V (from I,R)
IR
P - Power (from I, V)
i∆V
P - Power (from I, R)
I^2R
P - Power (from V, R)
(∆V)^2/R
R_net in series
∑R_i
R_net in parallel
1/∑(1/R_i)
R (based on physical characteristics)
ρℓ/A; ρ is the resistivity, ℓ with length
C; Capacitance (from Q, ∆V)
Q/∆V; Q - charge stored, ∆V from that charge
C; Capacitance for Parallel plate Capacitance (from physical characteristics)
κ(ε_0)A/d; κ - dielectric constant; ε_0 - permittivity of free space, A - Area of plate, d - distance between plates
U_C; Energy stored in a capacitor
0.5C∆V^2, 0.5Q∆V; not Q∆V because ∆V decreases as Q leaves. Q is charge on one side, net is zero
C_net,p (parallel)
∑C_i
C_net,s (series)
1/∑(1/C_i)
Charge of capacitors in series
is the same
Current between series components
is the same
Voltage between series components
is the same
Q of charging RC circuit (with τ)
C∆V(1-e^(-t/τ))
Q of charging RC circuit (without τ)
C∆V(1-e^(-t/(RC)))
I of charging RC circuit (with τ)
∆V/R(e^(-t/τ)
I of charging RC circuit (without τ)
∆V/R(e^(-t/(RC))
Kirchoff Loop Rule for charging RC circuit
V_b - IR - Q/C = 0, V_b - RdQ/dt - Q/C = 0
Kirchoff Loop Rule for discharging RC circuit
Q/C - IR, Q/C + RdQ/dt = 0
V of discharging RC circuit
V_0*e^(-t/(RC))
Q of discharging RC circuit
Q_0e^(-t/(RC)), CVe^(-t/(RC))
I of discharging RC circuit
I_0*e^(-t/(RC)), V_0/R * e^(-t/(RC))