(adsbygoogle = window.adsbygoogle || []).push({}); 1. The problem statement, all variables and given/known data

An infinitely long conductor carrying a current I in the positive z-direction lies on the z-axis.

A conducting triangle of wires lies in the yz-plane, which moves with a speed v in the positive y-direction.

The following figure shows the situation on time t = 0:

a) Calculate the induced voltages [itex]V_Q-V_P[/itex] and [itex]V_P-V_R[/itex] on t=0.

I got this, no problem.

b) Calculate the induced voltage [itex]V_Q-V_R[/itex] on time t=0.

Hint: First calculate the induced voltage on a little segment dl and notice that [itex]dl = \sqrt{dz^2 + dy^2} = \sqrt{2} dy[/itex].

2. Relevant equations

[tex]\epsilon = \int (\vec{v} \times \vec{B}) \cdot \vec{dl}[/tex]

[tex]B = \frac{ \mu_0 I}{2 \pi y}[/tex] (at a distance y, in the negative x-direction (into the screen)

3. The attempt at a solution

I got the answer right apart from a minus sign...

I first checked the direction of the crossproduct v*B and got it to be in the positive z-direction.

Dot product with dl is then

[tex]( \vec{v} \times \vec{B} ) \cdot \vec{dl} = vB \, dl \cos \theta = vB \, dl cos(135) = -\frac{1}{2} \sqrt{2} vB \, dl[/tex]

Because dl is pointing from Q to R, the angle is 90 + 45 = 135, right?

Then:

[tex]\epsilon = -\frac{1}{2} \sqrt{2} \int_a^{2a} B v dl = -\frac{1}{2} \sqrt{2} \int_a^{2a} \frac{\mu_0 I}{2 \pi y} v \sqrt{2} dy = - \frac{\mu_0 I v}{2 \pi} \int_a^{2a} \frac{dy}{y} = - \frac{\mu_0 I v}{2 \pi} \ln{2}[/tex]

As I said, the answer is correct apart from the minus sign... Where did I go wrong?

The answer I am given is this exactly:

[tex]d \epsilon = v \frac{\mu_0 I}{2 \pi y} \frac{1}{2}\sqrt{2} dl[/tex]

[tex]V_Q-V_R = \int_a^{2a}\frac{\mu_0 I v}{2 \pi y} dy = \frac{ \mu_0 I v}{2 \pi } \ln{2}[/tex]

That's all, nothing more... I can't quite figure out what they are doing, which equations they are using...

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# Homework Help: Missing minus sign - Motional EMF

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