Interaction with moving charges

The magnitude of the Lorentz force is $F = q\times v\times B\times\sen\alpha$ and its direction is given by the vector product $\vv{F} = q\times(\vv{v}\wedge\vv{B})$, which is determined using the right-hand rule. A proton moves horizontally to the east inside a uniform magnetic field also directed horizontally to the north. The situation, viewed from above, is shown in the figure.

1. a) Determine the direction and sense of the force acting on the proton.
2. b) What would the direction of the force be if the particle were an electron? Justify the difference.

From the expression for the magnitude of the Lorentz force, $F = q\times v\times B$ (perpendicular case):

1. a) Rearrange for $B$ and deduce what combination of SI units one tesla is equivalent to.
2. b) Using $1\ \text{C/s} = 1\ \text{A}$, express the tesla as $\text{T} = \frac{\text{N}}{\text{A}\times\text{m}}$ and explain in your own words what field is required so that a charge of $1\ \text{C}$ moving at $1\ \text{m/s}$ experiences a force of $1\ \text{N}$.

A proton ($q = 1.6\times10^{-19}\ \text{C}$) enters with $v = 3\times10^{6}\ \text{m/s}$ into a uniform magnetic field $B = 0.8\ \text{T}$, making an angle $\alpha = 30^\circ$ with it. Observe the diagram:

1. a) Calculate the magnitude of the Lorentz force, $F = q\times v\times B\times\sen\alpha$ ($\sen 30^\circ = 0.5$).
2. b) For what angle would the force be maximum? And for which would it be zero?

The Lorentz force on a moving charge is always perpendicular to its velocity.

1. a) Taking into account that work depends on the component of the force in the direction of displacement, explain why the magnetic force does no work on the charge.
2. b) What then happens to the speed of the charge?
3. c) And to its kinetic energy?

An electron ($m_e = 9.11\times10^{-31}\ \text{kg}$, $e = 1.6\times10^{-19}\ \text{C}$) enters perpendicularly with $v = 1\times10^{7}\ \text{m/s}$ into a uniform magnetic field $B = 1\times10^{-3}\ \text{T}$, as shown in the figure.

The radius of its circular trajectory is $r = \frac{m\times v}{q\times B}$. Calculate its value and express it in centimeters.

An electron ($m_e = 9.11\times10^{-31}\ \text{kg}$, $e = 1.6\times10^{-19}\ \text{C}$) orbits in a uniform magnetic field $B = 2\times10^{-3}\ \text{T}$, with its velocity perpendicular to the field.

1. a) Equate the Lorentz force to the centripetal force and, using $v = \frac{2\pi\times r}{T}$, show that the orbital period is $T = \frac{2\pi\times m}{q\times B}$.
2. b) Calculate its value.
3. c) The result does not contain $v$ or $r$: explain what this means physically.

Two straight parallel conductors carry currents in the same direction.

1. a) Draw in your notebook the magnetic field created by the first conductor at the position of the second (right-hand rule) and the force exerted on the second conductor.
2. b) Do they attract or repel each other?
3. c) What changes if the direction of one of the currents is reversed?

You can do it on paper and send a photo with your answer.

A straight conductor of length $L = 40\ \text{cm}$, placed perpendicular to a uniform magnetic field $B = 0.1\ \text{T}$, carries a current $I = 5\ \text{A}$. The magnetic force on it is $F = B\times I\times L$.

1. a) Calculate its magnitude.
2. b) Draw the situation in your notebook and determine, using the right-hand rule, the direction and sense of the force relative to the current and the field.
3. c) If the conductor made an angle of $30^\circ$ with the field, the force would be $F = B\times I\times L\times\sen 30^\circ$; calculate it.

A horizontal rod of length $L = 50\ \text{cm}$ and mass $m = 25\ \text{g}$ is in a uniform horizontal magnetic field $B = 0.5\ \text{T}$, perpendicular to the rod. It is desired that the magnetic force on the rod, $F = B\times I\times L$, exactly balances its weight (take $g = 9.8\ \text{m/s}^2$). The situation is shown in the figure.

1. a) Set up the condition for equilibrium between the magnetic force and the weight, and calculate the required current.
2. b) Determine, using the right-hand rule, what relative orientation the current and field must have for the force to be vertically upwards.
3. c) Reason what would happen if the current were increased by $10\ \%$: would the rod move? In which direction and with what initial net force?

In a mass spectrometer, an ion of $\text{He}^+$ ($m = 6.64\times10^{-27}\ \text{kg}$, $q = 1.6\times10^{-19}\ \text{C}$) describes a circular arc of radius $r = 12\ \text{cm}$ in a field $B = 0.5\ \text{T}$ perpendicular to its velocity. The situation is shown in the figure.

1. a) Rearrange for velocity in the expression $r = \frac{m\times v}{q\times B}$.
2. b) Calculate its value in scientific notation.

A proton ($m_p = 1.67\times10^{-27}\ \text{kg}$) and an electron ($m_e = 9.11\times10^{-31}\ \text{kg}$) enter with the same speed, perpendicularly, into the same uniform magnetic field.

1. a) Write down the ratio $\frac{r_p}{r_e}$ of the radii of their trajectories and calculate its value.
2. b) Taking into account that $T = \frac{2\pi\times m}{q\times B}$, calculate also the ratio of their periods and comment on which particle orbits faster.

The Van Allen belts trap charged particles in the Earth's magnetic field, which is much weaker than laboratory fields. An electron ($m_e = 9.11\times10^{-31}\ \text{kg}$, $e = 1.6\times10^{-19}\ \text{C}$) moves at $v = 3\times10^{7}\ \text{m/s}$ in the equatorial region, where $B = 3\times10^{-5}\ \text{T}$, with its velocity perpendicular to the field.

1. a) Calculate the radius of its trajectory, $r = \frac{m\times v}{q\times B}$.
2. b) At latitudes near the poles, the field is twice as strong, $B = 6\times10^{-5}\ \text{T}$; calculate the radius there.
3. c) Relate the results to the fact that the trajectories of the trapped particles become more tightly coiled as they approach the poles.

A proton ($m_p$, $q_p = e$) and an alpha particle ($m_\alpha = 4\times m_p$, $q_\alpha = 2\times e$) enter with the same velocity, perpendicularly, into the same uniform magnetic field.

1. a) Calculate the ratio $\frac{r_\alpha}{r_p}$ of the radii of their trajectories.
2. b) Calculate the ratio $\frac{T_\alpha}{T_p}$ of their orbital periods.
3. c) Repeat the ratio of radii assuming that both particles enter with the same kinetic energy (use $v = \sqrt{\frac{2\times E_c}{m}}$ in the expression for the radius) and comment on whether a mass spectrometer could separate them in each of the two cases.