A parallel plate capacitor is made up of two square plates of side
a
, separated by a distance
d
(
d
<
<
a
)
.An imaginary part of the curve
y
2
=
x
is applied as you can see in figure. The upper portion is filled with dielectric of dielectric constant
K
1
and the lower portion is filled with
K
2
as shown in figure. I have provided the view of figure from
−
Y
axis.
Find the capacitance of capacitor
Details and Assumptions
1
)
K
1
=
4
2
)
K
2
=
3
3
)
d
=
1
0
4
)
ϵ
0
=
1
5
)
a
=
1
0
0
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.
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@Steven Chase Can we parametrise solid sphere using cartesian coordinates??If yes. Please tell
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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
To check if this works, you could do a triple integral with volume element d x d y d z and see if it yields the proper volume for a sphere
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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).
@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 . rotating with some constant ω . Calculate the average electric field at ( 1 , 0 , 0 )
Consider a small element from a distance x from the left side of the given diagram of thickness d x . This can be treated as two elementary parallel plate capacitors in series.
d C 1 = y a d x K 2 ϵ o d C 2 = d − y a d x K 1 ϵ o
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 ⟹ d C = K 2 ( d − y ) + K 1 y a ϵ o K 1 K 2 d x
Now, y = x , and so:
d C = K 2 ( d − x ) + K 1 x a ϵ o K 1 K 2 d x
Plugging in numbers and simplifying gives:
d C = 3 0 + x 1 2 0 0 d x
C = 1 2 0 0 ∫ 0 1 0 0 3 0 + x d x ≈ 3 2 8 6 . 8 9
In your new problem, there is an r 2 in the denominator of the acos argument, where it should be an r . Not sure if that influences the end result
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Nice catch. Corrected now. Apologies for the error.
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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.
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@Karan Chatrath
–
@Karan Chatrath
Sir for the problem electric and magnetic field
α
=
x
,
β
=
y
,
γ
=
z
how can I get the values of
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
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@A Former Brilliant Member – Use the initial conditions.
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 = K 2 d + ( K 1 − K 2 ) y a ϵ 0 K 1 K 2 δ x and then pass on to the limit.
@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 The basic equations are
B D v − I R = L I ˙ m g − I D B = m v ˙ . Please correct me if I am wrong.
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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.
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@Karan Chatrath No problem Sir . Cheers!
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