Motional emf with gravity as the pulling force

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SUMMARY

The discussion focuses on calculating the induced electromotive force (emf) and current in a square loop subjected to gravitational force while partially immersed in a magnetic field. The induced emf is determined using the formula emf = Blv, where B is the magnetic field strength, l is the side length of the loop, and v is the velocity. The magnetic force opposing gravity is expressed as magnetic force = vb - mg, leading to the conclusion that at equilibrium, vb equals 2mg, resulting in the velocity v = 2mg / B. The participant also explores the relationship between gravitational and magnetic forces to derive the loop's velocity as a function of time.

PREREQUISITES
  • Understanding of Faraday's Law of Induction
  • Knowledge of magnetic force equations, specifically FM = I l x B
  • Familiarity with basic mechanics, particularly Newton's laws of motion
  • Concept of induced current in electromagnetic systems
NEXT STEPS
  • Study the implications of Faraday's Law in different geometries of loops
  • Learn about the dynamics of charged particles in magnetic fields
  • Explore the relationship between induced emf and resistance in circuits
  • Investigate the effects of varying magnetic fields on induced currents
USEFUL FOR

Physics students, electrical engineers, and educators interested in electromagnetism and its applications in mechanical systems.

darkpsi
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Homework Statement


A square loop of mass m resistance R and side l] is halfway inside a magnetic field pointing into the page. It is then released from rest and gravity pulls it out of the magnetic field.
a) Calculate the induced emf and the current as functions of the velocity.
b) Calculate the magnitude and direction of the magnetic force.
c) At some time the magnetic force will be equal to the gravitational force, calculate the velocity of the loop at this time.
d) Calculate the velocity of the loop as a function of time.


Homework Equations


induced emf = -d(phi)/dt
phi = integral(B * da)
V= emf = IR
magnetic force = qv X B (I think there are two components so this one is in the direction opposite gravity?)



The Attempt at a Solution


a)
I'm pretty confident I figured out the emf and current that are induced.
Since:
da = l*v (with v = -dx/dt)
so:
d(phi)/dt = -Blv and emf = Blv
then:
I = Blv / R

b)
for the magnetic force the component opposing the graviational pull is in the positive x direction and is equal to the force of gravity in magnitude so it is equal to:
=-mg
and then there is a horizontal component that is allowing the charges to move in the positive y direction (or collectively counter-clockwise) with magnitude:
=vb per unit charge q
so finally:
magnetic force = vb - mg

I'm not so sure how to compute the direction unless I just described it like I have just now
I tried using the fact that the components form a triangle and saying:
tan(theta) = -vb/mg but I'm sure this isn't the way to go about it.

c)
I set the gravitational pull equal to the magnetic force so:
vb - mg = mg; vb = 2mg so:
v = 2mg / B

d)
I tried using f= ma and saying:
gravitational force - magnetic force= mg - VB + mg = ma
so:
a = 2g - vB/m
but if I tried to find the velocity and integrated I would get and answer that doesn't depend on time and that doesn't even involve gravity which puzzles me.

Any help at all would be greatly appreciated
 
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darkpsi said:
magnetic force = qv X B (I think there are two components so this one is in the direction opposite gravity?)
The v in the equation that you have is the velocity of a charge carrier in a magnetic field. You don't want that. You need to use FM = I l x B where I is the induced current (your expression for I is correct.)
 

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