How Does a Conducting Bar on Rails Behave in a Magnetic Field?

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Homework Help Overview

The discussion revolves around the behavior of a conducting bar on rails within a magnetic field, specifically focusing on the dynamics of the bar as it moves under the influence of electromagnetic forces. The problem involves concepts from electromagnetism and mechanics, including forces, induced electromotive force (emf), and differential equations.

Discussion Character

  • Exploratory, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the need to set up a differential equation to describe the motion of the bar, questioning the applicability of constant acceleration equations. There are attempts to express the relationship between force, current, and velocity, leading to a differential equation form. Some participants express confusion regarding the integration process and the meaning of certain variables introduced in the discussion.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the equations involved. Some guidance has been provided regarding setting up the differential equation, but there is no consensus on the correct expression or the integration process. Participants are actively questioning each other's reasoning and seeking clarification on specific terms and steps.

Contextual Notes

Participants note the complexity of the problem due to the non-constant acceleration and the need for a proper understanding of the changing area in the magnetic flux calculation. There is also mention of the resistor's role and the initial conditions provided in the problem statement.

krh68
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A conducting bar of length L = 21.2 cm and mass M = 60.0 g 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 = 30.0 Ohms. Initially the rod is given an initial speed of v0 = 64.0 meters per second. There is a uniform magnetic field perpendicular to the plane containing the rod and rails of magnitude B = 1.3 T.
What is the speed of the rod at time t = 26.068 s?

I know:
v=v0 + at
F=ma
F=iLB
i=(emf)/R
emf = dflux/dt
flux = BA

I know I need to solve for the area to get the flux and the length (L) is constant while the width is changing but I don't understand how to get the integral or set up the integral for the width. Please help ASAP.
 
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v = v0+at is out of the picture. This is not a constant acceleration situation. All your other equations are relevant.
You need to set up a differential equation and solve it. Start with

F = m (dv/dt)

Replace F with iLB and then replace i with (1/R)(dΦ/dt). The expression for dΦ/dt is proportional to v. So you end up with the differential equation that is essentially

dv/dt = (const)v

You should be able to find what "const" is and to integrate the above equation.
 
Okay, so dv/dt = v(const) or dv/dt = v(LB/mR)
I still don't know how to solve for v.
When I integrate dv/dt, do I get r(LB/mR)? and if so, what is r?
 
krh68 said:
Okay, so dv/dt = v(const) or dv/dt = v(LB/mR)
This is incorrect. Please show how you got it, then I can point out where you went wrong.
I still don't know how to solve for v.
Worry about that later. First get the correct expression for dv/dt.
When I integrate dv/dt, do I get r(LB/mR)?
No, you do not.
and if so, what is r?
I don't know, but r it appears in your expression above. You made it up so you should know what it represents.
 

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