MA 3972-MA-Book April 11, 2018 16:1
Areas and Volumes 275
Solution:
(a) Sinces=
∫t
0
f(x)dx, thenv(t)=s′(t)=f(t).
Thus,v(4)=−8 ft/sec.
(b) s(3)=
∫ 3
0
f(x)dx=
∫ 2
0
f(x)dx+
∫ 3
2
f(x)dx=
1
2
(10)(2)−
1
2
(1)(5)=
15
2
ft.
(c) a(t)=v′(t). Sincev′(t)=f′(t),v′(t)=0att=4. Thus,a(4)=0 ft/sec^2.
(d) The particle is moving to the right whenv(t)>0. Thus, the particle is moving to the
right on intervals (0, 2) and (7, 8).
(e) The area offbelow thex-axis fromx=2tox=7 is larger than the area offabove the
x-axis fromx=0tox=2 andx=7tox=8. Thus,
∫ 8
0
f(x)dx<0 and the particle
is on the left side of the origin.
TIP • Do not forget that (fg)′= f′g+g′f andnot f′g′. However, lim(fg)=(limf)
(limg).
13.2 Approximating the Area Under a Curve
Main Concepts:Rectangular Approximations, Trapezoidal Approximations
Rectangular Approximations
Iff ≥0, the area under the curve offcan be approximated using three common types of
rectangles: left-endpoint rectangles, right-endpoint rectangles, or midpoint rectangles.
(See Figure 13.2-1.)
0 a
y f(x)
x
x 1 x 2 x 3 b
left-endpoint
0 a
y f(x)
x
x 1 x 2 x 3 b
right-endpoint
0 a
y f(x)
x
x 1 x 2 x 3 b
midpoint
Figure 13.2-1