Physics formulas: Electrodynamics

Quick reference for school physics (electrodynamics). Browse by topic or search by name.

Electrostatics

Coulomb's law

F=kq1q2r2F = \frac{k|q_1 q_2|}{r^2}
Symbols
  • FFmagnitude of the force between point charges, N (newton)
  • kkCoulomb constant, 9×10⁹ N·m²/C²
  • q1,q2q_1, q_2magnitudes of the charges, C (coulomb)
  • rrdistance between the charges, m (meter)
k=9109Nm2/C2k = 9 \cdot 10^9\,\text{N}\cdot\text{m}^2/\text{C}^2 is Coulomb's constant.
Electrostatics

Electric field strength

E=FqE = \frac{F}{q}
Symbols
  • EEelectric field intensity, V/m
  • FFforce acting on the test charge, N (newton)
  • qqmagnitude of the test charge, C (coulomb)
Electrostatics

Electric field of a point charge

E=kqr2E = \frac{k|q|}{r^2}
Symbols
  • EEelectric field of a point charge, V/m
  • kkCoulomb constant, 9×10⁹ N·m²/C²
  • qqmagnitude of the charge, C (coulomb)
  • rrdistance from the charge to the field point, m (meter)
Electrostatics

Electric field of a charged sphere

E=kqr2E = \frac{k|q|}{r^2}
E=0E = 0
Symbols
  • EEelectric field intensity, V/m
  • kkCoulomb constant, 9×10⁹ N·m²/C²
  • qqtotal charge of the sphere, C (coulomb)
  • rrdistance from the center of the sphere (outside), m (meter)
  • RRradius of the charged sphere, m (meter)
Outside the sphere (r>Rr > R) — first formula; inside a conductor (rRr \leq R) — E=0E = 0.
Electrostatics

Principle of superposition of electric fields

E=E1+E2+E3+E = E_1 + E_2 + E_3 + \ldots
Symbols
  • EEresultant electric field, V/m
  • E1,E2,E_1, E_2, \ldotsfield intensities of individual charges, V/m
Electrostatics

Electric potential

φ=Wq\varphi = \frac{W}{q}
Symbols
  • φ\varphielectric potential at a field point, V (volt)
  • WWwork of electric forces when moving the charge, J (joule)
  • qqcharge being moved, C (coulomb)
Electrostatics

Potential of a point charge

φ=kqr\varphi = \frac{kq}{r}
Symbols
  • φ\varphipotential of a point charge field, V (volt)
  • kkCoulomb constant, 9×10⁹ N·m²/C²
  • qqmagnitude of the charge, C (coulomb)
  • rrdistance from the charge to the field point, m (meter)
Electrostatics

Potential of a charged sphere

φ=kqr\varphi = \frac{kq}{r}
φ=kqR\varphi = \frac{kq}{R}
Symbols
  • φ\varphielectric potential, V (volt)
  • kkCoulomb constant, 9×10⁹ N·m²/C²
  • qqtotal charge of the sphere, C (coulomb)
  • rrdistance from the center of the sphere (outside), m (meter)
  • RRradius of the charged sphere, m (meter)
Outside (r>Rr > R) — φ=kq/r\varphi = kq/r; on the surface and inside (rRr \leq R) — φ=kq/R\varphi = kq/R.
Electrostatics

Potential in a uniform electric field

φ=Ed\varphi = Ed
Symbols
  • φ\varphipotential difference between the points, V (volt)
  • EEintensity of the uniform field, V/m
  • dddistance along the field lines, m (meter)
Electrostatics

Potential of a system of point charges

φ=φ1+φ2+\varphi = \varphi_1 + \varphi_2 + \ldots
Symbols
  • φ\varphitotal potential at the point, V (volt)
  • φ1,φ2,\varphi_1, \varphi_2, \ldotspotentials of individual charges, V (volt)
Electrostatics

Work moving a charge in an electric field

W=qUW = qU
Symbols
  • WWwork done by the electric field, J (joule)
  • qqcharge being moved, C (coulomb)
  • UUpotential difference (voltage), V (volt)
Electrostatics

Relation between field strength and voltage

E=UdE = \frac{U}{d}
Symbols
  • EEintensity of a uniform electric field, V/m
  • UUvoltage between the plates, V (volt)
  • dddistance between the plates, m (meter)
Electrostatics

Potential energy of two point charges

W=kq1q2rW = \frac{kq_1 q_2}{r}
Symbols
  • WWpotential energy of interaction of two charges, J (joule)
  • kkCoulomb constant, 9×10⁹ N·m²/C²
  • q1,q2q_1, q_2magnitudes of the charges, C (coulomb)
  • rrdistance between the charges, m (meter)
Electrostatics

Capacitance

C=qUC = \frac{q}{U}
Symbols
  • CCcapacitance of the capacitor, F (farad)
  • qqcharge on the plates, C (coulomb)
  • UUvoltage across the capacitor, V (volt)
Electrostatics

Capacitance of a parallel-plate capacitor

C=εε0SdC = \frac{\varepsilon\varepsilon_0 S}{d}
Symbols
  • CCcapacitance of a parallel-plate capacitor, F (farad)
  • ε\varepsilonrelative permittivity of the medium, dimensionless quantity
  • ε0\varepsilon_0electric constant (vacuum permittivity), 8.85×10⁻¹² F/m
  • SSarea of the plates, m² (square meter)
  • dddistance between the plates, m (meter)
Electrostatics

Capacitors in parallel

C=C1+C2+C = C_1 + C_2 + \ldots
Symbols
  • CCtotal capacitance in parallel connection, F (farad)
  • C1,C2,C_1, C_2, \ldotscapacitances of individual capacitors, F (farad)
Electrostatics

Capacitors in series

1C=1C1+1C2+\frac{1}{C} = \frac{1}{C_1} + \frac{1}{C_2} + \ldots
Symbols
  • CCtotal capacitance in series connection, F (farad)
  • C1,C2,C_1, C_2, \ldotscapacitances of individual capacitors, F (farad)
Electrostatics

Energy of a charged capacitor

W=CU22W = \frac{CU^2}{2}
Symbols
  • WWenergy stored in the capacitor electric field, J (joule)
  • CCcapacitance of the capacitor, F (farad)
  • UUvoltage across the capacitor, V (volt)
Also W=q22CW = \frac{q^2}{2C} and W=qU2W = \frac{qU}{2}.
Electrostatics

Surface charge density

σ=qS\sigma = \frac{q}{S}
Symbols
  • σ\sigmasurface charge density, C/m²
  • qqcharge on the surface, C (coulomb)
  • SSarea of the surface, m² (square meter)
Direct current

Electric current

I=qtI = \frac{q}{t}
Symbols
  • IIelectric current, A (ampere)
  • qqelectric charge passing through the conductor cross-section, C (coulomb)
  • tttime during which the charge passes, s (second)
Direct current

Current (drift model)

I=neSvI = neSv
Symbols
  • IIelectric current, A (ampere)
  • nnconcentration of charge carriers, m⁻³
  • eecharge of one carrier (electron), 1.6×10⁻¹⁹ C
  • SScross-sectional area of the conductor, m² (square meter)
  • vvdrift speed of the charge carriers, m/s
Direct current

Current density

j=IS=nevj = \frac{I}{S} = nev
Symbols
  • jjelectric current density, A/m²
  • IIelectric current, A (ampere)
  • SScross-sectional area, m² (square meter)
  • nnconcentration of charge carriers, m⁻³
  • eecharge of one carrier, 1.6×10⁻¹⁹ C
  • vvdrift speed of the carriers, m/s
Direct current

Ohm's law

I=URI = \frac{U}{R}
Symbols
  • IIcurrent in the circuit section, A (ampere)
  • UUvoltage across the section, V (volt)
  • RRelectrical resistance of the section, Ω (ohm)
Direct current

Resistance of a conductor

R=ρlSR = \frac{\rho l}{S}
Symbols
  • RRresistance of the conductor, Ω (ohm)
  • ρ\rhoresistivity of the material, Ω·m
  • lllength of the conductor, m (meter)
  • SScross-sectional area, m² (square meter)
Direct current

Temperature dependence of resistance

R=R0(1+α(tt0))R = R_0(1 + \alpha(t - t_0))
Symbols
  • RRresistance at temperature t, Ω (ohm)
  • R0R_0resistance at the reference temperature t_0, Ω (ohm)
  • α\alphatemperature coefficient of resistance, °C⁻¹
  • ttcurrent temperature, °C (degree Celsius)
  • t0t_0reference temperature, °C (degree Celsius)
Direct current

Resistors in series

R=R1+R2+R = R_1 + R_2 + \ldots
Symbols
  • RRtotal resistance in series connection, Ω (ohm)
  • R1,R2,R_1, R_2, \ldotsresistances of individual resistors, Ω (ohm)
Direct current

Resistors in parallel

1R=1R1+1R2+\frac{1}{R} = \frac{1}{R_1} + \frac{1}{R_2} + \ldots
Symbols
  • RRtotal resistance in parallel connection, Ω (ohm)
  • R1,R2,R_1, R_2, \ldotsresistances of individual resistors, Ω (ohm)
Direct current

Work of electric current

W=UItW = UIt
Symbols
  • WWwork done by the electric current, J (joule)
  • UUvoltage across the circuit section, V (volt)
  • IIelectric current, A (ampere)
  • tttime during which the current flows, s (second)
Direct current

Electric power

P=UIP = UI
Symbols
  • PPelectric power, W (watt)
  • UUvoltage, V (volt)
  • IIelectric current, A (ampere)
Direct current

Joule–Lenz law

Q=I2RtQ = I^2 R t
Symbols
  • QQheat released in the conductor, J (joule)
  • IIelectric current, A (ampere)
  • RRresistance of the conductor, Ω (ohm)
  • tttime during which the current flows, s (second)
Direct current

Electromotive force (EMF)

E=Wextq\mathcal{E} = \frac{W_{\text{ext}}}{q}
Symbols
  • E\mathcal{E}electromotive force (EMF), V (volt)
  • WextW_{\text{ext}}work of external forces moving charge around a closed loop, J (joule)
  • qqcharge being moved, C (coulomb)
Direct current

Ohm's law for a complete circuit

I=ER+rI = \frac{\mathcal{E}}{R + r}
Symbols
  • IIcurrent in the complete circuit, A (ampere)
  • E\mathcal{E}EMF of the source, V (volt)
  • RRexternal resistance of the circuit, Ω (ohm)
  • rrinternal resistance of the source, Ω (ohm)
Direct current

Current with sources connected in series

I=nER+nrI = \frac{n\mathcal{E}}{R + nr}
Symbols
  • IIcurrent with sources connected in series, A (ampere)
  • nnnumber of identical sources, dimensionless quantity
  • E\mathcal{E}EMF of one source, V (volt)
  • RRexternal resistance, Ω (ohm)
  • rrinternal resistance of one source, Ω (ohm)
Direct current

Current with sources connected in parallel

I=ER+r/nI = \frac{\mathcal{E}}{R + r/n}
Symbols
  • IIcurrent with sources connected in parallel, A (ampere)
  • E\mathcal{E}EMF of one source, V (volt)
  • RRexternal resistance, Ω (ohm)
  • rrinternal resistance of one source, Ω (ohm)
  • nnnumber of identical sources, dimensionless quantity
Direct current

Faraday's law of electrolysis

m=kItm = kIt
Symbols
  • mmmass of substance deposited on the electrode, kg (kilogram)
  • kkelectrochemical equivalent of the substance, kg/(A·s)
  • IIelectric current, A (ampere)
  • tttime of electrolysis, s (second)
Magnetic field of electric current

Magnitude of magnetic induction

B=FIlB = \frac{F}{Il}
Symbols
  • BBmagnitude of the magnetic induction vector, T (tesla)
  • FFAmpère force on the conductor (perpendicular to B), N (newton)
  • IIcurrent in the conductor, A (ampere)
  • lllength of the conductor segment in the field, m (meter)
When force FF is perpendicular to B\vec{B}.
Magnetic field of electric current

Ampère's force

F=BIsinαF = BI\ell\sin\alpha
Symbols
  • FFforce on a current-carrying conductor in a magnetic field, N (newton)
  • BBmagnetic induction, T (tesla)
  • IIelectric current, A (ampere)
  • \elllength of the conductor in the field, m (meter)
  • α\alphaangle between B and the current direction, rad
Magnetic field of electric current

Lorentz force

F=qvBsinαF = qvB\sin\alpha
Symbols
  • FFLorentz force acting on a charged particle, N (newton)
  • qqcharge of the particle, C (coulomb)
  • vvspeed of the particle, m/s
  • BBmagnetic induction, T (tesla)
  • α\alphaangle between v and B, rad
Magnetic field of electric current

Momentum of a charged particle in a magnetic field

p=qBRp = qBR
Symbols
  • ppmomentum of the charged particle in the magnetic field, kg·m/s
  • qqcharge of the particle, C (coulomb)
  • BBmagnetic induction, T (tesla)
  • RRradius of the particle trajectory (circle), m (meter)
Magnetic field of electric current

Magnetic flux

Φ=BScosα\Phi = BS\cos\alpha
Symbols
  • Φ\Phimagnetic flux through a surface, Wb (weber)
  • BBmagnetic induction, T (tesla)
  • SSarea of the surface, m² (square meter)
  • α\alphaangle between B and the surface normal, rad
Electromagnetic induction

Law of electromagnetic induction

E=ΔΦΔt\mathcal{E} = -\frac{\Delta\Phi}{\Delta t}
Symbols
  • E\mathcal{E}induced EMF, V (volt)
  • ΔΦ\Delta\Phichange in magnetic flux, Wb (weber)
  • Δt\Delta ttime interval of the flux change, s (second)
Electromagnetic induction

Magnetic flux through a surface

Φ=BScosα\Phi = BS\cos\alpha
Symbols
  • Φ\Phimagnetic flux through a surface, Wb (weber)
  • BBmagnetic induction, T (tesla)
  • SSarea of the surface, m² (square meter)
  • α\alphaangle between B and the surface normal, rad
Electromagnetic induction

Maximum EMF of a frame rotating in a magnetic field

Emax=BSω\mathcal{E}_{\max} = BS\omega
Symbols
  • Emax\mathcal{E}_{\max}maximum induced EMF in a rotating frame, V (volt)
  • BBmagnetic induction, T (tesla)
  • SSarea of the frame, m² (square meter)
  • ω\omegaangular velocity of rotation of the frame, rad/s
Electromagnetic induction

Self-induction EMF

Es=LΔIΔt\mathcal{E}_s = -L\,\frac{\Delta I}{\Delta t}
Symbols
  • Es\mathcal{E}_sself-induction EMF, V (volt)
  • LLinductance of the coil, H (henry)
  • ΔI\Delta Ichange in current, A (ampere)
  • Δt\Delta ttime interval of the current change, s (second)
Electromagnetic induction

Motional EMF in a moving conductor

E=Blvsinα\mathcal{E} = Blv\sin\alpha
Symbols
  • E\mathcal{E}motional EMF of a conductor in a magnetic field, V (volt)
  • BBmagnetic induction, T (tesla)
  • lllength of the conductor, m (meter)
  • vvspeed of the conductor, m/s
  • α\alphaangle between B and v, rad
Electromagnetic induction

Induced charge

q=ΔΦRq = \frac{\Delta\Phi}{R}
Symbols
  • qqinduced charge in the circuit, C (coulomb)
  • ΔΦ\Delta\Phichange in magnetic flux, Wb (weber)
  • RRresistance of the circuit, Ω (ohm)
Electromagnetic oscillations

Oscillating charge

q(t)=qmcosωtq(t) = q_m\cos\omega t
Symbols
  • q(t)q(t)charge on the capacitor plates at time t, C (coulomb)
  • qmq_mamplitude of charge oscillations, C (coulomb)
  • ω\omegaangular frequency of oscillations, rad/s
  • tttime, s (second)
Electromagnetic oscillations

Oscillating voltage

u(t)=umcosωtu(t) = u_m\cos\omega t
Symbols
  • u(t)u(t)voltage across the capacitor at time t, V (volt)
  • umu_mamplitude of voltage oscillations, V (volt)
  • ω\omegaangular frequency, rad/s
  • tttime, s (second)
Electromagnetic oscillations

Oscillating current

i(t)=imcos(ωt+π2)i(t) = i_m\cos\left(\omega t + \frac{\pi}{2}\right)
Symbols
  • i(t)i(t)current in the circuit at time t, A (ampere)
  • imi_mamplitude of current oscillations, A (ampere)
  • ω\omegaangular frequency, rad/s
  • tttime, s (second)
Electromagnetic oscillations

Maximum oscillation current

im=ωqmi_m = \omega q_m
Symbols
  • imi_mamplitude of current oscillations, A (ampere)
  • ω\omegaangular frequency, rad/s
  • qmq_mamplitude of charge oscillations, C (coulomb)
Electromagnetic oscillations

Thomson oscillation period

T=2πLCT = 2\pi\sqrt{LC}
Symbols
  • TTperiod of electromagnetic oscillations (Thomson period), s (second)
  • LLinductance of the coil, H (henry)
  • CCcapacitance of the capacitor, F (farad)
Electromagnetic oscillations

Energy of the coil magnetic field

Wm=LI22W_m = \frac{LI^2}{2}
Symbols
  • WmW_menergy of the magnetic field of the coil, J (joule)
  • LLinductance of the coil, H (henry)
  • IIcurrent in the coil, A (ampere)
Electromagnetic oscillations

Total oscillation energy

W=CU22+LI22W = \frac{CU^2}{2} + \frac{LI^2}{2}
Symbols
  • WWtotal energy of the oscillatory circuit, J (joule)
  • CCcapacitance of the capacitor, F (farad)
  • UUvoltage across the capacitor, V (volt)
  • LLinductance of the coil, H (henry)
  • IIcurrent in the coil, A (ampere)
Electromagnetic oscillations

RMS current

Irms=Im2I_{\text{rms}} = \frac{I_m}{\sqrt{2}}
Symbols
  • IrmsI_{\text{rms}}root-mean-square (effective) current, A (ampere)
  • ImI_mpeak (amplitude) alternating current, A (ampere)
Electromagnetic oscillations

RMS voltage

Urms=Um2U_{\text{rms}} = \frac{U_m}{\sqrt{2}}
Symbols
  • UrmsU_{\text{rms}}root-mean-square (effective) voltage, V (volt)
  • UmU_mpeak (amplitude) alternating voltage, V (volt)
Electromagnetic oscillations

Inductive reactance

XL=ωL=2πfLX_L = \omega L = 2\pi f L
Symbols
  • XLX_Linductive reactance, Ω (ohm)
  • ω\omegaangular frequency, rad/s
  • LLinductance, H (henry)
  • fffrequency of the alternating current, Hz (hertz)
Electromagnetic oscillations

Capacitive reactance

XC=1ωC=12πfCX_C = \frac{1}{\omega C} = \frac{1}{2\pi f C}
Symbols
  • XCX_Ccapacitive reactance, Ω (ohm)
  • ω\omegaangular frequency, rad/s
  • CCcapacitance, F (farad)
  • fffrequency of the alternating current, Hz (hertz)
Electromagnetic oscillations

Total AC impedance

Z=R2+(XLXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}
Symbols
  • ZZtotal impedance of the AC circuit, Ω (ohm)
  • RRresistance (ohmic), Ω (ohm)
  • XLX_Linductive reactance, Ω (ohm)
  • XCX_Ccapacitive reactance, Ω (ohm)
Electromagnetic oscillations

Ohm's law for an AC circuit

I=UZI = \frac{U}{Z}
Symbols
  • IIeffective (RMS) current, A (ampere)
  • UUeffective (RMS) voltage, V (volt)
  • ZZtotal impedance of the circuit, Ω (ohm)