Chapter 11: Problem 12
Show that none of the principal moments of inertia can exceed the sum of the other two.
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Chapter 11: Problem 12
Show that none of the principal moments of inertia can exceed the sum of the other two.
These are the key concepts you need to understand to accurately answer the question.
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A homogeneous slab of thickness \(a\) is placed atop a fixed cylinder of radius \(R\) whose axis is horizontal. Show that the condition for stable equilibrium of the slab, assuming no slipping, is \(R>a / 2 .\) What is the frequency of small oscillations? Sketch the potential energy \(U\) as a function of the angular displacement \(\theta\). Show that there is a minimum at \(\theta=0\) for \(R>a / 2\) but not for \(R
A door is constructed of a thin homogeneous slab of material: it has a width of 1 \(\mathrm{m} .\) If the door is opened through \(90^{\circ},\) it is found that on release it closes itself in 2 s. Assume that the hinges are frictionless, and show that the line of hinges must make an angle of approximately \(3^{\circ}\) with the vertical.
Consider a symmetrical rigid body rotating freely about its center of mass. A frictional torque \(\left(N_{f}=-b \omega\right)\) acts to slow down the rotation. Find the component of the angular velocity along the symmetry axis as a function of time.
Solve Example 11.2 for the case when the physical pendulum does not undergo small oscillations. The pendulum is released from rest at \(67^{\circ}\) at time \(t=0 .\) Find the angular velocity when the pendulum angle is at \(1^{\circ} .\) The mass of the pendulum is \(340 \mathrm{g}\), the distance \(L\) is \(13 \mathrm{cm}\), and the radius of gyration \(k\) is \(17 \mathrm{cm}\).
Consider a thin disk composed of two homogeneous halves connected along a diameter of the disk. If one half has density \(\rho\) and the other has density \(2 \rho,\) find the expression for the Lagrangian when the disk rolls without slipping along a horizontal surface. (The rotation takes place in the plane of the disk.)
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