An asymmetric top (I1 < 12 < I3) executes torque-free motion with 2E12 = L². If the angular velocity w initially lies in the plane of ê1 and ê3, integrate Euler's equations to obtain the solution I w₁(t) = Woo 12 (13 - 12) 11 (13-11)] 1/2 sech(t/T), w2 (t) =&oo tanh(t/T), w3 (t): sech(t/T), where wo = 2E/L and 7= w[(13-12) (12 - 11)/(1311)]-1/2. Discuss the time dependence of w²= ||² and sketch the motion of as seen in the body-fixed frame. 12 (12-11) 1¹/2 13(13-11). = Woo

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Question 1
```plaintext
1. An asymmetric top (\(I_1 < I_2 < I_3\)) executes torque-free motion with \(2EI_2 = L^2\). If the angular velocity \(\omega\) initially lies in the plane of \(\mathbf{e}_1\) and \(\mathbf{e}_3\), integrate Euler’s equations to obtain the solution

\[
\omega_1(t) = \omega_\infty \left[\frac{I_2(I_3 - I_2)}{I_1(I_3 - I_1)}\right]^{1/2} \text{sech}(t/\tau), \quad \omega_2(t) = \omega_\infty \tanh(t/\tau), \quad \omega_3(t) = \omega_\infty \left[\frac{I_2(I_2 - I_1)}{I_3(I_3 - I_1)}\right]^{1/2} \text{sech}(t/\tau),
\]

where \(\omega_\infty \equiv 2E/L\) and \(\tau \equiv \omega_\infty^{-1}((I_3 - I_2)(I_2 - I_1)/(I_3 - I_1))^{-1/2}\). Discuss the time dependence of \(\omega^2 = |\vec{\omega}|^2\) and sketch the motion of \(\vec{\omega}\) as seen in the body-fixed frame.

2. A Thumbtack on an inclined plane

A rigid body in the shape of a thumbtack formed from a thin disk of mass \(M\) and radius \(a\) and a massless stem is placed on an inclined plane that makes an angle \(\alpha\) with
```

The problem likely involves understanding the dynamic behavior of a rotating object (asymmetric top) and analyzing its stability and motion over time. Additionally, the mention of a thumbtack on an inclined plane may involve questions of equilibrium and forces acting on the rigid body in a gravitational field.
Transcribed Image Text:```plaintext 1. An asymmetric top (\(I_1 < I_2 < I_3\)) executes torque-free motion with \(2EI_2 = L^2\). If the angular velocity \(\omega\) initially lies in the plane of \(\mathbf{e}_1\) and \(\mathbf{e}_3\), integrate Euler’s equations to obtain the solution \[ \omega_1(t) = \omega_\infty \left[\frac{I_2(I_3 - I_2)}{I_1(I_3 - I_1)}\right]^{1/2} \text{sech}(t/\tau), \quad \omega_2(t) = \omega_\infty \tanh(t/\tau), \quad \omega_3(t) = \omega_\infty \left[\frac{I_2(I_2 - I_1)}{I_3(I_3 - I_1)}\right]^{1/2} \text{sech}(t/\tau), \] where \(\omega_\infty \equiv 2E/L\) and \(\tau \equiv \omega_\infty^{-1}((I_3 - I_2)(I_2 - I_1)/(I_3 - I_1))^{-1/2}\). Discuss the time dependence of \(\omega^2 = |\vec{\omega}|^2\) and sketch the motion of \(\vec{\omega}\) as seen in the body-fixed frame. 2. A Thumbtack on an inclined plane A rigid body in the shape of a thumbtack formed from a thin disk of mass \(M\) and radius \(a\) and a massless stem is placed on an inclined plane that makes an angle \(\alpha\) with ``` The problem likely involves understanding the dynamic behavior of a rotating object (asymmetric top) and analyzing its stability and motion over time. Additionally, the mention of a thumbtack on an inclined plane may involve questions of equilibrium and forces acting on the rigid body in a gravitational field.
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