Superconducting Loop

A quadratic undeformable superconducting loop of mass m m and side a a lies in a horizontal plane in a nonuniform magnetic field whose induction varies in space according to the law B x = α x B_{x}=- \alpha x B y = 0 B_{y}=0 B z = α z + B 0 B_{z}=\alpha z +B_{0}
The inductance of the loop is L L .
At the initial moment, the centre of the loop coincides with the origin O O , and its sides are parallel to the x x and y y axes. The current in the loop is zero, and it is released.

Where will it be ( ( z z coordinate ) ) in time t t after the beginning of the motion ? ?

Answer comes in the form of z = m g L a β α γ ( ϕ + cos ( a γ α L m t ) ) \Large z=\frac{mgL}{a^{\beta} \alpha^{\gamma}}\Bigg(\phi +\cos \bigg(\frac{a^{\gamma} \alpha}{\sqrt{Lm}} t\bigg) \Bigg)

Type your answer as β + γ + ϕ = ? \beta +\gamma +\phi=?

Details and Assumptions
1) β , γ , ϕ \beta ,\gamma ,\phi all are integers.
2) Gravity is acting in z -z direction.

The problem is not original.


The answer is 5.

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1 solution

Karan Chatrath
Jun 7, 2020

Disregarding any sign conventions:

FLux through the loop at any instant:

ϕ = a 2 B z \phi = a^2 B_z

Therefore magnitude of induced EMF:

ϕ ˙ = a 2 α z ˙ \lvert \dot{\phi} \rvert= a^2 \alpha \dot{z}

Using Kirchoff's voltage law:

a 2 α z ˙ = L I ˙ a^2 \alpha \dot{z} = L\dot{I}

When t = 0 t=0 , z = 0 z=0 and I = 0 I=0 . Integrating:

a 2 α z = L I a^2 \alpha z = LI

At any instant of time, the total magnetic force along the vertical ( F = I a B x F=IaB_x applied for side of the loop and added):

F B = α a 2 I F_B = -\alpha a^2 I

Newton's second law:

m z ¨ = F B m g m\ddot{z} = F_B -mg

Simplifying: z ¨ + α 2 a 4 z m L = g \ddot{z} + \frac{\alpha^2 a^4z}{mL} = -g

z ( 0 ) = z ˙ ( 0 ) = 0 z(0) = \dot{z}(0)=0

General solution:

z = A cos ( α a 2 t m L ) + B sin ( α a 2 t m L ) m L g α 2 a 4 z = A \cos\left(\frac{\alpha a^2t}{\sqrt{mL}}\right) + B \sin\left(\frac{\alpha a^2t}{\sqrt{mL}}\right) -\frac{mLg}{\alpha^2 a^4}

Applying initial conditions and solving for A A and B B :

z = m L g α 2 a 4 ( 1 + cos ( α a 2 t m L ) ) \boxed{z = \frac{mLg}{\alpha^2 a^4}\left(-1 + \cos\left(\frac{\alpha a^2t}{\sqrt{mL}}\right)\right)}

@Karan Chatrath Accurate solution.
BTW even disregarding sign convention how you reached the correct answer??

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If you choose a wrong sign convention, the general solution will have the form:

A e ω t + B e ω t + C A\mathrm{e}^{\omega t} + B\mathrm{e}^{-\omega t} + C

A,B and C are constants. Since the form of the solution is given, I already knew what the final differential equation should look like. I took a shortcut.

Karan Chatrath - 1 year ago

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@Karan Chatrath Sir enjoy the previous problem also, and I will be happy if you upgrade it.

I also disregarded the sign convention at first and then just fixed it at the end to give me the right physics.

Steven Chase - 1 year ago

from the circuit equation, it can be shown that the current is linear with z. writing the energy equation, the inductor energy can be written as if it were that of a spring. we determine the effective spring constant, and the rest of the analysis becomes that of a spring mass system under gravity.

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this is krotov problem 3.54

@Karan Chatrath 3.103 ( b ) 3.103(b) Here is my solution which is giving wrong answer
Steven sir has posted the solution of this problem in discussion section also.
But that was different method, I just want to know what is wrong in my method.
Thanks in advance.

You have found the charge density at either plate of the capacitor. My result is the bound charge density at the dielectric interface. They are different things.

Steven Chase - 12 months ago

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@Steven Chase sir please check your last 24 hour notifications, I have commented you on that place where we were talking.

A Former Brilliant Member - 11 months, 3 weeks ago

@Steven Chase sir i am planning to post a mechanics problem right now. Are you ready??

A Former Brilliant Member - 11 months, 2 weeks ago

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I am indeed

Steven Chase - 11 months, 2 weeks ago

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@Steven Chase @Steven Chase
Sir it is up now
Sorry for being late.

A Former Brilliant Member - 11 months, 2 weeks ago

@Steven Chase @Steven Chase sir can you please bear the pain to solve this equations.
After solving I think your new problem wedge block and spring can be solved very easily
Thanks in advance.

A Former Brilliant Member - 11 months, 2 weeks ago

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@A Former Brilliant Member You can try using code to solve your equations

Steven Chase - 11 months, 2 weeks ago

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@Steven Chase @Steven Chase sir i don't know how to solve equations using code
My planning is that first I will calculate the time for the block to reach the ground after that, that time will be used to calculate the distance travelled by that wedge, is it possible to do so in code.
If you are free, can you solve using your code.
Then I will be very Happy.
Thanks in advance

A Former Brilliant Member - 11 months, 2 weeks ago

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