Why is the magnetic force directed downward in this scenario?

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SUMMARY

The discussion centers on the direction of the magnetic force in a non-uniform magnetic field, specifically why it is directed downward despite initial expectations based on the right-hand rule. The key equations involved are the potential energy equation, E = -μ · B, and the force equation, F = -∇E. The torque τ = μ × B indicates that a magnetic dipole experiences torque but no net force in a uniform field. The force arises from the dipole moving towards regions of stronger magnetic fields, leading to a decrease in potential energy.

PREREQUISITES
  • Understanding of magnetic dipoles and their behavior in magnetic fields
  • Familiarity with the right-hand rule for determining force direction
  • Knowledge of potential energy concepts in physics
  • Basic grasp of vector calculus, particularly gradients
NEXT STEPS
  • Study the implications of torque in magnetic fields using the equation τ = μ × B
  • Explore the concept of potential energy in magnetic systems, focusing on E = -μ · B
  • Learn about the behavior of magnetic dipoles in non-uniform magnetic fields
  • Investigate the mathematical foundations of gradients in vector calculus
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Physics students, educators, and professionals in electromagnetism who seek to understand the behavior of magnetic forces and dipoles in varying magnetic fields.

Amaelle
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Good day All!
while trying to solve this question
coil 1.png

I use the right hand rule and according to it the Force should be directed outward (pointing toward me)
but here is the answer that puzzeld me
coil 2.png


I really don't get why it is down , and would feel very grateful if someone can explain me the reason
thanks in advance!
 

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The way I know how to work this one is to use potential energy ## E=-\mu \cdot B ##, and use the force ## F=-\nabla E ##. The first equation comes about because torque ## \tau=\mu \times B ## with a ## \sin(\theta) ## in the cross product, and the integral of ## E=\int \tau \, d \theta ## gives the ## \cos(\theta) ## which comes in the dot product ## E=- \mu \cdot B ##. ## \\ ## In a uniform magnetic field, a magnetic dipole can experience a torque, but no net force. The force is a result of the non-uniform magnetic field. In simple terms, the equation ## E=-\mu \cdot B ## will result in an attraction of a magnetic moment that is aligned with the magnetic field to a region of stronger magnetic field, because the potential energy ## E ## at the region of stronger magnetic field is more negative. The second equation ## F=-\nabla E ## is a quantitative expression of what I have just described qualitatively. ## \\ ## Notice also, if the magnetic moment is anti-parallel with the field, the dot product will make ## \cos(180^o)=-1 ##, and the potential energy ## E ## will be more positive if you move to a region of stronger magnetic field ## B ##.
 
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Thanks a lot!
 
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