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9.94: a) From the parallel-axis theorem, the moment of inertia is<br />

2 2<br />

I P<br />

= (2 5) MR + ML , and<br />

2<br />

I P<br />

⎛ 2<br />

1<br />

.<br />

2<br />

5 ⎟ ⎞<br />

⎜ ⎛ ⎞⎛<br />

R ⎞<br />

= +<br />

⎜ ⎟⎜<br />

⎟<br />

ML<br />

⎝ ⎝ ⎠⎝<br />

L ⎠ ⎠<br />

2<br />

2<br />

If R = (0.05)L, the difference is 2 5)(0.05) = 0.001. b) ( I ML ) = ( m 3M<br />

), which<br />

is 0.33% when m = (0.01) M.<br />

rod<br />

(<br />

rod<br />

rod<br />

9.95: a) With respect to O, each element<br />

2<br />

i<br />

2 2<br />

i<br />

y i<br />

r in Eq. (9.17) is x + , and so<br />

2<br />

2 2<br />

2<br />

2<br />

∑miri<br />

= ∑mi<br />

( xi<br />

+ yi<br />

) = ∑mi<br />

xi<br />

+ ∑ mi<br />

yi<br />

= I<br />

x<br />

+<br />

I =<br />

I .<br />

O<br />

i i i i<br />

b) Two perpendicular axes, both perpendicular to the washer’s axis, will have the<br />

same moment of inertia about those axes, and the perpendicular-axis theorem predicts<br />

M 2 2<br />

that they will sum to the moment of inertia about the washer axis, which is ( R + ),<br />

and so I<br />

x<br />

M<br />

= = ( R + ).<br />

I<br />

y<br />

2 2<br />

4 1<br />

R2<br />

y<br />

1<br />

R<br />

2 2<br />

1 2<br />

c) From Table (9.2), I = m(<br />

L<br />

2<br />

2<br />

+ L ) = 1<br />

mL .<br />

12<br />

1 2<br />

Since I<br />

0<br />

= I<br />

x<br />

+ I<br />

y, and I<br />

x<br />

= I<br />

y,<br />

both I<br />

x<br />

and I<br />

y<br />

must be<br />

12<br />

mL .<br />

6<br />

M<br />

9.96: Each side has length a and mass , and the moment of inertia of each side about<br />

4<br />

1<br />

an axis perpendicular to the side and through its center is M 2<br />

2<br />

Ma<br />

12 4<br />

a =<br />

48<br />

. The moment of<br />

inertia of each side about the axis through the center of the square is, from the<br />

2<br />

2<br />

2<br />

Ma M a Ma<br />

+ = . The total moment of inertia is the sum of<br />

perpendicular axis theorem, ( )<br />

48 4 2 12<br />

2<br />

2<br />

Ma Ma<br />

the contributions from the four sides, or × = .<br />

4<br />

12 3

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