A hollow spherical shell with mass 1.65 kg rolls without slipping down a slope that makes an angle of 40.0 ∘ with the horizontal.
PART A) Find the magnitude of the acceleration
acm of the center of mass of the spherical shell.
Take the free-fall acceleration to be g = 9.80 m/s2 .
Part B
Find the magnitude of the frictional force acting on the spherical shell.
Take the free-fall acceleration to be g = 9.80 m/s2 .
Two forces act along the line of motion. Gravity down
the slope, m g sin(α), and friction up the slope, F. They provide
the linear acceleration and F also provides the torque about the
CoM. This gives the equations of motion:
m a = m g sin(α) - F
I dω/dt = F R
A spherical shell of mass m has moment of inertia I = 2/3 m R^2.
Furthermore a pure rolling relates dω/dt and a through a = R dω/dt.
So the two equations become
m a = m g sin(α) - F
2/3 m a = F
These we solve for a and F:
Substituting F from the second equation gives
m a = m g sin(α) - 2/3 m a
a = 3/5 g sin(α)
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For part A this gives
a = 3/5 * 9.80m/s^2*sin(40.0)= 3.77m/s^2
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With that we can substitute back to find F:
F = 2/3 m 3/5 g sin(α)
F = 2/5 mg sin(α)
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For part B this gives
F = 2/5*1.65kg*9.80N/kg*sin(40) = 4.15 N
A hollow spherical shell with mass 1.65 kg rolls without slipping down a slope that makes...
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