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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.
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.
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.
So, the tesla is
(note that C/s = A).
Another smaller unit, called the gauss (G), where $\mathrm{1\; G}={\text{10}}^{-4}\phantom{\rule{0.25em}{0ex}}\mathrm{T}$ , 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 $5\times {\text{10}}^{-5}\phantom{\rule{0.25em}{0ex}}\mathrm{T}$ , or 0.5 G.
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.
The direction of the magnetic force $\mathbf{\text{F}}$ is perpendicular to the plane formed by $\mathbf{\text{v}}$ and $\mathbf{\text{B}}$ , as determined by the right hand rule 1 (or RHR-1), which is illustrated in [link] . 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 $\mathbf{\text{v}}$ , the fingers in the direction of $\mathbf{\text{B}}$ , and a perpendicular to the palm points in the direction of $\mathbf{\text{F}}$ . 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.
If a charged particle moves in a straight line through some region of space, can you say that the magnetic field in that region is necessarily zero?
What is the direction of the magnetic force on a positive charge that moves as shown in each of the six cases shown in [link] ? Note that $\odot $ indicates "coming out of the page" and $\otimes $ means "going into the page."
(a) Left (West)
(b) Into the page
(c) Up (North)
(d) No force
(e) Right (East)
(f) Down (South)
Repeat [link] for a negative charge.
What is the direction of the velocity of a negative charge that experiences the magnetic force shown in each of the three cases in [link] , assuming it moves perpendicular to $\mathbf{\text{B}}\mathrm{?}$ Note that $\odot $ indicates "coming out of the page" and $\otimes $ means "going into the page."
(a) East (right)
(b) Into page
(c) South (down)
Repeat [link] for a positive charge.
What is the direction of the magnetic field that produces the magnetic force on a positive charge as shown in each of the three cases in the figure below, assuming $\mathbf{\text{B}}$ is perpendicular to $\mathbf{\text{v}}$ ? Note that $\otimes $ means "going into the page."
(a) Into page
(b) West (left)
(c) Out of page
Repeat [link] for a negative charge.
What is the maximum force on an aluminum rod with a $0\text{.}\text{100}\text{-\mu C}$ charge that you pass between the poles of a 1.50-T permanent magnet at a speed of 5.00 m/s? In what direction is the force?
$7\text{.}\text{50}\times {\text{10}}^{-7}\phantom{\rule{0.25em}{0ex}}\text{N}$ perpendicular to both the magnetic field lines and the velocity
(a) Aircraft sometimes acquire small static charges. Suppose a supersonic jet has a $0\text{.}\text{500}\text{-\mu C}$ charge and flies due west at a speed of 660 m/s over the Earth’s south magnetic pole, where the $8\text{.}\text{00}\times {\text{10}}^{-5}\text{-T}$ magnetic field points straight up. What are the direction and the magnitude of the magnetic force on the plane? (b) Discuss whether the value obtained in part (a) implies this is a significant or negligible effect.
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