Electrodynamic Tether experiement

  • Thread starter Thread starter shubhankar1
  • Start date Start date
  • Tags Tags
    Electrodynamic
AI Thread Summary
Electrodynamic tether experiments in low Earth orbit aim to generate electricity using the equation ε=Bvl. However, the magnetic field (B) is not constant along the tether's path, complicating emf calculations. To accurately determine the emf, one must integrate the varying magnetic field over the length of the tether, leading to the equation ε = ∫_a^b B(s) v(s) ds. This approach accounts for the changes in both velocity and magnetic field along the tether's trajectory. Understanding this integration is crucial for effective tether design and energy generation.
shubhankar1
Messages
1
Reaction score
0
I was reading about the electrodynamic tether experiments in low Earth orbits to generate electricity. I had a doubt regarding the mathematics that went behind calculating the emf across the tether. I read further and i realized they use the equation ε=Bvl, but the problem with this is that the B is not constant throughout all points in orbit. So how do you find the emf across the tether in this case where there is relative motion with velocity v and B changes at all points in the path of the wire?
 
Physics news on Phys.org
Integrate over the length of the wire.

##\epsilon = \int_a^b B(s) v(s) ds##
 
Thread 'Motional EMF in Faraday disc, co-rotating magnet axial mean flux'
So here is the motional EMF formula. Now I understand the standard Faraday paradox that an axis symmetric field source (like a speaker motor ring magnet) has a magnetic field that is frame invariant under rotation around axis of symmetry. The field is static whether you rotate the magnet or not. So far so good. What puzzles me is this , there is a term average magnetic flux or "azimuthal mean" , this term describes the average magnetic field through the area swept by the rotating Faraday...

Similar threads

Back
Top