10.5

Magnetic Field Strength: Force on a Moving Charge in a Magnetic Field

Chapter contents: Chapter 10: Magnetism

The magnetic field strength is the magnitude B of the magnetic field, measured in teslas.
What is the mechanism by which one magnet exerts a force on another? The answer is related to the fact that all magnetism is caused by current, the flow of charge. Magnetic fields exert forces on moving charges, and so they exert forces on other magnets, all of which have moving charges.

Magnetic Force on a Moving Charge

The magnetic force on a moving charge is one of the most fundamental known. Magnetic force is as important as the electrostatic or Coulomb force. Yet the magnetic force is more complex, in both the number of factors that affects it and in its direction, than the relatively simple Coulomb force.
The magnitude of the magnetic force F on a charge depends on: the quantity of charge q, its speed v, the strength of magnetic field B, and the direction of motion relative to the magnetic field’s direction. Motion, and its direction, are critical.
The maximum force occurs when the direction of motion and the magnetic field’s direction are perpendicular to one another (i.e. ninety degree angle between directions).
v⊥B
In that situation, the magnitude of the magnetic force is
F=qvB
The minimum force occurs when the direction of motion and the magnetic field’s direction are parallel to one another (i.e. zero or 180 degree angle between directions).
v∥B
In that situation, the magnitude of the magnetic force is
F=0
We define the magnetic field strength B in terms of the force on a charged particle moving in a magnetic field. The SI unit for magnetic field strength B is called the tesla (T) after the eccentric but brilliant inventor Nikola Tesla (1856–1943). To determine how the tesla relates to other SI units, we solve for the magnetic field strength.
B=Fqv
(10.5.1)
So, the tesla is
1T=1NC⋅m/s=1NA⋅m
(10.5.2)
(note that C/s = A).
Another smaller unit, called the gauss (G), where 1 G=10−4T, is sometimes used. The strongest permanent magnets have fields near 2 T; superconducting electromagnets may attain 10 T or more. The Earth’s magnetic field on its surface is only about 5×10−5T, or 0.5 G.

Making Connections: Charges and Magnets

There is no magnetic force on static charges. However, there is a magnetic force on moving charges. When charges are stationary, their electric fields do not affect magnets. But, when charges move, they produce magnetic fields that exert forces on other magnets. When there is relative motion, a connection between electric and magnetic fields emerges—each affects the other.

Direction of Force: Right Hand Rule 1

The direction of the magnetic force F is perpendicular to the plane formed by v and B, as determined by the right hand rule 1 (or RHR-1), which is illustrated in Figure 10.5.1. RHR-1 states that, to determine the direction of the magnetic force on a positive moving charge, you point the thumb of the right hand in the direction of v, the fingers in the direction of B, and a perpendicular to the palm points in the direction of F. One way to remember this is that there is one velocity, and so the thumb represents it. There are many field lines, and so the fingers represent them. The force is in the direction you would push with your palm. The force on a negative charge is in exactly the opposite direction to that on a positive charge.
The right hand rule 1. An outstretched right hand rests palm up on a piece of paper on which a vector arrow v points to the right and a vector arrow B points toward the top of the paper. The thumb points to the right, in the direction of the v vector arrow. The fingers point in the direction of the B vector. B and v are in the same plane. The F vector points straight up, perpendicular to the plane of the paper, which is the plane made by B and v. The angle between B and v is theta. The magnitude of the magnetic force F equals q v B sine theta.
Figure 10.5.1. Magnetic fields exert forces on moving charges. This force is one of the most basic known. The direction of the magnetic force on a moving charge is perpendicular to the plane formed by v and B and follows right hand rule–1 (RHR-1) as shown. The magnitude of the force is proportional to q, v, B, and depends on the angle between v and B.
Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review. Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.
Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.Continue to this item in the chapter review.