Pendulum with horizontal spring

AI Thread Summary
The discussion focuses on calculating the angular frequency of a pendulum system involving a mass connected to a spring. The user attempts to derive the equation for angular frequency by equating gravitational and spring torques but encounters a dependency on the angle theta, which should be constant for small oscillations. The user correctly identifies that for small angles, sin(theta + π/2) simplifies to cos(theta), which equals 1. The confusion arises in the formulation of the torque equations, leading to an incorrect dependency on theta. Clarification is sought on resolving this issue to achieve a constant angular frequency.
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Homework Statement



A 5kg sphere is connected to a thin massless but rigid rod of length L=1.3 m to form a simple pendulum. The rod is connected to a nearby vertical wall by a spring with a spring constant k= 75N/m, connected to it at a distance h=1.1 m below the pivot point of the pendulum. What is the angular frequency (in rad/s) of the system for small amplitude oscillations.



Homework Equations



\alpha = \omega2*\theta
I=m*r2
Torque=f*d*sin\theta

or small oscillations, sin\theta=\theta and cos\theta=1



The Attempt at a Solution



sum the torque and set them equal to \alphaI

gravitational torque= Lmg\theta

if theta is the angle between the rod and its equilibrium position, the angle of the spring torque is (theta + \pi/2), so the spring torque is
f*d*sin(theta + \pi/2). The force is k*\Deltax, or h*sin(theta + \pi/2) and the distance is h, giving

torque from spring =k*h2*sin\theta*sin(theta + \pi/2)
or k*h2*\theta*(theta + \pi/2)

My final equation is

mL2\omega2tex]\theta[/tex] = Lmg\theta + k*h2*\theta*(theta + \pi/2)

The problem is that this gives me a \omega that is dependant on \theta, which isn't possible. It should be constant. Can someone please tell me where I'm going wrong?

 

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sin(theta+pi/2)= cos(theta). For small angles, cos(theta) =1.

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