Magnetic Field from Current Segments

AI Thread Summary
The discussion revolves around calculating the z-component of the magnetic field at a specific point using the Biot-Savart law. The initial attempts to derive the formula involved confusion over the radius and the cross product, leading to incorrect submissions. Clarifications were made regarding the need to correctly compute the cross product of the current element and the radius vector, emphasizing the importance of including the correct components. The final understanding highlighted that the denominator should include the term raised to the power of 3/2, resulting from the squared magnitude of the radius. The participant ultimately grasped the concept and arrived at the correct formulation with guidance.
theshonen8899
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Homework Statement


Find Bz(0,0,z1), the z component of the magnetic field at the point P located at x=y=0,z=z1 from the current I flowing over a short distance dl = |dl|*j located at the point rc = x1*i.

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Homework Equations



Biot-Savart law:
(μo/4∏)*[I*(dL x r)/(|r|^2)]

The Attempt at a Solution



I concluded that the radius would be √(( x1 )2 + (z1 )2) and submitted:

(μo/4∏)*[I*dL/√(( x1 )2 + (z1 )2)]

which was wrong. Then I remember that the equation called for r^2 not r, so I submitted:

(μo/4∏)*[I*dL/(( x1 )2 + (z1 )2)]

which was also wrong. I thought that the cross product would be even but just in case I tried:

(μo/4∏)*[I*-dL/(( x1 )2 + (z1 )2)]

which was still wrong.

Am I getting the radius wrong? I'm not quite sure what's going on.
 
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Start by writing out the vectors involved. Your radius magnitude squared is okay as ##x_1^2 + z_1^2##, but you'll need the radius vector and dL vector components to perform the cross product. Do the cross product!
 
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So the cross product I want is \vec{dl} x \hat{r} and the homework tells me that \vec{dl} x \vec{r_{x}} = dlx_{1}\hat{k}. Shouldn't \vec{dl} x \vec{r_{x}} be negative since \hat{j} \times \hat{i} = -\hat{k}?

So assuming \vec{dl} x \vec{r_{x}} = dlx_{1}\hat{k}, we know \hat{r} = \frac{\vec{r}}{r}. Then would the answer be (μo/4∏)*[(I*dL)/(√(( x1 )2 + (z1 )2)^3)] since there's now an extra r on the bottom?
 
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theshonen8899 said:
So the cross product I want is \vec{dl} x \hat{r} and the homework tells me that \vec{dl} x \vec{r_{x}} = dlx_{1}\hat{k}. Shouldn't \vec{dl} x \vec{r_{x}} be negative since \hat{j} \times \hat{i} = -\hat{k}?

So assuming \vec{dl} x \vec{r_{x}} = dlx_{1}\hat{k}, we know \hat{r} = \frac{\vec{r}}{r}. Then would the answer be (μo/4∏)*[(I*dL)/(√(( x1 )2 + (z1 )2)^3)] since there's now an extra r on the bottom?

There shouldn't be an "extra" r on the bottom. You've extracted the z-component of the cross product but then ignored it? The z-component of the cross product contains an x1, so why does it disappear when you write the result? And I'm not sure why you've introduced a unit vector in the r direction; they're asking for the z-component only, not the whole vector (and it wouldn't be in the same direction as the r vector anyways).

So the z-component of the cross product, as you've found, is ##dl x_1## . The square of the magnitude of r is ##x_1^2 + z_1^2##. That, along with the current magnitude and constants of the Biot-Savart law should be sufficient to write the result.
 
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I forgot to mention that I tried (μo/4∏)*[(I*dL*x1)/(( x1 )2 + (z1 )2)] which wasn't correct.

From what I understand the Biot-Savart law is (μo/4∏)*[I*(dL x r hat)/(|r|^2)]. Am I not suppose to be finding the cross product dl x r hat?

Sorry I'm having so much trouble understanding and visualizing this. Thank you for your patience.
 
Okay, I think I owe you an apology there. The cross product does indeed involve the unit vector in the direction of r. That puts another ##\sqrt{x_1^2 + z_1^2}## in the denominator along with the ##x_1^2 + z_1^2## that's already there. That yields ##(x_1^2 + z_1^2)^{3/2}## net. With that and the ##x_1## in the numerator I think you'll be alright.
 
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Not at all, you helped me get the correct answer and more importantly I get it now. Thanks so much!
 
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