Magnetic Force on a Current-Carrying Wire — Question 6

Section 28-7 · Physics pages 4602–4603

Question 6 A field gradient shifts the effective point of application of the force on a straight wire A straight wire from x=0 to L carries current I along +x. The external field is⃗ B(x) = B0(1 + αx/L)ˆz, with B0 positive and alpha greater than -1. I 0 L increasing downward force density Schematic; labels, not drawing lengths, specify the data. (a) Find the total force and torque about the origin. (b) Find the x coordinate at which a single equivalent transverse force would act. Evaluate that coordinate for alpha=2.
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Question 6 - Solution A field gradient shifts the effective point of application of the force on a straight wire I 0 L increasing downward force density (a) Method and calculation dFy = −IB0(1 + αx/L) dx ⇒Fy = −IB0L(1 + α/2). τz = ∫L 0 x dFy = −IB0L2(1/2 + α/3). (b) Interpretation and further calculation xF = τz/Fy = L1/2 + α/3 1 + α/2 . α = 2 : xF = 7 12L > L/2. Physical check The resultant acts closer to the end where the magnetic field is stronger.

Question 6

A field gradient shifts the effective point of application of the force on a straight wire

A straight wire from x=0 to L carries current I along +x. The external field is B→(x)=B0(1+αx/L)ẑ\vec B(x)=B_0(1+\alpha x/L)\hat z, with B0 positive and alpha greater than -1.

Diagram shown in the original SVG worksheet.

  1. Find the total force and torque about the origin.

  2. Find the x coordinate at which a single equivalent transverse force would act. Evaluate that coordinate for alpha=2.

Question 6 - Solution

A field gradient shifts the effective point of application of the force on a straight wire

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dFy=−IB0(1+αx/L)dx⇒Fy=−IB0L(1+α/2).dF_y=-IB_0(1+\alpha x/L)\,dx\Rightarrow F_y=-IB_0L(1+\alpha/2).τz=∫0LxdFy=−IB0L2(1/2+α/3).\tau_z=\int_0^Lx\,dF_y=-IB_0L^2(1/2+\alpha/3).

(b) Interpretation and further calculation

xF=τz/Fy=L1/2+α/31+α/2.x_F=\tau_z/F_y=L\frac{1/2+\alpha/3}{1+\alpha/2}.α=2:xF=712L>L/2.\alpha=2:\quad x_F=\frac7{12}L>L/2.

Physical check

The resultant acts closer to the end where the magnetic field is stronger.