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30 Cards in this Set
- Front
- Back
C=Q/V |
capacitance = charge over voltage |
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C=ε₀A/d |
parallel plate capacitor: capacitance = epsilon naught * Area / distance between the plates |
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E=E(free)/κ |
Electric field in dielectric = electric field in free space over kappa |
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C=κC₀ |
the capacitance of a capacitor with a dielectric = kappa * the capacitance without dielectric |
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U=1/2Q∆V=1/2Q²/C=1/2C(∆V)² |
The potential energy of a capacitor = 1/2 * charge * potential difference = 1/2 * charge squared / capacitance = 1/2 * capacitance * potential difference squared |
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I=∆Q/∆t=dq/dt |
current = change in charge over change in time |
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R=ρL/A |
resistance = resistivity * length over area |
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∆R = αR₀∆T |
change in resistance due to temperature change = temperature coefficient of resistivity (alpha) * original resistance * change in temperature |
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j=I/A |
current density = current over area |
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R(eq)=R₁+R₂ |
In series, equivalent resistance is the sum of the resistances |
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1/R(eq) = 1/R₁ + 1/R₂ |
In parallel, inverse equivalent resistance is the sum of the inverse resistances |
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∆V=IR |
Ohm's Law: potential difference = current * resistance |
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the sum of emfs and voltage drops of a closed loop is zero |
Kirchoff's loop rule |
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the total current going into a junction equals the total current going out of the junction |
Kirchoff's current rule |
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P = εI |
The power supplied by an emf source is emf * current |
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P = ∆VI = I²R = (∆V)²/R |
Power dissapaited by a resistor is potential difference times current is current squared times resistance is potential difference squared over resistance |
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τ = RC |
characteristic time for RC circuit = resistance * capacitance |
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Q(t) = Cε(1-e^(-t/τ)) |
charge on charging capacitor as function of time is capacitance times emf * (1 - e to the negative time over characteristic time) |
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Q(t) = Cεe^(-t/τ) |
charge on discharging capacitor as function of time is capacitance times emf times e to the negative time over characteristic time |
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F=μ₀/2π*qvI/r |
Magnetic force on particle moving with speed v due to current in wire is mu naught over two pi times the charge * velocity * current over distance between particle and wire |
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F = qv×B |
magnetic force on charged moving particle is charge times velocity cross magnetic field |
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F = qE + qv×B |
Lorentz force: force on charged particle moving with velocity v is charge times electric field plus charge times velocity cross magnetic field |
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dB = μ₀/4π*Ids×r/r³ = μ₀/4π*Ids*sinθ/r² |
Biot-Savart: dmagnetic field is mu naught over four pi times current times ds cross r over r cubed |
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∫B·ds = μ₀I |
Ampere's Law: surface integral of magnetic field dot ds = mu naught times current enclosed |
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r = mv/qB |
radius of circular orbit in magnetic field |
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dF=IdL×B |
dforce = current times dlength cross magnetic field |
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F/L = μ₀/2π*I₁I₂/r |
force per unit length on a wire due to another wire = mu naught over 2pi times current in one wire times current in other wire divided by distance between wires |
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μ=IA |
magnetic moment of current loop = current times area |
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τ = μ×B |
torque on current loop in magnetic field = magnetic moment cross magnetic field |
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U = -μ·B |
potential energy of current loop in magnetic field is negative magnetic moment dot magnetic field |