ch 5 - Electrostatics and Magnetism Flashcards

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1
Q

electrical potential of dipole

A

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

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2
Q

dipole moment (p)

A

SI units are C x m: p = qd

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3
Q

perpendicular bisector of the dipole

A

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.

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4
Q

electric dipole

A

result of two equal and opposite charges being separated a small distance (d) from each other; can be transient or permanent

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5
Q

magnitude of the electric field on the perpendicular bisector of the dipole

A

E = 1/(4pi x epsilonsub0) x p/r^3

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6
Q

electrostatic constant (k)

A

8.99 x 10^9 (N x m^2)/C^2

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7
Q

net torque on dipole

A

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

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8
Q

equipotential lines

A

lines on which the potential at every point is the same; potential difference bt any two points on an equipotential line is zero

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9
Q

SI unit for magnetic field strength

A

tesla (T) 1 T = 1 (N x s)/(m x C); or when smaller measured in gauss. 10^4 gauss = 1 T

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10
Q

diamagnetic materials

A

made of atoms with no unpaired electrons and that have no net magnetic field; can be called weakly antimagnetic

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11
Q

Paramagnetic materials

A

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)

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12
Q

Ferromagnetic materials

A

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)

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13
Q

for infinitely long and straight current-carrying wire, equation for magnitude of magnetic field

A

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)

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14
Q

right hand rule for straight wire magnetic fields

A

point thumb in direction of current and wrap fingers around current-carrying wire. Fingers mimic circular field lines curling around wire

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15
Q

magnitude of magnetic field at center of circular loop of current carrying wire

A

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

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16
Q

Lorentz force

A

sum of the electrostatic and magnetic forces acting on charges in magnetic field

17
Q

magnetic force

A

F sub B = qvB sin theta; q = the charge; v = magnitude of velocity, B = magnitude of magnetic field; theta = smallest angle between the velocity vector v and the magnetic field vector B; unit is N

18
Q

right-hand rule of magnetic forces

A

to determine direction of the magnetic force on moving charge; position right thumb in direction of the velocity vector; put fingers in direction of magnetic field lines; palm points in the direction of the force vector for a positive charge, while back points in direction of force vector a negative charge

19
Q

For a straight wire, magnitude of force created by external magnetic field

A

F sub B = ILB sin theta; I (i)= current; L = length of wire in the field; B = magnitude of magnetic field; theta = angle between L and B

20
Q

fancy uC = how many coulomb?

A

1 x 10^-6 C