I\'m looking for explanations of how you arrived at this particular answer and n
ID: 1499121 • Letter: I
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I'm looking for explanations of how you arrived at this particular answer and not simply the answer please readable handwriting or not use handwriting.
In this question, you will calculate the force between two identical magnetic dipoles. Assume that the magnetic dipole moment of both of the dipoles are 1-112 (a) We had shown that the torque that one dipole feels due to a external magnetic field is given by T = × B. Show that the corresponding potential energy is given by U =-i. (b) Even though the previous result is derived for a rotations in a uniform magnetic field, it is true in general, i.e. also for a nonuni form magnetic field. Assuming that the magnetic moment is kept fixed at -: What is the force acting on the magnetic dipole? Hint: Review how the force acting on a particle is related to its potential energy)Explanation / Answer
Part a)
The potential energy is determined by the work done by the Bampo field to align the dipole, the expression of the work is
dW = d
we substitute the expression of torque = x B = b Sin
dW = B sin d
W = if B sin d
The work is the variation of the energy system
Uf – Ui = B if sin d = B (-)( Cos f – Cos i)
Uf – Ui = B ( Cos i – Cos f)
We must choose the condition for initial energy
Ui= 0 cuando i = 90
with this and making Uf =U
U = - B Cos
remember that the definition of scalar product a.b = a b Cos
U = - . B
Part b)
Let's use the suggestion given,
F = - dU/dz
U = - ( ^k . B ^k)
^ where k is a unitary vector.
Producer climb the only part remaining is the one in the direction of the axis z
^k. ^k = 1 ^k. Î = ^k .^j =0
F = - d ( B ) /dk
F = - B d/dz - d B/dz
and indicate that B = uniform dB/dz = 0
F = - B d/dz
Part c)
For this part we will use the Biot - Savart
dB = o/4 I (ds x ^r )/ r2
Approximate the dipole as a loop, a it is the radius of the coil or wire separation of the dipole
B = o1 I/( 2 (z2 + a 2) 3/2
z = d ^k
B = o I/(2 (d2 + a 2) 3/2
if d >>a
B = o I/2d3
Part d)
The magnetic field created by the dipole 1 in this point is
B1 = o I/(2 (d2 + a 2) 3/2
The force on the dipole 2 is given by the expression calculated in part b
F = - B1 d/dz
= I a b ^k
a b It is the area of the dipole
F = - o I/(2 (d2 + a 2) 3/2 I d (ab ^k)/dz
F = - o I/(2 (d2 + a 2) 3/2 I ab
They are many questions and I run out of time so I leave it up to this part
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