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

AI Thread Summary
A conducting bar on rails experiences forces due to a magnetic field, leading to a differential equation for its velocity. The initial speed of the bar is 64.0 m/s, and it is subjected to a magnetic field of 1.3 T with a resistance of 30.0 Ohms. The discussion emphasizes the need to set up the correct differential equation, which relates the force to the current and magnetic field. Participants clarify that the integration process must be approached carefully, as previous assumptions about constants and variables were incorrect. The focus remains on accurately deriving the expression for the bar's velocity over time.
krh68
Messages
2
Reaction score
0
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.
 
Physics news on Phys.org
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.
 
Kindly see the attached pdf. My attempt to solve it, is in it. I'm wondering if my solution is right. My idea is this: At any point of time, the ball may be assumed to be at an incline which is at an angle of θ(kindly see both the pics in the pdf file). The value of θ will continuously change and so will the value of friction. I'm not able to figure out, why my solution is wrong, if it is wrong .
Thread 'Correct statement about a reservoir with an outlet pipe'
The answer to this question is statements (ii) and (iv) are correct. (i) This is FALSE because the speed of water in the tap is greater than speed at the water surface (ii) I don't even understand this statement. What does the "seal" part have to do with water flowing out? Won't the water still flow out through the tap until the tank is empty whether the reservoir is sealed or not? (iii) In my opinion, this statement would be correct. Increasing the gravitational potential energy of the...
Thread 'A bead-mass oscillatory system problem'
I can't figure out how to find the velocity of the particle at 37 degrees. Basically the bead moves with velocity towards right let's call it v1. The particle moves with some velocity v2. In frame of the bead, the particle is performing circular motion. So v of particle wrt bead would be perpendicular to the string. But how would I find the velocity of particle in ground frame? I tried using vectors to figure it out and the angle is coming out to be extremely long. One equation is by work...
Back
Top