Proof dealing w/ Simple Harmonic Oscillations

[nix]

Prove that the period of a simple pendulum doing small oscillations is equal to:

2(py)x(square root of: l/g)

where py is 3.14..(obviously..lol)... l is length of the string of the pendulum and g is gravity

Also.... the pendulum is basically just a ball on a string moving from side to side. and the equations we have been given to solve it is the fundamental eq. of an oscillation:

k = mw^2 = m x(2py^2/T) = m (2(py)f^2)

where f is the frequency, m is the mass, w is omega (the angle), and k is the spring constant and T is period

tricky..eh?

thanks for any help or suggestions..

[nix]

oops i just read the thing i was supposed to read before posting...

anyways this is what ive done and i dont think it makes sense maybe i should clarify the question with my teacher later..

m(2(py)^2/T) = m(2(py)f^2)

T = m(2(py)^2)/m(2(py)f^2)
T = py/f^2

f = 1/T

T = (py)T^2..maybe im using the wrong equation...

And another thing about the question is that the angle is less than or equal to 5 degrees...the angle btw the original position of the pendulum and the position of the pendulum when its movind to the side.

[himanshu121]

T = py/f^2

f = 1/T
First equation has got wrong dimensions whereas second equation is correct.

Equations which might help u are
\omega^2 = \frac{k}{m}
\omega=2\pi f
T=\frac{2\pi}{\omega}
kl=mg

All equations are valid for small angle \theta\leq 5^0

[nix]

thanks so much for the help with the equations...i got it! yay!

but can you explain to me how kl = mg...

thanks again
[:D]

[himanshu121]

That requires u to know the Force equation
i.e. F=-mgsin\theta
for small theta sin\theta = \theta
therefore the equation is F=-m\theta = -\frac{mgx}{l}
displacement along the arc=\theta l

also if u draw a free body diagram fo the forces . u have
k(l+\delta x)=mgcos\theta for small displacement u can assume \delta x=0 & cos\theta=1
so u get kl=mg