CHAPTER XI
DIFFERENTIAL CALCULUS. STANDARD FORMS.
PARTIAL DIFFERENTIATION
1. The differential coefficient of any particular function can, of course, be obtained by direct calculation, but the process can usually be simplified by the application of the following general rules. The general similarity to the propositions already demonfor Finite Differences will be apparent.
- I.The differential coefficient of any constant term is zero. This is evident since a constant is a quantity which does not change in value in any mathematical operation.
The differential coefficient of the product of a constant and a function of x is equal to the product of the constant and of the differential coefficient of the function.
Thus[c . f (x)] = Ltfio cf (x + h c f (x)= Lt f (x + h) f (x)nyoh
df(x)
c(1). dx
- III.
The differential coefficient of the algebraic sum of a number of functions of x is the sum of the differential coefficients of the several functions.
Let y = u + v + w + ..., where u, v, w, ... are functions of x,thenAy = Au + Av + Ow + ...and~y _ Du+Ov+Aw+...,andOx Ox Lxwhich, by proceeding to the limit, becomesdy _ du dv dwdx dx+dx+ _ dx + (2).
- IV.
The differential coefficient of the product of two functions is the sum of the products of each function and the differential coefficient of the other,
H. T. B. L5
66 DIFFERENTIAL CALCULUS
Let y = uv,
where u and v are both functions of x.
Then Dy=(u+Au)(v+w)uv =u0v+vLu+&(Ov =u0v+(v+Ov)Au
and x=uA+(v+4v) Au Ax'
whence, taking the limit, when v + Ov v, dy _ dv du
dx udx +vdx (3),
which may be written
1dy Ida ldv
ydx udx + vdx (4). This result may be extended to include the product of any number of functions.
For if y =uvw; let vw = z, then y = uz.
Whence 1 dy 1 du + 1 dz . ydx udx zdx
But ldz ldv+ldw. z dx vdx wdx
1dy1du ldv 1 dw
Therefore ydx = u dx + vdx + wdx """"""...(5). Multiplying by uvw, we obtain
dy =vwdu+wuv+uv dw
(6)
dx dx dx-- dx
Similarly for the product of any number of functions.
V. The differential coefficient of the quotient of two functions is (Di Coeff. of Numr.) (Denr.) (Di,'f. Coef . of Denr.) (Numr.) Square of Denominator
Let u
y v'
u -i-AuuvLu uLv
Then D y = _ v -r Av v v (v + Av )
Du Av A vLxuAx
and y Ax v (v + Av)
STANDARD FORMS 67
whence, taking the limit,
du dv
dy dx dx
dx v
which may be written
ldy ldu ldv
y dx u, dx v dx (8).
VI. The differential coefficient of y with respect to x, where y is a function of u and u is a function of x, is the product of the difcoefficients of y with respect to u and u with respect to x.
For Ay Ay Du
Ax Du Ax'
whence, taking the limit,
dy dy du
dx du' dx (9).
Similarly d?/ _ dy du dv
x du'dv.dx (10), d
and so for any number of functions.
2. Various standard forms can now be developed, mainly from first principles. It is instructive to note the points of analogy with the corresponding forms for Finite Differences.
(i) y = xn
,
dy=Lt(x+)r)nxn
dx h-~0 h
xn (1+le)n -1
= Lt x
hyo h
Expanding by the Binomial we have
xn s+...1
dx rx
=Ltnxn-' L1 +n lh+...l
h-1.0
x
= naaa1
52
68 DIFFERENTIAL CALCULUS
- (ii)y = ax
edy=Lt ax+h ax dx h~o hah -1 =a2'Lth-.0 it7=ahLtoh[1+hloge a+j2(loge a)2+...1rh= ax Lt [loge a + (loge a)2 + ...h-.0= a'' loge a.Ify=ex, dx=exloge e=efD.
- (iii)y = log,,x.
Thena' = x.Butd (aY) d (a') dydxdy dx'Hence, using the result established in (ii) and remembering that ay = x, we havedx a'logea.dx dxor1 =xloge a.dx.Whenced_y = 1 dx x loge ad11Ify loge x,- -dx x loge e
- (iv)y = [f (x)]"; y = e12' ; y = log, f(x)
Ify = [f (x)]",dy d [ f (x)]" df (x)dxdf(x)dx= n [f (x)]"-1. f ' (x). Similarly ify=ef(), dx=ef(x).f'(x),and ify = loge f (x), dy =f (x)
f (x)
STANDARD FORMS 69
- (v)y = sin x,
dryLt sin (x + h) sin xdx h>oh
2sin-.cos(x+2)
= Lt
hyo h
h
sin 2 / h)
= Lt . cos I x + 2)
hy0
2
= cos x.
- (vi)y = sin1 x.
Thensin y = x,whencedx = cos y = 11 sine y =VT: .yThereforedy _ 1 = 1dx dx 1 x2dy
3. The values of differential coefficients for the other trigonometrical functions can be found by methods similar to those employed in (v) and (vi). The results are given in the table below and should be verified as an exercise by the student.
|
Function |
DifferentialCoefficient |
Function |
DifferentialCoefficient |
| |
nxn1 |
sin-1x |
1 |
|
ax |
ax log, a |
|
1 - x2 |
|
ex |
ex |
cos-1 |
1 |
|
logax |
1 |
|
1-xs |
| |
xlog, a |
tan-lx |
1 |
|
log,x |
1 |
|
1+x9 |
| |
x |
cot-1 x |
1 |
|
sin x |
cos x |
|
1 +x2 |
|
cos x |
- sin x |
sec-1 x |
1 |
|
tan x |
eec2 x |
|
xxa - 1 |
|
cot x |
- cosec2 x |
cosec1 x |
- |
|
sec xcosec x |
sec x . tan x
- cosec x . cot x |
|
x,./x2 -1 |
70 DIFFERENTIAL CALCULUS
- Logarithmic Differentiation. This method is of special value in two cases. Thus if y = uvw ..., where u, v, w, ... are functions of x, then
log y = logloglogw+...,1 dy l du l dv l dwand- -+- +-+... ydx udx vdx wdx
or dy =uvw 1 du + 1 dv + 1 dw +
dx udx vdx wdx
a result which agrees with that already obtained in § 1. Secondly if y = u", u and v both being functions of x, log y = v log u,
and ydx=udx+login
or dx=vu"-'--+uvlogudx.
- We will now give some miscellaneous examples of differen
- - b+x
By the ordinary rule for a quotientdy (b + x) d (dx x2) (a + x2) d (b + x)dx(b+x)'(b+x)2x-(a+x2) x2+2bx-a(b + x)2- (b + x)27x-1
- = 1 - 5x + 6x2'
This can best be treated by resolving the expression into partial fractions. Then
4 5
= 1 3x 1 2x'
dy-4d(1-3x)-' d(1-3x)5d(1-2x)-1 d(1-2x) dx d (1 - 3x) dx d (1 - 2x) dx
"= 12 _ 10
(1 - 3x)2 (1 - 2x)2
STANDARD FORMS 71
- (iii)y = ZVa + x.
dyd(a+x)" d(a+x)1ndx d(a+x)dxn(a+x)
- (iv)y = log (log x).
dy d log (log x) d_(log x)1dx d (log x)dxx log cc'
- (v)y = tan
1vx'1.11 1dyd (tan-1 - -- 1J dVx'1 d(x'1)dx1d(x'1)'dxd'Vx'1l. (a'1)-g.2ro1 1+x'11 _xx'1'x-2 x
- (vi)y (x 3) .
logy=1 logx21 logx3, xxldy1d(log x2) d(x2)1ydx x d(x2)dx +logx2.1 d(logx3) d(x3)1x d x3 ' dxogx_11 1 to x2x(x2) x(x3) x' gx3'Whencedy - - x 2 z r1+ 1 to m 21dx(x3) [x (x2)(x3)gx3J'
72 DIFFERENTIAL CALCULUS
(vii) y = ax . bcx.
log y = x log a + cx log b,
1 d =loga+cxlogclogb, y dx
dx=az.V(log a+cxlogclogb).
(viii) y = xx + xx.
In this case logarithmic differentiation must be used, but for this purpose the two terms must be taken separately.
Let xx = u and xx = . dydu dv
Then + dx dx dxx
log u = x log x,
u d u
=xx+logx,
x du- =xx(1+logx).
dx
Also log v = 1 log x, x
v dx=x.x~-logx ,
dv 1
dx- =xx. (1 log x).
Therefore dx = xx (1 + log x) + xx (1 log x).
(ix) Differentiate loge x with regard to x'.
Let y = log, x and z = x2.
Then dy dy dx d_y 1 dz dx' dz dx'dz' dx
Therefore dy = 1 1 1 dz x' 2x 2x2
STANDARD FORMS 73
- In dealing with cases where a function of two variables is involved it is convenient to adopt methods similar to those used in Finite Differences (see Chapter IX, 4). Thus we define Partial Differentiation as the process of differentiating a function of several variables with reference to any one of them, treating the other variables as constants.
This process is denoted by the symbols ax , sy , etc. We will also use the symbol Sx to denote a small change in the value of x. Letu = f (x, y).Thenu+Su= f(x+h, y+k)andSu = f (x + h, y + k) f (x, y) f(x+h,y+k)f(x,y+k).h+f(x,y+k).f(x,y).k. h Proceeding to the limit when h and k each > 0,f(x+It,y+k) f(x, y+k)_haxf(x,y+k)ax f (x, y), since k - 0. ThereforeSu =aua. Sx + u . Sy,yandSu _ au + au SySx ax ay Sxdu au or, when Sx 0,dx ax + ay . dx (11).7. If f (x, y) = 0, dx = 0 andau au dy°-ax+ ay' yau dyaxWhencedx=du (12).ay Example. Ifx' + xy + y' = 0,thenax=2x+y, a=x+2y,anddy2x+,y andxx+2y'