The inverted pendulum shown consists of a

uniform rod of length L and mass M hinged at its base. A spring is
attached a distance h from the pendulum’s pivot and has a spring
constant k. At equilibrium the pendulum is perfectly vertical. For
small amplitude oscillations from equilibrium, find the frequency of this
pendulum.

To find the frequency of the pendulum for small amplitude oscillations from equilibrium, we can use the principles of simple harmonic motion. Here's how you can find the frequency:

1. Start by identifying the restoring force acting on the pendulum. In this case, the restoring force comes from both the gravitational force and the spring force.

2. The gravitational force tries to bring the pendulum back to its equilibrium position, while the spring force opposes the displacement from equilibrium. Since the pendulum is assumed to have small amplitude oscillations, we can consider the restoring force to be linearly proportional to the displacement from equilibrium.

3. Write down the equation for the restoring force. The force due to gravity is given by F_gravity = M * g * h, where M is the mass of the pendulum and h is the distance from the pivot to the center of gravity. The spring force is given by F_spring = -k * x, where k is the spring constant and x is the displacement from equilibrium.

4. Since the motion is simple harmonic, we can write the equation of motion as F = -k * x = -m * d^2x/dt^2, where m is the effective mass of the system and d^2x/dt^2 represents the second derivative of x with respect to time.

5. Rewrite the equation using the given parameters. In this case, the effective mass of the system can be approximated as m = M * L^2, where L is the length of the rod. Therefore, we have -k * x = -(M * L^2) * d^2x/dt^2.

6. Simplify the equation by canceling out the negative signs and rearranging. This gives us k * x = (M * L^2) * d^2x/dt^2.

7. Solve the differential equation by assuming a solution of the form x = A * cos(ω * t), where A is the amplitude of the motion and ω is the angular frequency.

8. Substitute this assumed solution into the equation and solve for ω. This involves taking the second derivative of x with respect to time and substituting it back into the equation.

9. After solving for ω, the angular frequency, the frequency of the pendulum can be calculated using the formula f = ω / (2 * π).

By following these steps, you can find the frequency of the pendulum for small amplitude oscillations from equilibrium.

To find the frequency of the pendulum for small amplitude oscillations, we can use the equation for the period of a simple pendulum.

The period T of a simple pendulum is given by the formula:

T = 2π √(L/g)

where L is the length of the pendulum and g is the acceleration due to gravity.

In this case, since the pendulum is inverted and in equilibrium at a perfectly vertical position, the equilibrium position is when the spring is stretched by a distance h. Therefore, the effective length of the pendulum is L + h.

So, the period T of the inverted pendulum is given by:

T = 2π √((L + h)/g)

Now, to find the frequency f, which is the reciprocal of the period, we can use the formula:

f = 1/T

Substituting the value of T, we get:

f = 1/(2π √((L + h)/g))

Therefore, the frequency of the pendulum for small amplitude oscillations is:

f = 1/(2π √((L + h)/g))

Note: This formula assumes small amplitude oscillations and neglects any damping effects or non-linear behavior of the spring.