Figure 10.31 shows an object of mass M with one axis through its center of mass and a parallel axis through an arbitrary point A . Both axes are perpendicular to the page. The figure shows an arbitrary mass element dm and vectors connecting the center of mass, the point A , and dm . (a) Use the law of cosines (Appendix A) to show that r 2 = r c m 2 + h 2 − 2 h → ⋅ r → c m . (b) Use this result in I = ∫ r 2 dm to calculate the object’s rotational inertia about the axis through A . Each term in your expression for r 2 leads to a separate integral. Identify one as the rotational inertia about the CM, an-other as the quantity Mh 2 , and argue that the third is zero. Your result is a statement of the parallel-axis theorem (Equation 10.17). FIGURE 10.31 Problem 78
Figure 10.31 shows an object of mass M with one axis through its center of mass and a parallel axis through an arbitrary point A . Both axes are perpendicular to the page. The figure shows an arbitrary mass element dm and vectors connecting the center of mass, the point A , and dm . (a) Use the law of cosines (Appendix A) to show that r 2 = r c m 2 + h 2 − 2 h → ⋅ r → c m . (b) Use this result in I = ∫ r 2 dm to calculate the object’s rotational inertia about the axis through A . Each term in your expression for r 2 leads to a separate integral. Identify one as the rotational inertia about the CM, an-other as the quantity Mh 2 , and argue that the third is zero. Your result is a statement of the parallel-axis theorem (Equation 10.17). FIGURE 10.31 Problem 78
Figure 10.31 shows an object of mass M with one axis through its center of mass and a parallel axis through an arbitrary point A.
Both axes are perpendicular to the page. The figure shows an arbitrary mass element dm and vectors connecting the center of mass, the point A, and dm. (a) Use the law of cosines (Appendix A) to show that
r
2
=
r
c
m
2
+
h
2
−
2
h
→
⋅
r
→
c
m
. (b) Use this result in I = ∫r2dm to calculate the object’s rotational inertia about the axis through A. Each term in your expression for r2 leads to a separate integral. Identify one as the rotational inertia about the CM, an-other as the quantity Mh2, and argue that the third is zero. Your result is a statement of the parallel-axis theorem (Equation 10.17).
A block of mass m₁
=
10.0 kg is connected to a block of mass m₂
34.0 kg by a massless string that passes over a light, frictionless pulley. The 34.0-kg block is connected to a spring that has negligible mass and a force constant of k = 200 N/m as shown in the figure below. The spring is
unstretched when the system is as shown in the figure, and the incline is frictionless. The 10.0-kg block is pulled a distance h = 22.0 cm down the incline of angle = 40.0° and released from rest. Find the speed of each block when the spring is again unstretched.
Vm1
×
1.32
Vm2
= 1.32
×
m/s
m/s
A block of mass m₁ = 10.0 kg is connected to a block of mass m₂ = 34.0 kg by a massless string that passes over a light, frictionless pulley. The 34.0-kg block is connected to a spring that has negligible mass and a force constant of k = 200 N/m as shown in the figure below. The spring is
unstretched when the system is as shown in the figure, and the incline is frictionless. The 10.0-kg block is pulled a distance h = 22.0 cm down the incline of angle 0 = 40.0° and released from rest. Find the speed of each block when the spring is again unstretched.
m/s
Vm1
Vm2
m/s
mi
m2
k
i
Truck suspensions often have "helper springs" that engage at high loads. One such arrangement is a leaf spring with a helper coil spring mounted on the axle, as in the figure below. The helper spring engages when the main leaf spring is compressed by distance yo, and then helps to
support any additional load. Consider a leaf spring constant of 5.45 × 105 N/m, helper spring constant of 3.60 × 105 N/m, and y = 0.500 m.
Truck body
Dyo
Axle
(a) What is the compression of the leaf spring for a load of 4.90 × 105 N?
m
(b) How much work is done compressing the springs?
]
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