A 140-g ball containing excess electrons is dropped into a 110-m vertical shaft. At the bottom of the shaft, the ball suddenly enters a uniform horizontal magnetic field that has magnitude 0.300 T and direction from east to west. If air resistance is negligibly small, find the magnitude ond direction of the force that this magnetic field exerts on the ball just as it enters the field.

Short Answer

Expert verified

F=9.14×10-10N

Step by step solution

01

27.17 - magnitude

This force is due to the magnetic field, so to find the magnitude we apply our formula.

F=qv×BF=qvBsin(ϕ)

Where Fis the force we are looking for, qis the charge, vis the velocity of our ball, and ϕis the angle between the velocity vector and the magnetic field.

We have everything except the velocity. The charge is the charge of an electron times the number of electrons. The angle is 90 degrees so the sin term drops out, and the magnetic field strength is given.

To find the velocity, we can use energy concepts. Initially the ball is at rest, so the only energy is the gravitational potential energy. At the bottom of the shaft this has all converted into kinetic energy. Thus

localid="1650564691539" mgh=12mv2v=2gh

Putting it all together, we have

localid="1650564694724" F=qvBsin(ϕ)F=q2ghB

Now we can plug in our numbers and solve.

localid="1650564699179" F=(4.10×108)·(-1.60*10-19C)2·9.8m/s2·110m·(0.300T)F=9.14×10-10N

02

27.17 - direction

We find the direction by applying the right hand rule.

The velocity vector is pointed down, and the magnetic field is pointed to the west, so our thumb points to the north. These are electrons though, and the right hand rule is defined for positive charges, so we must flip the direction of the force meaning the force is pointed to the south.

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