Solenoid Exercise

A wire solenoid has the following shape:

x = cos θ y = sin θ z = 10 + θ 100 π 0 θ 2000 π x = \cos \theta \\ y = \sin \theta \\ z = -10 + \frac{\theta}{100 \pi} \\ 0 \leq \theta \leq 2000 \pi

The solenoid carries 1 1 unit of electric current. Let B 1 B_1 be the magnitude of the magnetic flux density at point ( x 1 , y 1 , z 1 ) = ( 0 , 0 , 0 ) (x_1, y_1, z_1) = (0,0,0) , and let B 2 B_2 be the magnitude of the magnetic flux density at point ( x 2 , y 2 , z 2 ) = ( 2 , 0 , 0 ) (x_2, y_2, z_2) = (2,0,0) .

What is B 1 B 2 \frac{B_1}{B_2} ?

Details and Assumptions:
1) Magnetic permeability μ 0 = 1 \mu_0 = 1
2) Only the fields from the solenoid are to be counted (don't worry about completing the circuit, etc.)

Note: How does the value of B 1 B_1 compare to the value given by the standard formula for a solenoid magnetic field?


The answer is 201.15.

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2 solutions

As sir @Karan Chatrath has provided a very nice solution. I will just elaborate the solution. This problem can be considered as a biot-savart law problem because we have the exact information of solenoid structure.

Karan Chatrath
Apr 1, 2020

Consider a point on the solenoid as such:

r p = cos θ i ^ + sin θ j ^ + ( 10 + θ 100 π ) k ^ \vec{r}_p = \cos{\theta} \hat{i} + \sin{\theta} \hat{j} + \left(-10+\frac{\theta}{100 \pi}\right)\hat{k}

An arc length element tangential to the point is:

d r p = ( sin θ i ^ + cos θ j ^ + ( 1 100 π ) k ^ ) d θ d\vec{r}_p = \left(-\sin{\theta} \hat{i} + \cos{\theta} \hat{j} + \left(\frac{1}{100 \pi}\right)\hat{k}\right) \ d\theta

Consider the point of interest at which field is to be computed to be:

r c 1 = 0 i ^ + 0 j ^ + 0 k ^ \vec{r}_{c1} = 0 \hat{i} + 0 \hat{j} +0\hat{k} r c 2 = 2 i ^ + 0 j ^ + 0 k ^ \vec{r}_{c2} = 2 \hat{i} + 0 \hat{j} +0\hat{k}

In general, the point of interest will be denoted by r c \vec{r}_{c} . The vector joining a point on the solenoid and the point of interest, and directed towards the point of interest, is:

r = r c r p \vec{r} = \vec{r}_c - \vec{r}_p

Now, Biot-Savart Law is applied:

d B = μ o I 4 π ( d r p × r r 3 ) = f x ( θ ) i ^ + f y ( θ ) j ^ + f z ( θ ) k ^ d\vec{B} = \frac{\mu_o I}{4 \pi}\left(\frac{d\vec{r}_p \times \vec{r}}{\lvert \vec{r} \rvert^3}\right)= f_x(\theta) \hat{i} + f_y(\theta) \hat{j} +f_z(\theta) \hat{k}

d B d\vec{B} has three components each of which is a function of θ \theta only. This gives three integrals:

B x = 0 2000 π f x ( θ ) d θ B_x = \int_{0}^{2000 \pi} f_x(\theta) \ d\theta
B y = 0 2000 π f y ( θ ) d θ B_y = \int_{0}^{2000 \pi} f_y(\theta) \ d\theta B z = 0 2000 π f z ( θ ) d θ B_z = \int_{0}^{2000 \pi} f_z(\theta) \ d\theta

I have written a script of code to compute the answer for each case which turns out to be:

B 1 B 2 201.1528 \boxed{\frac{B_1}{B_2} \approx 201.1528}

As for the bonus question, In the first case, the field magnitude turns out to be:

B 1 49.75 B_1 \approx 49.75

Which is almost close to the result produced by the standard formula which turns out to be 50 50 . This is unlike the case where

B 2 0.2473 B_2 \approx 0.2473

This result highly deviates from the standard formula prediction. It is surprising that just an offset of two units in the point of interest can produce such a different result. In my opinion, the standard formula holds true provided the test point is sufficiently and equally far from either end of the solenoid. I am yet to test this speculation, however.

@Karan Chatrath can you please post the analytical solution of Starfish orbit .

A Former Brilliant Member - 1 year, 2 months ago

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