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Suppose that the magnetic field in some region has the form

B→=kzxÁåœ

(where kis a constant). Find the force on a square loop (side a),lying in the yz

plane and centered at the origin, if it carries a current I,flowing counterclockwise,

when you look down the xaxis.

Short Answer

Expert verified

The force on a square loop of side a,lying in the yzplane and centered at the origin, carrying a current I,flowing counterclockwise in the presence of a magnetic fieldB→=kzxÁåœ is Ia2kzÁåœ.

Step by step solution

01

Given data

There is a magnetic field of the formB→=kzxÁåœ .

There is a square loop of side alying in the yzplane, centered at the origin and carries a current I,flowing counterclockwise.

02

Force on a current carrying wire in a magnetic field

The force on a wire carrying current I, length Iin a magnetic fieldBis

F→=||→×B→......(1)

03

Force on the current carrying loop

The force on y=a/2and y=-a/2wires are exactly equal and opposite and so they cancel out.

From equation (1), force on the z=a/2 wire

F→1=IaB\z-a/2zÁåœ=Iaka2zÁåœ=Ia2k2zÁåœ

From equation (1), force on the z=-a/2 wire

F→2=IaB\z-a/2-zÁåœ=Iak-a2-zÁåœ=Ia2k2zÁåœ

Thus, the net force on the wire is Ia2kzÁåœ .

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Most popular questions from this chapter

Two long coaxial solenoids each carry current I , but in opposite directions, as shown in Fig. 5.42. The inner solenoid (radius a) has turns per unit length, and the outer one (radius b) has .n2Find B in each of the three regions: (i) inside the inner solenoid, (ii) between them, and (iii) outside both.

Consider a planeloop of wire that carries a steady current I;we

want to calculate the magnetic field at a point in the plane. We might as well take

that point to be the origin (it could be inside or outside the loop). The shape of the

wire is given, in polar coordinates, by a specified function r(θ)(Fig. 5.62).

(a) Show that the magnitude of the field is

role="math" localid="1658927560350" B=μ0I4π∮(5.92)

(b) Test this formula by calculating the field at the center of a circular loop.

(c) The "lituus spiral" is defined by a

r(θ)=aθ â¶Ä‰â¶Ä‰â¶Ä‰â¶Ä‰0<θ≤2Ï€

(for some constant a).Sketch this figure, and complete the loop with a straight

segment along the xaxis. What is the magnetic field at the origin?

(d) For a conic section with focus at the origin,

r(θ)=p1+±ð³¦´Ç²õθ

where pisthe semi-latus rectum (the y intercept) and eis the eccentricity (e= 0

for a circle, 0 < e< 1 for an ellipse, e= 1 for a parabola). Show that the field is

B=μ0I2pregardless of the eccentricity.

Question: Use Eq. 5.41 to obtain the magnetic field on the axis of the rotating disk in Prob. 5.37(a). Show that the dipole field (Eq. 5.88), with the dipole moment you found in Prob. 5.37, is a good approximation if z>> R.

For a configuration of charges and currents confined within a volume

V,show that

∫V⇶Ĵ³»åÏ„=dp⇶Ädt

where p⇶Äis the total dipole moment.

Question: Find the magnetic field at point Pfor each of the steady current configurations shown in Fig. 5.23.

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