Find the frequency of the oscillation of a horizontal beam.

AI Thread Summary
The discussion focuses on finding the frequency of oscillation for a uniform meter stick pivoted at one end and held horizontally by a spring. The torque equation is established using the spring force and the torque from the center of mass, leading to the equation ∑τ = Iθ'' = -kL²θ - mgL/2. The contributor expresses confusion about solving the differential equation due to the presence of gravity, which complicates the oscillatory motion. Another participant clarifies that the gravitational term is a constant, and the solution will still be sinusoidal, affecting only the equilibrium position, not the frequency. Ultimately, the key takeaway is that the frequency remains unchanged despite the additional gravitational force in the system.
Ishaan S
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Homework Statement



A uniform meter stick of mass M is pivoted on a hinge at one end and held horizontal by a spring with spring constant k attached at the other end. If the stick oscillates up and down slightly, what is its frequency? [Hint: Write a torque equation about the hinge.] The length of the beam is 1.25 m.

Homework Equations



τ = Iα

Fspring = -kx

The Attempt at a Solution



I have found the question online and have linked it to this comment in case someone needs to see a picture of the scenario.

I started by writing a torque equation, with the beam angled θ above the horizontal and x being the displacement of the spring tip above the horizontal.

The torques about the pivot on the wall on the stick, using the small angle approximation, are:

1) The spring exerts a force, -kx = -kLθ , a distance, L, away from the pivot. Thus, the torque exerted by the spring is, for small angles, -kxL2θ.

2) The center of mass exerts a torque, given by -mgL/2.

The torque equation is. therefore, ∑τ = Iθ'' = -kL2θ - mgL/2.

This is where I was stuck. I don't know how to solve differential equations beyond separable ones as of yet. The book I am using shows that the solution to a simple harmonic oscillator's equation of motion is just a sinusoid; however, this does not seem like a simple oscillator as there is gravity in this system, which is odd as this is the simple oscillatory section of my book.

I tried substituting a function of cosine; however it does not seem to work. If anyone could shed light as to what I did incorrectly or what I am overlooking, it would be greatly appreciated.

Thank you in advance.
 

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I forgot to mention, the problem in the attachment is number 5.
 
Consider the function y=sin(x)+47

When you differentiate, the constant will just disappear, so the function will be a solution to y''= -(y-47)

You could do this more generally to find the solution of y'' = -C1y+C2 (which is the form of your equation) but I just wanted to make a point.

mgL/2 is just a constant, so the solution to your equation will be a sinusoid plus a constant. Adding a constant doesn't affect the frequency of oscillation (it just shifts the equilibrium position which it is oscillating about).
 
Ok. Thank you very much. I get it now.
 
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