So asx→∞,
ex
xn
→∞–i.e.exis ‘stronger’ thanxn; for any positive integern.Sofor
example:
xn
ex
=xne−x→0asx→∞
In fact, it is not difficult to extend the above proof to apply for any value ofn, not
necessarily integer. This limit is very useful in Laplace transforms and should be thoroughly
understood (➤502).
Exercise on 14.3
Evaluate the following limits
(i) lim
x→ 0
sin 2x
x
(ii) lim
x→ 3
x^3 − 27
x− 3
(iii) lim
x→∞
2 x^3 −x
e^3 x
Answer
(i) 2 (ii) 27 (iii) 0
14.4 Continuity
We can now use the idea of a limit to put the concept of continuity into mathematical
form. If we focus on a particular pointx=aon the curve of a functionf(x), then clearly
if the curve is continuous at that point then we would want the limit atx=ato be the
same ‘from both sides’ and to be equal tof(a). Only in this way can the two parts of the
curve on either side ofx=a‘join up’ without leaving a hole in the curve. We express
this formally in the following definition:
A functionf(x)iscontinuous atx=aif limx→af(x)=f(a).
The graphs of continuous functions are continuous curves, and some examples of contin-
uous and discontinuous curves are illustrated in Figure 14.5.
y
0 x
y
0
0 0
y y
x x = a x
x = a x
Continuous
and
smooth
Continuous
but not
differentiable at x = a
Finite
discontinuity
at x = a
Infinite
discontinuity
at x = a
a
Figure 14.5Continuous and discontinuous curves.