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I\'m looking for explanations of how you arrived at this particular answer and n

ID: 1499121 • Letter: I

Question

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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