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02:42
@JohnRennie Sir, will you get free by 10:30 AM (UK time zone) :-) ?
In Sommerfeld’s Lectures on Theoretical Physics, Vol II, Chapter 2, Section 6, Page 43 we derive an expression for the equilibrium of liquids as $$ grad ~p = \mathbf F$$ Where $p$ is the pressure and $F$ is the exertnal force. Then he writes,
[ The equation above ]includes a very remarkable Theorem: equilibrium is only possible if the external force has a potential, that is, if $\mathbf F$!can be represented as the gradient of a scalar function: $$ \mathbf F = -grad ~U$$ Where the minus sign is prompted by the relation to the potential energy. The existence of the potential function $U$is n
 
2 hours later…
04:49
Consider the electric potential. This is a single values scalar potential and we get the electric field from it using $E = -dU/dx$.
Single valued means suppose we start at a point $x$ and transport a charge around a loop back to $x$ then the total work done on the charge has to be zero.
But now consider a magnetic field. Magnetic field lines form loops, and if we transported a magnetic charge round a loop and back to it's starting point the net work done would not be zero.
That means a magnetic potential is not single valued, so this would be an example of a scalar function that is not single valued.
Physically we take this to mean a magnetic potential cannot be defined and the magnetic field cannot be written as the gradient of some magnetic potential.
 
1 hour later…
06:10
@JohnRennie Sir I’m so sorry but I couldn’t understand the explanation.
@Knight I'm working for a couple of hours - Monday mornings are always busy :-(
Yes sir. Hope you will get free before lunch :-)
 
2 hours later…
08:37
@Knight hi, I'm free now
09:31
-1
Q: What is the difference between $F_2$ and $W_A$?

Math geek Underlined statements are definitions of $F_1$ and $F_2.$ I am learning the basics of free body diagram. I am not able to judge the distinction between $F_2$ and $W_A$. $W_A$ is the weight of $A$ acting on $B$. $F_1$ is the reaction force of $B$ to $A$ as the consequence of Newton's th...

 
1 hour later…
10:39
sorry for the above link
11:35
@JohnRennie Hello
@Knight hi :-)
How are you sir?
I'm good :-) How are you?
@JohnRennie I’m very fine. Can you explain me what that “single-valued” meant?
Please
Take the function $y = \arcsin(x)$
11:41
Okay
This isn't single valued because for every value of x there can by multiple values of y.
For example if $x=0$ then $y$ can be $0$, $\pi$, $2\pi$, $-\pi$ and so on. Yes?
Yes yes yes.
:)
In principle we could have a scalar field $U(\mathbf x)$ that was also multiple valued. Mathematically there's nothing wrong with this.
i.e. for every position $\mathbf x$ in space $U(\mathbf x)$ could have many different vaues.
The problem with this is that in physics it doesn't make sense to have a potential that can have multiple different values at the same point.
But sir in the above case we cannot call $arcsin ~x$ a function because a single $x$ results in multiple values of $y$, ha?
People have a tendency to use the term function in a vague sense to mean any form of mapping, single or multiple valued.
11:46
Yes, I understand.
1 min ago, by John Rennie
The problem with this is that in physics it doesn't make sense to have a potential that can have multiple different values at the same point.
^ is totally clear to me.
I have confusion in taking free body diagram :(
May I get help
@Mathgeek Yes you will be helped but just a little later, sorry :-)
okay sir
@Knight Sommerfeld is just saying that if you're going to write the force field as the derivative of a potential function $U$ then that function must be single valued.
@JohnRennie Doesn’t that always happen sir?
Means all he was saying is that $U$ cannot be any of the circular function and their inverses (to say a few)
?
11:50
The point I was making earlier is that if you attempt to define a potential for the magnetic field then you find the potential you end up with is multiple valued.
That is, you cannot write the magnetic field as the derivative of some scalar potential $U(\mathbf x)$.
If you’re not too busy (as I have understood the meaning of “single-valued”) can you please explain that magnetic field example of yours ?
This is going to get involved and I don't have time right now as I have to go soon.
:-) Thank you very much sir
I apologise for being too demanding
Do you know what a conservative field is?
Yes, work depends only on net displacement and curl of the field must vanish everywhere
11:55
Yes. So the integral between two points does not depend on the path taken. Yes?
Yes
But in magnetic fields the integral between two points can be different for different paths.
Yes sir got you.
That's the problem. It means the magnetic field is non-conservative.
Physically it happens because magnetic field lines form loops.
$$\int_{x}^{x} U(t) dt = U(x) - U(x) \neq 0$$
11:57
And if you get loops that always means the curl is non-zero.
Yes
@Knight yes, exactly, and that has to mean $U(x)$ is multiple valued.
Yes, if the integrals depends only on end values, and even if the end values are same there are no assurance that the integral will vanish, one example of such $U$ is $\frac{1}{ \sqrt {1-x^2}}$
$$\int_{0}^{0} \frac{1}{ \sqrt {1-x^2}} dx = \sin^{-1} (0) - \sin^{-1} (0) = 2 \pi $$
Thanks sir, thank you so much!
Have a good lunch sir !
And healthy too :)
12:03
I fast on Mondays
So no lunch for me today!
Oho!
Have a good fast sir! And healthy too!
LOL
@Mathgeek You there?
yes
@Knight
$F_2$ is same in magnitude as $W_A$ but we didn’t write $F_2$ as $W_A$ because $F_2$ is a contact force, it is caused by $A$ on $B$ while $W_A$ is the force caused on $A$ by the earth. Does it help ? @Mathgeek
My question is applying the freebody diagram to object $A$. we get $F_1-W_A=m_a a_A$
@Knight let me read sir
Ask away!
12:11
For this diagram. shouldn't we apply one more force like $F_2$ here?
Why? And which?
$W_A$ is the force caused by earth. Force apply on ground , let it be $F$ and its reaction force $N$.
$W_A$ is force on $A$ caused by the earth
@Knight Yes
So, we got just two force on $A$, one caused by the earth and the other caused by the ground (normal force)
12:17
@Knight why there is three forces above $F_1, W_A, F_2$?
Where?
Which diagram ?
May I take 1 minute for thinking sir?
Yes
:-)
This figure is clear to me
That’s nice
12:22
$F_1$ is the reaction force from $B$ to $A$
Yes
I will be back in 3 minutes, don’t go anywhere
okay sir
while looking at the figure 2
What are the forces acting on $B$ by $A$?
sorry
What are the forces acting on $B$ by $A$?
You know, you can delete your own messages)
@Mathgeek $F_2$
@Suvitruf-AndreiApanasik I was late to judge the message was irrelevent.
12:36
@Suvitruf-AndreiApanasik Hello!
@Mathgeek The force on $B$ by $A$ is $F_2$ which is in same magnitude as the weight of A
@Suvitruf-AndreiApanasik It really feels good when some very nice people like you still have an avatar of Monica. I salute thee
@Knight never forget (;
@Suvitruf-AndreiApanasik Yes because next could be us
@Suvitruf-AndreiApanasik Which Are you from?
@Knight (。•́︿•̀。)
@Knight Russia.
Or, you mean, site? )
12:40
No, I really meant your country
@Suvitruf-AndreiApanasik Keep always coming here.
@Mathgeek Is your problem solved?
@Knight Can we take $F_2$ as $W_A$ without ambiguity in the second diagram?
In calculation we can replace $F_2$ by $W_A$
Yes
here, we know by intuition, force exerted on $B$ by $A$ is only weight of $A$
12:46
Yes
due to that reaction force $F_1$ acted by $B$ on $A$ is $F_1$
this solves my problem. Thank you very much.
You are welcome :)

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