given by the difference of their n-th derivatives over n factorial.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(b) - f(a) = (b - a) f'(\xi)For a function with a derivative on the interval from a to b, the change in f equals the interval length times the derivative at some point xi between a and b.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(a + h) - f(a) = hf'(a + \theta_{1} h)The increase of f over a step h equals h times the derivative at a point a + theta_1 h inside the step, with 0 < theta_1 < 1.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(a + h) = f(a) + hf'(a) + \tfrac{1}{2}h^{2} f''(a + \theta_{2}h)The value of f at a + h equals its first-order expansion at a plus a second-order term with the second derivative at a point inside the step.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(a + h) - S_{n} = R_{n}The difference between f(a + h) and the partial sum S_n of its expansion equals the remainder R_n.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(a + h) = \lim_{n\to\infty} S_{n}If the remainder tends to zero, f(a + h) equals the limit of the partial sums of its Taylor expansion.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
R_{n} = \frac{h^{n}}{n!} f^{(n)}(a + \theta_{n} h)The remainder after n terms of Taylor's expansion equals h^n over n factorial times the n-th derivative at a point inside the step.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(h) = f(0) + hf'(0) + \frac{h^{2}}{2!} f''(0) + \dotsTaylor's series with a = 0 expresses f(h) as a power series in h using the derivatives at zero.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
(1 + x)^{m} = 1 + \binom{m}{1}x + \binom{m}{2}x^{2} + \dotsThe power (1 + x) raised to any rational m is expanded as a series in x with binomial coefficients.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\sin h = h - \frac{h^{3}}{3!} + \frac{h^{5}}{5!} - \dotsThe sine of h is given by its alternating power series, valid for all values of h.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
x = \xi - \frac{f(\xi)}{f'(\xi)}Starting from an approximate root xi, the next approximation to a root of f(x) = 0 is xi minus f(xi) divided by f'(xi).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
y - f(\xi) = (x - \xi)f'(\xi)The tangent to y = f(x) at x = xi is the line through (xi, f(xi)) with slope f'(xi).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\psi(x) = f(x)/\phi(x)Psi is defined as the ratio of f to phi, a function that is not defined where phi vanishes.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(x)/\phi(x) \to f'(\xi)/\phi'(\xi)If f and phi vanish at xi and their first derivatives at xi are not zero, the ratio f/phi tends to the ratio of the derivatives.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(x)/\phi(x) \to f^{(p)}(\xi)/\phi^{(p)}(\xi)When the first non-vanishing derivatives of f and phi are of the same order p, the ratio f/phi tends to the ratio of those p-th derivatives at xi.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\phi(\xi + h) - \phi(\xi) = \frac{h^{n}}{n!} \phi^{(n)} (\xi + \theta_{n} h)When the first n-1 derivatives of phi vanish at xi, the change in phi over a small step is h^n over n factorial times the n-th derivative at a point inside the step.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\lim \frac{QR}{h^{2}} = \tfrac{1}{2}\{\phi''(\xi) - f''(\xi)\}When two curves touch at xi, the gap QR between their ordinates is of second order in h, with coefficient half the difference of their second derivatives.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
r = \frac{(1 + \eta_{1}^{2})^{3/2}}{\eta_{2}}The radius of curvature of y = f(x) at a point equals (1 + eta_1 squared) to the power 3/2 divided by eta_2, where eta_1 and eta_2 are the first and second derivatives there.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
(x - a)^{2} + (y - b)^{2} = r^{2}A circle of centre (a, b) and radius r is the set of points (x, y) satisfying this equation.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(x) = a_{0} + a_{1}x + a_{2}x^{2} + \dots + (a_{n} + \epsilon_{x}) x^{n}If the n-th derivative of f is continuous at zero, f is a polynomial of degree n in x plus a remainder term that vanishes faster than x^n.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
a_{r} = f^{(r)}(0)/r!The coefficient of x to the power r in the expansion equals the r-th derivative of f at zero divided by r factorial.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
(\sin x\arcsin x - x^{2})/x^{6} \to \frac{1}{18}As x tends to zero, the expression (sin x arcsin x minus x squared) divided by x to the sixth tends to 1/18.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\lim_{x \to n} (x - n)\cosec x\pi = \frac{(-1)^{n}}{\pi}For any integer n, (x - n) times cosec(pi x) tends to (-1) to the n over pi as x tends to n.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\lim_{h\to 0}\frac{f(x + h, y) - f(x, y)}{h}The partial derivative of f with respect to x is the limit of the difference quotient taken with y held fixed.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{\dd r}{\dd x} = \frac{x}{\sqrtp{x^{2} + y^{2}}}With x = r cos θ and y = r sin θ, the partial derivative of r with respect to x at fixed y equals x over r.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{\dd \theta}{\dd x} = -\frac{y}{x^{2} + y^{2}}The partial derivative of the polar angle θ with respect to x at fixed y is minus y over x squared plus y squared.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{\dd x}{\dd r} = \cos\thetaWith x and y regarded as functions of r and θ, the partial derivative of x with respect to r at fixed θ is cos θ.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{\dd x}{\dd \theta} = -r\sin\thetaThe partial derivative of x with respect to θ at fixed r is minus r times sin θ.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\lim (\Delta r/\Delta x) = \lim (PP_{2}/PP_{1}) = \sec\thetaAlong the other hypothesis (r increased with θ fixed), the ratio Δr/Δx tends to sec θ.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\lim (\delta r/\Delta r) = \cos^{2}\thetaThe two partial-derivative hypotheses give ratios whose quotient tends to cos squared θ, so dx/dr and dr/dx are not reciprocals.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
b(\dd z/\dd x) = a(\dd z/\dd y)If z = f(ax + by), then b times the partial derivative of z with respect to x equals a times the partial derivative of z with respect to y.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\dd u/\dd x = 1For u = x + y + z with x, y, z independent, the partial derivative of u with respect to x is 1.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{df}{dt} = \frac{\dd f}{\dd x}\, \frac{dx}{dt} + \frac{\dd f}{\dd y}\, \frac{dy}{dt}The derivative of f along a curve x = φ(t), y = ψ(t) is the sum of the partial derivatives of f times the derivatives of x and y with respect to t.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{df}{dx} = \frac{\dd f}{\dd x} + \frac{\dd f}{\dd y}\, \frac{dy}{dx}When t is x, the total derivative of f{x, ψ(x)} equals the partial derivative in x plus the partial derivative in y times dy/dx.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{\dd f}{\dd x}\, \frac{dx}{dt} + \frac{\dd f}{\dd y}\, \frac{dy}{dt} = 0If eliminating t between x = φ(t) and y = ψ(t) gives f(x, y) = 0, then the total derivative of f along the curve vanishes.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
r' = (xx' + yy')/rThe derivative of the polar distance r with respect to t is (x x' + y y') divided by r, where dashes denote d/dt.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\theta' = (xy' - yx')/r^{2}The derivative of the polar angle θ with respect to t is (x y' minus y x') divided by r squared.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\phi(x + h) - \phi(x) = hf'(x + \theta h)The increment of φ over an interval h equals h times f' at some point between x and x + h.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\delta z = f(x + h, y + k) - f(x, y)The increment of z = f(x, y) when x and y receive increments h and k.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\delta z = (f_{x}' + \epsilon)\, \delta x + (f_{y}' + \eta)\, \delta yThe increment of z equals the partial derivatives times the increments, plus small corrections ε and η that vanish as the increments vanish.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\delta z = f_{x}'\, \delta x + f_{y}'\, \delta yThe increment of z is approximately equal to the partial derivatives times the increments, with error small compared with the larger increment.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\delta y = f'(x)\, \delta xFor a function of one variable, the increment of y is approximately f'(x) times the increment of x.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
dy = f'(x)\, \delta xThe differential dy is defined as f'(x) times the increment δx of x.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
dx = \delta xThe differential of the independent variable x equals its increment.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
dy = f'(x)\, dxThe differential of y equals the derivative of f times the differential of x.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{dy}{dx} = f'(x)The quotient of the differentials dy and dx equals the derivative of f.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\lim \frac{dy}{\delta y} = 1When f' is continuous, the ratio of dy to δy tends to 1 as δx tends to zero, so dy is the principal part of δy.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
dz = f_{x}'\, \delta x + f_{y}'\, \delta yThe differential of z = f(x, y) is defined as the partial derivatives times the increments of x and y.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
dz = f_{x}'\, dx + f_{y}'\, dyThe differential of z equals the partial derivatives times the differentials of x and y, whether or not x and y are independent.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
A = \pi abThe area of an ellipse with semiaxes a and b is π times a times b.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{dA}{A} = \frac{da}{a} + \frac{db}{b}The relative change of the ellipse's area equals the sum of the relative changes of its semiaxes.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{d\Delta}{\Delta} = \cot A\, dA + \frac{db}{b} + \frac{dc}{c}The relative change of a triangle's area expressed through angle A and sides b and c.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{d\Delta}{\Delta} = 2\frac{da}{a} + \frac{c\, dB}{a\sin B} + \frac{b\, dC}{a\sin C}The relative change of a triangle's area expressed through side a and angles B and C.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
d\Delta = R(\cos A\, da + \cos B\, db + \cos C\, dc)The differential of the triangle's area in terms of its sides, with R the circumradius.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{\dd a}{\dd b} = -\frac{\cos B}{\cos A}If the triangle's area stays constant, the partial derivative of a with respect to b is minus cos B over cos A.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{\dd a}{\dd c} = -\frac{\cos C}{\cos A}If the triangle's area stays constant, the partial derivative of a with respect to c is minus cos C over cos A.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{da}{\cos A} + \frac{db}{\cos B} + \frac{dc}{\cos C} = 0If the circumradius R stays constant, the sides of the triangle satisfy this linear relation among their differentials.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{\dd a}{\dd b} = -\frac{\cos A}{\cos B}With the circumradius constant, the partial derivative of a with respect to b is minus cos A over cos B.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{\dd z}{\dd x} = \frac{\dd z}{\dd u}\, \frac{\dd u}{\dd x} + \frac{\dd z}{\dd v}\, \frac{\dd v}{\dd x}The partial derivative of z with respect to x, where z depends on u and v which depend on x, is the sum of the chained partial derivatives through u and through v.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
P = -\frac{a_{1}p + a_{2}q - a_{3}}{c_{1}p + c_{2}q - c_{3}}After a linear change of variables, the partial derivative P of Z with respect to X is expressed in terms of p and q, the partial derivatives of z.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{dy}{dx} = -\frac{f_{a}'}{f_{b}'}For the implicit relation f(x, y) = 0 through (a, b), dy/dx equals minus the ratio of the partial derivatives of f at (a, b).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
(x - x_{0}) f_{x_{0}}'(x_{0}, y_{0}) + (y - y_{0}) f_{y_{0}}'(x_{0}, y_{0}) = 0The tangent to the curve f(x, y) = 0 at (x0, y0) is the line whose equation uses the partial derivatives of f at that point.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
F'(x) = f(x)The derivative of the area function F(x) under the graph of f is f(x), now justified by the definition of area.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
s = m_{0}\delta_{0} + m_{1}\delta_{1} + \dots + m_{n}\delta_{n}The lower sum s is the sum of each sub-interval length times the lower bound of f on that sub-interval.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
s \leq M(b - a)Each lower sum is at most M times the length of the whole interval, where M is an upper bound of f.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
S \geq m(b - a)Each upper sum is at least m times the length of the whole interval, where m is a lower bound of f.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
0 \leq J - s < \epsilonFor a fine enough subdivision, the lower sum lies within ε below the common limit J of the lower and upper sums.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
S - s = \tsum (M_{\nu} - m_{\nu})\, \delta_{\nu} < \epsilonThe gap between the upper and lower sums can be made less than any ε by making every sub-interval short enough.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\sigma = \tsum f_{\nu}\delta_{\nu}The sum σ takes f at any point of each sub-interval times the sub-interval length and lies between s and S.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
F(x) = \int f(x)\, dxThe indefinite integral of f is written as the function F whose derivative is f.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
(PpqQ) = \int_{a}^{b} f(x)\, dxThe area PpqQ under the curve y = f(x) between x = a and x = b is written as a definite integral.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\ds\int_{a}^{b} f(x)\, dx = F(b) - F(a)The definite integral of f from a to b equals the difference of any integral function F at the two limits.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
F(x) = F(a) + \int_{a}^{x} f(t)\, dtAny indefinite integral F can be written as a constant F(a) plus a definite integral with variable upper limit.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\arctan m = \int_{0}^{m} \frac{dt}{1 + t^{2}}The arctangent of m is defined as the integral of 1/(1+t^2) from 0 to m.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\phi(m) = \tfrac{1}{2} m\mu^{2} + \int_{\mu}^{1} \sqrtp{1 - x^{2}}\, dxThe area of the sector of the unit circle between OA and OP, as a function of the slope m, equals a triangle term plus an integral of the circle's height.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\phi'(m) = \frac{1}{2(1 + m^{2})}The derivative of the sector-area function with respect to m is 1/(2(1+m^2)).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\phi(m) = \tfrac{1}{2} \int_{0}^{m} \frac{dt}{1 + t^{2}}The sector-area function equals half the integral of 1/(1+t^2) from 0 to m.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\ds\int_{a}^{b} f(x)\, dx = -\int_{b}^{a} f(x)\, dxInterchanging the limits of a definite integral changes its sign.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\ds\int_{a}^{a} f(x)\, dx = 0A definite integral over an interval of zero length is zero.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\ds\int_{a}^{b}f(x)\, dx + \int_{b}^{c}f(x)\, dx = \int_{a}^{c}f(x)\, dxDefinite integrals over adjacent intervals add to the integral over the combined interval.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\ds\int_{a}^{b}kf(x)\, dx = k \int_{a}^{b}f(x)\, dxA constant factor can be taken outside a definite integral.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\ds\int_{a}^{b}\{f(x) + \phi(x)\}\, dx = \int_{a}^{b}f(x)\, dx + \int_{a}^{b}\phi(x)\, dxThe definite integral of a sum is the sum of the definite integrals.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\ds\int_{a}^{b}f(x)\, dx \geq 0If f(x) is nonnegative on [a, b], its definite integral over [a, b] is nonnegative.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
H(b - a) \leq \int_{a}^{b}f(x)\, dx \leq K(b - a)If f lies between constants H and K on [a, b], the integral of f lies between H(b-a) and K(b-a).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\ds\int_{a}^{b}f(x)\, dx = (b-a)f(\xi)For continuous f there is a point xi between a and b at which the integral equals (b - a) times f(xi).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
F(b) - F(a) = (b - a)F'(\xi)Restated with an integral function F, the first mean value theorem for integrals is the ordinary mean value theorem of the differential calculus.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
H\int_{a}^{b} \phi(x)\, dx \leq \int_{a}^{b} f(x)\phi(x)\, dx \leq K\int_{a}^{b} \phi(x)\, dxWhen phi is positive, the integral of f times phi lies between H and K times the integral of phi.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{a}^{b} f(x)\phi(x)\, dx = f(\xi) \int_{a}^{b} \phi(x)\, dxFor continuous f and positive phi, the integral of f times phi equals f at some point xi times the integral of phi.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
F(x) = \int_{a}^{x} f(t)\, dtThe integral of f from a to x is a function of x whose derivative is f(x), and is therefore continuous.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{a}^{b} f(x)\phi'(x)\, dx = f(b)\phi(b) - f(a)\phi(a) - \int_{a}^{b} f'(x)\phi(x)\, dxThe integral of f times the derivative of phi equals the boundary terms minus the integral of f' times phi.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int f\{\phi(x)\}\phi'(x)\, dx = F\{\phi(x)\}If F is an integral function of f, then the integral of f(phi(x)) times phi'(x) is F(phi(x)); this is the rule for substitution in an indefinite integral.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{c}^{d} f(t)\, dt = F(d) - F(c) = F\{\phi(b)\} - F\{\phi(a)\} = \int_{a}^{b} f\{\phi(x)\}\phi'(x)\, dxWith c = phi(a) and d = phi(b), a definite integral in t equals the definite integral in x after substituting t = phi(x).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(a + h) = f(a) + hf'(a) + \dots + \frac{h^{n-1}}{(n - 1)!} f^{(n-1)}(a) + R_{n}A function with n continuous derivatives equals its Taylor polynomial of degree n-1 about a, plus a remainder R_n.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
R_{n} = \frac{h^{n}}{(n - 1)!} \int_{0}^{1} (1 - t)^{n-1} f^{(n)}(a + th)\, dtThe remainder after n terms of Taylor's expansion is an integral of the nth derivative, with the variable t running from 0 to 1.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
R_{n} = \frac{(1 - \theta)^{n-p} f^{(n)}(a + \theta h)h^{n}}{p(n - 1)!}The Taylor remainder can be written with a point a + theta h, 0 < theta < 1, and an integer p between 1 and n; p = n gives Lagrange's form.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
R_{n} = \frac{(1 - \theta)^{n-1} f^{(n)}(a + \theta h) h^{n}}{(n - 1)!}Taking p = 1 gives Cauchy's form of the Taylor remainder, with a point a + theta h, 0 < theta < 1.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
R_{n} = \frac{m(m - 1)\dots (m - n + 1)}{1·2\dots (n - 1)}\, \frac{(1 - \theta )^{n-1} x^{n}}{(1 + \theta x)^{n-m}}For f(x) = (1 + x)^m, Cauchy's form of the remainder after n terms of the binomial series.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
|R_{n}| < K |m| \left|\binom{m - 1}{n - 1}\right| |x^{n}| = \rho_{n}The binomial-series remainder is bounded by rho_n, which tends to zero as n tends to infinity, so the remainder tends to zero.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{a}^{b} f(x)\, dx = \int_{a}^{b} \{\phi(x) + i\psi(x)\}\, dx = \int_{a}^{b} \phi(x)\, dx + i \int_{a}^{b} \psi(x)\, dxThe integral of a complex function of a real variable is defined as the integral of its real part plus i times the integral of its imaginary part.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\left|\int_{a}^{b} f(x)\, dx\right| \leq \int_{a}^{b} |f(x)|\, dxThe modulus of the integral of a complex function is at most the integral of its modulus.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
|\tsum f_{\nu}\, \delta_{\nu}| \leq \tsum |f_{\nu}|\, \delta_{\nu}The modulus of a finite sum of complex terms times increments is at most the sum of the moduli.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\tan x &= x + \tfrac{1}{3} x^{3} + \tfrac{2}{15} x^{5} + \dotsThe first terms of the Taylor series of tan x about 0 (to be verified).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\sec x &= 1 + \tfrac{1}{2} x^{2} + \tfrac{5}{24} x^{4} + \dotsThe first terms of the Taylor series of sec x about 0 (to be verified).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
x\cosec x &= 1 + \tfrac{1}{6} x^{2} + \tfrac{7}{360} x^{4} + \dotsThe first terms of the Taylor series of x cosec x about 0 (to be verified).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
x\cot x &= 1 - \tfrac{1}{3} x^{2} - \tfrac{1}{45} x^{4} - \dotsThe first terms of the Taylor series of x cot x about 0 (to be verified).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\theta_{n} = \frac{1}{n + 1} + \frac{n}{2(n + 1)^{2}(n + 2)} \left\{\frac{f^{(n+2)}(0)}{f^{(n+1)}(0)} + \epsilon_{x}\right\}xThe value of theta_n in Lagrange's form of the remainder after n terms, expanded for small x, where epsilon_x tends to 0 as x tends to 0.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(b) = f(a) + \tfrac{1}{2}(b - a) \{f'(a) + f'(b)\} - \tfrac{1}{12}(b - a)^{3} f'''(\alpha)Expresses f(b) through f(a), f' at the ends and f''' at an intermediate point alpha, where a < alpha < b.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(b) = f(a) + (b - a) f'\{\tfrac{1}{2}(a + b)\} + \tfrac{1}{24}(b - a)^{3}f'''(\alpha)Expresses f(b) using the derivative at the midpoint of [a, b] plus a third-derivative remainder at an intermediate point alpha.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(b) = f(a) + \tfrac{1}{6}(b - a) [f'(a) + f'(b) + 4f'\{\tfrac{1}{2}(a + b)\}] - \tfrac{1}{2880}(b - a)^{5} f^{(5)}(\DPtypo{a}{\alpha})Expresses f(b) through end-point and midpoint derivatives plus a fifth-derivative remainder at an intermediate point.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(b) = f(a) + \tfrac{1}{2}(b - a) \{f'(a) + f'(b)\} - \tfrac{1}{12}(b - a)^{2} \{f''(b) - f''(a)\} + \tfrac{1}{720}(b - a)^{5} f^{(5)}(\alpha)Expresses f(b) through first and second derivatives at the end points plus a fifth-derivative remainder at an intermediate point alpha.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\begin{vmatrix} f(a) & f(b)\\ g(a) & g(b) \end{vmatrix} = (b - a) \begin{vmatrix} f(a) & f'(\beta)\\ g(a) & g'(\beta) \end{vmatrix}A second-order determinant of function values equals (b - a) times a determinant with f' at an intermediate point beta.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\begin{vmatrix} f(a) & f(b) & f(c)\\ g(a) & g(b) & g(c)\\ h(a) & h(b) & h(c) \end{vmatrix} = \tfrac{1}{2} (b - c)(c - a)(a - b) \begin{vmatrix} f(a) & f'(\beta) & f''(\gamma)\\ g(a) & g'(\beta) & g''(\gamma)\\ h(a) & h'(\beta) & h''(\gamma) \end{vmatrix}A third-order determinant of function values equals a product of differences times a determinant of f, f' and f'' at intermediate points beta and gamma.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
A(x^{n}/n!) \leq F(x) \leq B(x^{n}/n!)If the n-th derivative of F lies between A and B on [0, h] and the lower derivatives vanish at 0, then F lies between A and B times x^n/n!.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\Delta_{h}^{n}\phi(x) = \sum_{r=0}^{n}(-1)^{r} \binom{n}{r} \phi(x + rh) = (-h)^{n} \phi^{(n)}(\xi)The n-th finite difference of phi equals a binomial-weighted sum, and also equals (-h)^n times the n-th derivative at an intermediate point xi.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\{\Delta_{h}^{n}\phi(x)\}/h^{n} \to (-1)^{n}\phi^{(n)}(x)As h tends to 0 the scaled n-th difference tends to (-1)^n times the n-th derivative, when that derivative is continuous.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
x^{n-m}\, \Delta_{h}^{n} x^{m} \to m(m - 1) \dots (m - n + 1)h^{n}As x tends to infinity, x^(n-m) times the n-th difference of x^m tends to m(m-1)...(m-n+1) h^n.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
x\sqrt{x} \{\sqrt{x} - 2\sqrtp{x + 1} + \sqrtp{x + 2}\} \to -\tfrac{1}{4}A specific instance: the scaled second difference of sqrt(x) tends to -1/4 as x tends to infinity.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
y = \phi(x) = x + a_{2}x^{2} + a_{3}x^{3} + (a_{4} + \epsilon_{x})x^{4}Series expansion of y = phi(x) near x = 0 with phi(0) = 0 and phi'(0) = 1, where epsilon_x tends to 0.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
x = \psi(y) = y - a_{2}y^{2} + (2a_{2}^{2} - a_{3})y^{3} - (5a_{2}^{3} - 5a_{2}a_{3} + a_{4} + \epsilon_{y})y^{4}Series of the inverse function x = psi(y) for the branch vanishing with y, where epsilon_y tends to 0.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{\phi(x)\psi(x) - x^{2}}{x^{4}} \to a_{2}^{2}The limit of (phi(x) psi(x) - x^2)/x^4 as x tends to 0 equals a_2 squared.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
-(\xi - x)/y' = (\eta - y)/x' = (x'^{2} + y'^{2})/(x'y'' - x''y')The coordinates (xi, eta) of the centre of curvature of a parametric curve at (x, y) satisfy this relation, with dashes denoting derivatives with respect to t.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
(x'^{2} + y'^{2})^{3/2}/(x'y'' - x''y')The radius of curvature of the parametric curve x = f(t), y = F(t) is this expression.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
3a(\xi + x) + 2x^{2} = 0For the curve 27a y^2 = 4x^3, the x-coordinate of the centre of curvature satisfies this relation.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\eta = 4y + (9ay)/x.For the curve 27a y^2 = 4x^3, the y-coordinate of the centre of curvature is given by this relation.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
(1 + y_{1}^{2})y_{3} = 3y_{1}y_{2}^{2}Condition at a point for the circle of curvature to have contact of the third order with the curve.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
a^{3}y = a^{4}x^{2} + a^{2}bxy + (ac - b^{2})y^{2}The conic of closest contact with y = ax^2 + bx^3 + cx^4 + ... at the origin.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
18\eta_{2}^{3}T = 9\eta_{2}^{4}(x - \xi)^{2} + 6\eta_{2}^{2}\eta_{3}(x - \xi)T + (3\eta_{2}\eta_{4} - 4\eta_{3}^{2})T^{2}The conic of closest contact at the point (xi, eta) of the curve y = f(x), where eta_k are derivatives of f and T = (y - eta) - eta_1 (x - xi).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
T = (y - \eta) - \eta_{1}(x - \xi)Definition of T as the deviation of y from the tangent line at (xi, eta).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
x\frac{\dd u}{\dd x} + y\frac{\dd u}{\dd y} + z\frac{\dd u}{\dd z} + \dots = nuFor a homogeneous function u of degree n, the sum of each variable times its partial derivative equals n times u.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
u = x^{n} f(y/x, z/x, \dots)Definition of a homogeneous function u of degree n in the variables x, y, z.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
xF_{\xi} + yF_{\eta} + zF_{\zeta} = 0The equation of the tangent at (xi, eta) to the curve f(x, y) = 0, written from its homogeneous form F(x, y, z) = 0.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
u_{x}v_{y} - u_{y}v_{x} = 0The Jacobian of u and v vanishes; this is a necessary condition for u and v to be functionally dependent.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{\dd \phi}{\dd u}\, \frac{\dd u}{\dd x} + \frac{\dd \phi}{\dd v}\, \frac{\dd v}{\dd x} = 0Differentiating the relation phi(u, v) = 0 with respect to x gives this equation.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
J = \begin{vmatrix} u_{x} & u_{y}\\ v_{x} & v_{y} \end{vmatrix} = u_{x}v_{y} - u_{y}v_{x} = 0The Jacobian J of u and v is the determinant of their partial derivatives; it must vanish if u and v are dependent.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
J = \frac{\dd(u, v)}{\dd(x, y)}Notation for the Jacobian of u and v with respect to x and y.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
J = \begin{vmatrix} u_{x} & u_{y} & u_{z}\\ v_{x} & v_{y} & v_{z}\\ w_{x} & w_{y} & w_{z} \end{vmatrix} = \frac{\dd(u, v, w)}{\dd(x, y, z)}The Jacobian of three functions of three variables is the 3x3 determinant of their partial derivatives; it vanishes exactly when they are functionally dependent.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
abc + 2fgh - af^{2} - bg^{2} - ch^{2} = 0Condition for the quadratic form ax^2 + by^2 + cz^2 + 2fyz + 2gzx + 2hxy to factor into two linear functions.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\frac{\dd(u, v)}{\dd(x, y)} = \frac{\dd(u, v)}{\dd(\xi, \eta)}\, \frac{\dd(\xi, \eta)}{\dd(x, y)}Chain rule for Jacobians when u, v depend on xi, eta which depend on x, y.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(x) + f(y) = f(xy)The functional equation satisfied by f when f' = 1/x and f(1) = 0.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(x) + f(y) = f\left(\frac{x + y}{1 - xy}\right)The functional equation satisfied by f when f' = 1/(1 + x^2) and f(0) = 0.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(x) = \int_{0}^{x} \frac{dt}{\sqrtp{1 - t^{4}}}Definition of f as an integral of 1/sqrt(1 - t^4) from 0 to x.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f(x) + f(y) = f\left\{\frac{x\sqrtp{1 - y^{4}} + y\sqrtp{1 - x^{4}}}{1 + x^{2}y^{2}}\right\}The addition formula for the integral f(x) = integral of dt/sqrt(1 - t^4).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
f'(x)f'(y)f'(z) \{f(y) - f(z)\} \{f(z) - f(x)\} \{f(x) - f(y)\} = 0The condition for a functional relation between u, v, w built from f(x), f(y), f(z); it forces f to be constant.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{x_{0}}^{x_{1}} \frac{dx}{ax^{2} + 2bx + c} = \frac{1}{\sqrtp{ac - b^{2}}} \arctan\left\{ \frac{(x_{1} - x_{0}) \sqrtp{ac - b^{2}}} {ax_{1}x_{0} + b(x_{1} + x_{0}) + c} \right\}Evaluates the integral of 1/(ax^2 + 2bx + c) between x_0 and x_1 as an inverse tangent, for a > 0 and ac - b^2 > 0.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{-1}^{1} \frac{\sin\alpha\, dx}{1 - 2x\cos\alpha + x^{2}}The integral whose value, as a function of alpha, is discontinuous at multiples of pi (Ex. 34).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{x_{0}}^{x_{1}} \frac{dx}{y} = \frac{1}{\sqrt{a}} \log \frac{1 + X\sqrt{a}}{1 - X\sqrt{a}}Evaluates integral of dx/y with y = sqrt(ax^2 + 2bx + c) as a logarithm when a is positive.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{0}^{a} \frac{dx}{x + \sqrtp{a^{2} - x^{2}}} = \tfrac{1}{4}\piThe definite integral from 0 to a of 1/(x + sqrt(a^2 - x^2)) equals pi/4.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{-1}^{1} \frac{\sqrtp{1 - x^{2}}}{a - x}\, dx = \pi\{a - \sqrtp{a^{2} - 1}\}For a > 1 the integral of sqrt(1 - x^2)/(a - x) over [-1, 1] equals pi(a - sqrt(a^2 - 1)).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{0}^{1} \frac{dx}{\sqrtbr{\{1 + (p^{2} - 1)x\}\{1 - (1 - q^{2}) x\}}} = \frac{2\omega}{(p + q)\sin\omega}For p > 1 and 0 < q < 1 the integral equals 2 omega/((p+q) sin omega), where omega is the acute angle with cosine (1 + pq)/(p + q).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{0}^{2\pi} \frac{\sin^{2}\theta\, d\theta}{a - b\cos\theta} = \frac{2\pi}{b^{2}} \{a - \sqrtp{a^{2} - b^{2}}\}For a > b > 0 the integral of sin^2 theta over (a - b cos theta) from 0 to 2pi equals (2pi/b^2)(a - sqrt(a^2 - b^2)).
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{0}^{\pi} \frac{d\theta}{a + b\cos\theta + c\sin\theta} = \frac{2}{\sqrtp{a^{2} - b^{2} - c^{2}}} \arctan \left\{\frac{\sqrtp{a^{2} - b^{2} - c^{2}}}{c}\right\}For a > sqrt(b^2 + c^2) the integral over [0, pi] equals an inverse tangent expression, with the inverse tangent between 0 and pi.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\left(\int_{a}^{b} \phi\psi\, dx\right)^{2} \leq \int_{a}^{b} \phi^{2}\, dx \int_{a}^{b} \psi^{2}\, dxThe square of the integral of phi psi is at most the product of the integrals of phi^2 and psi^2.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
P_{n}(x) = \frac{1}{(\beta - \alpha)^{n} n!} \left(\frac{d}{dx}\right)^{n} \{(x - \alpha)(\beta - x)\}^{n}Definition of P_n(x) as an n-th derivative (Rodrigues-type formula) of (x - alpha)^n (beta - x)^n; it is a polynomial of degree n.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{\alpha}^{\beta} P_{n}(x)\theta(x)\, dx = 0P_n is orthogonal to every polynomial theta of degree less than n on the interval from alpha to beta.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{\alpha}^{\beta} P_{m}(x) P_{n}(x)\, dx = 0Polynomials P_m and P_n are orthogonal on [alpha, beta] when m differs from n.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{\alpha}^{\beta} (Q_{n} - \kappa P_{n})^{2}\, dx = 0Step in Ex. 45: the square of Q_n minus a multiple of P_n integrates to zero.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\int_{0}^{1} \phi(x)\, dx = \tfrac{1}{18}\{5\phi(\alpha) + 8\phi(\tfrac{1}{2}) + 5\phi(\beta)\}For a fifth-degree polynomial phi, the integral over [0, 1] is given exactly by a three-point rule with alpha and beta the roots of x^2 - x + 1/10 = 0.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
x^{2} - x + \frac{1}{10} = 0The quadratic whose roots alpha and beta are the three-point nodes of the rule in Ex. 47.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
\tfrac{1}{4}\pi = \int_{0}^{1} \frac{dx}{1 + x^{2}}pi/4 equals the integral of 1/(1 + x^2) from 0 to 1, used in Ex. 48 to approximate pi with Simpson's Rule.
ADDITIONAL THEOREMS IN THE DIFFERENTIAL AND \\ INTEGRAL CALCULUS
8.9 < \int_{3}^{5} \sqrtp{4 + x^{2}}\, dx < 9Bounds on the integral of sqrt(4 + x^2) from 3 to 5.
Problems
Exercise LXIII
Exercise LXIII, problem 10a, p. 289
Prove that $\ds\int_{0}^{\pi} \cos mx \cos nx\, dx$ and $\ds\int_{0}^{\pi} \sin mx \sin nx\, dx$ are each equal to zero except when $m = n$, when each is equal to $\frac{1}{2}\pi$; and that _0^ mx nx dx = 2nn^2 - m^2,0pt minus 3pt_0^ mx nx dx = 0, according as $n - m$ is odd or even.
Printed answer:- to zero except when $m = n$, when each is equal to $\frac{1}{2}\pi$
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Exercise LXIII, problem 10b, p. 289
Prove that $\ds\int_{0}^{\pi} \cos mx \cos nx\, dx$ and $\ds\int_{0}^{\pi} \sin mx \sin nx\, dx$ are each equal to zero except when $m = n$, when each is equal to $\frac{1}{2}\pi$; and that _0^ mx nx dx = 2nn^2 - m^2,0pt minus 3pt_0^ mx nx dx = 0, according as $n - m$ is odd or even.
Printed answer:- to zero except when $m = n$, when each is equal to $\frac{1}{2}\pi$
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Exercise LXIII, problem 10c, p. 289
Prove that $\ds\int_{0}^{\pi} \cos mx \cos nx\, dx$ and $\ds\int_{0}^{\pi} \sin mx \sin nx\, dx$ are each equal to zero except when $m = n$, when each is equal to $\frac{1}{2}\pi$; and that _0^ mx nx dx = 2nn^2 - m^2,0pt minus 3pt_0^ mx nx dx = 0, according as $n - m$ is odd or even.
Printed answer:- _0^ mx nx dx = 2nn^2 - m^2
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integrate: the printed answer does not match the problem2*n/(n**2 - m**2)
Exercise LXIII, problem 10d, p. 289
Prove that $\ds\int_{0}^{\pi} \cos mx \cos nx\, dx$ and $\ds\int_{0}^{\pi} \sin mx \sin nx\, dx$ are each equal to zero except when $m = n$, when each is equal to $\frac{1}{2}\pi$; and that _0^ mx nx dx = 2nn^2 - m^2,0pt minus 3pt_0^ mx nx dx = 0, according as $n - m$ is odd or even.
Printed answer:- _0^ mx nx dx = 0
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integrate: the printed answer does not match the problem0
Exercise LXIII, problem 1a, p. 289
Show that _a^b x^n dx = b^n+1 - a^n+1n + 1, and in particular that _0^1 x^n dx = 1n + 1.
Printed answer:- _a^b x^n dx = b^n+1 - a^n+1n + 1
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integrate: the printed answer does not match the problem(b**(n+1) - a**(n+1))/(n + 1)
Exercise LXIII, problem 1b, p. 289
Show that _a^b x^n dx = b^n+1 - a^n+1n + 1, and in particular that _0^1 x^n dx = 1n + 1.
Printed answer:- _0^1 x^n dx = 1n + 1
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Exercise LXIII, problem 2a, p. 289
$\ds\int_{a}^{b} \cos mx\, dx = \frac{\sin mb - \sin ma}{m}$, $\ds\int_{a}^{b} \sin mx\, dx = \frac{\cos ma - \cos mb}{m}$.
Printed answer:- _a^b mx dx = mb - mam
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integrate: the record may be misread(sin(m*b) - sin(m*a))/m
Exercise LXIII, problem 2b, p. 289
$\ds\int_{a}^{b} \cos mx\, dx = \frac{\sin mb - \sin ma}{m}$, $\ds\int_{a}^{b} \sin mx\, dx = \frac{\cos ma - \cos mb}{m}$.
Printed answer:- _a^b mx dx = ma - mbm
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Exercise LXIII, problem 3a, p. 289
$\ds\int_{a}^{b}\frac{dx}{1 + x^{2}} = \arctan b - \arctan a$, $\ds\int_{0}^{1}\frac{dx}{1 + x^{2}} = \tfrac{1}{4}\pi$. [There is an apparent difficulty here owing to the fact that $\arctan x$ is a many valued function. The difficulty may be avoided by observing that, in the equation _0^x dt1 + t^2 = x, $\arctan x$ must denote an angle lying between $-\frac{1}{2}\pi$ and $\frac{1}{2}\pi$. For the integral vanishes when $x = 0$ and increases steadily and continuously as $x$ increases. Thus the same is true of $\arctan x$, which therefore tends to $\tfrac{1}{2}\pi$ as $x \to \infty$. In the same way we can show that $\arctan x \to -\frac{1}{2}\pi$ as $x \to -\infty$. Similarly, in the equation _0^x dt1 - t^2 = x, where $-1 < x < 1$, $\arcsin x$ denotes an angle lying between $-\frac{1}{2}\pi$ and $\frac{1}{2}\pi$. Thus, if $a$ and $b$ are both numerically less than unity, we have _a^b dx1 - x^2 = b - a.]
Printed answer:- _a^bdx1 + x^2 = b - a
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Exercise LXIII, problem 3b, p. 289
$\ds\int_{a}^{b}\frac{dx}{1 + x^{2}} = \arctan b - \arctan a$, $\ds\int_{0}^{1}\frac{dx}{1 + x^{2}} = \tfrac{1}{4}\pi$. [There is an apparent difficulty here owing to the fact that $\arctan x$ is a many valued function. The difficulty may be avoided by observing that, in the equation _0^x dt1 + t^2 = x, $\arctan x$ must denote an angle lying between $-\frac{1}{2}\pi$ and $\frac{1}{2}\pi$. For the integral vanishes when $x = 0$ and increases steadily and continuously as $x$ increases. Thus the same is true of $\arctan x$, which therefore tends to $\tfrac{1}{2}\pi$ as $x \to \infty$. In the same way we can show that $\arctan x \to -\frac{1}{2}\pi$ as $x \to -\infty$. Similarly, in the equation _0^x dt1 - t^2 = x, where $-1 < x < 1$, $\arcsin x$ denotes an angle lying between $-\frac{1}{2}\pi$ and $\frac{1}{2}\pi$. Thus, if $a$ and $b$ are both numerically less than unity, we have _a^b dx1 - x^2 = b - a.]
Printed answer:- _0^1dx1 + x^2 = 14
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Exercise LXIII, problem 4a, p. 289
$\ds\int_{0}^{1} \frac{dx}{1 - x + x^{2}} = \frac{2\pi}{3\sqrt3}$, $\ds\int_{0}^{1} \frac{dx}{1 + x + x^{2}} = \frac{\pi}{3\sqrt3}$
Printed answer:- _0^1 dx1 - x + x^2 = 233
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integrate: the record may be misread2*pi/(3*sqrt(3))
Exercise LXIII, problem 4b, p. 289
$\ds\int_{0}^{1} \frac{dx}{1 - x + x^{2}} = \frac{2\pi}{3\sqrt3}$, $\ds\int_{0}^{1} \frac{dx}{1 + x + x^{2}} = \frac{\pi}{3\sqrt3}$
Printed answer:- _0^1 dx1 + x + x^2 = 33
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integrate: the record may be misreadpi/(3*sqrt(3))
Exercise LXIII, problem 5, p. 289
$\ds\int_{0}^{1} \frac{dx}{1 + 2x\cos\alpha + x^{2}} = \frac{\alpha}{2\sin\alpha}$ if $-\pi < \alpha < \pi$, except when $\alpha = 0$, when the value of the integral is $\frac{1}{2}$, which is the limit of $\frac{1}{2}\alpha\cosec\alpha$ as $\alpha \to 0$.
Printed answer:- 2
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integrate: the printed answer does not match the problemalpha/(2*sin(alpha))
Exercise LXIII, problem 6a, p. 289
$\ds\int_{0}^{\DPtypo{}{1}} \sqrtp{1 - x^{2}}\, dx = \tfrac{1}{4}\pi$, $\ds\int_{0}^{a} \sqrtp{a^{2} - x^{2}}\, dx = \tfrac{1}{4}\pi a^{2}$0pt minus 3pt $(a > 0)$.
Printed answer:- _0^ 1 - x^2 dx = 14
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integrate: the record may be misreadpi/4
Exercise LXIII, problem 6b, p. 289
$\ds\int_{0}^{\DPtypo{}{1}} \sqrtp{1 - x^{2}}\, dx = \tfrac{1}{4}\pi$, $\ds\int_{0}^{a} \sqrtp{a^{2} - x^{2}}\, dx = \tfrac{1}{4}\pi a^{2}$0pt minus 3pt $(a > 0)$.
Printed answer:- _0^a a^2 - x^2 dx = 14a^2
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integrate: the record may be misreadpi*a**2/4
Exercise LXIII, problem 7, p. 289
$\ds\int_{0}^{\pi} \frac{dx}{a + b\cos x} = \frac{\pi}{\sqrt{a^{2} - b^{2}}}$, if $a > |b|$. [For the form of the indefinite integral see liii. 3, 4. If $|a| < |b|$ then the subject of integration has an infinity between $0$ and $\pi$. What is the value of the integral when $a$ is negative and $-a > |b|$?]
Printed answer:- a^2 - b^2
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integrate: the record may be misreadpi/sqrt(a**2 - b**2)
Exercise LXIII, problem 8, p. 289
$\ds\int_{0}^{\frac{1}{2}\pi} \frac{dx}{a^{2}\cos^{2}x + b^{2}\sin^{2}x} = \frac{\pi}{2ab}$, if $a$ and $b$ are positive. What is the value of the integral when $a$ and $b$ have opposite signs, or when both are negative?
Printed answer:- 2ab
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integrate: the printed answer does not match the problempi/(2*a*b)
Exercise LXIII, problem 9a, p. 289
**’s integrals.** Prove that if $m$ and $n$ are positive integers then _0^2 mx nx dx is always equal to zero, and _0^2 mx nx dx,0pt minus 3pt_0^2 mx nx dx are equal to zero unless $m = n$, when each is equal to $\pi$.
Printed answer:- is always equal to zero
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Exercise LXIII, problem 9b, p. 289
**’s integrals.** Prove that if $m$ and $n$ are positive integers then _0^2 mx nx dx is always equal to zero, and _0^2 mx nx dx,0pt minus 3pt_0^2 mx nx dx are equal to zero unless $m = n$, when each is equal to $\pi$.
Printed answer:- _0^2 mx nx dx
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Exercise LXIII, problem 9c, p. 289
**’s integrals.** Prove that if $m$ and $n$ are positive integers then _0^2 mx nx dx is always equal to zero, and _0^2 mx nx dx,0pt minus 3pt_0^2 mx nx dx are equal to zero unless $m = n$, when each is equal to $\pi$.
Printed answer:- _0^2 mx nx dx
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Exercise LXIV
Exercise LXIV, problem 1, p. 290
Evaluate $\ds\int_{a}^{b} x\, dx$ by dividing $\DPmod{(a, b)}{[a, b]}$ into $n$ equal parts by the points of division $a = x_{0}$, $x_{1}$, $x_{2}$, …, $x_{n} = b$, and calculating the limit as $n \to \infty$ of (x_1 - x_0)f(x_0) + (x_2 - x_1)f(x_1) + …+ (x_n - x_n-1)f(x_n-1).
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Exercise LXIV, problem 2, p. 290
Calculate $\ds\int_{a}^{b} x^{2}\, dx$ in the same way.
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Exercise LXIV, problem 3a, p. 290
Calculate $\ds\int_{a}^{b} x\, dx$, where $0 < a < b$, by dividing $\DPmod{(a, b)}{[a, b]}$ into $n$ parts by the points of division $a$, $ar$, $ar^{2}$, … $ar^{n-1}$, $ar^{n}$, where $r^{n} = b/a$. Apply the same method to the more general integral $\ds\int_{a}^{b} x^{m}\, dx$.
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Exercise LXIV, problem 3b, p. 290
Calculate $\ds\int_{a}^{b} x\, dx$, where $0 < a < b$, by dividing $\DPmod{(a, b)}{[a, b]}$ into $n$ parts by the points of division $a$, $ar$, $ar^{2}$, … $ar^{n-1}$, $ar^{n}$, where $r^{n} = b/a$. Apply the same method to the more general integral $\ds\int_{a}^{b} x^{m}\, dx$.
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Exercise LXIV, problem 4a, p. 290
Calculate $\ds\int_{a}^{b}\cos mx\, dx$ and $\ds\int_{a}^{b}\sin mx\, dx$ by the method of Ex. 1.
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Exercise LXIV, problem 4b, p. 290
Calculate $\ds\int_{a}^{b}\cos mx\, dx$ and $\ds\int_{a}^{b}\sin mx\, dx$ by the method of Ex. 1.
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Exercise LXIV, problem 5, p. 290
Prove that $n\sum\limits_{r=0}^{n-1} \dfrac{1}{n^{2} + r^{2}} \to \tfrac{1}{4}\pi$ as $n \to \infty$.
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Exercise LXIV, problem 6, p. 290
Prove that $\dfrac{1}{n^{2}} \sum\limits_{r=0}^{n-1} \sqrtp{n^{2} - r^{2}} \to \tfrac{1}{4}\pi$.
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Exercise LXV
Exercise LXV, problem 10, p. 293
Prove that [ tfrac12 < int_0^1 fracdxsqrtp4 - x^2 + x^3 < tfrac16pi. ]
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Exercise LXV, problem 11, p. 293
Prove that $(3x + 8)/16 < 1/\\sqrtp{4 - 3x + x^{3}} < 1/\\sqrtp{4 - 3x}$ if $0 < x < 1$, and hence that [ tfrac1932 < int_0^1 fracdxsqrtp4 - 3x + x^3 < tfrac23. ]
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Exercise LXV, problem 12, p. 293
Prove that [ .573 < int_1^2 fracdxsqrtp4 - 3x + x^3 < .595. ]
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Exercise LXV, problem 13, p. 293
If $\alpha$ and $\phi$ are positive acute angles then < _0^ dx1 - ^2^2 x < 1 - ^2^2. If $\alpha = \phi = \frac{1}{6}\pi$, then the integral lies between $.523$ and $.541$.
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Exercise LXV, problem 14, p. 293
Prove that [ left|int_a^b f(x), dxright| leq int_a^b|f(x)|, dx. ]
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Exercise LXV, problem 15, p. 293
If $|f(x)| \\leq M$, then [ left|int_a^b f(x)phi(x), dxright| leq Mint_a^b|phi(x)|, dx. ]
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Exercise LXV, problem 1a, p. 293
Show, by means of the direct definition of the definite integral, and equations Eq(1)--Eq(5) above, that CenterLineItemp(i)$\\ds\\int_{-a}^{a} \\phi(x^{2})\\, dx = 2\\int_{0}^{a} \\phi(x^{2})\\, dx$,quad $\\ds\\int_{-a}^{a} x\\phi(x^{2})\\, dx = 0$; CenterLineItemp(ii)$\\ds\\int_{0}^{\\frac{1}{2}\\pi} \\phi(\\cos x)\\, dx = \\int_{0}^{\\frac{1}{2} \\pi} \\phi(\\sin x)\\, dx = \\tfrac{1}{2} \\int_{0}^{\\pi} \\phi(\\sin x)\\, dx$; CenterLineItemp(iii)$\\ds\\int_{0}^{m\\pi} \\phi(\\cos^{2} x)\\, dx = m\\int_{0}^{\\pi} \\phi(\\cos^{2} x)\\, dx$, $m$ being an integer.
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Exercise LXV, problem 1b, p. 293
Show, by means of the direct definition of the definite integral, and equations Eq(1)--Eq(5) above, that CenterLineItemp(i)$\\ds\\int_{-a}^{a} \\phi(x^{2})\\, dx = 2\\int_{0}^{a} \\phi(x^{2})\\, dx$,quad $\\ds\\int_{-a}^{a} x\\phi(x^{2})\\, dx = 0$; CenterLineItemp(ii)$\\ds\\int_{0}^{\\frac{1}{2}\\pi} \\phi(\\cos x)\\, dx = \\int_{0}^{\\frac{1}{2} \\pi} \\phi(\\sin x)\\, dx = \\tfrac{1}{2} \\int_{0}^{\\pi} \\phi(\\sin x)\\, dx$; CenterLineItemp(iii)$\\ds\\int_{0}^{m\\pi} \\phi(\\cos^{2} x)\\, dx = m\\int_{0}^{\\pi} \\phi(\\cos^{2} x)\\, dx$, $m$ being an integer.
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Exercise LXV, problem 1c, p. 293
Show, by means of the direct definition of the definite integral, and equations Eq(1)--Eq(5) above, that CenterLineItemp(i)$\\ds\\int_{-a}^{a} \\phi(x^{2})\\, dx = 2\\int_{0}^{a} \\phi(x^{2})\\, dx$,quad $\\ds\\int_{-a}^{a} x\\phi(x^{2})\\, dx = 0$; CenterLineItemp(ii)$\\ds\\int_{0}^{\\frac{1}{2}\\pi} \\phi(\\cos x)\\, dx = \\int_{0}^{\\frac{1}{2} \\pi} \\phi(\\sin x)\\, dx = \\tfrac{1}{2} \\int_{0}^{\\pi} \\phi(\\sin x)\\, dx$; CenterLineItemp(iii)$\\ds\\int_{0}^{m\\pi} \\phi(\\cos^{2} x)\\, dx = m\\int_{0}^{\\pi} \\phi(\\cos^{2} x)\\, dx$, $m$ being an integer.
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Exercise LXV, problem 2, p. 293
Prove that $\ds\int_{0}^{\pi} \frac{\sin nx}{\sin x}\, dx$ is equal to $\pi$ or to $0$ according as $n$ is odd or or even.
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Exercise LXV, problem 3, p. 293
Prove that $\ds\int_{0}^{\pi} \sin nx \cot x\, dx$ is equal to $0$ or to $\pi$ according as $n$ is odd or even.
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Exercise LXV, problem 4, p. 293
If $\phi(x) = a_{0} + a_{1}\cos x + b_{1}\sin x + a_{2}\cos 2x + \dots + a_{n}\cos nx + b_{n}\sin nx$, and $k$ is a positive integer not greater than $n$, then _0^2 (x) dx = 2a_0,0pt minus 3pt_0^2 kx (x) dx = a_k,0pt minus 3pt_0^2 kx (x) dx = b_k. If $k > n$ then the value of each of the last two integrals is zero.
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Exercise LXV, problem 5, p. 293
If $\phi(x) = a_{0} + a_{1} \cos x + a_{2}\cos 2x + \dots + a_{n}\cos nx$, and $k$ is a positive integer not greater than $n$, then _0^ (x) dx = a_0,0pt minus 3pt_0^ kx (x) dx = 12a_k. If $k > n$ then the value of the last integral is zero.
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Exercise LXV, problem 6, p. 293
Prove that if $a$ and $b$ are positive then [ int_0^2pi fracdxa^2cos^2 x + b^2sin^2 x = frac2piab. ]
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Exercise LXV, problem 7, p. 293
If $f(x) \leq \phi(x)$ when $a \leq x \leq b$, then $\ds\int_{a}^{b} f\, dx \leq \int_{a}^{b}\phi\, dx$.
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Exercise LXV, problem 8, p. 293
Prove that beginalignat*2 0 &< int_0^frac12pi sin^n+1x, dx &&< int_0^frac12pi sin^nx, dx, 0 &< int_0^frac14pi tan^n+1x, dx &&< int_0^frac14pi tan^nx, dx. endalignat*
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Exercise LXV, problem 9, p. 293
If $n > 1$ then [ .5 < int_0^frac12 fracdxsqrtp1 - x^2n < .524. ]
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Exercise LXVI
Exercise LXVI, problem 1, p. 295
Prove that _a^b x f”(x) dx = bf’(b) - f(b) - af’(a) - f(a).
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Exercise LXVI, problem 10, p. 295
Deduce that $u_{n}$ is equal to 2·4·6 …(n - 1)3·5·7 …n,0pt minus 3pt121·3·5 …(n - 1)2·4·6 …n, according as $n$ is odd or even.
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Exercise LXVI, problem 11, p. 295
**Second Mean Value Theorem.** If $f(x)$ is a function of $x$ which has a differential coefficient of constant sign for all values of $x$ from $x = a$ to $x = b$, then there is a number $\xi$ between $a$ and $b$ such that _a^b f(x)(x) dx = f(a) _a^ (x) dx + f(b) _^b (x) dx.
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Exercise LXVI, problem 12a, p. 295
**’s form of the Second Mean Value Theorem.** If $f'(x)$ is of constant sign, and $f(b)$ and $f(a) - f(b)$ have the same sign, then _a^b f(x)(x) dx = f(a) _a^X (x) dx, where $X$ lies between $a$ and $b$.
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Exercise LXVI, problem 12b, p. 295
Prove similarly that if $f(a)$ and $f(b) - f(a)$ have the same sign, then _a^b f(x)(x) dx = f(b) _X^b (x) dx, where $X$ lies between $a$ and $b$.
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Exercise LXVI, problem 13, p. 295
Prove that |_X^X’ xx dx| < 2X if $X' > X > 0$.
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Exercise LXVI, problem 14, p. 295
Establish the results of % [examples:lxv]Ex. lxv%. 1 by means of the rule for substitution.
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Exercise LXVI, problem 15, p. 295
Prove that _a^b F(x) dx = _a^b F(a + b - x) dx.
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Exercise LXVI, problem 16, p. 295
Prove that _0^12 ^m x^m x dx = 2^-m _0^12 ^m x dx.
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Exercise LXVI, problem 17, p. 295
Prove that _0^ x(x) dx = 12_0^ (x) dx.
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Exercise LXVI, problem 18, p. 295
Prove that _0^ xx1 + ^2 x dx = 14^2.
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Exercise LXVI, problem 19, p. 295
Show by means of the transformation $x = a\cos^{2}\theta + b\sin^{2}\theta$ that _a^b (x - a)(b - x) dx = 18(b - a)^2.
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Exercise LXVI, problem 2, p. 295
More generally, _a^b x^m f^(m+1)(x) dx = F(b) - F(a), where multline* F(x) = x^m f^(m)(x) - mx^m-1 f^(m-1)x + m(m - 1)x^m-2 f^(m-2)x - … + (-1)^m m! f(x). multline*
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Exercise LXVI, problem 20, p. 295
Show by means of the substitution $(a + b\cos x) (a - b\cos y) = a^{2} - b^{2}$ that _0^ (a + bx)^-n dx = (a^2 - b^2)^-(n - 12) _0^ (a - by)^n-1 dy, when $n$ is a positive integer and $a > |b|$, and evaluate the integral when $n = 1$, $2$, $3$.
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Exercise LXVI, problem 21, p. 295
If $m$ and $n$ are positive integers then _a^b (x - a)^m (b - x)^n dx = (b - a)^m+n+1 m! n!(m + n + 1)!.
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Exercise LXVI, problem 3a, p. 295
Prove that _0^1 x dx = 12- 1,0pt minus 3pt_0^1xx dx = 14- 12.
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Exercise LXVI, problem 3b, p. 295
Prove that _0^1 x dx = 12- 1,0pt minus 3pt_0^1xx dx = 14- 12.
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Exercise LXVI, problem 4, p. 295
Prove that if $a$ and $b$ are positive then _0^12 xxx dx(a^2^2x + b^2^2x)^2 = 4ab^2(a + b).
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Exercise LXVI, problem 5, p. 295
If f_1(x) = _0^xf(t) dt,0pt minus 3ptf_2(x) = _0^xf_1(t) dt, …,0pt minus 3ptf_k(x) = _0^x f_k-1(t) dt, then f_k(x) = 1(k - 1)! _0^x f(t)(x - t)^k-1 dt.
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Exercise LXVI, problem 6, p. 295
Prove by integration by parts that if u_m, n = _0^1 x^m (1 - x)^n dx, where $m$ and $n$ are positive integers, then $(m + n + 1) u_{m, n} = nu_{m, n-1}$, and deduce that u_m, n = m! n!(m + n + 1)!.
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Exercise LXVI, problem 7, p. 295
Prove that if u_n = _0^14 ^nx dx then $u_{n} + u_{n-2} = 1/(n - 1)$. Hence evaluate the integral for all positive integral values of $n$.
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Exercise LXVI, problem 8, p. 295
Deduce from the last example that $u_{n}$ lies between $1/\{2(n - 1)\}$ and $1/\{2(n + 1)\}$.
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Exercise LXVI, problem 9, p. 295
Prove that if u_n = _0^12 ^n x dx then $u_{n} = \{(n - 1)/n\} u_{n-2}$. [Write $\sin^{n-1}x\sin x$ for $\sin^{n}x$ and integrate by parts.]
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Exercise Misc-VII
Exercise Misc-VII, problem None, p. 300
The record holds no text for this problem.
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Exercise LX
Exercise LX, problem 1, p. 275
0.375em plus 0.75em minus 0.25emProve that if $x = r\cos\theta$, $y = r\sin\theta$, so that $r = \sqrtp{x^{2} + y^{2}}$, $\theta = \arctan(y/x)$, then align* rx &= xx^2 + y^2, &ry &= yx^2 + y^2, &x &= -yx^2 + y^2, &y &= xx^2 + y^2, % xr &= , &yr &= , &x &= -r, &y &= r. align*
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Exercise LX, problem 2, p. 275
Account for the fact that $\dfrac{\dd r}{\dd x}\neq 1\bigg/\biggl(\dfrac{\dd x}{\dd r}\biggr)$ and $\dfrac{\dd \theta}{\dd x}\neq 1\bigg/\biggl(\dfrac{\dd x}{\dd \theta}\biggr)$. [When we were considering a function $y$ of one variable $x$ it followed from the definitions that $dy/dx$ and $dx/dy$ were reciprocals. This is no longer the [pg]276 case when we are dealing with functions of two variables. Let $P$ ([fig:46]Fig. 46) be the point $(x, y)$ or $(r, \theta)$. To find $\dd r/\dd x$ we must increase $x$, say by an increment $MM_{1} = \delta x$, while keeping $y$ constant. This brings $P$ to $P_{1}$. If along $OP_{1}$ we take $OP' = OP$, the increment of $r$ is $P'P_{1} = \delta r$, say; and $\dd r/\dd x = \lim(\delta r/\delta x)$. If on the other hand we want to calculate $\dd x/\dd r$, $x$ and $y$ %[Illustration: Fig. 46.] [2.25in]46p276 being now regarded as functions of $r$ and $\theta$, we must increase $r$ by $\Delta r$, say, keeping $\theta$ constant. This brings $P$ to $P_{2}$, where $PP_{2} = \Delta r$: the corresponding increment of $x$ is $MM_{1} = \Delta x$, say; and x/r = (x/r). Now $\Delta x = \delta x$: Of course the fact that $\Delta x = \delta x$ is due merely to the particular value of $\Delta r$ that we have chosen (viz. $PP_{2}$). Any other choice would give us values of $\Delta x$, $\Delta r$ proportional to those used here. but $\Delta r \neq \delta r$. Indeed it is easy to see from the figure that (r/x) = (P’P_1/PP_1) = , but (r/x) = (PP_2/PP_1) = , so that (r/r) = ^2. The fact is of course that *$\dd x/\dd r$ and $\dd r/\dd x$ are not formed upon the same hypothesis as to the variation of $P$.*]
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Exercise LX, problem 3, p. 275
Prove that if $z = f(ax + by)$ then $b(\dd z/\dd x) = a(\dd z/\dd y)$.
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Exercise LX, problem 4, p. 275
Find $\dd X/\dd x$, $\dd X/\dd y$, … when $X + Y = x$, $Y = xy$. Express $x$, $y$ as functions of $X$, $Y$ and find $\dd x/\dd X$, $\dd x/\dd Y$, ….
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Exercise LX, problem 5, p. 275
Find $\dd X/\dd x$, … when $X + Y + Z = x$, $Y + Z = xy$, $Z = xyz$; express $x$, $y$, $z$ in terms of $X$, $Y$, $Z$ and find $\dd x/\dd X$, ….
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Exercise LXI
Exercise LXI, problem 1, p. 277
Suppose $\phi(t) = (1 - t^{2})/(1 + t^{2})$, $\psi(t) = 2t/(1 + t^{2})$, so that the locus of $(x, y)$ is the circle $x^{2} + y^{2} = 1$. Then align* ’(t) &= -4t/(1 + t^2)^2,0pt minus 3pt’(t) = 2(1 - t^2)/(1 + t^2)^2, F’(t) &= -4t/(1 + t^2)^2f_x’ + 2(1 - t^2)/(1 + t^2)^2f_y’, align* where $x$ and $y$ are to be put equal to $(1 - t^{2})/(1 + t^{2})$ and $2t/(1 + t^{2})$ after carrying out the differentiations. [pg]278 0.375em plus 0.75em minus 0.25emWe can easily verify this formula in particular cases. Suppose, *e.g.*, that $f(x, y) = x^{2} + y^{2}$. Then $f_{x}' = 2x$, $f_{y}' = 2y$, and it is easily verified that $F'(t) = 2x\phi'(t) + 2y\psi'(t) = 0$, which is obviously correct, since $F(t) = 1$.
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Exercise LXI, problem 2a, p. 277
Verify the theorem in the same way when (*a*) $x = t^{m}$, $y = 1 - t^{m}$, $f(x, y) = x + y$; (*b*) $x = a\cos t$, $y = a\sin t$, $f(x, y) = x^{2} + y^{2}$.
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Exercise LXI, problem 2b, p. 277
Verify the theorem in the same way when (*a*) $x = t^{m}$, $y = 1 - t^{m}$, $f(x, y) = x + y$; (*b*) $x = a\cos t$, $y = a\sin t$, $f(x, y) = x^{2} + y^{2}$.
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Exercise LXI, problem 3, p. 277
One of the most important cases is that in which $t$ is $x$ itself. We then obtain D_xfx, (x) = D_xf(x, y) + D_yf(x, y)’(x). where $y$ is to be replaced by $\psi(x)$ after differentiation. It was this case which led to the introduction of the notation $\dd f/\dd x$, $\dd f/\dd y$. For it would seem natural to use the notation $df/dx$ for *either* of the functions $D_{x}f\{x, \psi(x)\}$ and $D_{x}f(x, y)$, in one of which $y$ is put equal to $\psi(x)$ before and in the other after differentiation. Suppose for example that $y = 1 - x$ and $f(x, y) = x + y$. Then $D_{x}f(x, 1 - x) = D_{x}1 = 0$, but $D_{x}f(x, y) = 1$. The distinction between the two functions is adequately shown by denoting the first by $df/dx$ and the second by $\dd f/\dd x$, in which case the theorem takes the form dfdx = fx + fy dydx; though this notation is also open to objection, in that it is a little misleading to denote the functions $f\{x, \psi(x)\}$ and $f(x, y)$, whose forms as functions of $x$ are quite different from one another, by the same letter $f$ in $df/dx$ and $\dd f/\dd x$.
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Exercise LXI, problem 4, p. 277
If the result of eliminating $t$ between $x = \phi(t)$, $y = \psi(t)$ is $f(x, y) = 0$, then fx dxdt + fy dydt = 0.
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Exercise LXI, problem 5, p. 277
If $x$ and $y$ are functions of $t$, and $r$ and $\theta$ are the polar coordinates of $(x, y)$, then $r' = (xx' + yy')/r$, $\theta' = (xy' - yx')/r^{2}$, dashes denoting differentiations with respect to $t$.
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Exercise LXII
Exercise LXII, problem 1, p. 281
The area of an ellipse is given by $A = \pi ab$, where $a$, $b$ are the semiaxes. Prove that dAA = daa + dbb, and state the corresponding approximate equation connecting the increments of the axes and the area.
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Exercise LXII, problem 2, p. 281
Express $\Delta$, the area of a triangle $ABC$, as a function of (i) $a$, $B$, $C$, (ii) $A$, $b$, $c$, and (iii) $a$, $b$, $c$, and establish the formulae gather* d = 2daa + c dBaB + b dCaC,0pt minus 3ptd = A dA + dbb + dcc, d= R(A da + B db + C dc), gather* %[** TN: Sole instance of circumcircle, not hyphenated in the original] where $R$ is the radius of the circumcircle.
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Exercise LXII, problem 3, p. 281
The sides of a triangle vary in such a way that the area remains constant, so that $a$ may be regarded as a function of $b$ and $c$. Prove that ab = -BA,0pt minus 3ptac = -CA. [This follows from the equations da = ab db + ac dc,0pt minus 3ptA da + B db + C dc = 0.
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Exercise LXII, problem 4, p. 281
If $a$, $b$, $c$ vary so that $R$ remains constant, then daA + dbB + dcC = 0, and so ab = -AB,0pt minus 3ptac = -AC. [Use the formulae $a = 2R\sin A$, …, and the facts that $R$ and $A + B + C$ are constant.]
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Exercise LXII, problem 5, p. 281
If $z$ is a function of $u$ and $v$, which are functions of $x$ and $y$, then zx = zu ux + zv vx,0pt minus 3ptzy = zu uy + zv vy. [We have dz = zu du + zv dv,0pt minus 3ptdu = ux dx + uy dy,0pt minus 3ptdv = vx dx + vy dy. Substitute for $du$ and $dv$ in the first equation and compare the result with the equation dz = zx dx + zy dy.]
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Exercise LXII, problem 6, p. 281
Let $z$ be a function of $x$ and $y$, and let $X$, $Y$, $Z$ be defined by the equations x = a_1 X + b_1 Y + c_1 Z,0pt minus 3pty = a_2 X + b_2 Y + c_2 Z,0pt minus 3ptz = a_3 X + b_3 Y + c_3 Z. Then $Z$ may be expressed as a function of $X$ and $Y$. Express $\dd Z/\dd X$, $\dd Z/\dd Y$ in terms of $\dd z/\dd x$, $\dd z/\dd y$. [Let these differential coefficients be denoted by $P$, $Q$ and $p$, $q$. Then $dz - p\, dx - q\, dy = 0$, or (c_1 p + c_2 q - c_3) dZ + (a_1 p + a_2 q - a_3) dX + (b_1 p + b_2 q - b_3) dY = 0. [pg]283 Comparing this equation with $dZ - P\, dX - Q\, dY = 0$ we see that P = -a_1p + a_2q - a_3c_1p + c_2q - c_3,0pt minus 3ptQ = -b_1p + b_2q - b_3c_1p + c_2q - c_3.]
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Exercise LXII, problem 7, p. 281
If (a_1 x + b_1 y + c_1 z)p + (a_2 x + b_2 y + c_2 z)q = a_3 x + b_3 y + c_3 z, then (a_1 X + b_1 Y + c_1 Z) P + (a_2 X + b_2 Y + c_2 Z) Q = a_3 X + b_3 Y + c_3 Z. % [0]% (*Math. Trip.* 1899.)% [1]%
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Exercise LXII, problem 8, p. 281
**of implicit functions.** Suppose that $f(x, y)$ and its derivative $f_{y}'(x, y)$ are continuous in the neighbourhood of the point $(a, b)$, and that f(a, b) = 0,0pt minus 3ptf_b’(a, b) 0. Then we can find a neighbourhood of $(a, b)$ throughout which $f_{y}'(x, y)$ has always the same sign. Let us suppose, for example, that $f_{y}'(x, y)$ is positive near $(a, b)$. Then $f(x, y)$ is, for any value of $x$ sufficiently near to $a$, and for values of $y$ sufficiently near to $b$, an increasing function of $y$ in the stricter sense of [§]95. It follows, by the theorem of [§]108, that there is a unique continuous function $y$ which is equal to $b$ when $x = a$ and which satisfies the equation $f(x, y) = 0$ for all values of $x$ sufficiently near to $a$. Let us now suppose that $f(x, y)$ possesses a derivative $f_{x}'(x, y)$ which is also continuous near $(a, b)$. If $f(x, y) = 0$, $x = a + h$, $y = b + k$, we have 0 = f(x, y) - f(a, b) = (f_a’ + ) h + (f_b’ + ) k, where $\DPtypo{}{\epsilon}$ and $\eta$ tend to zero with $h$ and $k$. Thus kh = -f_a’ + f_b’ + -f_a’f_b’, or dydx = -f_a’f_b’.
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Exercise LXII, problem 9, p. 281
The equation of the tangent to the curve $f(x, y) = 0$, at the point $x_{0}$, $y_{0}$, is (x - x_0) f_x_0’(x_0, y_0) + (y - y_0) f_y_0’(x_0, y_0) = 0.
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Exercise LV
Exercise LV, problem 1, p. 264
Suppose that $f(x)$ is a polynomial of degree $r$. Then $f^{(n)}(x)$ is identically zero when $n > r$, and the theorem leads to the algebraical identity f(a + h) = f(a) + hf’(a) + h^22! f”(a) + … + h^rr! f^(r)(a).
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Exercise LV, problem 10, p. 264
Show that the error in taking the root to be $\xi - (f/f') - \frac{1}{2}(f^{2}f''/f'^{3})$, where $\xi$ is the argument of every function, is in general of the third order.
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Exercise LV, problem 11, p. 264
The equation $\sin x = \alpha x$, where $\alpha$ is small, has a root nearly equal to $\pi$. Show that $(1 - \alpha)\pi$ is a better approximation, and $(1 - \alpha + \alpha^{2})\pi$ a better still. [The method of Exs. 7--10 does not depend on $f(x) = 0$ being an algebraical equation, so long as $f'$ and $f''$ are continuous.]
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Exercise LV, problem 12, p. 264
Show that the limit when $h \to 0$ of the number $\theta_{n}$ which occurs in the general Mean Value Theorem is $1/(n + 1)$, provided that $f^{(n+1)}(x)$ is continuous. [For $f(x + h)$ is equal to each of f(x) + …+ h^nn! f^(n)(x + _nh),0pt minus 3ptf(x) + …+ h^nn! f^(n)(x) + h^n+1(n + 1)! f^(n+1)(x + _n+1h), where $\theta_{n+1}$ as well as $\theta_{n}$ lies between $0$ and $1$. Hence f^(n)(x + _nh) = f^(n)(x) + hf^(n+1)(x + _n+1h)n + 1 But if we apply the original Mean Value Theorem to the function $f^{(n)}(x)$, taking $\theta_{n}h$ in place of $h$, we find f^(n)(x + _nh) = f^(n)(x) + _nhf^(n+1)(x + _nh), [pg]266 where $\theta$ also lies between $0$ and $1$. Hence _n f^(n+1)(x + _n h) = f^(n+1)(x + _n+1 h)n + 1, from which the result follows, since $f^{(n+1)}(x + \theta\theta_{n} h)$ and $f^{(n+1)}(x + \theta_{n+1} h)$ tend to the same limit $f^{(n+1)}(x)$ as $h \to 0$.]
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Exercise LV, problem 13, p. 264
Prove that $\{f(x + 2h) - 2f(x + h) + f(x)\}/h^{2} \to f''(x)$ as $h \to 0$, provided that $f''(x)$ is continuous. [Use equation (2) of [§]147.]
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Exercise LV, problem 14, p. 264
Show that, if the $f^{(n)}(x)$ is continuous for $x = 0$, then f(x) = a_0 + a_1x + a_2x^2 + …+ (a_n + _x) x^n, where $a_{r} = f^{(r)}(0)/r!$ and $\epsilon_{x} \to 0$ as $x \to 0$. It is in fact sufficient to suppose that *$f^{(n)}(0)$ exists*. See R. H. Fowler, “The elementary differential geometry of plane curves” (*Cambridge Tracts in Mathematics*, No. 20, p. 104).266
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Exercise LV, problem 15, p. 264
Show that if a_0 + a_1x + a_2x^2 + …+ (a_n + _x) x^n = b_0 + b_1x + b_2x^2 + …+ (b_n + _x) x^n, where $\epsilon_{x}$ and $\eta_{x}$ tend to zero as $x \to 0$, then $a_{0} = b_{0}$, $a_{1} = b_{1}$, …, $a_{n} = b_{n}$. [Making $x \to 0$ we see that $a_{0} = b_{0}$. Now divide by $x$ and afterwards make $x \to 0$. We thus obtain $a_{1} = b_{1}$; and this process may be repeated as often as is necessary. It follows that if $f(x) = a_{0} + a_{1}x + a_{2}x^{2} + \dots + (a_{n} + \epsilon_{x}) x^{n}$, and the first $n$ derivatives of $f(x)$ are continuous, then $a_{r} = f^{(r)}(0)/r!$.]
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Exercise LV, problem 2, p. 264
By applying the theorem to $f(x) = 1/x$, and supposing $x$ and $x + h$ positive, obtain the result 1x + h = 1x - hx^2 + h^2x^3 - … + (-1)^n-1 h^n-1x^n + (-1)^n h^n(x + _n h)^n+1. [Since 1x + h = 1x - hx^2 + h^2x^3 - … + (-1)^n-1 h^n-1x^n + (-1)^n h^nx^n(x + h),0pt minus 3pt%[** TN: Quick spacing hack] we can verify the result by showing that $x^{n}(x + h)$ can be put in the form $(x + \theta_{n}h)^{n+1}$, or that $x^{n+1} < x^{n}(x + h) < (x + h)^{n+1}$, as is evidently the case.]
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Exercise LV, problem 3, p. 264
Obtain the formula multline* (x + h) = x + hx - h^22!x - h^33!x + … + (-1)^n-1h^2n-1(2n - 1)!x + (-1)^n h^2n2n!(x + _2n h), multline* the corresponding formula for $\cos(x + h)$, and similar formulae involving powers of $h$ extending up to $h^{2n+1}$.
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Exercise LV, problem 4, p. 264
Show that if $m$ is a positive integer, and $n$ a positive integer not greater than $m$, then (x + h)^m = x^m + m1x^m-1 h + … + mn - 1x^m-n+1 h^n-1 + mn(x + _n h)^m-n h^n. Show also that, if the interval $\DPmod{(x, x + h)}{[x, x + h]}$ does not include $x = 0$, the formula holds for all real values of $m$ and all positive integral values of $n$; and that, even if $x < 0 < x + h$ or $x + h < 0 < x$, the formula still holds if $m - n$ is positive.
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Exercise LV, problem 5, p. 264
The formula $f(x + h) = f(x) + hf'(x + \theta_{1}h)$ is not true if $f(x) = 1/x$ and $x < 0 < x + h$. [For $f(x + h) - f(x) > 0$ and $hf'(x + \theta_{1} h) = -h/(x + \theta_{1} h)^{2} < 0$; it is evident that the conditions for the truth of the Mean Value Theorem are not satisfied.]
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Exercise LV, problem 6, p. 264
If $x = -a$, $h = 2a$, $f(x) = x^{1/3}$, then the equation f(x + h) = f(x) + hf’(x + _1 h) is satisfied by $\theta_{1} = \frac{1}{2} ± \frac{1}{18}\sqrt{3}$. [This example shows that the result of the theorem may hold even if the conditions under which it was proved are not satisfied.]
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Exercise LV, problem 7, p. 264
**’s method of approximation to the roots of equations.** Let $\xi$ be an approximation to a root of an algebraical equation $f(x) = 0$, the actual root being $\xi + h$. Then 0 = f(+ h) = f() + hf’() + 12 h^2f”(+ _2h), so that h = -f()f’() - 12 h^2 f”(+ _2h)f’(). It follows that in general a better approximation than $x = \xi$ is x = - f()f’(). If the root is a simple root, so that $f'(\xi + h) \neq 0$, we can, when $h$ is small enough, find a positive constant $K$ such that $|f'(x)| > K$ for all the values of $x$ which we are considering, and then, if $h$ is regarded as of the first order of smallness, $f(\xi)$ is of the first order of smallness, and the error in taking $\xi - \{f(\xi)/f'(\xi)\}$ as the root is of the second order.
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Exercise LV, problem 8, p. 264
Apply this process to the equation $x^{2} = 2$, taking $\xi = 3/2$ as the first approximation. [We find $h = -1/12$, $\xi + h = 17/12 = 1.417\dots$, which is quite a good approximation, in spite of the roughness of the first. If now we repeat the process, taking $\xi = 17/12$, we obtain $\xi + h = 577/408 = 1.414\MS215\dots$, which is correct to $5$ places of decimals.
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Exercise LV, problem 9, p. 264
By considering in this way the equation $x^{2} - 1 - y = 0$, where $y$ is small, show that $\sqrtp{1 + y} = 1 + \frac{1}{2} y - \{\frac{1}{4}y^{2}/(2 + y)\}$ approximately, the error being of the fourth order.
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Exercise LVI
Exercise LVI, problem 1, p. 267
Let $f(x) = \sin x$. Then all the derivatives of $f(x)$ are continuous for all values of $x$. Also $|f^{n}(x)| \leq 1$ for all values of $x$ and $n$. Hence in this case $|R_{n}| \leq h^{n}/n!$, which tends to zero as $n \to \infty$ (% [examples:xxvii]Ex. xxvii%. 12) whatever value $h$ may have. It follows that (x + h) = x + hx - h^22!x - h^33!x + h^44!x + …, for all values of $x$ and $h$. In particular h = h - h^33! + h^55! - …, for all values of $h$. Similarly we can prove that (x + h) = x - hx - h^22!x + h^33! x + …,0pt minus 3pth = 1 - h^22! + h^44! - ….
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Exercise LVI, problem 2, p. 267
**Binomial Series.** Let $f(x) = (1 + x)^{m}$, where $m$ is any rational number, positive or negative. Then $f^{(n)}(x) = m(m - 1) \dots (m - n + 1) (1 + x)^{m-n}$ and Maclaurin’s Series takes the form (1 + x)^m = 1 + m1x + m2x^2 + …. When $m$ is a positive integer the series terminates, and we obtain the ordinary formula for the Binomial Theorem with a positive integral exponent. In the general case R_n = x^nn! f^(n)(_nx) = mnx^n(1 + _nx)^m-n, and in order to show that Maclaurin’s Series really represents $(1 + x)^{m}$ for any range of values of $x$ when $m$ is not a positive integer, we must show that $R_{n} \to 0$ for every value of $x$ in that range. This is so in fact if $-1 < x < 1$, and may be proved, when $0\leq x < 1$, by means of the expression given above for $R_{n}$, since $(1 + \theta_{n}x)^{m-n} < 1$ if $n > m$, and $\dbinom{m}{n} x^{n} \to 0$ as $n \to \infty$ (% [examples:xxvii]Ex. xxvii%. 13). But a difficulty arises if $-1 < x < 0$, since $1 + \theta_{n}x < 1$ and $(1 + \theta_{n}x)^{m-n} > 1$ if $n > m$; knowing only that $0 < \theta_{n} < 1$, we cannot be assured that $1 + \theta_{n}x$ is not quite small and $(1 + \theta _{n}x)^{m-n}$ quite large. In fact, in order to prove the Binomial Theorem by means of Taylor’s Theorem, we need some different form for $R_{n}$, such as will be given later ([§]162).
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Exercise LVII
Exercise LVII, problem 1, p. 268
Verify the result when $\phi(x) = (x - a)^{m}$, $m$ being a positive integer, and $\xi = a$.
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Exercise LVII, problem 2, p. 268
Test the function $(x - a)^{m} (x - b)^{n}$, where $m$ and $n$ are positive integers, for maxima and minima at the points $x = a$, $x = b$. Draw graphs of the different possible forms of the curve $y = (x - a)^{m} (x - b)^{n}$.
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Exercise LVII, problem 3, p. 268
Test the functions $\sin x - x$, $\sin x - x + \dfrac{x^{3}}{6}$, $\sin x - x + \dfrac{x^{3}}{6} - \dfrac{x^{5}}{120}$, …, $\cos x - 1$, $\cos x - 1 + \dfrac{x^{2}}{2}$, $\cos x - 1 + \dfrac{x^{2}}{2} - \dfrac{x^{4}}{24}$, … for maxima or minima at $x = 0$.
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Exercise LVIII
Exercise LVIII, problem 1, p. 270
Find the limit of x - (n + 1)x^n+1 + nx^n+2/(1 - x)^2, as $x \to 1$. [Here the functions and their first derivatives vanish for $x = 1$, and $f''(1) = n(n + 1)$, $\phi''(1) = 2$.]
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Exercise LVIII, problem 2a, p. 270
Find the limits as $x \to 0$ of (x - x)/(x - x),0pt minus 3pt(nx - nx)/(nx - nx).
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Exercise LVIII, problem 2b, p. 270
Find the limits as $x \to 0$ of (x - x)/(x - x),0pt minus 3pt(nx - nx)/(nx - nx).
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Exercise LVIII, problem 3, p. 270
Find the limit of $x\{\sqrtp{x^{2} + a^{2}} - x\}$ as $x \to \infty$. [Put $x = 1/y$.]
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Exercise LVIII, problem 4a, p. 270
Prove that _x n (x - n)x= (-1)^n,0pt minus 3pt_x n 1x - n x- (-1)^n(x - n) = (-1)^n6, $n$ being any integer; and evaluate the corresponding limits involving $\cot x\pi$.
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Exercise LVIII, problem 4b, p. 270
Prove that _x n (x - n)x= (-1)^n,0pt minus 3pt_x n 1x - n x- (-1)^n(x - n) = (-1)^n6, $n$ being any integer; and evaluate the corresponding limits involving $\cot x\pi$.
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Exercise LVIII, problem 4c, p. 270
Prove that _x n (x - n)x= (-1)^n,0pt minus 3pt_x n 1x - n x- (-1)^n(x - n) = (-1)^n6, $n$ being any integer; and evaluate the corresponding limits involving $\cot x\pi$.
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Exercise LVIII, problem 5a, p. 270
Find the limits as $x \to 0$ of 1x^3(x - 1x - x6),0pt minus 3pt1x^3(x - 1x + x3).
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Exercise LVIII, problem 5b, p. 270
Find the limits as $x \to 0$ of 1x^3(x - 1x - x6),0pt minus 3pt1x^3(x - 1x + x3).
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Exercise LVIII, problem 6a, p. 270
$(\sin x\arcsin x - x^{2})/x^{6} \to \frac{1}{18}$, $(\tan x\arctan x - x^{2})/x^{6} \to \frac{2}{9}$, as $x \to 0$.
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Exercise LVIII, problem 6b, p. 270
$(\sin x\arcsin x - x^{2})/x^{6} \to \frac{1}{18}$, $(\tan x\arctan x - x^{2})/x^{6} \to \frac{2}{9}$, as $x \to 0$.
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Exercise LIX
Exercise LIX, problem 1, p. 272
Let $\phi(x) = ax + b$, so that $y = \phi(x)$ is a straight line. The conditions for contact at the point for which $x = \xi$ are $f(\xi) = a\xi + b$, $f'(\xi) = a$. If we determine $a$ and $b$ so as to satisfy these equations we find $a = f'(\xi)$, $b = f(\xi) - \xi f'(\xi)$, and the equation of the tangent to $y = f(x)$ at the point $x = \xi$ is y = xf’() + f() - f’(), or $y - f(\xi) = (x - \xi)f'(\xi)$. Cf. % [examples:xxxix]Ex. xxxix%. 5.
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Exercise LIX, problem 10, p. 272
Verify that the curvature of a circle is constant and equal to the reciprocal of the radius; and show that the circle is the only curve whose curvature is constant.
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Exercise LIX, problem 11, p. 272
0.375em plus 0.75em minus 0.25emFind the centre and radius of curvature at any point of the conics $y^{2} = 4ax$, $(x/a)^{2} + (y/b)^{2} = 1$.
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Exercise LIX, problem 12, p. 272
In an ellipse the radius of curvature at $P$ is $CD^{3}/ab$, where $CD$ is the semi-diameter conjugate to $CP$.
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Exercise LIX, problem 13, p. 272
Show that in general a conic can be drawn to have contact of the fourth order with the curve $y = f(x)$ at a given point $P$. [Take the general equation of a conic, viz. ax^2 + 2hxy + by^2 + 2gx + 2fy + c = 0, and differentiate four times with respect to $x$. Using suffixes to denote differentiation we obtain align* ax + hy + g + (hx + by + f) y_1 &= 0, a + 2hy_1 + by_1^2 + (hx + by + f) y_2 &= 0, 3(h + by_1) y_2 + (hx + by + f) y_3 &= 0, 4(h + by_1) y_3 +3by_2^2 + (hx + by + f) y_4 &= 0. align* If the conic has contact of the fourth order, then these five equations must be satisfied by writing $\xi$, $\eta$, $\eta_{1}$, $\eta_{2}$, $\eta_{3}$, $\eta_{4}$, for $x$, $y$, $y_{1}$, $y_{2}$, $y_{3}$, $y_{4}$. We have thus just enough equations to determine the ratios $a : b : c : f : g : h$.]
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Exercise LIX, problem 14, p. 272
An infinity of conics can be drawn having contact of the third order with the curve at $P$. Show that their centres all lie on a straight line. [Take the tangent and normal as axes. Then the equation of the conic is of the form $2y = ax^{2} + 2hxy + by^{2}$, and when $x$ is small one value of $y$ may be expressed (Ch.V, [misc:V]Misc. Ex. 22) in the form y = 12ax^2 + (12ah + _x) x^3, where $\epsilon_{x} \to 0$ with $x$. But this expression must be the same as y = 12f”(0) x^2 + 16f”’(0) + ’_x x^3, where $\epsilon'_{x} \to 0$ with $x$, and so $a = f''(0)$, $h = f'''(0)/3f''(0)$, in virtue of the result of % [examples:lv]Ex. lv%. 15. But the centre lies on the line $ax + hy = 0$.]
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Exercise LIX, problem 15, p. 272
Determine a parabola which has contact of the third order with the ellipse $(x/a)^{2} + (y/b)^{2} = 1$ at the extremity of the major axis.
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Exercise LIX, problem 16, p. 272
The locus of the centres of conics which have contact of the third order with the ellipse $(x/a)^{2} + (y/b)^{2} = 1$ at the point $(a\cos\alpha, b\sin\alpha)$ is the diameter $x/(a\cos\alpha) = y/(b\sin\alpha)$. [For the ellipse itself is one such conic.]
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Exercise LIX, problem 2, p. 272
The fact that the line is to have simple contact with the curve completely determines the line. In order that the tangent should have *contact of the second order* with the curve we must have $f''(\xi) = \phi''(\xi)$, *i.e.* $f''(\xi) = 0$. A point at which the tangent to a curve has contact of the second order is called a **of inflexion**. %[** TN: Differs from the modern definition]
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Exercise LIX, problem 3, p. 272
Find the points of inflexion on the graphs of the functions $3x^{4} - 6x^{3} + 1$, $2x/(1 + x^{2})$, $\sin x$, $a\cos^{2}x + b\sin^{2}x$, $\tan x$, $\arctan x$.
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Exercise LIX, problem 4, p. 272
Show that the conic $ax^{2} + 2hxy + by^{2} + 2gx + 2fy + c = 0$ cannot have a point of inflexion. [Here $ax + hy + g + (hx + by + f)y_{1} = 0$ and a + 2hy_1 + by_1^2 + (hx + by + f)y_2 = 0, suffixes denoting differentiations. Thus at a point of inflexion a + 2hy_1 + by_1^2 = 0, or a(hx + by + f)^2 - 2h(ax + hy + g)(hx + by + f) + b(ax + hy + g)^2 = 0, or (ab - h^2)ax^2 + 2hxy + by^2 + 2gx + 2fy + af^2 - 2fgh + bg^2 = 0. But this is inconsistent with the equation of the conic unless af^2 - 2fgh + bg^2 = c(ab - h^2) or $abc + 2fgh - af^{2} - bg^{2} - ch^{2} = 0$; and this is the condition that the conic should degenerate into two straight lines.]
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Exercise LIX, problem 5, p. 272
The curve $y = (ax^{2} + 2bx + c)/(\alpha x^{2} + 2\beta x + \gamma)$ has one or three points of inflexion according as the roots of $\alpha x^{2} + 2\beta x + \gamma = 0$ are real or complex. [The equation of the curve can, by a change of origin (cf. % [examples:xlvi]Ex. xlvi%. 15), be reduced to the form = /(A^2 + 2B+ C) = /A(- p)(- q), where $p$, $q$ are real or conjugate. The condition for a point of inflexion will be found to be $\xi^{3} - 3pq\xi + pq(p + q) = 0$, which has one or three real roots according as $\DPtypo{\{pq(p - q)\}}{\{pq(p - q)\}^{2}}$ is positive or negative, *i.e.* according as $p$ and $q$ are real or conjugate.] [pg]273
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Exercise LIX, problem 6, p. 272
Discuss in particular the curves $y = (1 - x)/(1 + x^{2})$, $y = (1 - x^{2})/(1 + x^{2})$, $y = (1 + x^{2})/(1 - x^{2})$.
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Exercise LIX, problem 7, p. 272
Show that when the curve of Ex. 5 has three points of inflexion, they lie on a straight line. [The equation $\xi^{3} - 3pq\xi + pq(p + q) = 0$ can be put in the form $(\xi - p)(\xi - q)(\xi + p + q) + (p - q)^{2}\xi = 0$, so that the points of inflexion lie on the line $\xi + A(p - q)^{2}\eta + p + q = 0$ or $A\xi - 4(AC - B^{2})\eta = 2B$.]
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Exercise LIX, problem 8, p. 272
Show that the curves $y = x\sin x$, $y = (\sin x)/x$ have each infinitely many points of inflexion.
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Exercise LIX, problem 9, p. 272
**of a circle with a curve. Curvature. A much fuller discussion of the theory of curvature will be found in Mr Fowler’s %[** TN: Reference on page 272 of orig. points to page 266.] tract referred to on p.272266.** The general equation of a circle, viz. (x - a)^2 + (y - b)^2 = r^2, (1) contains three arbitrary constants. Let us attempt to determine them so that the circle has contact of as high an order as possible with the curve $y = f(x)$ at the point $(\xi, \eta)$, where $\eta = f(\xi)$. We write $\eta_{1}$, $\eta_{2}$ for $f'(\xi)$, $f''(\xi)$. Differentiating the equation of the circle twice we obtain align (x - a) + (y - b)y_1 &= 0, (2) 1 + y_1^2 + (y - b)y_2 &= 0. (3) align If the circle touches the curve then the equations (1) and (2) are satisfied when $x = \xi$, $y = \eta$, $y_{1} = \eta_{1}$. This gives $(\xi - a)/\eta_{1} = -(\eta - b) = r/\sqrtp{1 + \eta_{1}^{2}}$. If the contact is of the second order then the equation (3) must also be satisfied when $y_{2} = \eta_{2}$. Thus $b = \eta + \{(1 + \eta_{1}^{2})/\eta_{2}\}$; and hence we find a = - _1(1 + _1^2)_2,0pt minus 3ptb = + 1 + _1^2_2,0pt minus 3ptr = (1 + _1^2)^3/2_2. The circle which has contact of the second order with the curve at the point $(\xi, \eta)$ is called the **of curvature**, and its radius the **of curvature**. The **of curvature** (or simply the *curvature*) is the reciprocal of the radius: thus the measure of curvature is $f''(\xi)/\{1 + [f'(\xi)]^{2}\}^{3/2}$, or d^2d^2 / 1 + (dd)^2^3/2.
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