Capacitor Exercise (part 3)

A parallel plate capacitor is made up of two square plates of side a a , separated by a distance d ( d < < a ) d(d<<a) .An imaginary part of the curve y 2 = x y^{2}=x is applied as you can see in figure. The upper portion is filled with dielectric of dielectric constant K 1 K_{1} and the lower portion is filled with K 2 K_{2} as shown in figure. I have provided the view of figure from Y -Y axis. Find the capacitance of capacitor
Details and Assumptions
1 ) K 1 = 4 1)K_{1}=4
2 ) K 2 = 3 2)K_{2}=3
3 ) d = 10 3) d=10
4 ) ϵ 0 = 1 4) \epsilon_{0}=1
5 ) a = 100 5) a=100
Everything is in SI units
Assume that the standard formula of capacitor holds.

From now onwards I will tell in each problem that it is original or not as it is a request from a person.
The problem is purely original.


The answer is 3286.89.

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2 solutions

Steven Chase
May 3, 2020

My solution, just for fun.

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import math

Num = 10**6

K1 = 4.0
K2 = 3.0
d = 10.0
e0 = 1.0
a = 100.0

e1 = K1*e0
e2 = K2*e0

dx = a/Num
dA = a*dx

############################

C = 0.0

x = dx

while x <= a - dx:

    y = math.sqrt(x)

    dC1 = e1*dA/(d-y)
    dC2 = e2*dA/y

    dC = dC1*dC2/(dC1 + dC2)

    C = C + dC

    x = x + dx

############################

print Num
print C

#>>> 
#100000
#3286.82579219
#>>> ================================ RESTART ================================
#>>> 
#1000000
#3286.88428375
#>>> 

@Steven Chase Can we parametrise solid sphere using cartesian coordinates??If yes. Please tell

A Former Brilliant Member - 1 year, 1 month ago

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In cartesian coordinates:

R x R R 2 x 2 y R 2 x 2 R 2 x 2 y 2 z R 2 x 2 y 2 -R \leq x \leq R \\ -\sqrt{R^2 - x^2} \leq y \leq \sqrt{R^2 - x^2} \\ -\sqrt{R^2 - x^2 - y^2} \leq z \leq \sqrt{R^2 - x^2 - y^2}

To check if this works, you could do a triple integral with volume element d x d y d z dx \, dy \, dz and see if it yields the proper volume for a sphere

Steven Chase - 1 year, 1 month ago

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@Steven Chase I also got the same, but it looks me so weird, so I thought that I am wrong somewhere. Thanks for clarification. Well I decided to make question that a charge is placed at a random position inside anywhere in sphere and find the average field at (2, 0).

A Former Brilliant Member - 1 year, 1 month ago

@Steven Chase Have a look. Uploaded. I was making one more question . A 1m rod is placed in origin with linear charge density as λ = + 1 \lambda=+1 . rotating with some constant ω \omega . Calculate the average electric field at ( 1 , 0 , 0 ) (1, 0,0)

A Former Brilliant Member - 1 year, 1 month ago
Karan Chatrath
May 3, 2020

Consider a small element from a distance x x from the left side of the given diagram of thickness d x dx . This can be treated as two elementary parallel plate capacitors in series.

d C 1 = a d x K 2 ϵ o y dC_1 = \frac{a \ dx \ K_2 \epsilon_o}{y} d C 2 = a d x K 1 ϵ o d y dC_2 = \frac{a \ dx \ K_1 \epsilon_o}{d-y}

Since these two elementary capacitors are in series, its equivalent capacitance is:

d C = d C 1 d C 2 d C 1 + d C 2 dC = \frac{dC_1 \ dC2}{dC_1 + dC_2} d C = a ϵ o K 1 K 2 d x K 2 ( d y ) + K 1 y \implies dC = \frac{a \epsilon_o K_1 K_2 \ dx}{K_2(d-y) + K_1 y}

Now, y = x y=\sqrt{x} , and so:

d C = a ϵ o K 1 K 2 d x K 2 ( d x ) + K 1 x dC = \frac{a \epsilon_o K_1 K_2 \ dx}{K_2(d-\sqrt{x}) + K_1 \sqrt{x}}

Plugging in numbers and simplifying gives:

d C = 1200 d x 30 + x dC = \frac{1200 \ dx}{30 + \sqrt{x}}

C = 1200 0 100 d x 30 + x 3286.89 C = 1200 \int_{0}^{100} \frac{dx}{30 + \sqrt{x}} \approx 3286.89

In your new problem, there is an r 2 r^2 in the denominator of the acos argument, where it should be an r r . Not sure if that influences the end result

Steven Chase - 1 year, 1 month ago

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Nice catch. Corrected now. Apologies for the error.

Karan Chatrath - 1 year, 1 month ago

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Would like to know your thoughts on that problem. I request you to do so, at your convenience. I was reading about relativity and I came across a section on vector transformations. The result of that problem is one that I find strange.

Karan Chatrath - 1 year, 1 month ago

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@Karan Chatrath @Karan Chatrath Sir for the problem electric and magnetic field α = x \alpha =x , β = y \beta =y , γ = z \gamma =z how can I get the values of c 1 , c 2 , c 3 , c 4 , c 5 , c 6 c_{1}, c_{2}, c_{3}, c_{4},c_{5}, c_{6} I will be happy if you reply Sir
Thanks in advance! Please reply

A Former Brilliant Member - 1 year, 1 month ago

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@A Former Brilliant Member Use the initial conditions.

Karan Chatrath - 1 year, 1 month ago

You can't write the expression for the equivalent capacitance directly. First write the equation as δ C = δ C 1 δ C 2 δ C 1 + δ C 2 = a ϵ 0 K 1 K 2 δ x K 2 d + ( K 1 K 2 ) y \delta C=\dfrac{\delta C_1\delta C_2}{\delta C_1+\delta C_2}=\dfrac{a\epsilon_0K_1K_2\delta x}{K_2d+(K_1-K_2)y} and then pass on to the limit.

A Former Brilliant Member - 1 year, 1 month ago

@Karan Chatrath Sir, but I reached this expression, and it has terminal velocity also. m L v ¨ + m R v ˙ + B 2 D 2 v = m g R mL\ddot{v}+mR\dot{v}+B^{2}D^{2}v=mgR The basic equations are

B D v I R = L I ˙ BDv-IR=L\dot{I} m g I D B = m v ˙ mg-IDB=m\dot{v} . Please correct me if I am wrong.

A Former Brilliant Member - 1 year, 1 month ago

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No, you are not wrong. I made an algebraic mistake. Just checked it. My apologies for that.

Also, I noticed that you reached out to me on another social media platform. I do not encourage that, so please do not do that in future. Thanks.

Karan Chatrath - 1 year, 1 month ago

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@Karan Chatrath No problem Sir . Cheers!

A Former Brilliant Member - 1 year, 1 month ago

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