• Shuffle
    Toggle On
    Toggle Off
  • Alphabetize
    Toggle On
    Toggle Off
  • Front First
    Toggle On
    Toggle Off
  • Both Sides
    Toggle On
    Toggle Off
  • Read
    Toggle On
    Toggle Off
Reading...
Front

Card Range To Study

through

image

Play button

image

Play button

image

Progress

1/19

Click to flip

Use LEFT and RIGHT arrow keys to navigate between flashcards;

Use UP and DOWN arrow keys to flip the card;

H to show hint;

A reads text to speech;

19 Cards in this Set

  • Front
  • Back

Lambda

Lambda = Q / L

Eta

Eta = Q / A

E field of a dipole

E = K*2p / r^3 -- on axis


E = -K*p / r^3 -- on bisecting plane

E field of a capacitor

Ideal capacitors have no field outside their plates. Inside: Q / Epsilon0*A

Kinematics Equations

xf = xi + vi*t + 1/2*a*t^2


vf = vi + a*t


a = constant


vf^2 = vi^2 + 2*a*(xf-xi)

Electric Flux (simple version)

PHI = E*A*cos(theta)


theta between A's normal vector and E field

Electric Potential Energy

U = q*E*s

Potential of a capacitor from potential and distance s from negative electrode

V = (s / d)*Vc

Capacitance from a dielectric

Cf = K*Ci

Kappa

E0 / En

Resistors and Capacitors in series have the same __________ / ____________

Current / Charge



Resistors and Capacitors in parallel have the same ________________

Potential across them

omega for LC circuits

w = sqrt(1/(L*C))

Imax for LC circuits

Qi * omega

Reference frame transformations for E field and B fields

Eb = Ea + vba x Ba


Bb = Ba - (1/c^2) vba x Ea


Fields measured in their reference frames from a stationary vantage point. v is velocity of B relative to A

Lorentz force equation

F = q(E + v x B)

S, the Poynting vector =

EB/mu0


E^2/cmu0


cEps0E62



E for electromagnetism

E0*(sin(2pi(x/lambda - ft)))

E field to B field conversion

E = c*B