where g=9.8 m/s, mc is the cart's mass, m is the mass of the pole, I is the half length of the pole, and u is the applied force. a) b) Find a linearized state equation if the desired equilibrium value for each state is zero. Find a linearized state equation if it is desired to position the pendulum at a 45°.

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**Problem 2.** Consider the inverted pendulum on a cart given in Figure 1.

![Inverted pendulum schematic.](image)

**Figure 1.** Inverted pendulum schematic.

The state variables for this system can be defined to be: \( x_1(t) = \theta(t) \), \( x_2(t) = \dot{\theta}(t) \). Assume that the equation of motion for the pendulum can be written as follows:

\[
\begin{bmatrix}
\dot{x}_1 \\
\dot{x}_2
\end{bmatrix}
=
\begin{bmatrix}
x_2 \\
\frac{g \sin(x_1)}{l \left(\frac{4}{3} - \frac{m \cos^2(x_1)}{m_c + m}\right)} + \frac{\cos(x_1)}{l \left(\frac{4}{3} - \frac{m \cos^2(x_1)}{m_c + m}\right)} u
\end{bmatrix}
\]

**Explanation:**

- **Diagram:** The figure shows a schematic of an inverted pendulum mounted on a cart. The cart moves horizontally, and the pendulum pivots about its base, depicting the angle \( \theta = x_1 \).
  
- **Forces:** The forces acting on the pendulum include gravitational force \( mg \sin \theta \) and control input \( u \) which affects the motion of the cart.

- **Variables:**
  - \( x_1(t) = \theta(t) \): Angle of the pendulum with the vertical.
  - \( x_2(t) = \dot{\theta}(t) \): Angular velocity of the pendulum.

- **Equation of Motion:** Describes how the system evolves over time, considering both the gravitational force and external input \( u \). The complexity arises from the terms involving trigonometric functions \( \sin(x_1) \) and \( \cos(x_1) \), reflecting the pendulum's rotation dynamics.
Transcribed Image Text:**Problem 2.** Consider the inverted pendulum on a cart given in Figure 1. ![Inverted pendulum schematic.](image) **Figure 1.** Inverted pendulum schematic. The state variables for this system can be defined to be: \( x_1(t) = \theta(t) \), \( x_2(t) = \dot{\theta}(t) \). Assume that the equation of motion for the pendulum can be written as follows: \[ \begin{bmatrix} \dot{x}_1 \\ \dot{x}_2 \end{bmatrix} = \begin{bmatrix} x_2 \\ \frac{g \sin(x_1)}{l \left(\frac{4}{3} - \frac{m \cos^2(x_1)}{m_c + m}\right)} + \frac{\cos(x_1)}{l \left(\frac{4}{3} - \frac{m \cos^2(x_1)}{m_c + m}\right)} u \end{bmatrix} \] **Explanation:** - **Diagram:** The figure shows a schematic of an inverted pendulum mounted on a cart. The cart moves horizontally, and the pendulum pivots about its base, depicting the angle \( \theta = x_1 \). - **Forces:** The forces acting on the pendulum include gravitational force \( mg \sin \theta \) and control input \( u \) which affects the motion of the cart. - **Variables:** - \( x_1(t) = \theta(t) \): Angle of the pendulum with the vertical. - \( x_2(t) = \dot{\theta}(t) \): Angular velocity of the pendulum. - **Equation of Motion:** Describes how the system evolves over time, considering both the gravitational force and external input \( u \). The complexity arises from the terms involving trigonometric functions \( \sin(x_1) \) and \( \cos(x_1) \), reflecting the pendulum's rotation dynamics.
where \( g = 9.8 \, \text{m/s}^2 \), \( m_c \) is the cart's mass, \( m \) is the mass of the pole, \( l \) is the half length of the pole, and \( u \) is the applied force.

a) Find a linearized state equation if the desired equilibrium value for each state is zero.

b) Find a linearized state equation if it is desired to position the pendulum at a \( 45^\circ \).
Transcribed Image Text:where \( g = 9.8 \, \text{m/s}^2 \), \( m_c \) is the cart's mass, \( m \) is the mass of the pole, \( l \) is the half length of the pole, and \( u \) is the applied force. a) Find a linearized state equation if the desired equilibrium value for each state is zero. b) Find a linearized state equation if it is desired to position the pendulum at a \( 45^\circ \).
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