To find the magnetic moment of the flat spiral coil, we consider an elemental concentric circular strip of radius r and infinitesimal width dr.
The total number of turns N is uniformly distributed over the radial distance from r1 to r2. Therefore, the number of turns per unit radial length, n, is given by:
n=r2−r1N
The number of turns in the elemental ring of thickness dr is:
dN=ndr=r2−r1Ndr
The magnetic moment dM contributed by these dN turns, each carrying a current I and enclosing an area A=πr2, is:
dM=dN⋅I⋅(πr2)=r2−r1πNIr2dr
To find the total magnetic moment M of the coil, we integrate dM from r=r1 to r=r2:
M=∫r1r2r2−r1πNIr2dr
M=r2−r1πNI[3r3]r1r2=3(r2−r1)πNI(r23−r13)
Using the algebraic identity r23−r13=(r2−r1)(r22+r1r2+r12), the expression simplifies to:
M=31πNI(r22+r1r2+r12)
Given parameters:
- N=200
- I=20 mA=20×10−3 A
- r1=3 cm=3×10−2 m
- r2=6 cm=6×10−2 m
Calculating the term (r22+r1r2+r12):
r12=(3×10−2)2=9×10−4 m2
r22=(6×10−2)2=36×10−4 m2
r1r2=(3×10−2)(6×10−2)=18×10−4 m2
r22+r1r2+r12=(36+18+9)×10−4=63×10−4 m2
Now, substituting these values into the formula for M:
M=31π(200)(20×10−3)(63×10−4)
M=31π⋅(4)⋅(63×10−4)
M=84π×10−4 A⋅m2
Taking π≈3.1416:
M=84×3.1416×10−4≈263.89×10−4 A⋅m2=2.64×10−2 A⋅m2
Comparing this with M=α×10−2 A⋅m2, we get:
α=2.64
Thus, the correct option is B.