Circuits and electricity

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Last updated 11:27 AM on 5/17/26
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29 Terms

1
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What is Kirchhoff’s voltage law (KVL)?

CEdl=0\oint_{C}\underline{E}\cdot\underline{dl}=0

Where E is the electrostatic field and dl is a vector element of the path/loop.

The sum of all electromotive forces and potential differences around any closed loop of a circuit is zero.

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Equation for vector current density

j=nqvd\underline{j}=nq\underline{v}_{d}

where n is the concentration of moving charged particles, q is charge per particle and vd is drift velocity.

(Current per cross-sectional area - scalar)

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Current density

dI=jdSdI=\underline{j}\cdot\underline{dS}

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What is Kirchhoff’s current law (KCL)?

ρct+j=0\frac{\partial\rho_{c}}{\partial t}+\underline{\nabla}\cdot\underline{j}=0

Where j is the current density vector.

The sum of all currents entering a junction equals the sum of all currents leaving a junction.

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<p>Draw receptor convention (circuits) </p>

Draw receptor convention (circuits)

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<p>Draw generator convention (circuits)</p>

Draw generator convention (circuits)

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What is the electromotive force?

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What is Faraday’s Law?

CEdl=dΦBdt\oint_{C}\underline{E}\cdot d\underline{l}=-\frac{d\Phi_{B}}{dt}

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What is Lenz’s law?

The direction of magnetic induction effect is in the direction opposing the cause of that effect.

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Maxwell-flux equation

B=0\underline{\nabla}\cdot\underline{B}=0

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Maxwell-Gauss equation

E=ρcϵ0\underline{\nabla}\cdot\underline{E}=\frac{\rho_{c}}{\epsilon_0}

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Maxwell-Faraday equation

×E=Bt\underline{\nabla}\times\underline{E}=-\frac{\partial{\underline{B}}}{\partial t}

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Maxwell-Ampere equation

×B=μ0j+μ0ϵ0Et\underline{\nabla}\times\underline{B}=\mu_0\underline{j}+\mu_0\epsilon_0\frac{\partial\underline{E}}{\partial t}

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Laplace force (derived from magnetic of Lorenz)

FL=wireIdl×B\underline{F_{L}}=\int_{wire}I\underline{dl}\times\underline{B}

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Resistance equation (receptor convention)

VR=RIV_{R}=RI

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Capacitance equation (receptor convention)

VC=QCV_{C}=\frac{Q}{C}

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Equation for capacitor in parallel and in series (receptor convention)

  • In parallel: Ceq=C1+C2C_{eq}=C_1+C_2

  • In series: 1Ceq=1C1+1C2\frac{1}{C_{eq}}=\frac{1}{C_1}+\frac{1}{C_2} or Ceq=C1C2C1+C2C_{eq}=\frac{C_1C_2}{C_1+C_2}

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Voltage of an inductor equation (receptor convention)

VL=LdIdtV_{L}=L\frac{dI}{dt} where L is inductance

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Power consumed by an electrical component (receptor convention)

P=VIP=VI

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What is the electric field inside a conductor?

E=0\underline{E}=0

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Current and current density equation

I=SjdSI=\iint_{S}\underline{j}\cdot d\underline{S}

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Definition of self-inductance

ΦB=LI\Phi_{B}=LI where L is the self-inductance

The ability of a circuit to create magnetic flux through itself

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Definition of mutual inductance

ΦB=MI\Phi_{B}=MI where M is the mutual inductance (between two circuits)

The ability of a circuit to create magnetic flux through another circuit is mutual inductance.

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Known result for self-inductance of a solenoid

L=μ0n2SlL=\mu_0n^2Sl

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How do we find mutual inductance (M)?

  • Calculate magnetic field through one circuit

  • Calculate the flux through the second circuit

  • Use the definition of mutual inductance to find M

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Mutual inductance of two solenoids (known result)

M=μ0n1n2SlM=\mu_0n_1n_2Sl

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What is the surface enclosed by a solenoid?

SnS\cdot n_{} where n is the number of loops. And S is approximated to the area of a circle.

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Magnetic curl definition

  • A measure of whether the electromagnetic field rotates around a point and how much

  • essential for determining how electric currents and changing electric fields generate rotating magnetic fields

  • curl(A)=×A\underline{curl}\left(\underline{A}\right)=\underline{\nabla}\times\underline{A}

  • curl >0 is anti-clockwise, < 0 is clockwise and =0 is no curl

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Power supplied by a voltage source

P=IcellVterminalP_{}=I_{cell}\cdot V_{ter\min al}