MAGNETISM
1. Like poles repel each other and
unlike poles attract each other.
2. Coulomb’s law of magnetic force –
It states that the force of
attraction or repulsion between two magnetic poles is directly proportional to
the product of their pole strength and inversely proportional to the square of
the distance between them.
F = µ0 /
4π (M1 M2 / r2)
Here µ0 / 4π = 10-7 NA-2
or Wb A-1 m-1
µ0 = Permeability of free
space = 4π x 10-7 Wb A-1
m-1
3. M = m x 2L
Here M = magnetic moment
m = Pole strength
2l = Magnetic length
4. S.I. unit of magnetic moment is
Ampere. Metre2 or Joule / tesla.
5. Magnetic lines of force start from
north pole and end on south pole.
6. Two magnetic lines of force never
cross each other.
7. The magnetic lines of force have a
tendency to contract lengthwise. This explains two unlike poles attract each
other.
8. The lines of force have a tendency
to expand sidewise. This explains repulsion between two like poles.
9. B axial = µ0 / 4π (2M / r3)
10. B equatorial = µ0 / 4π (M / r3)
11. τ = MB sin ᴓ = M x B
Here τ = torque
M = Magnetic moment
B = Magnetic induction
12. U = MB (cos ᴓ1 – cos ᴓ2)
13. M = I A
Here M = magnetic moment
A = area
14. µB = eh / 4πm = 9.27 x 10-24 Am2
15. The angle between the geographical
meridian and the magnetic meridian at a plane is called the magnetic
declination at that place.
16.
The angle made by earth’s total magnetic field B with the horizontal
direction in the magnetic meridian is called angle of dip at any place.
17. Angle of dip is zero at the
magnetic equator.
18. Angle of dip is 900 at
the magnetic poles.
19. It is the component of earth’s
total magnetic field B in the
horizontal direction in the magnetic meridian.
20. Neutral point is the point where
the resultant magnetic field intensity is zero.
21. B = F / m
Here B = magnetic induction
F = force
m = pole strength
22. I = M / V
Here I = intensity of magnetisation
M = magnetic moment
V = volume
23. I = m / a
Here m = pole strength
a = area
24. µ= B / H
Here µ = magnetic permeability
B = magnetic induction
H = Magnetic intensity
25. µr = µ / µ0
Here µr = Relative
permeability
µ = Permeability of medium
µ0 = Permeability of free
space
26. k = I / H
Here k = magnetic susceptibility
I = Intensity of magnetisation
H = Magnetic intensity
27. Magnetic susceptibility is
unitless and dimensionless.
28. µ = µ0 (1 + k)
29. µ0 = 1 + k
Here µ0 = permeability of
free space
µ = Permeability of medium
k = magnetic susceptibility
30. Diamagnetic substances are those
which develops feeble magnetisation in the opposite direction of the magnetising
field. Such substances are feebly repeled by the magnets and tend to move from
stronger to weaker parts of a magnetic field.
Ex – Bismuth, copper, lead, Zinc, Tin
etc.
31. Susceptibility of diamagnetic
material is small and negative.
32. The relative permeability is less
than one for a diamagnetic material.
33. Paramagnetic substances are those
which develops feeble magnetisation in the direction of magnetising field. Such
substances are feebly attracted by the magnet and tend to move weaker parts to
stronger part of a magnetic field.
Ex – Iron, oxygen, Cobalt, Nickel etc.
34. Susceptibility of paramagnetic
material is small but positive value.
35. The relative permeability for a
paramagnetic material has a value slightly greater than one.
36. Curie’s Law –
The magnetic susceptibility of a paramagnetic
material varies inversely as the absolute temperature.
k α 1 / T
Or, k = C / T
Here C = Curie constant
37. Ferromagnetic substances are those
which develops stronger magnetisation in the direction of magnetising field.
They are strongly attracted by the magnets and tend to move from weaker part to
stronger part of a magnetic field.
Ex- Iron, Cobalt, Nickel and alloys
like alnico
38. Susceptibility of ferromagnetic
material has a large positive value.
39. The relative permeability of a
ferromagnetic material has a large positive value.
40. The susceptibility of a
ferromagnetic material decreases with temperature in accordance to Curie Weiss
law.
41. At certain temperature, called curie
point, the susceptibility suddenly falls and the ferromagnetic substance
becomes paramagnetic.
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