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09:18
Hello @JohnRennie
How could I invite you in jee math chat room on math SE
@HarjotDhillon Hi :-)
 
2 hours later…
11:18
@JohnRennie Will you be around at 9:30PM IST ?
11:30
@KavinIshwaran Yes :-)
11:49
Ok :-)
 
1 hour later…
12:55
@JohnRennie As you are a scientist who has been working in the natural sciences for many years, I wanted to ask if you knew the answer to this question: what conditions must something pass in order to be classified as scientific knowledge?
 
2 hours later…
15:24
Hello @JohnRennie !
Hi :-)
I'm sending the question
This is a similar question. Can I go through my solution? So that you could point the mistake
OK ...
If pulley moves by x, the block moves by 2x
Not at x, let the acceleration of cm of pulley be $$\frac{a+b+Mg-kx}{M}$$
Where a and b are the tensions from left to right
Then since pulley is not slipping:
$$\frac{2(b-a)}{M} + \frac{a+b+Mg-kx}{M}=\frac{mg-b}{m}$$
@PandaScientist I think this is wrong ...
The Mg shouldn't be there.
15:33
I felt that before, but then I thought if gravity is working on block , shouldn't it be working on the pulley too?
@JohnRennie and...I did it without mg too. Still got no answer :-(
I will have to think about this one. I don't immediately see how to do it.
Can I proceed without mg and continue?
And I don't want to to do it right now. I will try to look at it tomorrow morning.
Sorry :-(
15:37
Np sir :-) your assurance is enough !
One quick doubt, in cases where we have torsional SHMs, their actual $\omega$ is different from the $\omega$ in $-{\omega}^2 \theta$ , right?
No, I don't think so.
Can you pls explain?
Obviously we get ω² = k/I instead of k/m but otherwise it's the same equation.
I Think I didn't convey my doubt properly ! Let me rephrase ...
OK ... ?
15:44
Say, there's a circular disc rotating but follows SHM
It's omega is diff. from the omega in ${\omega}^2 \theta$ right?
So when we rotate it an angle θ there is a restoring torque τ = kθ
Yes?
And τ = Iα so we end up with:
α = -(k/I) θ
Oh I think I see.
...and now, I got it :-)
OK :-)
15:48
They are different.
@JohnRennie thank you sir :-)
16:05
@JohnRennie Hi !
Hi :-)
16:23
@JohnRennie How to do this ?
@KavinIshwaran You need to first find the current at steady state. If you use Kirchoff round the outer loop you will find the current is zero. Yes?
@JohnRennie At Steady state, the branch A B is ineffective right ?
Yes. There is zero current through the capacitor at steady state.
@JohnRennie Yes
Now consider the top loop. The voltage drop in R is zero because I = 0, so the only voltage changes are the two batteries and the capacitor. Yes?
16:29
But we are applying it at steady state knowing no current flows through AB right ?
Yes
Because we know the steady state current through a capacitor is always zero.
So if you go round the top loop since the voltage across R is zero, and we know the voltage across the batteries, we can find the voltage cross the capacitor.
Yes?
And that voltage comes out as ... ?
(actually this surprised me a bit)
16:36
@JohnRennie Suppose if we take a point next to the middle loop's battery's positive terminal as C (lets take it as zero) and going form C to B through A gives the potential drop to be zero
So PD = zero ?
@KavinIshwaran Yes :-) Option (1)
I get it :-)
I must admit I wouldn't have guessed that without doing the analysis.
Oh !
But this question troubled me a lot :-)
But you are happy you know how to approach it now?
16:39
Yes !
OK :-)
@JohnRennie Thank you for the clarification :-)
You're welcome :-)

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