Magnetism

Magnetic Force on a Moving Charge

A charge $q$ moving with velocity $\vec{v}$ in a magnetic field $\vec{B}$ experiences:

\vec{F} = q\vec{v} \times \vec{B}

The magnitude is $F = qvB\sin\theta$ Where $\theta$ is the angle between $\vec{v}$ and $\vec{B}$ . The direction is given by the right-hand rule.

Key Properties

The magnetic force is always perpendicular to both $\vec{v}$ and $\vec{B}$ .
The magnetic force does no work ( $\vec{F} \perp \vec{v}$ So $W = \int \vec{F} \cdot d\vec{l} = 0$ ).
The magnetic force changes the direction of motion, not the speed.

Circular Motion in a Magnetic Field

A charged particle moving perpendicular to a uniform magnetic field follows a circular path. Setting $F = ma$ :

QvB = \frac{mv^2}{r} \implies r = \frac{mv}{qB}

The cyclotron frequency is:

F = \frac{qB}{2\pi m}, \qquad \omega = \frac{qB}{m}

Motion at an Angle to the Field

If $\vec{v}$ makes angle $\theta$ with $\vec{B}$ The motion is helical. The parallel component $v_\parallel = v\cos\theta$ is unaffected. The perpendicular component $v_\perp = v\sin\theta$ produces Circular motion with radius $r = mv_\perp/(qB)$ and pitch $p = v_\parallel \cdot T = 2\pi m v_\parallel/(qB)$ .

Magnetic Force on a Current-Carrying Wire

For a wire of length $L$ carrying current $I$ in a uniform field:

\vec{F} = I\vec{L} \times \vec{B}

For a non-uniform field or curved wire, use the differential form:

D\vec{F} = I\, d\vec{l} \times \vec{B}

A semicircular wire of radius $R$ carries current $I$ in a uniform magnetic field $\vec{B}$ directed into the page. The straight ends of the wire are along the diameter.

The force on the straight segment of length $2R$ is $F = I(2R)B$ (by the right-hand rule, directed Upward). For the curved part, consider a segment at angle $\theta$ :

DF = I(R\, d\theta)B

Only the $y$ -components survive: $dF_y = dF \sin\theta$ . Integrating from $\theta = 0$ to $\pi$ :

F_y = \int_0^\pi IRB\sin\theta\, d\theta = IRB[-\cos\theta]_0^\pi = 2IRB

The total force on the semicircular wire is $2IRB$ The same as on a straight wire of length $2R$ .

Torque on a Current Loop

A rectangular loop of area $A$ carrying current $I$ in a uniform field $\vec{B}$ experiences torque:

\vec{\tau} = \vec{\mu} \times \vec{B}

Where the magnetic dipole moment is $\vec{\mu} = NI\vec{A}$ With $\vec{A}$ directed normal to the loop By the right-hand rule and $N$ is the number of turns.

The magnitude is $\tau = NIAB\sin\alpha$ Where $\alpha$ is the angle between $\vec{\mu}$ and $\vec{B}$ .

Biot-Savart Law

The magnetic field produced by a current element $I\, d\vec{l}$ at position $\vec{r}$ from the element:

D\vec{B} = \frac{\mu_0}{4\pi} \frac{I\, d\vec{l} \times \hat{r}}{r^2}

Where $\mu_0 = 4\pi \times 10^{-7}$ T $\cdot$ M/A is the permeability of free space.

Field of a Long Straight Wire

B = \frac{\mu_0 I}{2\pi r}

Derivation: Place the wire along the $z$ -axis. A current element $I\, dz$ at the origin produces:

DB = \frac{\mu_0}{4\pi}\frac{I\, dz}{r^2}\sin\theta

Where $\sin\theta = R/r$ and $r = \sqrt{z^2 + R^2}$ . Let $z = R\tan\phi$ , $dz = R\sec^2\phi\, d\phi$ :

DB = \frac{\mu_0 I}{4\pi} \frac{R\sec^2\phi\, d\phi}{R^2\sec^2\phi} \cdot \sin\phi = \frac{\mu_0 I}{4\pi R}\sin\phi\, d\phi

Integrating from $\phi = 0$ to $\pi$ (infinite wire):

B = \frac{\mu_0 I}{4\pi R}\int_0^\pi \sin\phi\, d\phi = \frac{\mu_0 I}{4\pi R}[-\cos\phi]_0^\pi = \frac{\mu_0 I}{2\pi R}

Field on the Axis of a Circular Loop

B = \frac{\mu_0 I R^2}{2(R^2 + x^2)^{3/2}}

At the center ( $x = 0$ ): $B = \dfrac{\mu_0 I}{2R}$ .

Derivation: Each current element $I\, dl$ produces $dB = \frac{\mu_0}{4\pi}\frac{I\, dl}{r^2}\sin 90°$ . By symmetry, only the axial component survives:

DB_x = \frac{\mu_0 I}{4\pi r^2}\cdot\frac{R}{r}\, dl = \frac{\mu_0 IR}{4\pi(R^2+x^2)^{3/2}}\, dl

B_x = \frac{\mu_0 IR}{4\pi(R^2+x^2)^{3/2}}\oint dl = \frac{\mu_0 I \cdot 2\pi R^2}{4\pi(R^2+x^2)^{3/2}} = \frac{\mu_0 IR^2}{2(R^2+x^2)^{3/2}}

Ampere’s Law

Ampere’s law relates the line integral of $\vec{B}$ around a closed loop to the enclosed current:

\oint_C \vec{B} \cdot d\vec{l} = \mu_0 I_{\text{enc}

Field Inside a Long Solenoid

For a solenoid with $n$ turns per unit length carrying current $I$ Choose a rectangular Amperian loop with one side inside the solenoid and one outside.

B = \mu_0 n I

This result is valid for an ideal (infinitely long) solenoid and is a good approximation near the center Of a long solenoid.

Field Inside a Toroid

A toroid with $N$ turns carrying current $I$ Inner radius $a$ Outer radius $b$ :

B = \frac{\mu_0 N I}{2\pi r}

Valid for $a < r < b$ .

Example: Thick conductor with non-uniform current density A long cylindrical conductor of radius $R$ carries current $I$ with current density $J(r) = J_0 r/R$ for $0 \le r \le R$ . Find $B$ inside and outside.

Inside ( $r \le R$ ): Use a circular Amperian loop of radius $r$ .

I_{\text{enc} = \int_0^r J(r') \cdot 2\pi r'\, dr' = \frac{2\pi J_0}{R}\int_0^r r'^2\, dr' = \frac{2\pi J_0 r^3}{3R}

B \cdot 2\pi r = \mu_0 \frac{2\pi J_0 r^3}{3R} \implies B = \frac{\mu_0 J_0 r^2}{3R}

To express in terms of $I$ Find the total current:

I = \frac{2\pi J_0 R^3}{3R} = \frac{2\pi J_0 R^2}{3} \implies J_0 = \frac{3I}{2\pi R^2}

B = \frac{\mu_0 I r^2}{2\pi R^3}

Outside ( $r > R$ ): $I_{\text{enc} = I$ .

B = \frac{\mu_0 I}{2\pi r}

Faraday’s Law

Faraday’s law states that a changing magnetic flux induces an EMF:

\mathcal{E} = -\frac{d\Phi_B}{dt}

Where the magnetic flux through a surface is:

\Phi_B = \int_S \vec{B} \cdot d\vec{A}

For a uniform field perpendicular to a flat surface of area $A$ : $\Phi_B = BA$ .

Lenz’s Law

The negative sign in Faraday’s law encodes Lenz’s law: the induced EMF drives a current whose magnetic Field opposes the change in flux that produced it. The induced current acts to maintain the status quo.

Motional EMF

A conducting bar of length $L$ moving with velocity $v$ perpendicular to a uniform field $B$ :

\mathcal{E} = BLv

Derivation: The free charges in the bar experience a magnetic force $F = qvB$ . This is equivalent To an electric field $E = vB$ along the bar. The EMF is:

\mathcal{E} = \int_0^L E\, dl = \int_0^L vB\, dl = BLv

Example: Induced EMF in a changing field A circular loop of radius $r = 0.1$ m is in a region where the magnetic field increases as $B(t) = (0.5 + 0.2t)$ T. The loop has resistance $R = 2\,\Omega$ . Find the induced current.

\Phi_B = B \cdot \pi r^2 = (0.5 + 0.2t)\pi(0.1)^2 = (0.5 + 0.2t)(0.0314)\,\text{Wb

\mathcal{E} = -\frac{d\Phi_B}{dt} = -0.2 \times 0.0314 = -0.00628\,\text{V

I = \frac{|\mathcal{E}|}{R} = \frac{0.00628}{2} = 3.14\,\text{mA

By Lenz’s law, the current flows counterclockwise (viewed along $\vec{B}$ ) to oppose the increasing flux.

Inductance

Self-Inductance

The self-induced EMF in a coil is:

\mathcal{E} = -L\frac{dI}{dt}

Where $L$ is the inductance, measured in henrys (H). For a long solenoid with $N$ turns, length $\ell$ Cross-sectional area $A$ :

L = \frac{\mu_0 N^2 A}{\ell} = \mu_0 n^2 A \ell

Where $n = N/\ell$ is the turns per unit length.

Mutual Inductance

When the current in coil 1 changes, it induces an EMF in coil 2:

\mathcal{E}_2 = -M\frac{dI_1}{dt}

Where $M$ is the mutual inductance. For a solenoid with a secondary coil of $N_2$ turns:

M = \frac{\mu_0 N_1 N_2 A}{\ell}

Energy Stored in an Inductor

U = \frac{1}{2}LI^2

Derivation: The power delivered to the inductor is $P = \mathcal{E}I = LI(dI/dt)$ . Integrating:

U = \int_0^t P\, dt' = L\int_0^I I'\, dI' = \frac{1}{2}LI^2

RL Circuits

When a switch is closed in a circuit with resistance $R$ and inductance $L$ :

\mathcal{E} - IR - L\frac{dI}{dt} = 0

This is a first-order linear ODE with solution:

I(t) = \frac{\mathcal{E}}{R}\left(1 - e^{-t/(L/R)}\right) = I_{\max}\left(1 - e^{-t/\tau_L}\right)

Where $\tau_L = L/R$ is the inductive time constant.

When the switch is opened (current decaying):

I(t) = I_0 e^{-t/\tau_L}

Voltage across the inductor during charging:

V_L = L\frac{dI}{dt} = \mathcal{E} e^{-t/\tau_L}

At $t = 0$ All the voltage is across the inductor. At $t \to \infty$ All the voltage is across the resistor.

LC Circuits

An LC circuit (inductor and capacitor, no resistance) exhibits simple harmonic oscillation. By KVL:

-L\frac{dI}{dt} + \frac{Q}{C} = 0

Since $I = dQ/dt$ and $dI/dt = d^2Q/dt^2$ :

\frac{d^2Q}{dt^2} + \frac{1}{LC}Q = 0

This is the equation for simple harmonic motion with angular frequency:

\omega = \frac{1}{\sqrt{LC}}, \qquad f = \frac{1}{2\pi\sqrt{LC}}

The solutions are:

Q(t) = Q_0\cos(\omega t + \phi)

I(t) = -Q_0\omega\sin(\omega t + \phi) = -I_0\sin(\omega t + \phi)

The charge and current oscillate $90°$ out of phase. Energy oscillates between the capacitor ( $U_C = Q^2/(2C)$ ) and the inductor ( $U_L = LI^2/2$ ), with total energy conserved:

U_{\text{total} = \frac{Q_0^2}{2C} = \frac{1}{2}LI_0^2

An LC circuit has $L = 10$ mH and $C = 100\,\mu\text{F$ . The capacitor is initially charged to $Q_0 = 50\,\mu\text{C$ . Find (a) the oscillation frequency, (b) the maximum current, and (c) the Charge when the current is half its maximum value.

(a) $f = \frac{1}{2\pi\sqrt{LC}} = \frac{1}{2\pi\sqrt{(0.01)(10^{-4})}} = \frac{1}{2\pi \times 10^{-3}} = 159\,\text{Hz$

(b) $I_0 = Q_0\omega = Q_0/\sqrt{LC} = (50 \times 10^{-6})/\sqrt{10^{-6}} = 50 \times 10^{-6}/10^{-3} = 0.05\,\text{A = 50\,\text{mA$

U_L = \frac{1}{2}LI^2 = \frac{1}{2}(0.01)(0.025)^2 = 3.125 \times 10^{-6}\,\text{J

U_C = U_{\text{total} - U_L = \frac{(50 \times 10^{-6})^2}{2(10^{-4})} - 3.125 \times 10^{-6} = 12.5 \times 10^{-6} - 3.125 \times 10^{-6} = 9.375 \times 10^{-6}\,\text{J

Q = \sqrt{2CU_C} = \sqrt{2(10^{-4})(9.375 \times 10^{-6})} = \sqrt{1.875 \times 10^{-9}} = 43.3\,\mu\text{C

Maxwell’s Equations (Integral Form)

The four Maxwell’s equations unify electricity and magnetism:

Equation	Law	Integral Form
Gauss’s Law for Electricity	Electric charges produce electric fields	$\oint \vec{E} \cdot d\vec{A} = \dfrac{Q_{\text{enc}}{\epsilon_0}$
Gauss’s Law for Magnetism	No magnetic monopoles	$\oint \vec{B} \cdot d\vec{A} = 0$
Faraday’s Law	Changing magnetic fields produce electric fields	$\oint \vec{E} \cdot d\vec{l} = -\dfrac{d\Phi_B}{dt}$
Ampere-Maxwell Law	Currents and changing electric fields produce magnetic fields	$\oint \vec{B} \cdot d\vec{l} = \mu_0 I_{\text{enc} + \mu_0\epsilon_0\dfrac{d\Phi_E}{dt}$

The Displacement Current

Maxwell added the displacement current term $\mu_0\epsilon_0 \frac{d\Phi_E}{dt}$ to Ampere’s law. This Term accounts for the fact that a changing electric field (as between capacitor plates) also produces a Magnetic field, even in the absence of a physical current.

I_d = \epsilon_0 \frac{d\Phi_E}{dt}

Example: Displacement current in a charging capacitor A parallel plate capacitor with plate area $A$ and separation $d$ is being charged by a current $I$ . Find the magnetic field at distance $r$ from the axis between the plates ( $r < R_{\text{plate}$ ).

The displacement current equals the conduction current (by charge conservation):

I_d = I

The electric flux through a disk of radius $r$ is:

\Phi_E = E \cdot \pi r^2 = \frac{V}{d}\pi r^2

Since $V = Q/C = Qd/(\epsilon_0 A)$ We have $E = Q/(\epsilon_0 A)$ So $\Phi_E = Q\pi r^2/(\epsilon_0 A)$ .

Apply Ampere-Maxwell law with a circular Amperian loop of radius $r$ :

B \cdot 2\pi r = \mu_0 \epsilon_0 \frac{d\Phi_E}{dt} = \mu_0 \epsilon_0 \frac{d}{dt}\left(\frac{Q\pi r^2}{\epsilon_0 A}\right) = \mu_0 \frac{\pi r^2}{A}\frac{dQ}{dt} = \mu_0 I \frac{r^2}{R^2}

B = \frac{\mu_0 I r}{2\pi R^2}

This is the same as the field inside a wire of radius $R$ carrying current $I$ .

Intuition

Magnetism is electricity in motion, moving charges create magnetic fields, and magnetic fields exert forces on moving charges. The magnetic force is always perpendicular to the velocity, so it changes direction but not speed, this is why charged particles spiral in magnetic fields.

Why magnetic force does no work: Since $\vec{F} = q\vec{v} \times \vec{B}$ is perpendicular to $\vec{v}$ , the power $P = \vec{F} \cdot \vec{v} = 0$ . The magnetic field redirects charges but never speeds them up or slows them down. This is fundamentally different from electric fields, which do work.

Faraday’s law intuition: A changing magnetic flux induces an EMF, nature abhors a change in flux. Lenz’s law tells you the direction: the induced current creates a field that opposes the change. If flux increases, the induced field points opposite to the original field. This is why dropping a magnet through a copper tube is slow, the induced currents create opposing fields.

Inductance intuition: An inductor opposes changes in current, just as mass opposes changes in velocity. When you try to increase current through an inductor, it generates a back-EMF that fights the increase. When you try to decrease it, the inductor maintains the current. The time constant $\tau_L = L/R$ tells you how quickly the current responds.

LC circuit intuition: An LC circuit is the electromagnetic analog of a mass-spring system. Energy oscillates between the capacitor (electric field, like potential energy) and the inductor (magnetic field, like kinetic energy). The charge and current are 90° out of phase, when one is maximum, the other is zero.

Common Pitfalls

Wrong direction for the magnetic force. Use $\vec{F} = q\vec{v} \times \vec{B}$ Not $\vec{B} \times \vec{v}$ . The cross product is not commutative. For negative charges, reverse the direction.
Confusing Gauss’s law for magnetism with Gauss’s law for electricity. $\oint \vec{B} \cdot d\vec{A} = 0$ always (no magnetic monopoles). This does not mean $B = 0$ everywhere; it means the net flux through any closed surface is zero.
Incorrect sign in Faraday’s law. The negative sign matters. It represents Lenz’s law. If you forget it, your induced current will be in the wrong direction.
Using Ampere’s law without symmetry. Like Gauss’s law, Ampere’s law is always true but only useful when symmetry allows you to extract $B$ from the integral. Choose Amperian loops that match the symmetry: circles for straight wires and solenoids.
Forgetting that inductors oppose changes in current. At $t = 0$ in an RL circuit, the inductor acts as an open circuit ( $I = 0$ ). At steady state, it acts as a short circuit ( $V_L = 0$ ). This is the opposite of a capacitor.
Confusing self-inductance and mutual inductance. Self-inductance $L$ relates the EMF in a coil to its own changing current. Mutual inductance $M$ relates the EMF in one coil to the changing current in another coil.
Incorrectly computing flux for non-perpendicular fields. When $\vec{B}$ is not perpendicular to the surface, use $\Phi_B = BA\cos\theta$ Not $BA$ . The angle $\theta$ is between $\vec{B}$ and the surface normal.
Forgetting the displacement current in Ampere-Maxwell law. When applying Ampere’s law between capacitor plates (or in any region where $d\vec{E}/dt \neq 0$ ), you must include the displacement current term. Without it, Ampere’s law gives incorrect results.
Assuming the magnetic field inside a solenoid is zero. The field inside an ideal solenoid is uniform and given by $B = \mu_0 nI$ . The field outside is approximately zero.

Practice Questions

A proton ( $m_p = 1.67 \times 10^{-27}$ kg, $q = 1.6 \times 10^{-19}$ C) enters a magnetic field of $B = 0.5$ T with velocity $v = 3 \times 10^6$ m/s perpendicular to the field. Find the radius of the circular orbit and the cyclotron frequency.
A wire carrying $I = 10$ A is bent into a right angle. Find the magnetic field at point $P$ located at distance $d = 5$ cm from the vertex along the angle bisector.
A solenoid of length $0.3$ m has 1000 turns and carries a current of $5$ A. Find the magnetic field inside and the inductance if the cross-sectional area is $4 \times 10^{-4}$ m $^2$ .
A square loop of side $0.2$ m is in a magnetic field $B = 0.5$ T perpendicular to the loop. The field decreases to zero in $0.1$ s. If the loop has resistance $2\,\Omega$ Find the induced current and the energy dissipated.
An RL circuit has $R = 50\,\Omega$ and $L = 0.2$ H connected to a $12$ V battery. Find (a) the time constant, (b) the current at $t = 10$ ms, and (c) the voltage across the inductor at $t = 10$ ms.
An LC circuit has $L = 25$ mH and $C = 40\,\mu\text{F$ . The maximum charge on the capacitor is $80\,\mu\text{C$ . Find (a) the oscillation frequency, (b) the maximum current, and (c) the total energy in the circuit.

Question 7: AP Exam-Style -- Biot-Savart and Ampere combined

A long straight wire carries current $I_1 = 10$ A. A circular loop of radius $R = 0.05$ m lies in the Same plane as the wire, with its center at distance $d = 0.1$ m from the wire. The loop carries current $I_2 = 5$ A. Find the net magnetic field at the center of the loop.

Answer

The field from the straight wire at the center of the loop (distance $d = 0.1$ m):

B_{\text{wire} = \frac{\mu_0 I_1}{2\pi d} = \frac{(4\pi \times 10^{-7})(10)}{2\pi(0.1)} = \frac{2 \times 10^{-5}}{0.1} = 2.0 \times 10^{-4}\,\text{T

By the right-hand rule, if the wire is vertical and the loop is to the right, the field from the wire At the loop center points out of the page.

The field from the circular loop at its center:

B_{\text{loop} = \frac{\mu_0 I_2}{2R} = \frac{(4\pi \times 10^{-7})(5)}{2(0.05)} = \frac{2\pi \times 10^{-6}}{0.05} = 1.257 \times 10^{-4}\,\text{T

The direction depends on the current direction in the loop. If the loop current flows counterclockwise (viewed from above), the field at the center points out of the page (same direction as the wire’s Field).

If both fields are in the same direction:

B_{\text{net} = (2.0 + 1.257) \times 10^{-4} = 3.26 \times 10^{-4}\,\text{T

If opposite:

B_{\text{net} = (2.0 - 1.257) \times 10^{-4} = 0.74 \times 10^{-4}\,\text{T

Question 8: AP Exam-Style -- Faraday's law with a falling loop

A rectangular conducting loop of width $w = 0.1$ m and height $h = 0.2$ m falls vertically into a region of uniform magnetic field $B = 0.5$ T directed into the page. The field region extends from $y = 0$ to $y = 0.3$ m. The loop has mass $m = 0.01$ kg and resistance $R = 0.5\,\Omega$ . Find the Terminal velocity of the loop as it enters the field.

Answer

As the loop enters the field, the flux through the loop changes. Only the bottom edge of width $w$ is Inside the field during entry.

The motional EMF: $\mathcal{E} = Bwv$ .

The induced current: $I = \mathcal{E}/R = Bwv/R$ .

By Lenz’s law, the induced current creates a force opposing the motion (upward). The force on the bottom wire is:

F_B = BIw = \frac{B^2 w^2 v}{R}

At terminal velocity, this magnetic force balances gravity:

mg = \frac{B^2 w^2 v_T}{R}

v_T = \frac{mgR}{B^2 w^2} = \frac{(0.01)(9.8)(0.5)}{(0.5)^2(0.1)^2} = \frac{0.049}{0.0025} = 19.6\,\text{m/s

Question 9: AP Exam-Style -- RL circuit analysis

An RL circuit with $R = 100\,\Omega$ and $L = 0.5$ H is connected to a DC source of $\mathcal{E} = 20$ V. At $t = 0$ The switch is closed. (a) Derive the current as a function of time. (b) At what time is The current increasing at half its initial rate? (c) How much energy has been stored in the inductor When the current reaches 80% of its maximum value?

Answer

(a) The ODE is $\mathcal{E} = L\frac{dI}{dt} + IR$ .

Rearranging: $\frac{dI}{dt} = \frac{\mathcal{E}}{L} - \frac{R}{L}I$ .

Let $I_{\max} = \mathcal{E}/R = 20/100 = 0.2$ A and $\tau = L/R = 0.5/100 = 5 \times 10^{-3}$ s.

Solution: $I(t) = I_{\max}(1 - e^{-t/\tau}) = 0.2(1 - e^{-200t})$ .

(b) The initial rate of current increase is $dI/dt|_{t=0} = \mathcal{E}/L = 20/0.5 = 40$ A/s.

Half of this is $20$ A/s:

\frac{dI}{dt} = \frac{\mathcal{E}}{L}e^{-t/\tau} = 40e^{-200t} = 20

e^{-200t} = 0.5 \implies t = \frac{\ln 2}{200} = 3.47 \times 10^{-3}\,\text{s = 3.47\,\text{ms

Note: this occurs at $t = \tau \ln 2$ .

U_L = \frac{1}{2}LI^2 = \frac{1}{2}(0.5)(0.16)^2 = \frac{1}{2}(0.5)(0.0256) = 6.4 \times 10^{-3}\,\text{J = 6.4\,\text{mJ

Question 10: AP Exam-Style -- Displacement current and Maxwell's equations

A parallel plate capacitor with circular plates of radius $R = 5$ cm and separation $d = 2$ mm is being Charged by a current $I = 3$ A. (a) Find the displacement current between the plates. (b) Find the Magnetic field at $r = 3$ cm from the axis, midway between the plates. (c) Find the rate of change of The electric field between the plates.

Answer

(a) By conservation of charge and the continuity of the displacement current:

I_d = I = 3\,\text{A

(b) Apply the Ampere-Maxwell law with a circular Amperian loop of radius $r = 0.03$ m (note $r < R$ ):

B \cdot 2\pi r = \mu_0 I_d \frac{r^2}{R^2} = \mu_0(3)\frac{(0.03)^2}{(0.05)^2} = \mu_0(3)(0.36)

B = \frac{(4\pi \times 10^{-7})(1.08)}{2\pi(0.03)} = \frac{4.32\pi \times 10^{-7}}{6\pi \times 10^{-2}} = \frac{4.32 \times 10^{-7}}{0.06} = 7.2 \times 10^{-6}\,\text{T = 7.2\,\mu\text{T

I_d = \epsilon_0 \frac{d\Phi_E}{dt} = \epsilon_0 \frac{d}{dt}(E \cdot \pi R^2) = \epsilon_0 \pi R^2 \frac{dE}{dt}

\frac{dE}{dt} = \frac{I_d}{\epsilon_0 \pi R^2} = \frac{3}{(8.854 \times 10^{-12})\pi(0.05)^2} = \frac{3}{6.95 \times 10^{-14}} = 4.32 \times 10^{13}\,\text{V/m\cdot\text{s

Summary

This topic covers the fundamental principles of magnetism, including the key equations, experimental methods, and applications relevant to the specification.

Key concepts include:

fundamental principles and equations
SI units and dimensional analysis
mathematical modelling of physical phenomena
experimental techniques and measurement
applications to real-world problems

A strong understanding of these principles, combined with regular practice of quantitative problems and past paper questions, is essential for success in examinations.

Worked Examples

Worked examples demonstrating the application of key concepts are covered in the detailed sub-pages linked above.

Cross-References

Electrostatics: Electric charges produce electric fields; moving charges produce magnetic fields.
Circuits: Inductors store energy in magnetic fields; changing magnetic flux induces EMF in circuits.
Work, Energy, and Power: Magnetic forces do no work on individual charges but can transfer energy between circuit elements.
AP Calculus, Integrals: Magnetic flux is computed as a surface integral of the magnetic field, and Faraday’s law involves differentiating the flux integral, connecting magnetism to both integration and differentiation.

Mark this page as reviewed