Two spherical metal object
A
and
B
are placed outer in a very free space , of masses
M
A
and
M
B
and have charges
Q
A
Q
B
and both have equal radius of
R
.
The distance between centre of
A
and
B
is
3
.
Find the time taken by them to collide with each other.
Details and Assumptions
1)
M
A
=
7
,
M
B
=
1
1
2)
Q
A
=
1
7
,
Q
B
=
2
3
3)
R
=
1
4)
G
=
1
,
ϵ
0
=
1
This problem is made by me and is dedicated to my teachers
Steven Chase
and
Karan Chatrath
on the account of Teachers Day.
So, Happy Teachers Day.
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Thank you for dedicating this problem to me
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@Karan Chatrath
Thanks.
Please take a look in this problem
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I'll repeat what I said earlier. Show an attempt.
Start by thinking about what would cause the ring to rotate in the first place.
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@Karan Chatrath
–
@Karan Chatrath
Ok sir.Don't go
I am sharing my attempt within 10 min :)
@Karan Chatrath
sorry for late.
I want to ask one thing
The flux due to big cylinder in that ring will be equal to, the the current in the ring, which will make flux??
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Sorry, I do not understand your question. You may ask it in hindi if that is convenient.
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@Karan Chatrath
can we chat somewhere else, please
Brilliant feels me very tough for chatting.
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@Talulah Riley – @Karan Chatrath i am. Very simple guy.
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@Talulah Riley – I am sorry, but that is not possible. Be patient, convey your questions to me on this platform and I will do my best to answer them when I can. Again, please be patient.
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@Karan Chatrath
–
@Karan Chatrath
Again blocked ha ha :)
I think Brilliant has sponsored you to chat here only.
Ok wait let me convey my message in hindi.
@Karan Chatrath sir I have posted a discussion.
Nice one. This is a great exercise for practicing numerical simulation.
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@Steven Chase
Thanks , you solved it before starting of Teachers day.
By the way, I solved it completely analytically.
The Code is very simple still it gives answer of such difficult problems
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How difficult was it to do by hand?
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@Steven Chase are you kidding me??
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@Talulah Riley – No, I am not
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@Steven Chase – @Steven Chase Ok hmmm. It was more difficult than taking a reply of Good Morning from Steven sir.
Greetings @Steven Chase ! I do not consider myself a seasoned python user, but I attempted to solve the final integral in my posted solution using python. And for some reason, I am unable to spot why my result is not consistent as I vary the numerical resolution. Please let me know your thoughts on it. Here is my code:
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It looks like your integrand has a singularity at x = 3 . Such singularities are very problematic for numerical methods. That's counter-intuitive, since the centers of the spheres never coincide.
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Yes, I think this explains it. I re-ran the code by simulation till x = 3 − ϵ where ϵ is a very small number (smaller than the time step), however, the inaccuracy still persists.
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Consider the mass M A to have an x coordinate of x 1 and the mass M B to have an x coordinate of x 2 .
The mass M A has its centre initially located at the origin and the mass M B has its centre located at the point (3,0).
Applying Newton's second law for each of the masses gives:
M A x ¨ 1 = ( x 2 − x 1 ) 2 G M A M B + 4 π ( x 2 − x 1 ) 2 Q A Q B M B x ¨ 2 = − ( x 2 − x 1 ) 2 G M A M B − 4 π ( x 2 − x 1 ) 2 Q A Q B
Let:
x = x 2 − x 1
Now, the equations of motion can be re-written as:
x ¨ 1 = x 2 M B − 4 π M A x 2 Q A Q B x ¨ 2 = − x 2 M A + 4 π M B x 2 Q A Q B
Subtracting both these equations gives:
x ¨ 1 − x ¨ 2 = [ M A + M B − 4 π Q A Q B ( M A 1 + M B 1 ) ] x 2 1
Let:
K = M A + M B − 4 π Q A Q B ( M A 1 + M B 1 )
The equation of motion simplifies to:
x ¨ = x 2 K x ( 0 ) = 3 x ˙ ( 0 ) = 0
The above equation can be re-arranged as such:
x ¨ = x ˙ d x d x ˙ = x 2 K ⟹ x ˙ d x d x ˙ = − x 2 K
An extra minus sign is introduced above as x decreases x ˙ increases. Separating variables and integrating:
x ˙ 2 = 2 K ( x 1 − 3 1 )
⟹ x ˙ = − 2 K ( x 1 − 3 1 )
Minus sign introduced here, for the same reason as stated above:
⟹ x ˙ = − f ( x )
The particles collide at the instant when x = 2 . Separating the variables and integrating again gives:
∫ 2 3 f ( x ) d x = T ≈ 1 . 2 1 9 3 3 4 6 8 0 3 9 2 2 1 2