Chapter 11 Gravity
Chapter 11 Gravity
Chapter 11 Gravity
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
<strong>Gravity</strong><br />
expressing the mass of the sphere in terms of C. We can then use the definition of<br />
the gravitational field to find the gravitational field of the sphere inside its surface.<br />
The work done by the field equals the negative of the change in the potential<br />
energy of the system as the small object falls in the hole.<br />
Use conservation of energy to relate<br />
the work done by the gravitational<br />
field to the speed of the small object<br />
as it strikes the bottom of the hole:<br />
Express the mass of a differential<br />
element of the sphere:<br />
Integrate to express the mass of<br />
K f − Ki<br />
+ ΔU<br />
= 0<br />
or, because Ki = 0 and W = −ΔU,<br />
1 2 2W<br />
W = mv 2 ⇒ v = (1)<br />
m<br />
where v is the speed with which the<br />
object strikes the bottom of the hole<br />
and W is the work done by the<br />
gravitational field.<br />
dm = ρ dV = ρ<br />
2 ( 4π r dr)<br />
2<br />
M 4 π C rdr = ( 50m<br />
) π C<br />
the sphere in terms of C:<br />
Solving for C yields:<br />
Substitute numerical values and<br />
5.<br />
0<br />
= ∫<br />
0<br />
m<br />
M<br />
C = 2 ( 50m<br />
)π<br />
1.<br />
0×<br />
10<br />
C =<br />
evaluate C: 2 ( 50m<br />
)<br />
<strong>11</strong><br />
kg<br />
8<br />
= 6.<br />
37×<br />
10 kg/m<br />
π<br />
Use its definition to express the gravitational field of the sphere at a distance from<br />
its center less than its radius:<br />
2<br />
4π<br />
r ρ dr<br />
Fg<br />
GM 0<br />
g = = = G = G<br />
2<br />
2<br />
m r r<br />
Express the work done on the small<br />
object by the gravitational force<br />
acting on it:<br />
Substitute in equation (1) and<br />
simplify to obtain:<br />
r<br />
∫<br />
r<br />
∫<br />
0<br />
4π<br />
r<br />
r<br />
2<br />
2<br />
r<br />
C<br />
dr 4π<br />
C r dr<br />
r ∫<br />
0<br />
= G = 2π<br />
GC<br />
2<br />
r<br />
3.0m<br />
W = − ∫ mgdr = ( 2m)mg<br />
v =<br />
=<br />
5.<br />
0<br />
2<br />
m<br />
( 2.<br />
0m)<br />
m(<br />
2π<br />
GC)<br />
m<br />
( 8.<br />
0m)<br />
π GC<br />
2<br />
237