ELECTROMAGNETIC MOMENT(M)
This is the magnetic torque acting on the coil when it is parallel to a uniform field whose flux density is one tesla.It is the property of the coil is defined as the couple required to hold the coil at right angles to
field.
Thus, in equation τ=m when B=1I
from
Consider a rectangular coil ABCD placed at an angle to the magnetic field of flux density B
The perpendicular distance between the parallel force is and not b. Then the magnetic force or compile is given
Special cases
(i) When
Plane of the loop is parallel to the direction of magnetic field
Thus, the Torque on a current loop is maximum when the plane of the loop is parallel to the direction of magnetic field is given by
(ii) when 𜃠= 900
Plane of the loop is perpendicular to the direction of magnetic field
Thus , the torque on a current loop is minimum (zero) when the plane of the loop is perpendicular
(iii) When B = 1T
when B = 1T, then the magnetic torque is numerical equal to magnetic moment
From
B = 1T
MAGNETIC TORQUE AT AN ANGLE α BETWEEN THE AXIS OF THE COIL AND NORMAL TO THE PLANE OF THE COIL
We can also express torque in another useful form. If normal to the plane of coil makes an angle α with the direction of the magnetic field
From
τ = BANI cos (90 – α)
τ = ANIBSin α
Since M = IAN
When a current carrying coil is placed in a uniform magnetic field, torque acts on it which tends to rotate the coil so that the plane of the coil is perpendicular to the direction of magnetic field.
WORK DONE BY TORQUE
If the magnetic torque displaces the coil through the small angular displacement
The work done by the torque is given by
The total work done is obtained by integration the above equation within limits
If the magnetic field displaces the coil through small angular displacement the work done by torque is given by
dw = τdα
dw = mbSinαdα
WORKED EXAMPLES
1. A vertical rectangular coil of sides 5cm by 2cm has 10 turns and carries a current of 2A. Calculate the torque on the coil when it is placed in a uniform horizontal magnetic field of 0.1T with its plane.
(a) Parallel to the field
(b) Perpendicular to the field
(c) 600 to the field
Solution
The area of the coil
A= (5 x 10 -2) x (2 x10-2)
A= 10-3 m2
(a) From
A=10-3
I = 2A
N=10
B=0.1T
τ= 0.1 X10-3 X10 X2
τ = 2 X10-3NM
(b)
τ=BANI
τ= 0
(c)
τ = BANICos ðœƒ
τ= 0.1 x10-3 x10x2xCos 600
τ= 10 -3NM
2. 2.Given a uniform magnetic field of 100T in East to West direction and a 44cm long wire with a current carrying capacity of at most 10A. what is the shape and orientation of the loop made of this wire which yields maximum turning effect on the loop?
Solution
A current carrying planar loop will experience maximum together if its area to the direction of the magnetic field for a given perimeter , a circle has the maximum area.
If 44cm wire is bent into a circular
2πr = 44
πr = 22
22r = 22
7
r = 1
7
R = 7cm
Area of loop = πr2
= πx72
= 154cm2
= 154×10-4m2
Magnetic toque τ
τ = BANI
τ = (154 X10-4) X 100 X100
τ = 150 T
3. A circular coil of wire of 50 turns and radius 0.05 carries current of 1A the wire is suspended vertically in a uniform magnetic field of 1.5T. the direction of magnetic field is parallel to the plane of the coil
(a) Calculate the Toque on the coil
(b) Would your answer charged if the circular coil is replaced by a plane coil of some irregular shape that has the same area (all other particulars are unaltered? )
(a) Solution
B = 1.5T
A = πr2 = π (0.05) M2
A = 7.85 X 10-3
N = 50
I = 1A
τ = 1.5 X (7.85 X10-3) X50X1
τ = 0.589NM
(b) Since torque on the loop is independent of its shape provide area (A) remains the same the magnitude of the torque will remain unaltered.
4. A circular coil of 20turns and radius 10 cm is placed in a uniform magnetic field of 0.2T normal to the coil. If current in the coil is 5A find.
(i) Total torque on the coil
(ii) Total force on the coil
(iii) Average force on each electron in the coil due to the magnetic field. The coil is made of copper wire of cross-sectional area 10-5m2 and force of electron density in the wire is 1029m-3
Solution
(i) The toque on the coil is given by
Since
τ = 0
(ii) The net force on a planar current loop in a uniform magnetic field is always zero
(iii) Magnetic force on each electron
F = BeVd
F = Be.
F =
F= 10-24N