**10. Review Conceptual Example 3 and Figure 22.7b. A conducting rod slides down between two frictionless vertical copper tracks at a constant speed of 4.0 m/s perpendicular to a 0.50-T magnetic field. The resistance of the rod and tracks is negligible. The rod maintains electrical contact with the tracks at all times and has a length of 1.3 m. A 0.75- resistor is attached between the tops of the tracks. (a) What is the mass of the rod? (b) Find the change in the gravitational potential energy that occurs in a time of 0.20 s. (c) Find the electrical energy dissipated in the resistor in 0.20 s.

 

Since the speed of the mass falling is constant and we know gravity is acting, the magnetic force must be acting up to oppose gravity and produce a zero acceleration.  Now, the current is induced as shown can also be determined by using Lenz’s law which says that the induced current must create a magnetic field which opposes the change in magnetic flux.  Since as the rod falls the loop it makes electrically must be getting larger, the constant magnetic field passing through an increasing area must make a larger magnetic flux.  So the induced current must create a magnetic field that is opposing the external field in an attempt to keep the magnetic flux constant.  So the induced current must go the direction as shown so that its magnetic field is opposite to the external magnetic field.  Again using the right hand rule!

 

Magnetic force is gotten from

Magnitude of this is

 

Angle is 90° as L is in the direction of the current which is perpendicular to B in the is case.

 

We can get current from Ohm’s law

We get emf from

So current is

And magnetic force is

Now we can find mass using sum of forces

 

 

Solving for mass

 

 

Change in gravitational potential in 0.20 s,

 

 

- sign due to falling a distance d, which we find from standard kinematics

 

 

Energy dissipated in 0.20 s, is due to the consumption of power

 

 

 

 

Same as change in gravitational potential energy as it should be!

 

 

 

 

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This page last updated on June 24, 2018