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02:02
@sammygerbil How was this derived?
The solution given is also the same explanation, but how do we do this by just displacing the Bob slightly?
02:46
@AbhigyanC The solution was "derived" by the insight of realising that the apparatus is a rigid structure which is constrained in such a way that the bob moves in a plane perpendicular to fixed axis AB and keeps a fixed distance from the axis, like a simple pendulum.
It is not difficult to make a model and play with it. This will help to develop your insight.
How open is this chat to absolute noob homework help? I'm pretty not good at physics, lol!
03:11
@invadingdingo That's what we're here for. :)
The restrictions on the Q&A site do not apply here.
Ok, so here is the problem I'm given: In the figure two tiny conducting balls of identical mass m and identical charge q hang from nonconducting threads of length L. Assume that θ is so small that tan θ can be replaced by its approximate equal, sin θ. Find the magnitude of q in terms of the given variables, using ε0 and g if necessary
And I have absolutely no idea how to even begin.
03:50
@invadingdingo Start by drawing a Free Body Diagram for each ball. Identify the forces on it. The resultant force must be zero.
04:00
So since they're the same charge, they will exert force on eachother, pushing eachother away. Since they have mass, gravity is also acting on them, right? So each ball has 2 forces acting on it?
Wait, 3 since you have tension from the threads.
ok do far.
What should I start doing after that?
I'll call the forces acting on the charge from the other charge F1
Well, F1 and F2
So F1 = -F2 since they're charges of the same value?
Resolve forces into horizontal and vertical components. The sum of each must be zero.
They are of same magnitude
So for vertical, FsubT1 - mg = 0 and FsubT2 - mg = 0
and for horizontal, Fsub2 - Fsub1 = 0?
04:14
You need to make use of the angle theta at which each string is inclined to the vertical.
What is FsubT1? Also note that since the strings have the same length and the balls have the same mass and charge then the arrangement is symmetrical about the vertical, so the electrostatic forces are horizontal.
The electrostatic forces are mutual and therefore always have the same magnitude even when the charges are different.
FsubT1 is the tension from the string. It
s pointed directly upward
04:30
So where are the electrostatic forces F1, F2?
Is Fsub1 the same as FsubT1?
You only need to consider the forces on one ball. The forces on the other will be the same, except the mirror image.
That's my current diagram
Ok, so if I label the left ball qsub1 and the right qsub2, then qsub1 = -qsub2?
04:49
f(x,y)=⎧⎩⎨xy(x2−y2)x2+y20 for (x,y)≠(0,0) for (x,y)=(0,0).
These mixed derivatives \dfrac{\partial^2 f}{\partial x \partial y}
∂x∂y

2
f
​ and \dfrac{\partial^2 f}{\partial y \partial x}
∂y∂x

2
f
​ evaluated at the origin (0, 0)(0,0)left parenthesis, 0, comma, 0, right parenthesis turn out to be 111 and -1−1minus, 1 respectively. Computing this is actually pretty tricky, and requires looking directly at the limit-based definition of the derivative. Wikipedia provides a nice explanation, should you find yourself feeling ambitious.
Let me resend
See the link khanadacemy...
See the portion symmetry of second order partial derivatives.
Now under exception example there is a problem which has been solved somewhere
in Math stackexchange by assuming y=mx
I am getting stuck up there
@invadingdingo Please review the discussion so far. Your own contributions as well as mine. Aren't qsub1, qsub2 the same as F1, F2? Have you included the tension in the string in your diagram?
Let me resend
khanacademy.org/math/…
See the link khanadacemy...
See the portion symmetry of second order partial derivatives.
Now under exception example there is a problem which has been solved somewhere
in Math stackexchange by assuming y=mx
I am getting stuck up there
How would I find the tension in the string?
@invadingdingo This is a classic central force question.Use kq2/r2 action on both the bodies where r(or x in this case) can be found by approximating arc length to that of a straight line provided the given angle theta is small.
I had F1 and F2 as the forces exerted on the balls by eachother
04:57
@invadingdingo It has horizontal and vertical components which are related via the angle theta. These components need to be included when you sum the horizontal and vertical forces on one ball and set the total to zero.
@sammygerbil Pls come to my rescue after solving this question...LOL
Alternatively if you are familiar with moments you can take moments about the top of the string. The tension in the string acts through this point so it has no moment. Although the other 2 forces are not aligned their moments about the top of the string must be equal because the string is not turning.
@invadingdingo From where did u find this problem?
@gateprep I shall have to sleep soon. Sorry I don't have the strength to help.
It's a problem from my physics book the professor assigned, but did it over the weekend with 8 other problems so I'm unable to seek help from the resources the college provides.
We have a whole tutoring staff that can help, but they don't work on weekends :/
Unfortunately I can't seem to get my head around what you guys are suggesting, so I think I'm going to sleep for now and see what I can make of it tomorrow. I've been staring at this stuff fo 7 hours straight now, haha!
05:22
@invadingdingo What is the name of the book?
05:47
@invadingdingo How much do they charge for getting the solutions of a book
06:19
@JohnRennie good morning
Are you free for some time
@harambe I'm around Ll morning but I'm working on and off so I won't always be available.
Okay.... I just had small doubts about angular momentum
Well, you can ask ...
Why isn't angular momentum mvR here
I am unable to interpret angular momentum physically
At the instant shown in the diagram the wheel is, in effect, rotating about the point O as well as rotating on its axis. So you need to calculate the two angular momenta separately then add them.
06:29
So do points that do not lie in axis have angular momentum w. r. t the axis that we have to count
That would mean angular momentum depends on a frame
@harambe correct, angular momentum does depend on the frme.
So like linear momentum is, is there any frame where angular momentum is zero
Like centre of mass frame has zero momentum
No. Unless you allow rotating frames (which are non-inertial and therefore should be avoided like the plague) there is in general no frame where the angular momentum is zero.
Though in special cases such a frame does exist.
Oh okay
For example consider a point mass passing you at a distance $d$ and velocity $v$. In your frame the angular momentum is $mvd$.
If the distance $d$ is zero, i.e. if you are in the path of the particle, then the angular momentum is zero.
But obviously that's a special case e.g. it only works for point particles.
07:27
@JohnRennie what is orbital angular momentum and spin angular momentum
Wikipedia also states it but I didn't get that
Is rotation about axis spin angular momentum like here and the momentum about point O orbital?
08:21
@JohnRennie Are you there
@Abcd hi
Very quick questions Please see:
@JohnRennie These 4.
For the first question the answer is obviously the density. They start with the same volumes and are both compressed by 50% so they both end at the same volumes.
@JohnRennie Why not initial energy???
@Abcd hmm, to be fair that should also be correct since the two samples start out identical.
But then the question doesn't say what it means by identical energy. $U$? H$?
08:30
@JohnRennie Or is it that one could be monoatomic and other diamotic? That's why energy is not same?
@JohnRennie obviously internal energy
Ah, yes, that's possible
@JohnRennie Okay, next question please.
@Abcd the rod is at equilibrium so the temperature profile will be a straight line within each bit of the rod. The gradient of the staight line will be proportional to the thermal resistivity i.e. inversely proportional to the thermal conductivity.
@JohnRennie so?
So the graph will be three straight lines with a higher gradient in the lower conductivity reagion.
08:35
@JohnRennie Is D correct?
Yes, D is correct
@JohnRennie Answer given is A. D was my choice
Hmm, I would have said B.
????
At equilibrium the amount of heat flowing into the hot end has to be the same as the amount of heat flowing out of the cold end. So the total heat flow must be constant thoughout the rod.
If they mean heat flow per unit area then that decreases as we move from left to right as the area increases.
08:42
area is not changing
Oops, sorry, I'd moved on to the third question. Let me go back and look at the second question.
I don't see how A can possibly be the correct answer to the second question.
@JohnRennie does it have to do something with "unlagged" ?
Nothing is insulated
And $i = \dfrac{-KA dT}{dx}$ is for insulated stuff
Ah ... yes, I completely missed that. Yes, heat will flow sideways out of the rod at a rate roughly proportional to the temperature.
@JohnRennie ??
So more heat will be lost at the hot end than at the cool end i.e. the temperature will fall faster with $x$ at the hot end than at the cold end.
08:48
not getting
@Abcd if the rod isn't lagged then heat will flow sideways out of the rod into the environment around it.
.. Okay leave it then @JohnRennie
@JohnRennie next question please
The answer to the third question is B
@sammygerbil Thanks...
It makes a lot of sense now...
Hi, people! Does anybody know any good astronomy/astrophysics courses for starters?
Courses as in online materials, books etc.
08:56
@Mr.Xcoder MIT 8.901
That's graduate level I think, I'm looking for something a bit more basic
@Mr.Xcoder maybe try khan Academy?
@JohnRennie are you free now again?
@harambe basically yes. I'm intermittently struggling with a special relativity calculation so I may be distracted occasionally.
BTW has your suspension finished?
@JohnRennie yea. It ended on Sunday somewhat 2 PM IST
I asked @ACuriousMind for making sure and he gave me permission so it's all right now
@harambe I'll try that and see if it's what I am looking for. Thanks for the suggestion.
09:07
Oh no problem
@harambe cool :-)
@JohnRennie is there a time when you are free from work and also have some spare time to chat?
@harambe I'm free now (mostly)
Okay.. I just do this want to impose on you that's it.
About the previous question, I did the calculation and got the answer but I didn't get the part where you said we have to include both momentum
I mean is the wheel rotsting on two axis?
Actually that was rubbish, ignore me.
There is only ever one axis of rotation.
An object can't simultaneously rotate about two different axes without tearing itself apart! :-)
Blame it on it being early in the morning
09:16
Okay.. I was having the same doubt. Two axis rotation is out of topic for us anyways
09:38
@JohnRennie I tried a similar question
In the frame of axis the mass at the other end will have relative velocity w. r. t the mass in the middle and using m(rxv) gives the answer
Question 3?
But why are we not including the angular momentum of axis here. We included it in the previous one
Yes
Incidentally, if you could photograph the questions the right way up that would make life a lot easier.
Oh my mistake
I caught the photo in a hurry
OK, the question is asking about the rotation of the end relative to the particle at the centre. That can get confusing because you're trying to calculate rotation relative to something else that is rotating.
However the angular velocity has to be equal to $\omega$ i.e. the same as the angular velocity of the whole system. So that makes things a lot easier.
09:43
Yea property of rigid body
So for the particle at the centre, the other particle is moving with angular velocity $\omega$ at a distance of $d/2$.
So the moment of inertia of the other particle is $mr^2 = md^2/4$
Okay
@JohnRennie I get what you are doing. You are transforming the mass kept at the centre to be another axis
And that will give us the angular momentum easily about it?
@harambe $L = I\omega = m \omega d^2/4$
Answer (b)
09:52
Got it. I just had one question
How is this case different from the previous question I asked
I mean in calculatimg angular momentum
It isn't different. In both cases we need to find the moment of inertia and the angular velocity about our chosen reference point. Then the angular momentum is just $L = I\omega$
For the wheel you used the parallel axis theorem to calculate $I$. For the last question the moment of inertia is simpler because for a point mass at some distance $r$ we get $I = mr^2$.
@JohnRennie but clockwise and anticlockwise rotation of disc is giving different answers
Why so
10:07
@harambe In the question the wheel is rolling along the floor so the point of the wheel in contact with the floor is stationary relative to the floor.
But if the wheel is rotation in the other direction it is skidding along the floor so the point of the wheel in contact with the floor is moving.
Okay but what does it tell us
That means you can't simply proceed as if the whole wheel is rotating around the point of contact with the floor.
About angular momentum
I'd have to thnik about how to do the calculation in that case, but it would certainly produce a different answer.
Okay so L=I w is valid only for inertial points
That too rotsting about a fixed axis
Got it
10:30
@JohnRennie I am getting some doubts again
In Q 4,the initial angular momentum is Iw
But for calculating the final angular momentum will the moment of inertia be 2I
Yes. Moments of inertia just add (assuming they are about the same axis). Since the two wheels are identical their combined moment of inertia is twice the moment of inertia of one wheel.
Oh kay.. I got confused in this adding of moment of inertia
Can't the axis change in these angular momentum conservation questions
Like for Q5 @JohnRennie
I am getting angular velocity to be w/2 considering axis doesn't change
The rotation axis before and after adding the stone is the same axis. Yes?
Yes
I don't understand why it doesn't change
The moment of inertia of the disk about this axis is ... erm ... I can't remember the equation for the moment of inertia of a disk about its centre.
10:36
I think I am just getting confused by my own silly doubts
MR2/2
@harambe yes, $I_\text{disk} = \tfrac{1}{2}mr^2 $
And if we can treat the particle as a point mass then its moment of inertia is bust $MR^2$ i.e. $I_\text{stone} = 2m (a/2)^2$
I proceed we just like that
But these silly doubts just come to me xd.
Yes, the total moment of inertia afterwards is just $\tfrac{1}{2}ma^2 + 2m(a/2)^2 = ma^2$
And equating it with intial angular momentum gives the required value of angular velocity
@sammygerbil good morning
@harambe Good morning. Just taking another look at gateprep's question.
10:53
@sammygerbil would you like to be a room owner here? You seem to be putting a lot of work into answering questions.
@JohnRennie What does the job involve?
@sammygerbil nothing really. It just gives you the power to delete posts and kick people out of the room.
I've used the superpowers to delete posts, but I've never had to eject anyone.
@JohnRennie ok count me in!
Done. If you ever feel the urge to abuse your new superpowers go right ahead :-)
11:15
@gateprep I located the "exception example" on the Khan Academy page, and I found a question about this on Mathematics SE (math.stackexchange.com/questions/2337004/…) but I cannot find the solution using y=mx. I don't understand the thinking behind this substitution.
If the calculation is "pretty tricky" then it is probably too long for this Chatroom. How about posting in Mathematics SE? They don't have the same HW policy as we have in Physics SE.
11:27
Why doesn't applying conservation of energy directly gives the answer
The kinetic energy of the bullet is converted into rotstional energy of rod
The bullet gets embedded in the rod so it is not an elastic collision.
If it was an elastic collision the bullet would bounce backwards off the rod.
Okay
So how should I proceed for this
I have calculated velocity of centre of mass of the system after impact
Will angular moment be conssrved
Yes, just use conservation of angular momentum. The moment of inertia of the bullet is $mL^2$ and its angular velocity is $\omega = v/L$.
@JohnRennie one little doubt
The velocity of centre of mass is in ground frame
You don't need the velocity of the centre of mass.
This isn't an inertial frame because the pivot is going to exert a force, so I wouldn't try and use the COM frame for this one.
11:38
But doesn't hinge make the pivot inertial
The hinge is going to exert a force, so the frame isn't intertial. Luckily the pivot doesn't move so even though it exerts a force it doesn't do any work.
Just calculate the angular momentum about the hinge just before and just after the collision and that will give you $\omega$ after the collision.
By frame do you mean centre of mass frame
@JohnRennie got the answer
But I still don't understand which frame were you talking about
Maybe centre of mass frame?
These frames are very confusing to me
When you're dealing with rotational motion do all your calculations in the rest frame of the axis of rotation.
12:00
I'm off now. I'll be back briefly later today then tomorrow morning.
 
4 hours later…
16:19
@JohnRennie A quick question
It isn't nevessarily for a continious function to be differentiable at every point, right
Or does continious function guarantee derivability
@harambe correct. For example a triangular wave is continuous but not differentiable everywhere.
Yea I just saw this in some book but I think they explained it wrong. Thanks for clarifying
 
3 hours later…
19:19
@sammygerbil Are you there?
@Abcd yes. Good evening.
@sammygerbil Hi, do you know about liquid solutions, the correpsonding laws, entropy, Van't hoff factor etc?
@Abcd Almost nothing. I took A level chemistry but that was a long time ago.
@sammygerbil Ohkay fine... No expert there to help us in chemistry room :(
@Abcd There is a room for JEE chemistry? Is that The Periodic Table?
19:25
@sammygerbil Yes, this one^ (not periodic table)
Hey guys do you have any answer to this
-1
Q: Can this thought experiment successfully prove that HUP is epistemological and not ontological?

Chakrapani N RaoHere's a thought experiment. Let's assume that we have the most cutting edge technology at our disposal. We need an electron detection sphere, as small as possible, it must detect a single electron when it hits the surface. Now assume that we introduce an electron in the sphere, as slowly as po...

@ChakrapaniNRao I think that would get more discussion in the hbar. We're mostly concerned with examination questions here.
@ChakrapaniNRao I don't think your idea of "stunning" an electron would work. Electric fields are conservative, even strong ones. Just because you confine an electron does not guarantee that you remove its kinetic energy. When you "confine" it you are just forcing it to move about in a smaller space. It keeps its kinetic energy and goes back to its previous motion when you release it.
19:44
@sammygerbil thanks for responding, I have tried hbar in vain
The idea was never to stun an electron, it was to create a very slow moving electron but was said in an ideal sense. Like if you try to stun an electron you must practically have a very slow moving electron, that was the point
@ChakrapaniNRao And it doesn't make sense to use the tag for Classical Mechanics at the same time as Quantum Mechanics unless you are asking about the transition between quantum and classical domains.
@sammygerbil very good observation, that's done purposefully, but if I reveal the intent of doing it, people will shut me down
but what do you think of the main question
?
20:45
@ChakrapaniNRao Sorry I do not understand your argument, nor the leap into philosophy at the end. It needs much more explanation, eg what you mean by epistemological and ontological and how you reached this conclusion. Raising philosophical issues in Physics SE and assuming users know what these terms mean rarely gets a good response. If you can use plain English you have a much better chance.

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