Type
of field |
Potential |
Field
strength |
Force
|
Potential
energy |
Gravitational |
V = Ep M Vg
= - GM r |
g =
-dV dr g =
- GM r2 |
F =
mg F =
- GM1m2 r2 |
Ep
= GM1m2 R DEp = GM1m2 1 1 r1 r2 |
Uniform
Electrical |
V = Q C C = e0erA d |
E = V D E = s (charge density) e0 |
F =
qE F = qV d |
Ep
= qV |
Non-uniform
electrical |
V = 1
Q 4pe0 r |
E = F q E = 1
Q 4pe0 r2 |
F = 1
Q1q2 4pe0 r2 |
Ep
= 1 Q1q2 4pe0 r |
KE = ½ mv2
Ep = GM1m2
r
½ mv2
= GM1m2
r
vesc = Ö(2GM/r)
g = GM/r2
vesc = Ö(2gr)
Electric
field
E
= F = V
q
d
Magnetic
field
B
= F
Il
Force
on a moving charge
F
= Bev
Hall
voltage
-F
= Bqv
-F
= qE
-E
= V
d
Bqv
= qE = qV
d
V
= Bvd
The
Hall Voltage
Using Faraday's Law |
Using F=Bev and F=qE |
e = -dF dt -d = vt e = -d(BA) dt e = -Bd(A) dt e = -Bd(length x distance) dt e
= -Bd(lv d Vh = Blv |
-F = Bqv -F = qE -E=V d B Bv = V d VH = Bvd |
-F = mv2
r
-F = Bev
-Energy = eV
-Energy = ½ mv2
½ mv2 = eV
Bev = mv2
r
v = Ber
m
½ mv2 = eV
½ m (Ber/m) 2 = eV
½ m B2e2r2
= eV
m2
e = 2V_
m B2r2
Time period of a satellite
F = GMm/r2
F = mrw2
GMm/r2 = mrw2
GM/r3 = w2
w2 = (2p/T)2
GM/r3 = 4p2
T2
T = Ö
(4p2r3/GM)