1. force
A magnetic charge m placed in a magnetic field B experiences a force.
F = mB .. (1)
2. Magnetic field due to magnetic charge
B = (µ0/4 π)(m/r²)
3. Pole strength due to current
m = IA ...(3)
Where
m = pole strength
I = surface current per unit length of the magnet
A = cross sectional of the magnet
4. Magnetic moment of a bar magnet
M = 2ml … (4)
Where
M = Magnetic moment of a bar magnet
M = pole strength
2l = magnetic length of the bar magnet
5. Potential energy at an angle θ
U(θ) = -MB cos θ = -M.B …(5)
6. Magnetic field due to a bar magnet
End on position. A position on the magnetic axis of a bar magnet is called an end on position
B = (µ0/4 π)[(2Md)/(d² – l²)²] …(6)
If d is very large compared to l, then
B = (µ0/4 π)(2M/d³) … (7)
8. Broad-on Position
B = (µ0/4 π)[m 2l/(d² + l²)3/2 ] …(8)
= (µ0/4 π)[M/(d² + l²)3/2 ]
If d is very large compared to l,
B = (µ0/4 π)[M/(d³)
10. Magnetic scalar potential
V(r2) – V(r1) = -r1∫r2 B.dr … (10)
11. The component of the magnetic field in any direction is given by
Bl = -dV/dl ... (11)
12.For a pole of pole strength m, the field at a distance r is
B = (µ0/4 π)[m/r²)
So the potential at a distance r is
V( r )= - ∞∫r (µ0/4 π)[m/r²)dr
= (µ0/4 π)[m/r) ... (12)
13. Magnetic scalar potential due to a magnetic dipole
Magnetic scalar potential at a point P which is at a distance r from the mid point of the magnetic dipole, and the angle between the dipole axis and the line joining the mid point of the dipole to the point P is θ
V = (µ0/4 π)[Mcos θ /r²)
Where
M = 2ml =magnetic moment of the dipole
14. Magnetic field due to dipole
Magnetic field at P =
(µ0/4 π)[M /r²)√(1 +3 cos² θ)] .. (14)
17. current in galvanometer
i = K tan θ .. (17)
where K = 2rBH/µ0 for the given galvanometer at a given place.
18. Current in moving coil galvanometer
i = (k/nAB) θ … (18)
the constant (k/nAB) is called the galvanometer constant and may be found by passing a known current, measuring the deflection θ and putting these values in equation (18).
19 Shunt
Shunt is a small resistance.
Current in galvanometer
ig = [Rs/(Rs+g)]*i
i = main current
ig = current that goes through galvanometer
20. tangent law of perpendicular fields
B = BHtan θ .. (20)
21. Deflection magnetometer
Tan A position
M/ BH = (4 π/µ0)[(d² – l²)²/2d] tan θ
22. Deflection magnetometer Tan B position
M/ BH = (4 π/µ0)[(d² – l²)3/2] tan θ.. (22)
23. Oscillation Magnetometer
Time period T = 2 π/ ω = 2 π√ (I/M BH) .. (23)
From equation (23)
M BH) = 4 π²I/T² … (24)
25. Gauss’s law for magnetism: the flux of the magnetic field through any closed surface is zero
integral over the closed surface ∫B.ds = 0 .. (25)
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