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Chapter 11 Gravity

Chapter 11 Gravity

Chapter 11 Gravity

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<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

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