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Amount of charge a capacitor can store depends on
voltage applied and capacitor’s physical characteristics, like size
Capacitance
C = Q/V, C = e0(A/d)
At constant Q or V
increasing distance decreases capacitance
Total capacitance in series
1/Cs = 1/C1 + 1/C2 + 1/C3…
Total capacitance in parallel
Cs = C1 + C2 + C3…
Energy stored in capacitor
Ecap = ½(QV) = ½CV^2 = Q^2/2C
Current
rate at which charge flows, I = ΔQ/Δt (A)
Direction of current
direction positive charge moves
Current equation (w/ drift velocity)
I = nqAvd, where A = cross-sectional area of wire, n = free-charge density of wire material, q = charge of each carrier, vd = drift velocity
Ohm’s law
V = IR
Resistance given cylinder length and area
R = pL/A, where p = resistivity of material, L = length, A = cross-sectional area of wire
Higher temperature
higher resistivity in metals (bc metal atoms vibrate more), lower resistivity in semiconductors/insulators (bc more charge carriers)
Electrical power
rate that energy is supplied by a source or dissipated by a device
Power equations
P = IV = V^2/R = I^2R
Total resistance in series
Rs = R1 + R2 + R3…
Total resistance in parallel
1/Rs = 1/R1 + 1/R2 + 1/R3…
Resistors in series - current
each resistor in a series circuit has the same amount of current flowing through it
Resistors in series - voltage/power
voltage drop/power dissipation across each individual resistor in series is different, combined total adds up to power source input
Resistors in parallel - current
current flowing through each resistor in a parallel circuit is different, depending on the resistance
Resistors in parallel - voltage/power
each resistor in a parallel circuit has the same full voltage of the source applied to it.
EMF
potential difference of a source when no current is flowing
Voltage output of a device - terminal voltage V
V = emf - Ir, where r = internal resistance of a voltage source
Multiple voltage sources in series
internal resistances add, emfs add algebraically
Kirchhoff’s junction rule
the sum of all currents entering a junction must equal the sum of all currents leaving the junction
Kirchhoff’s loop rule
the algebraic sum of changes in potential around any closed circuit path (loop) must be zero
Voltmeter
placed in parallel with voltage source to receive full voltage, must have large resistance to limit its effect on circuit
Ammeter
placed in series to get full current flowing through a branch, must have small resistance to limit its effect on circuit
RC circuit
has both a resistor and capacitor
Time constant RC circuit
τ = RC
Magnetic force exerted by field on moving charge q
F = qvBsinθ, where θ is the angle between the directions of v and B
RHR1 - direction of force on moving charge
thumb toward v, fingers toward B, palm points toward F
Magnetic force can supply centripetal force and cause a charged particle to move in a circular path of radius
r = mv/qB, where v is the component of the velocity perpendicular to B for a charged particle with mass m and charge q
Magnetic force on a current-carrying conductor
F = ILBsinθ, where I = current, L = length of a straight conductor in a uniform magnetic field B, θ = angle between I and B
RHR2
thumb toward I, fingers toward B, palm points toward F
Torque on a current-carrying loop of any shape in a uniform magnetic field
τ = NIABsinθ, where N = number of turns, I = current, A = the area of loop, B = magnetic field strength, and θ = angle between the perpendicular to the loop and the magnetic field
Strength of magnetic field created by current in a long straight wire
B = u0I/2𝜋r, where r = shortest distance to wire
RHR3 - direction of magnetic field created by long straight wire
thumb in direction of current, fingers curl in direction of magnetic field loops created by it
Magnetic field strength at the center of a circular loop
B = u0I/2R, where R = radius of loop
Magnetic field strength inside a solenoid
B = u0nI, where n = number of loops per unit length of the solenoid
Force between 2 parallel currents (I1 and I2) separated by distance r
F/l = u0I1I2/2𝜋r, where l = unit length
Force is ___ if the currents are in the same direction, ___ if they are in opposite directions
attractive, repulsive