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11.30: a) The volume would increase slightly. b) The volume change would be twice<br />

as great. c) The volume is inversely proportional to the bulk modulus for a given pressure<br />

change, so the volume change of the lead ingot would be four times that of the gold.<br />

250 N<br />

6<br />

11.31: a) = 3.33 10 Pa.<br />

- 4 2<br />

×<br />

0.75×<br />

10 m<br />

6<br />

−4<br />

2<br />

b) (3.33×<br />

10 Pa)(2)(200×<br />

10 m ) = 133 kN.<br />

11.32: a) Solving Eq. (11.14) for the volume change,<br />

∆V<br />

= −kV∆P<br />

= −(45.8×<br />

10<br />

−11<br />

3<br />

= −0.0531m .<br />

Pa<br />

−1<br />

3<br />

8<br />

)(1.00 m )(1.16 × 10<br />

Pa −1.0×<br />

10<br />

5<br />

Pa)<br />

b) The mass of this amount of water not changed, but its volume has decreased to<br />

1.000 m<br />

3<br />

3<br />

3<br />

1.03×<br />

10 kg<br />

3 3<br />

− 0.053 m = 0.947 m , and the density is now = 1.09×<br />

10 kg m .<br />

3<br />

3<br />

0.947 m<br />

3<br />

6<br />

( 600 cm )(3.6 × 10 Pa)<br />

9 1<br />

−10<br />

−1<br />

11.33: B =<br />

= 4.8×<br />

10 Pa, k = = 2.1×<br />

10 Pa .<br />

3<br />

(0.45 cm )<br />

B<br />

11.34: a) Using Equation ( 11.17),<br />

5<br />

F|| ( 9×<br />

10 N)<br />

−2<br />

Shear strain = =<br />

= 2.4×<br />

10 .<br />

AS<br />

10<br />

[(.10 m)(.005 m)][7.5 × 10 Pa]<br />

−3<br />

b) Using Equation ( 11.16), x = Shear stain ⋅ h = (.024)(.1m) = 2.4×<br />

10 m.<br />

11.35: The area A in Eq. ( 11.17)<br />

has increased by a factor of 9, so the shear strain for<br />

the larger object would be 1 9 that of the smaller.<br />

11.36: Each rivet bears one-quarter of the force, so<br />

4<br />

F<br />

1<br />

|| ( 1.20×<br />

10 N)<br />

4<br />

8<br />

Shear stress = =<br />

= 6.11×<br />

10 Pa.<br />

−2<br />

2<br />

A π(.125×<br />

10 m)

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