phy1020.DVI

(Darren Dugan) #1

Cancelingxin the numerator and denominator,


slopeD lim
x! 0

2xCx (4.15)

and asxapproaches zero,


slopeD2x (4.16)

So for at any point along the curvef.x/Dx^2 , its slope is given by2x.AtxD 3 , the slope is 2  3 D 6 ,in
agreement with our earlier approximations.
The slope is called thederivativeoff.x/with respect tox. As we have just shown, the derivative of
f.x/Dx^2 with respect toxis2x. We indicate the derivative ofyDf.x/with respect toxby the notation


dy
dx

or

d
dx

f.x/ (4.17)

Thus the derivative can be thought of as the quotient of two infinitesimal numbers, and is defined as


dy
dx

 lim
x! 0

y
x

D lim
x! 0

f.xCx/f.x/
x

(4.18)


For our exampleyDf.x/Dx^2 ,


dy
dx

D


d
dx

x^2 D2x (4.19)

More generally, it can be shown that for anyn,


d
dx

xnDnxn^1 (4.20)

For example,


d
dx

x^5 D5x^4 (4.21)

Herenneed not necessarily be an integer. For example, since


p
xDx1=2,wehave
d
dx

p
xD

d
dx

x1=2D

1


2


x1=2D

1


2


p
x

(4.22)


Similar results can be worked out for many common functions. Appendix E gives a short table of deriva-
tives. In conjunction with this table, we note the following properties (uandvare functions ofx, andais a
constant):


d
dx

.au/Da

du
dx

(4.23)


d
dx

.uCv/D

du
dx

C


dv
dx

(4.24)


d
dx

.uv/D

du
dx




dv
dx

(4.25)


d
dx

.uv/D

du
dx

vCu

dv
dx

(4.26)


d
dx

u
v




D


v.du=dx/u.dv=dx/
v^2

(4.27)

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