ch 5 - Electrostatics and Magnetism Flashcards
electrical potential of dipole
V=(kq)/rsub1 - (kq)/rsub2 = (kq(rsub2 - rsub1))/rsub1rsub2
At greater distance: V = ((kqd)/rsquared) x costheta;
d = distance between +q and -q (source charges); rsub1 = distance between the chosen point in space and +q; rsub2 = distance between said point and -q
dipole moment (p)
SI units are C x m: p = qd
perpendicular bisector of the dipole
plane that lies halfway between +q and -q. Because the angle between this plane and the dipole axis is 90 degrees (and cos 90 = 0) the electrical potential at any point along this plane is 0.
electric dipole
result of two equal and opposite charges being separated a small distance (d) from each other; can be transient or permanent
magnitude of the electric field on the perpendicular bisector of the dipole
E = 1/(4pi x epsilonsub0) x p/r^3
electrostatic constant (k)
8.99 x 10^9 (N x m^2)/C^2
net torque on dipole
T = pE sintheta where p = magnitude of dipole moment (p = qd), E = magnitude of uniform external electric field, and theta = angle the dipole moment makes with the electric field; this will cause dipole to reorient itself so that its dipole moment (p) aligns with the electric field E
equipotential lines
lines on which the potential at every point is the same; potential difference bt any two points on an equipotential line is zero
SI unit for magnetic field strength
tesla (T) 1 T = 1 (N x s)/(m x C); or when smaller measured in gauss. 10^4 gauss = 1 T
diamagnetic materials
made of atoms with no unpaired electrons and that have no net magnetic field; can be called weakly antimagnetic
Paramagnetic materials
have unpaired electrons; weakly magnetized in the presence of an external magnetic field, aligning the magnetic dipoles of the material with the external field (ex aluminum, copper and gold)
Ferromagnetic materials
have unpaired electrons and permanent atomic magnetic dipoles that are normally oriented randomly so that the material has no net magnetic dipole. will become strongly magnetized when exposed to a magnetic field or under certain temps (iron, nickel and cobalt)
for infinitely long and straight current-carrying wire, equation for magnitude of magnetic field
B = (fancy u sub 0 x I)/(2pi r) I (i) = current in the wire; r = perpendicular distance of the current from the wire; B = magnetic field; fancy u sub 0 = permeability of free space (4pi x 10^-7 (T x m)/A)
right hand rule for straight wire magnetic fields
point thumb in direction of current and wrap fingers around current-carrying wire. Fingers mimic circular field lines curling around wire
magnitude of magnetic field at center of circular loop of current carrying wire
B = (fancy u sub 0 x I)/2r r = radius of loop; fancy u sub 0 = permeability of free space (4pi x 10^-7 (T x m)/A); B = magnetic field; I = current in wire