Magnetic Force, Resistance, Faraday's Law

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SUMMARY

The discussion focuses on calculating the speed of a conducting bar in a magnetic field using Faraday's Law and related equations. The conducting bar has a length of 0.218 m, mass of 0.08 kg, and is subjected to a magnetic field of 2.2 T with a resistor of 20.0 Ohms. The initial speed is 42.0 m/s, and the user attempts to derive the velocity at t = 15.303 s and the distance traveled before coming to rest. The calculations involve integrating the forces and applying logarithmic functions to solve for velocity.

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  • Understanding of Faraday's Law of Electromagnetic Induction
  • Knowledge of Ohm's Law and its application in circuits
  • Familiarity with basic calculus, particularly integration
  • Concepts of magnetic force and motion in a magnetic field
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  • Review the derivation of Faraday's Law and its applications in electromagnetic systems
  • Learn about the integration techniques for solving differential equations in physics
  • Explore the relationship between magnetic fields and induced electromotive force (EMF)
  • Study the dynamics of motion under the influence of magnetic forces and resistive forces
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Students and educators in physics, particularly those studying electromagnetism and dynamics, as well as anyone involved in solving problems related to magnetic forces and motion in conductive materials.

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Homework Statement


A conducting bar of length L = .218 m and mass M = .08 kg lies across a pair of conducting rails. The contact friction between the bar and the rails is negligible, but there is a resistor at one end with a value R = 20.0 Ohms. Initially the rod is given an initial speed of v0 = 42.0 meters per second. There is a uniform magnetic field perpendicular to the plane containing the rod and rails of magnitude B = 2.2 T.
What is the speed of the rod at time t = 15.303 s?
How far does the rod slide before coming to rest?

Homework Equations


F=ILB
Ohm’s law: I=V/R
Faraday’s law: V = dΦ/dt = B(dA/dt)

The Attempt at a Solution


dA = Ldx, giving V=BL(dx/dt)=BLv

F=BLv/R(LB)=(B^2)(L^2)v/R
F=ma=m(dv/dt)
(B^2)(L^2)v/R= m(dv/dt)

If I rearrange this I get:
(B^2)(L^2)/R dt= m/v dv

Taking the integrals of both sides gives:
(B^2)(L^2)t/R (from t=0 to t=t) = m*ln(v) (from v0 to v)
So…
(B^2)(L^2)t/R = m*ln(v) – m*ln(v0)

Solve for v:
v= e^[(B^2)(L^2)t/(Rm)+ln(v0)]

When I put in the numbers I’m not getting the right answer. Is what I did right? Is there something that I’m doing wrong?

Regarding the question on how far the bar goes...I'm guessing that once I get the right equation for velocity, I would set v=0 and solve for t. Then integrate v to find and equation for position and use the t to solve for it. Is this right?

Thanks in advance for any help.
 
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good problem, i think. not sure why you haven't some help. Likely tomorrow am.
 

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