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TFM
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Homework Statement
A compass, consisting of a small bar magnet resting on a frictionless pivot through its centre, is placed in the middle of a long solenoid, which in turn is aligned with its axis pointing North-South. With a current of 1 Amp passing through the solenoid, a small displacement of the compass from its equilibrium orientation causes it to oscillate with a period of 2 seconds. If a current of 2 Amps is used, the restoring torque is zero and the period is infinite. Calculate the period of the oscillation when no current flows in the solenoid.
Homework Equations
Magnetic Field in a solenoid:
[tex] B=\mu_0 nI [/tex]
Where B is the magnetic field, n the number of coils, and I the current
Magnetic Force:
[tex] F = q(E+v\times B) [/tex]
Torque on a magnetic dipole:
[tex] G = m\times B [/tex]
where G is torque
Torque:
[tex] torque = I\alpha [/tex]
where I is the Moment of inertia
Oscillation:
[tex] x = A cos(\omega_0t + \phi) [/tex]
[tex] v = A\omega sin(\omega_0t + \phi) [/tex]
[tex] a = -A\omega^2 cos(\omega_0t + \phi) [/tex]
[tex] \omega_0^2 = \frac{k}{m} [/tex]
The Attempt at a Solution
The equation doesn't give you some of the required variables for the formulas I believe you need; most importantly, it doesn't give you the number of coils, so you can work out the B field.
So far, I have divided it into sections:
1 Amp:
[tex] B = \mu_0 n*1 [/tex]
[tex] G = m\times \left(\mu_0 n*1 \right) [/tex]
2 Amp:
[tex] B = \mu_0 n*2 [/tex]
[tex] G = m\times \left(\mu_0 n*2 \right) [/tex]
0 Amp:
[tex] B = \mu_0 n*0 = 0 [/tex]
There is no B field with no current
[tex] G = m\times \left(\mu_0 n*0 \right) [/tex]
No torque from magnetic dipole
does this look at all right?
TFM