Electrostatics and Magnetism Flashcards
fundamental unit of charge (e); charge of protons and electrons (but positive and negative)
e = 1.60 x 10^-19 C (coulomb)
quantifies magnitude of electrostatic force between two charges
Coulomb’s law
Coulomb’s law
F(e) = (k q1 q2) / r^2
where:
k = Coulomb’s constant (8.99 x 10^9 N*m^2/C^2)
q1 and q2 = magnitude of charges
r = distance between charges
Coulomb’s constant (k)
k = 8.99 x 10^9 N*m^2/C^2
generated by every charge, and exert force on other charges
electric field
electric field (E)
E = F(e) / q = kQ / r^2
where:
q = test charge
Q = source charge
F(e) = magnitude of force felt by point charge
k = Coulomb’s constant (8.99 x 10^9 N*m^2/C^2)
r = distance between charges
used to represent electric field vectors for a charge; point away from a positive charge and point toward a negative charge the denser the line, the stronger the field
field lines
the work necessary to move a test charge from infinity to a point in space in an electric field surrounding a source charge; if like charges, then U will be positive; if unlike charges, then U will be negative
electric potential energy (U)
electric potential energy (U)
U = kQq / r
where: k = Coulomb's constant (8.99 x 10^9 N*m^2/C^2) Q = source charge q = test charge r = distance between charges
ratio of electric potential energy per unit charge, measured in volts (V)
electric potential (V)
electric potential (V)
V = U / q = kQ / r
where:
k = Coulomb’s constant (8.99 x 10^9 N*m^2/C^2)
Q = source charge
r = distance between charges
essential electrostatic equations and derivations:
where:
k = Coulomb’s constant (8.99 x 10^9 N*m^2/C^2)
the change in electric potential that accompanies the movement of a test charge from one position to another
potential difference (voltage)
potential difference (voltage)
∆V = V(b) - V(a) = W(ab) / q
where:
W(ab) = work needed to move a test charge q through an electric field from point a to b
designate the set of points around a source charge or multiple source charges that have the same electric potential; always perpendicular to electric field lines
equipotential line