Magnetic Torque on Dipole; Oscillating Magnet question

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SUMMARY

The discussion focuses on calculating the angular frequency of a cylindrical bar magnet with a magnetic dipole moment of <5, 0, 0> A·m², suspended in a magnetic field of <1.4, 0, 0> T. The angular frequency is derived using the formula ω = √(μB/I), where I is the moment of inertia calculated as I = (mass * length²) / 12. The discussion also explores how the angular frequency changes when the magnetic field strength is increased to <2.8, 0, 0> T, emphasizing the relationship between magnetic torque and angular frequency.

PREREQUISITES
  • Understanding of magnetic dipole moment and its representation
  • Familiarity with the concept of torque in magnetic fields
  • Knowledge of moment of inertia for cylindrical objects
  • Basic principles of oscillatory motion and angular frequency
NEXT STEPS
  • Calculate angular frequency for different magnetic field strengths using ω = √(μB/I)
  • Explore the effects of varying the magnetic dipole moment on oscillation frequency
  • Investigate the relationship between torque and angular displacement in magnetic systems
  • Learn about the applications of oscillating magnets in electromagnetic devices
USEFUL FOR

Physics students, educators, and engineers interested in magnetism, oscillatory motion, and the dynamics of magnetic dipoles in external fields.

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Homework Statement


A cylindrical bar magnet whose mass is 0.08 kg, diameter is 1 cm, length is 3 cm, and whose magnetic dipole moment is <5, 0, 0> A · m2 is suspended on a low-friction pivot in a region where external coils apply a magnetic field of <1.4,0,0> T

You rotate the bar magnet slightly in the horizontal plane and release it. (For small angles in radians, assume
sin(θ) ≈ θ.)

a) What is the angular frequency of the oscillating magnet?

b) What would be the angular frequency if the applied magnetic field were <2.8,0,0> T?

Homework Equations


τ[/B] = μ × B
τ = μBsinθ
ω
= qB/m
μ
= IA

The Attempt at a Solution



My first instinct was to find the magnetic torque on the magnet, using the magnet's dipole moment and the applied magnetic field, but that gives zero.
 
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If you had just left it sitting as is, it would be zero since the magnetic dipole moment and applied magnetic field are in the same direction. But then, the problem statement says that you rotate it in the horizontal plane which presumptively is giving one of the other axes some value. It's hard to say which without a picture of the problem or defining how the magnet is oriented, but it's probably the y component.
 
I figured it out. Using the moment of inertia, I, for a cylinder, you can find the angular frequency of the spinning magnet.
I = (mass*length2) /12

Solve for I and use it and μ & B to solve for ω.

ω = √(μB/I)
 
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