# Physics Formulae/Electromagnetism Formulae

Lead Article: Tables of Physics Formulae
This article is a summary of the laws, principles, defining quantities, and useful formulae in the analysis of Electromagnetism.

## Laws of Electromagnetism
### Maxwell's Equations

Below is the set in the differential and integral forms, each form is found to be equivalant by use of vector calculus. There are many ways to formulate the laws using scalar/vector potentails, tensors, geometric algebra, and numerous variations using different field vectors for the electric and magnetic fields.
| Name | Differential form | Integral form |
| Gauss's law | $\nabla \cdot \mathbf {E} ={\frac {\rho }{\varepsilon _{0}}}$ | $\oint _{\partial V}\mathbf {E} \cdot \mathrm {d} \mathbf {A} ={\frac {q_{\mathrm {enc} }}{\varepsilon _{0}}}$ |
| Gauss's law for Magnetism | $\nabla \cdot \mathbf {B} =\mathbf {0}$ | $\oint _{\partial V}\mathbf {B} \cdot \mathrm {d} \mathbf {A} =0$ |
| Maxwell–Faraday Law (Faraday's law of induction) | $\nabla \times \mathbf {E} =-{\frac {\partial \mathbf {B} }{\partial t}}$ | $V=-\oint _{\partial S}\mathbf {E} \cdot \mathrm {d} \mathbf {l} =-\oint _{\partial S}{\frac {\partial \mathbf {B} }{\partial t}}\cdot \mathrm {d} \mathbf {A}$ |
| Maxwell-Ampère Circuital law (Ampere's Law with Maxwell's correction) | $\nabla \times \mathbf {B} =\mu _{0}\left(\mathbf {J} +\varepsilon _{0}{\frac {\partial \mathbf {E} }{\partial t}}\right)\$ | $\oint _{\partial S}\mathbf {B} \cdot \mathrm {d} \mathbf {l} =\mu _{0}\oint _{\partial S}\left(\mathbf {J} +\varepsilon _{0}{\frac {\partial \mathbf {E} }{\partial t}}\right)\cdot \mathrm {d} \mathbf {A}$ |
| Lorentz Electromagnetic Force Law | $\mathbf {F} =q_{e}\left(\mathbf {E} +\mathbf {v} \times \mathbf {B} \right)$ | |
The Field Vectors
Central to electromagnetism are the electric and magnetic field vectors. Often for free space (vacumm) only the familiar E and B fields need to be used; but for matter extra field vectors D, P, H, and M must be used to account for the electric and magnetic dipole incluences throughout the media (see below for mathematical definitions).
| The electric field vectors are related by: | $\mathbf {D} =\epsilon _{0}\mathbf {E} +\mathbf {P} \,\!$ |
| The magnetic field vectors are related by: | $\mathbf {B} =\mu _{0}\left(\mathbf {H} +\mathbf {M} \right)\,\!$ |
Interpretation of the Field Vectors
Intuitivley;
— the E and B (electric and magnetic flux densities) fields are the easiest to interpret; field strength is propotional to the amount of flux though cross sections of surface area, i.e. strength as a cross-section density.
— the P and M (electric polarization and magnetization respectivley) fields are related to the net polarization of the dipole moments thoughout the medium, i.e. how well they respond to an external field, and how the orientation of the dipoles can retain (or not) the field they set up in response to the external field.
— the D and H (electric displacement and magnetic intensity field) fields are the least clear to understand physically; they are introduced for convenient thoretical simplifications, but one could imagine they relate to the strength of the field along the flux lines, strength as a linear density along flux lines.
Hypothical Magnetic Monopoles
— As far as is known, there are no magnetic monopoles in nature, though some theories predict they could exist.
— The approach to introduce monopoles in equations is to define a magnetic pole strength, magnetic charge, or monopole charge (all synonomous), treating poles analogously to the electric charges.
— One pole would be north N (numerically positive by convention), the other south S (numerically negative). There are two units which can be used from the SI system for pole strength.
— Pole srength can be quantified into densities, currents and current densities, as electric charge is in the previous table, exactly in the same way.
Maxwell's Equations would become one of the columns in the table below, at least theoretically. Subscripts e are electric charge quantities; subscripts m are magnetic charge quantities.
| Name | Weber (Wb) Convention | Ampere meter (A m) Convention |
| Gauss's Law | $\nabla \cdot \mathbf {E} =\rho _{\mathrm {e} }/\epsilon _{0}$ | $\nabla \cdot \mathbf {E} =\rho _{\mathrm {e} }/\epsilon _{0}$ |
| Gauss's Law for magnetism | $\nabla \cdot \mathbf {B} =\rho _{\mathrm {m} }$ | $\nabla \cdot \mathbf {B} =\mu _{0}\rho _{\mathrm {m} }$ |
| Faraday's Law of induction | $-\nabla \times \mathbf {E} ={\frac {\partial \mathbf {B} }{\partial t}}+\mathbf {j} _{\mathrm {m} }$ | $-\nabla \times \mathbf {E} ={\frac {\partial \mathbf {B} }{\partial t}}+\mu _{0}\mathbf {j} _{\mathrm {m} }$ |
| Ampère's Law | $\nabla \times \mathbf {B} =\mu _{0}\epsilon _{0}{\frac {\partial \mathbf {E} }{\partial t}}+\mu _{0}\mathbf {j} _{\mathrm {e} }$ | $\nabla \times \mathbf {B} =\mu _{0}\epsilon _{0}{\frac {\partial \mathbf {E} }{\partial t}}+\mu _{0}\mathbf {j} _{\mathrm {e} }$ |
| Lorentz force equation | $\mathbf {F} =q_{\mathrm {e} }\left(\mathbf {E} +\mathbf {v} \times \mathbf {B} \right)+$ $+{\frac {q_{\mathrm {m} }}{\mu _{0}}}\left(\mathbf {B} -\mathbf {v} \times (\mathbf {E} /c^{2})\right)$ | $\mathbf {F} =q_{\mathrm {e} }\left(\mathbf {E} +\mathbf {v} \times \mathbf {B} \right)+$ $+q_{\mathrm {m} }\left(\mathbf {B} -\mathbf {v} \times (\mathbf {E} /c^{2})\right)$ |
They are consistent if no magnetic monopoles, since monopole quantities are then zero and the equations reduce to the original form of Maxwell's equations.

### Pre-Maxwell Laws

These laws are not fundamental anymore, since they can be derived from Maxwell's Equations. Coulomb's Law can be found from Gauss' Law (electrostatic form) and the Biot-Savart Law can be deduced from Ampere's Law (magnetostatic form). Lenz' Law and Faraday's Law can be incorperated into the Maxwell-Faraday equation. Nonetheless they are still very effective for simple calculations, especially for highly symmetrical problems.
| Coulomb's Law | $\mathbf {E} ={\frac {\mathbf {F} }{Q}}={\frac {q}{4\pi \epsilon _{0}\left|\mathbf {r} \right|^{2}}}\mathbf {\hat {r}} \,\!$ For a non uniform charge distribution, this becomes: $\mathbf {E} ={\frac {1}{4\pi \epsilon _{0}}}\int _{V_{n}}{\frac {\mathbf {r} \rho _{n}\mathrm {d} {V_{n}}}{\left|\mathbf {r} \right|^{3}}}\,\!$ |
| Biot-Savart Law | $\mathbf {B} ={\frac {\mu _{0}}{4\pi }}\int _{C}{\frac {I\left(\mathrm {d} \mathbf {l} \times \mathbf {r} \right)}{\left|\mathbf {r} \right|^{3}}},\,\!$ |
| Lenz's law | Induced current always opposes its cause. |

## Electric Quantities

Electric Charge and Current
| Quantity (Common Name/s) | (Common) Symbol/s | Defining Equation | SI Units | Dimension |
| Elementary Charge Quantum | $e\,\!$ | | C = A s | [I][T] |
| Quantized Electric Charge | q | $q=ne\,\!$ | C = A s | [I][T] |
| Electric Charge (any amount) | $q\,\!$ | | C = A s | [I][T] |
| Electric charge density of dimension n ($V_{n}\,\!$ = n-space) n = 1 for linear mass density, n = 2 for surface mass density, n = 3 for volume mass density, etc | linear charge density $\lambda \,\!$, surface charge density $\sigma \,\!$, volume charge density $\rho \,\!$, no general symbol for any dimension | n-space charge density: $\rho _{n}={\frac {\partial ^{n}m}{\partial x_{n}\cdots \partial x_{2}\partial x_{1}}}={\frac {\partial m}{\partial V_{n}}}\,\!$ special cases are: $\lambda ={\frac {\partial m}{\partial x}}\,\!$ $\sigma ={\frac {\partial ^{2}m}{\partial x_{2}\partial x_{1}}}={\frac {\partial ^{2}m}{\partial S}}\,\!$ $\rho ={\frac {\partial ^{3}m}{\partial x_{3}\partial x_{2}\partial x_{1}}}={\frac {\partial m}{\partial V}}\,\!$ | C m$^{-n}$ | [I][T][L]$^{-n}$ |
| Total descrete charge | $Q\,\!$ | $Q=\sum _{i}q_{i}\,\!$ | C | [I][T] |
| Total continuum charge | $Q\,\!$ | n-space charge density $Q=\int \rho _{n}\mathrm {d} ^{n}x=\int \cdots \int \int \rho _{n}\mathrm {d} x_{1}\mathrm {d} x_{2}\cdots \mathrm {d} x_{n}\,\!$ special cases are: $Q=\int \lambda \mathrm {d} x\,\!$ $Q=\int \sigma \mathrm {d} A=\iint \sigma \mathrm {d} x_{1}\mathrm {d} x_{2}\,\!$ $Q=\int \rho \mathrm {d} V=\iiint \rho \mathrm {d} x_{1}\mathrm {d} x_{2}\mathrm {d} x_{3}\,\!$ | C | [I][T] |
| Capacitance | $C\,\!$ | $C={\frac {\partial q}{\partial V}}\,\!$ | F = C V$^{-1}$ | |
| Electric Current | $I\,\!$ | $I={\frac {\mathrm {d} q}{\mathrm {d} t}}\,\!$ | A | [I] |
| Current Density | $\mathbf {J} \,\!$ | $\mathbf {J} =\mathbf {\hat {A}} {\frac {\partial I}{\partial A}}\,\!$ | A m$^{-2}$ | [I][L]$^{-2}$ |
| Displacement current | $I_{\mathrm {d} }\,\!$ | $I_{\mathrm {d} }=\epsilon _{0}{\frac {\partial \Phi _{E}}{\partial t}}\,\!$ | A | [I] |
| Charge Carrier Drift Speed | $\mathbf {v} _{d}$ | | m s$^{-1}$ | [L][T]$^{-1}$ |
Electric Fields
| Quantity (Common Name/s) | (Common) Symbol/s | Defining Equation | SI Units | Dimension |
| Electric Field, Field Strength, Flux Density, Potential Gradient | $\mathbf {E} \,\!$ | $\mathbf {E} =\mathbf {F} /q\,\!$ | N C$^{-1}$ = V m$^{-1}$ | [M][L][T]$^{-3}$[I]$^{-1}$ |
| Electric Flux | $\Phi _{E}\,\!$ | $\Phi _{E}=\int _{S}\mathbf {E} \cdot \mathrm {d} \mathbf {A} \,\!$ | N m$^2$ C$^{-1}$ | [M][L]$^3$[T]$^{-3}$[I]$^{-1}$ |
| Electric Permittivity | $\epsilon \,\!$ | $\epsilon =\epsilon _{\mathrm {r} }\epsilon _{0}\,\!$ | F m$^{-1}$ | |
| Dielectric constant, Relative Permittivity | $\epsilon _{\mathrm {r} }\,\!$ | | F m$^{-1}$ | |
| Electric Displacement Field | $\mathbf {D} \,\!$ | $\mathbf {D} ={\frac {\mathbf {E} }{\epsilon }}\,\!$ | C m$^{-2}$ | [I][T][L]$^{-2}$ |
| Electric Displacement Flux | $\Phi _{D}\,\!$ | $\Phi _{D}=\int _{S}\mathbf {D} \cdot \mathrm {d} \mathbf {A} \,\!$ | C | [I][T] |
| Electric Dipole Moment vector | $\mathbf {p} \,\!$ | $\mathbf {p} =2q\mathbf {a} \,\!$ $\mathbf {a} \,\!$ is the charge separation directed from -ve to +ve charge | C m | [I][T][L] |
| Electric Polarization | $\mathbf {P} \,\!$ | $\mathbf {P} ={\frac {\partial \langle \mathbf {p} \rangle }{\partial V}}\,\!$ | C m$^{-2}$ | [I][T][L]$^{-2}$ |
| Absolute Electric Potential relative to point $r_{0}\,\!$ Theoretical: $r_{0}=\infty \,\!$ Practical: $R_{0}=R_{\mathrm {earth} }\,\!$ (Earth's radius) | $\phi ,V\,\!$ | $V=-{\frac {W_{\infty r}}{q}}=-{\frac {1}{q}}\int _{\infty }^{r}\mathbf {F} \cdot \mathrm {d} \mathbf {r} =-\int _{r_{1}}^{r_{2}}\mathbf {E} \cdot \mathrm {d} \mathbf {r} \,\!$ | V = J C$^{-1}$ | |
| Electric Potential Difference | $\Delta V\,\!$ | $\Delta V=-{\frac {\Delta W}{q}}=-{\frac {1}{q}}\int _{r_{1}}^{r_{2}}\mathbf {F} \cdot \mathrm {d} \mathbf {r} =-\int _{r_{1}}^{r_{2}}\mathbf {E} \cdot \mathrm {d} \mathbf {r} \,\!$ | | |
| Electric Potential Energy | $U\,\!$ | $U=-W\,\!$ | J | [M][L]$^2$[T]$^2$ |

## Magnetic Quantities

| Quantity (Common Name/s) | (Common) Symbol/s | Defining Equation | SI Units | Dimension |
| Magnetic Field, Field Strength, Flux Density, Induction Field | $\mathbf {B} \,\!$ | $\mathbf {F} =q\left(\mathbf {v} \times \mathbf {B} \right)\,\!$ | T = N A$^{-1}$ m$^{-1}$ | |
| Magnetic Flux | $\Phi _{B}\,\!$ | $\Phi _{B}=\int _{S}\mathbf {B} \cdot \mathrm {d} \mathbf {A} \,\!$ | Wb = T m$^{-2}$ | |
| Magnetic Permeability | $\mu \,\!$ | $\mu =\mu _{\mathrm {r} }\mu _{0}\,\!$ | H m$^{-1}$ | |
| Relative Permeability | $\mu _{\mathrm {r} }\,\!$ | | H m$^{-1}$ | |
| Magnetic Field Intensity, (also confusingly the field strength) | $\mathbf {H} \,\!$ | $\mathbf {H} ={\frac {\mathbf {B} }{\mu }}\,\!$ | | |
| Magnetic Dipole Moment vector | $\mathbf {m} \,\!$ | $\mathbf {m} =NI\mathbf {A} \,\!$ N is the number of turns of conductor | A m$^2$ | [I][L]$^2$ |
| Magnetization | $\mathbf {M} \,\!$ | $\mathbf {M} ={\frac {\partial \langle \mathbf {m} \rangle }{\partial V}}\,\!$ | | |
| Self Inductance | $L\,\!$ | Two equivalent definitions are in fact possible: $L=N{\frac {\partial \Phi }{\partial I}}\,\!$ $L{\frac {\partial I}{\partial t}}=-NV\,\!$ | H = Wb A$^{-1}$ | |
| Mutual Inductance | $M\,\!$ | Again two equivalent definitions are in fact possible: $M_{X}=N{\frac {\partial \Phi _{Y}}{\partial I_{X}}}\,\!$ $M{\frac {\partial I_{Y}}{\partial t}}=-NV_{X}\,\!$ X,Y subscripts refer to two conductors mutually inducing voltage/ linking magnetic flux though each other | H = Wb A$^{-1}$ | |

## Electric Fields
### Electrostatic Fields

Common corolaries from Couloumb's and Gauss' Law (in turn corolaries of Maxwell's Equations) for uniform charge distributions are summarized in the table below.
| Uniform Electric Field accelerating a charged mass | $a={\frac {qE}{m}}\,\!$ |
| Point Charge | $\mathbf {E} ={\frac {q}{4\pi \epsilon _{0}\left|\mathbf {r} \right|^{2}}}\mathbf {\hat {r}} \,\!$ |
| At a point in a local array of Point Charges | $\mathbf {E} =\sum \mathbf {E} _{i}={\frac {1}{4\pi \epsilon _{0}}}\sum _{i}{\frac {q_{i}}{\left|\mathbf {r} _{i}-\mathbf {r} \right|^{2}}}\mathbf {\hat {r}} _{i}\,\!$ |
| Electric Dipole | $\mathbf {E} \approx {\frac {\left|\mathbf {p} \right|}{2\pi \epsilon _{0}z^{3}}}\mathbf {\hat {z}} \,\!$ $\left|\mathbf {r} \right|>>\left|\mathbf {a} \right|\,\!$ |
| Line of a Charge | $\mathbf {E} ={\frac {\lambda }{2\pi \epsilon _{0}\left|\mathbf {r} \right|}}\mathbf {\hat {r}} \,\!$ |
| Charged Ring | $\mathbf {E} ={\frac {qz}{4\pi \epsilon _{0}(z^{2}+R^{2})^{3/2}}}\mathbf {\hat {z}} \,\!$ |
| Charged Conducting Surface | $\mathbf {E} ={\frac {\sigma }{\epsilon _{0}}}\mathbf {\hat {n}} \,\!$ |
| Charged Insulating Surface | $\mathbf {E} ={\frac {\sigma }{2\epsilon _{0}}}\mathbf {\hat {n}} \,\!$ |
| Charged Disk | $\mathbf {E} ={\frac {\sigma (1-z)}{2\epsilon _{0}{\sqrt {z^{2}+R^{2}}}}}\mathbf {\hat {z}} \,\!$ |
| Outside Spherical Shell r>=R | $\mathbf {E} ={\frac {q}{4\pi \epsilon _{0}\left|\mathbf {r} \right|^{2}}}\mathbf {\hat {r}} \,\!$ |
| Inside Spherical Shell r<R | $\mathbf {E} =\mathbf {0} \,\!$ |
| Uniform Charge r<=R | $\mathbf {E} ={\frac {q\left|\mathbf {r} \right|}{4\pi \epsilon _{0}R^{3}}}\mathbf {\hat {r}} \,\!$ |
| Electric Dipole Potential Energy in a uniform Electric Eield | $U=-\mathbf {p} \cdot \mathbf {E} \,\!$ |
| Torque on an Electric Dipole in a uniform Electric Eield | ${\boldsymbol {\tau }}=\mathbf {p} \times \mathbf {E} \,\!$ |
| Electric Field Energy Density Linear media (constant $\epsilon \,\!$ throughout) | $u={\frac {\epsilon E^{2}}{2}}\,\!$ |
For non-uniform fields and electric dipole moments, the electrostatic torque and potential energy are:
    $U=\int \left(\mathbf {E} \cdot \mathrm {d} \mathbf {p} +\mathbf {p} \cdot \mathrm {d} \mathbf {E} \right)\,\!$ ${\boldsymbol {\tau }}=\int \left(\mathrm {d} \mathbf {p} \times \mathbf {E} +\mathbf {p} \times \mathrm {d} \mathbf {E} \right)\,\!$
Electric Potential and Electric Field
    $\Delta V=-\int _{r_{1}}^{r_{1}}\mathbf {E} \cdot d\mathbf {r} \,\!$ $\nabla V=-\mathbf {E} \,\!$

### Electrostatic Potentials

| Point Charge | $V={\frac {q}{4\pi \epsilon _{0}r}}\,\!$ |
| Pair of Point Charges | $V={\frac {q_{1}q_{2}}{4\pi \epsilon _{0}r}}\,\!$ |

### Electrostatic Capacitances

| Parallel Plates | $C={\frac {\epsilon _{0}A}{d}}\,\!$ |
| Cylinder | $C={\frac {\epsilon _{0}2\pi L}{\ln \left|{\frac {b}{a}}\right|}}\,\!$ |
| Sphere | $C=4\pi \epsilon _{0}{\frac {ba}{b-a}}\,\!$ |
| Isolated Sphere | $C=4\pi \epsilon _{0}R\,\!$ |
| Capacitors Connected in Parallel | $C_{\mathrm {net} }=\sum _{i}C_{i}\,\!$ |
| Capacitors Connected in Series | ${\frac {1}{C_{\mathrm {net} }}}=\sum _{i}{\frac {1}{C_{i}}}\,\!$ |
| Capacitor Potential Energy | $U={\frac {q^{2}}{2C}}={\frac {CV^{2}}{2}}\,\!$ |

## Magnetic Fields
### Magnetic Forces

Force on a Moving Charge
    $\mathbf {F} =q\mathbf {v} \times \mathbf {B} \,\!$
Force on a Current-Carrying Conductor
    $\mathbf {F} =I\mathbf {l} \times \mathbf {B} \,\!$

### Magnetostatic Fields

Common corolaries from the Biot-Savart Law and Ampere's Law (again corolaries of Maxwell's Equations) for steady (constant) current-carrying configerations are summarized in the table below.
For these types of current configerations, the magnetic field is easily evaluated using the Biot-Savart Law, containing the vector $\mathrm {d} \mathbf {l} \times \mathbf {r} \,\!$, which is also the direction of the magnetic field at the point evaluated.
For conveinence in the results below, let $\mathbf {b} =\mathrm {d} \mathbf {l} \times \mathbf {r} \,\!$ be a unit binormal vector to $\mathbf {l} \,\!$ and $\mathbf {r} \,\!$, so that
$\mathbf {\hat {b}} ={\frac {\mathrm {d} \mathbf {l} \times \mathbf {r} }{\left|\mathrm {d} \mathbf {l} \times \mathbf {r} \right|}}\,\!$
then $\mathbf {\hat {b}} \,\!$ also the unit vector for the direction of the magnetic field at the point evaluated.
| Hall Effect | $n={\frac {BI}{Vle}}\,\!$ |
| Circulating Charged Particle | $q\mathbf {v} \times \mathbf {B} ={\frac {m\left|\mathbf {v} \right|^{2}}{\left|\mathbf {r} \right|}}\mathbf {\hat {r}} \,\!$ |
| Infinite Line of Current | $\mathbf {B} ={\frac {\mu _{0}I}{2\pi \left|\mathbf {r} \right|}}\mathbf {\hat {b}} \,\!$ |
| Magnetic Field of a Ray | $\mathbf {B} ={\frac {\mu _{0}I}{4\pi \left|\mathbf {r} \right|}}\,\!$ |
| Center of a Circular Arc | $\mathbf {B} ={\frac {\mu _{0}I\phi }{4\pi \left|\mathbf {r} \right|}}\mathbf {\hat {b}} \,\!$ |
| Infinitley Long Solenoid | $\mathbf {B} =\mu _{0}nI\mathbf {\hat {b}} \,\!$ |
| Toroidal Inductors and Transformers | $\mathbf {B} ={\frac {\mu _{0}IN}{2\pi \left|\mathbf {r} \right|}}\mathbf {\hat {b}} \,\!$ |
| Current Carrying Coil | $\mathbf {B} ={\frac {\mu }{2\pi z^{3}}}\mathbf {\hat {b}} \,\!$ |
| Magnetic Dipole Potential Energy in a uniform Magnetic Eield | $U=-\mathbf {m} \cdot \mathbf {B} \,\!$ |
| Torque on a Magnetic Dipole in a uniform Magnetic Eield | ${\boldsymbol {\tau }}=\mathbf {m} \times \mathbf {B} \,\!$ |
For non-uniform fields and magnetic moments, the magnetic potential energy and torque are:
    $U=\int \left(\mathbf {B} \cdot \mathrm {d} \mathbf {m} +\mathbf {m} \cdot \mathrm {d} \mathbf {B} \right)\,\!$ ${\boldsymbol {\tau }}=\int \left(\mathrm {d} \mathbf {m} \times \mathbf {B} +\mathbf {m} \times \mathrm {d} \mathbf {B} \right)\,\!$

### Magnetic Energy

| Magnetic Energy for Linear Media ($\mu \,\!$ constant at all points in meduim) | $U={\frac {LI^{2}}{2}}\,\!$ |
| Magnetic Energy Density for Linear Media ($\mu \,\!$ constant at all points in meduim) | $u={\frac {B^{2}}{2\mu }}\,\!$ |

## EM Induction

| Self Induction of emf | ${\mathcal {E}}_{L}=-L{\frac {\mathrm {d} I}{\mathrm {d} t}}\,\!$ |
| Mutual Induction | ${\mathcal {E}}_{1}=-M{\frac {\mathrm {d} I_{2}}{\mathrm {d} t}},{\mathcal {E}}_{2}=-M{\frac {\mathrm {d} I_{1}}{\mathrm {d} t}}\,\!$ |
| transformation of voltage | $V_{s}N_{p}=V_{p}N_{s}\,\!$ $I_{s}N_{s}=I_{p}N_{p}\,\!$ $R_{\mathrm {eq} }=\left({\frac {N_{p}}{N_{s}}}\right)^{2}R\,\!$ |
| Induced Magnetic Field inside a circular capacitor | $B=(\mu _{0}I_{d}/2\pi R^{2})r\,\!$ |
| Induced Magnetic Field outside a circular capacitor | $B=\mu _{0}I_{d}/2\pi rr\,\!$ |

## External Links

Maxwell's Equations
Electric Field
Magnetic Field
Electric Charge
Magnetic Monopoles