In Example (1.21), investigate the stability of the two additional equilibrium points in the case \(\omega^{2} \sin \alpha>g / a\).

Short Answer

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Answer: To investigate the stability of the two additional equilibrium points in Example (1.21), follow these steps: 1. Identify the problem. 2. Determine the equilibrium points and equations of motion. 3. Linearize the equations of motion near equilibrium points. 4. Study the behavior of the linearized equations of motion. 5. Analyze the stability of the system.

Step by step solution

01

Identify the problem

We are given an inequality \(\omega^{2} \sin \alpha > g / a\), and the task is to investigate the stability of the additional equilibrium points. This would require us to identify the system's equations of motion and the equilibrium points first.
02

Determine the equilibrium points, and equations of motion

For this step, further information on the exact physical system and its corresponding equations of motion are needed. Based on the mention of \(\omega\), it is likely to involve pendulum motion, and a complete set of equations of motion can be obtained from considering kinetic and potential energy expressions. The identified equilibrium points will depend on the specific system and given parameters. For example, assuming a pendulum, there might be equilibrium points at the bottom and top of the motion.
03

Linearize the equations of motion

Once we have the equations of motion for the given problem, we will need to linearize them near the equilibrium points. That is, we will find out how the equations of motion behave when they are slightly perturbed from their equilibrium points. We can use the small-angle approximation and Taylor series expansion for this purpose.
04

Study the behavior of linearized equations of motion

After linearizing the equations of motion, we can now study their stability. We can analyze the behavior of the linearized equations by studying the Jacobian by evaluating the Jacobian matrix at the equilibrium points. Then, we can determine its eigenvalues, which will help us to infer the stability of the equilibrium points.
05

Analyze the stability of the system

Using the eigenvalues found in Step 4, we can analyze the stability of the equilibrium points. If the real part of all eigenvalues is negative, the equilibrium point is stable (attracting). If the real part of one or more eigenvalues is positive, the equilibrium point is unstable (repelling). If there are complex eigenvalues, their phases can give insights into the oscillatory nature of the system (e.g., stable spiral or unstable spiral). In conclusion, to investigate the stability of the two additional equilibrium points as given in Example (1.21), follow these five steps: 1. Identify the problem 2. Determine the equilibrium points and equations of motion 3. Linearize the equations of motion near equilibrium points 4. Study the behavior of the linearized equations of motion. 5. Analyze the stability of the system.

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Most popular questions from this chapter

Suppose that the matrix \(H\) in \((1.5)\) is given by $$ H=\frac{1}{\sqrt{6}}\left(\begin{array}{ccc} \sqrt{2} & \sqrt{2} & \sqrt{2} \\ -2 & 1 & 1 \\ 0 & -\sqrt{3} & \sqrt{3} \end{array}\right) $$ Check that \(H^{\mathrm{t}} H=H H^{\mathrm{t}}=I\). Write down the components of \(\boldsymbol{e}_{1}\), \(e_{2}\), and \(e_{3}\) in \(\tilde{T}\), and the components of \(\tilde{e}_{1}, \tilde{e}_{2}\), and \(\tilde{e}_{3}\) in \(\mathcal{T}\).

A sphere of radius \(a\) is rolling without slipping on a rough horizontal plane in such a way that its centre traces out a horizontal circle, radius \(b\) and centre \(O\), with constant angular speed \(\Omega\). Let \((i, j, k)\) be an orthonormal triad with \(k\) vertical and \(i\) in the direction from \(O\) to the centre of the sphere. Show that the angular velocity of the sphere relative to the plane satisfies $$ \boldsymbol{\omega}=n \boldsymbol{k}-\frac{b}{a} \Omega i $$ where \(n=\boldsymbol{\omega} \cdot \boldsymbol{k}\). Show that if \(n\) is constant, then the locus of the point of contact on the sphere is a circle. What is its radius?

A plastic ball is held at the bottom of a bucket of water and then released. As it is released, the bucket is dropped over the edge of a cliff. What happens?

Establish the properties of the line \(L\) defined by \((1.41)\) for the general motion of a rigid body. That is, show that if \(P\) is a point of \(L\), then \(\boldsymbol{v}_{P}\) is proportional to \(\omega\); and show conversely that if \(v_{P}\) is proportional to \(\omega\), then \(P\) lies on \(L\). (Assume that \(\omega \neq 0\).)

\({ }^{\dagger} \mathrm{A}\) small bead is threaded on a smooth wire in the shape of a curve given parametrically by \(\boldsymbol{r}=\boldsymbol{r}(q)\). The wire rotates with constant angular velocity about a vertical axis. Show that $$ \frac{\mathrm{d}}{\mathrm{d} t}\left[\frac{1}{2} \dot{q}^{2} \frac{\mathrm{d} \boldsymbol{r}}{\mathrm{d} q} \cdot \frac{\mathrm{d} \boldsymbol{r}}{\mathrm{d} q}\right]=\dot{q} \frac{\mathrm{d} \boldsymbol{r}}{\mathrm{d} q} \cdot \ddot{\boldsymbol{r}} $$ where the dot is the time derivative relative to a frame rotating with the wire, and \(\boldsymbol{r}\) is measured from an origin on the axis Deduce that $$ \frac{\mathrm{d} \boldsymbol{r}}{\mathrm{d} q} \cdot \frac{\mathrm{d} \boldsymbol{r}}{\mathrm{d} q} \dot{q}^{2}-(\boldsymbol{\omega} \wedge \boldsymbol{r}) \cdot(\boldsymbol{\omega} \wedge \boldsymbol{r})-2 \boldsymbol{g} \cdot \boldsymbol{r}=\text { constant. } $$ Does this result still hold when the axis of rotation is not vertical?

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