« first day (2512 days earlier)      last day (2713 days later) » 

user228700
01:30
Can anybody please help me with a quick question regarding total differentials? I am attempting to do a problem, stating:
user228700
> "The radius and height of a right circular cone are measure with errors of at most 2% and 4% respectively. Use differentials to approximate the maximum percentage error in the calculated volume"
user228700
This is how I worked it out:
user228700
user228700
The answer seems to be correct, but is the method also correct? I ask because my textbook has solved it a little differently than I have.
user228700
Do ping me if you have anything to say regarding this problem, thanks! :-)
01:35
The way seems correct to me @Kaumudi.H
the mathematical way is ok!
user228700
Ah, really? :-) Wokay, thanks!
Last night dream someone asked a weird question on PSE, and Leaky Lun's reply is as follows:
$$\sqrt{\frac{x}{y}}:\frac{x}{y\otimes \lvert 0\rangle} < \frac{y}{x\otimes \lvert 0\rangle}$$
user228700
Also, can anybody please tell me how it was possible for them to go from Step 1 to Step 2 in the following:
user228700
user228700
01:40
They seem to have differentiated all of the terms...but with respect to what, exactly?
Interestingly after I woke up momentarily, the second dream continued saying that only the reciprocals of the stuff in the inequality makes sense
@Kaumudi.H They are computing differentials, and presumably the functions f,v,u are all single variable
e.g. x
user228700
> computing differentials
user228700
Ah, erm, hmm, is that how we do it?
This kind of computation is common in experimental error calculations
it is part of the notion of total differential
user228700
@Secret Clearly, I don't have a firm understanding of this notion :-/
user228700
01:44
I will do some more Googling. Thanks :-)
note that if you simply compute the derivatives normally (hence having e.g. df/dx terms) then you are doing implicit differentiation, and then after you multiply it by some error bound dx, it will give you the errors of the function 2/f and the sum of functions 1/v-1/u
user228700
Nope, I did not understand that :-/
user228700
Specifically:
user228700
> and the sum of functions $1/v-1/u$
Ok what I mean is that $\frac{-2}{f^2}df$ is the error term to first order for the function $\frac{2}{f}$
01:48
@Kaumudi.H do you not know what a differential is
you compute the derivative then stick on a d(whatever)
user228700
> error term to first order
user228700
Huh?
user228700
@0ßelö7 Clearly not :-/
it won't make sense until a 5th course in calculus
user228700
:-(
01:49
maybe a 4th
or a 7th
idk
user228700
We don't follow the idea of set courses in a particular subject so I don't even know what a 4th/7th course in Calculus would entail.
something with manifolds
and $\frac{-1}{v^2}dv+\frac{1}{u^2}du$ is the error term of $\frac{1}{v}-\frac{1}{u}$

If your value of $f,u,v$ contains uncertainties (which is common in experimental physics), then the error terms shows the uncertainties of the functions $\frac{2}{f}$ and $\frac{1}{v}-\frac{1}{u}$
user228700
I...I see.
Each error term can be approximated by a taylor series, thus the linear term is what we called 1st order
and is given by the 1st total differential
01:52
I have no idea what you're on about
intuitively, you're just computing a small difference
so $df=f(x+dx)-f(x)=f'(x)dx$
etc.
yup and that's what we called a total differential
so d(dependent variable)=derivative * d(independent variable)
user228700
^ Right, this has been my understanding of this as well. OK, only sort of, but that understanding just widened to include the possibility of doing crap like this.
interpreting what that dx really means takes some work
@Kaumudi.H And if there are multiple variables you sum over the contributions.
user228700
Right.
01:55
and thus give you things like the multivariable chain rule
@Kaumudi.H that seems rather straightforward, what is the doubt?
I need to get chatjax on linux
user228700
I didn't realize that you could do this sort of thing even with implicit differentiation.
user228700
...now I do.
user228700
Sort of.
I'm the average stupid user
how the hell does chatjax work
user228700
01:57
Alright, thanks, guys :-)
ah, there
user228700
Calculus is exciting and also very, very weird, starting out.
I think calculus is one of those things where if you approach it from physics, you can understand the formal manipulations easily
the dirty proofs and rigorous definitions cannot be understood so easily though
but "calculus" just means the formal manipulations
Yeah, to get rigorous and justifying some of the concepts such as differentials such that it becomes analysis, a bag of machinery need to be introduced which is usually too much for average experimental physics and engineering uses
things like topology, continuity, limits, manifolds and so on
see, I don't think manifolds are fundamental to analysis
02:03
and to be frank, since I have not studied manifolds yet, I am not very familiar with differentials in a manifold setting
it pisses me off when analysis books stick in manifolds at the end as an afterthought
I guess... analysis don't need to always deal with non eucledian geometry, thus manifolds are not always included, but again I am not an expert on that...
analysis is the study of vector spaces that have topologies
well...and measures.
but disregarding that...
I'm so sick of UFO questions on astro SE
 
2 hours later…
03:46
@JohnRennie I need some heroin
fortran is killing me
They still teach Fortran in this day and age?
I suppose there are still millions of lines of Fortran in everyday use ...
it's pretty awful
the I/O is from the days when "print" meant "on a piece of paper"
It is if not one of the worst languages of all time then close to it
03:50
@JohnRennie behind cobol it is the best language for GDP
@0ßelö7 only because there is so much of it still around.
oh my god so many errors
fml
integer :: N_min, N_max, M
1
Error: Unexpected data declaration statement at (1)
how is that not valid, fortran
To be fair I believe the latest versions of the language are somewhat improved. I first used it in 1980 and in those days it was truly diabolical.
the errors make absolutely no sense
it doesn't like that I declared M to be an integer
why the hell not??
and it says I didn't declare a variable except I did in the line right above
sobs
@JohnRennie Jesus Christ, can I not declare inside of a case selector?
now it insists that i is square root of negative 1
what the HELL
04:08
@Kaumudi.H Yes, I'll certainly keep an eye open for the book. Do you know what it's going to be called, and the publication date?
04:28
@JohnRennie oh my GOD
one has to use the write command to change the format string for the print command
is suicide honorable when faced with fortran?
Might as well, it'll kill you anyway :-)
> ! Generate and show the dynamic formatting string
write(myformat, '("(", I3, "(I6))")') j - i + 1
print *, "Using formatting string: ", myformat
????????
is this supposed to make sense
05:13
ahahahahah I did it
@BernardoMeurer to get fortran to understand format = "(M(X2, I1, A, I1, A, I2))" I had to do write (format, '("(", I1, "(2X, I1, A, I1, A, I2))")') M and also limit format to 80 characters because FORTRAN puts an infinite number of blank spaces otherwise
worst language ever
but it works
@JohnRennie why does gamma equal 1+2/f?
where gamma = Cp/Cv is the heat capacity ratio of an ideal gas, and f is the degree of freedom
@LeakyNun Notice that $C_p = dU/dT$ where $U$ is the internal energy of a unit mol of the gas. By equipartition of unity $U = f \cdot RT/2$. Now differentiate, use $C_v = C_p - R$ and take ratio.
It's a formal computation. The crucial fact is equipartition of energy, which I never quite grokked.
05:29
why Cv = Cp - R?
That follows from first law of thermodynamics, if I remember right. Also I meant $C_v = dU/dT$.
Sid
Sid
A question: "it helps lexicographers to gain ____ to linguistic data". Should it be " access" or "insight"?
Access, surely?
Sid
Sid
I thought so too. Some of my friends claim it to be "insight"
Yeah. They are obviously wrong
@LeakyNun Yeah, if I heat up $V$ amount of gas so that the temperature increases by $dT$, and I counteract the expansion (say, volume increases by $dV$) of the gas by some exterior pressure $p$, then the total work is done by the force applied from the exterior is $pdV$. The internal energy increases by $dU = C_v dT$ (that's what specific heat means!), and the amount of heat we're applying is $\delta Q = C_p dT$.
Plug these in the first law of thermodynamics: $\delta Q = dU + pdV$ (modulo errors on my part).
Damn I remember these lol
05:42
hmm
equipartition of unity?
did you do too much abstract algebra lol
partition of unity is topology d00d
lol
$\delta Q/\delta T = C_p$
$\delta U/\delta T = C_v$
Well, the first partial is taken at constant pressure, second is taken at constant volume.
I don't see the relation between pressure and enthalpy though
why is Cp defined to be that?
You mean why we compute heat capacity at constant pressure?
05:53
I mean why Cp = dQ/dT
reiterate the definition of Cp
specific heat taken at constant pressure?
@LeakyNun heat capacity is always $dQ/dT$.
then what is dU/dT?
But at constant pressure the volume changes so some of the $dQ$ you put in goes into doing work instead of raising the temperature of the gas.
05:56
@Leaky I mean this comes from $H = mcT$
Just the infinitisimal version of that
At constant volume no work is done so all the $dQ$ goes into raising the temperature.
If no work is done $dQ = dU$ so $dQ/dT$ and $dU/dT$ are the same.
hmm
U=Q+W right
please, proper notation.
the 1st principle of thermodynamics is about 1-forms
stop using topology terms :c
"1-form" is diff geo not topology
06:01
its just symplectic topology tho
hm i wonder if nlab has anything to say about thermodynamics
AH it does
meh not interesting
where are the infinity categories
@BalarkaSen stop using those whatever category topology diff geo
This is one of the most rubbish answers I've ever posted and people keep upvoting it. That's the HNQ for you.
06:09
@JohnRennie are you asking for downvotes?
Sid
Sid
Jul 10 at 12:32, by Sid
@JohnRennie HNQ is the worst thing in SE unless I get rep from it. :P
@Mithrandir24601 I'm not asking for any votes, but I find myself faintly embarrassed by the whole thing. I posted it as a quick answer in between doing two things that I should have done several days ago. And now I find it's accepted and has 21 upvotes. And lots of comments saying it isn't an answer, which it isn't.
@Sid that's because I discovered I can exchange my rep for BitCoin :-)
06:39
(this may not be entirely true)
 
1 hour later…
07:49
I saw yesterday that heat capacity of a diatomic gaz rises up to 7/2R at high temperatures. Using the equipartition theorem one could very well explain 3/2 (translation) or 5/2 (trans. + rot.) but what are the additional dof from 7/2? I can only imagine vibration between them but would be only one additional dof, no?
@JohnRennie can you delete it and get yourself a shiny bronze badge?
In fact I can't delete it. Once an answer is accepted it's impossible for the OP to delete it. I'd have to ping the person asking the question and ask them to unaccept it.
@Felix.C each vibrational DOF contributes R not R/2
@JohnRennie I know, that's what I'm asking :) Translation, rotation and vibration are imho 6 dof's. So with the equipartition theorem this would result in 3R = 6/2R. But heat capacity goes up to 7/2R. So I wonder if classical mechanics has an answer for this
E.g. what is the 7th degree of freedom, if there is one?
@Felix.C in effect the KE and PE are separate degrees of freedom and you get R/2 for both
I think, though I wouldn't swear to it, that more precisely the vibration is a quadratic degree of freedom and when you work through the equipartition stuff you find these get twice as much energy as a linear DOF.
08:10
@JohnRennie Isn't it that ONLY quadratic dof's contribute to eq. theo. At least translation, rotation are quadratic and vibration are quadratic I guess. But PE seems to me as being no quadratic dof though...Thanks anyway for the KE, PE thing..this would explain it in some way.
Hmm, yes, I must be thinking of something else.
It's definitely the KE + PE thing though
 
3 hours later…
user228700
10:44
@JohnRennie Yes, it's titled "An Absolutely Remarkable Thing" :-)
user228700
user228700
<3
user228700
BTW, I am pleased to inform you that my USB adapter has stopped working, huzzah!
11:15
@Kaumudi.H Aha. Thanks :-)
Ah, it isn't listed on Amazon yet. I guess it's still too early.
@Kaumudi.H pish and tosh!
Let me see what I have in my pile of bits.
11:49
hey @JohnRennie care to dip into review for a minute? physics.stackexchange.com/review/low-quality-posts/189472
@EmilioPisanty Hmm, that's a rubbish answer. What are you suggesting? Vote to delete?
I did vote to delete and ... it's gone! :-)
@JohnRennie I was suggesting that you review as you see fit ;-)
on one hand, it's nice to see the 20k deletion ability actually pulling its weight
but, on the other hand, it is just you, me and Kyle on just about all of 'em
which is... less great
Deleting answers is somewhat controversial, but if I would be embarrassed to have someone I respect read an answer then I will vote to delete!
@JohnRennie Deleting salvageable answers is controversial, but I contend that the bottom of the barrel is not.
Agreed :-)
11:58
What we do need are self-correction mechanisms for when content is unduly deleted
Hi @JohnRennie
@Fawad Afternoon
I think my physics teacher was teaching wrong and I need some clarification from you
i.e. the ideal case would see the bottom-of-the-barrel posts deleted by a variety of different users (i.e. not just the same three faces every time), and a healthy population of people regularly checking the 10k tools for any deletions that cross the line
but we're not there yet
@Fawad Yes?
12:01
When certain charges are removed from x and put on y, final number of charge on x will be $1\mu-ne$ and final number of charges on y will be $1\mu+ne$ right?wrong?
I haven't used schrodinger formalism in a while so could someone maybe look over my Answer and warn me if I've given OP false info?
mornin
@Fawad: I calculate the initial force, the force before any electrons are moved, so be an attractive force of 89.9N. Do we aggree on that?
@JohnRennie yes. I got that. Let’s take approx 90N for easy calculation.
12:10
And for a force of 360N we need 2e-6C on each object
So you have to transfer 1e-6C charge from X to Y
@JohnRennie how?
@Fawad How what? How do we calculate the charge has to be 2uC?
@EmilioPisanty I'm not sure how many of our 10k users check the tools at all
@JohnRennie sorry I am dumbest person alive. I don’t get what you want to say
@EmilioPisanty Well... technically, everything you cast a delete vote on probably belongs in the VLQ review queue for one reason or another.
So the self-correction mechanism should simply be the VLQ review
12:15
@Fawad The question says the final force is 360N. Yes?
Yes. So final $q_1q_2=4*10^{14}$ @JohnRennie
$$ F = \frac{1}{4\pi\epsilon_0}{q_1 q_2}{r^2}$$ so $$q_1 q_1 = 4\pi \epsilon_0 r^2 F$$ Yes?
Yes
$$ = 4\pi \times 8.85\text{E-12} \times 0.01^2 \times 360 = 4\text{E-12} $$
+E don’t work with mathjax. 10^
12:21
I know, I'm too lazy to put in all the powers of 10 :-)
LOL
I am too lazy to type 'text'.
The point is that $q_1 q_2 = 4 \times 10^{-12}$, so $q_1 = 2 \times 10^{-6}$ and $q_2 = -2 \times 10^{-6}$
@JohnRennie :/
@Jasper at first I just typed the E-12 without the \text, but then I discovered it didn't format properly so I had to go back and put the \text in. It would probably have been easier to just use the proper notation :-)
When charge removed from x and put on y, they both have same amount of charge? (q1=q2=2*10^-6)
12:25
X starts with +1uC and Y starts with -1uC. So |q_x| = |q_y|.
@JohnRennie and while calculating final force?
Am I the only person who finds it funny that "Fawad" is asking questions about EM? x)
@Phase Yes, because r and w aren't that close :P
God damn it ACM stop ruining my fun :C
That was nice lol
12:27
@Fawad if we take a charge of $-e$ off X then X becomes more positive by $e$. So now q_x = +(1+e)uC and q_y = -(1+e)uC. The magnitude of the charges remains the same.
^^^^^^^^^ New favourite H bar member
Excellent timing John :D
Also, the pronunciations of the letter A in Fawad and Farad are different.
@Phase my, that's nice of you to say so :-)
@Fawad you appreciate awful jokes though, so you're good in my book
12:29
Are we doing electrostatics here or babbling aimlessly about puns on names?
3
@JohnRennie damn
Idk... is the stress giving you... indigestion..?
@Phase now there's a joke I haven't heard before :-)
@ACuriousMind well, that's what I've been saying all along, but the official position was always a stern "no"
particularly via @DavidZ
hang on ill try inventing a new one
but I don't think that the VLQ works as a review mechanism for deletions that already happened
12:31
@JohnRennie that’s what I wanted to know. Thanks :)
@Phase I've already heard all the jokes about my surname that are funny as well as lots that aren't.
tbh
What jokes ARE there besides the obvious
I can't even think of any
@JohnRennie I can't even think of one, lol.
The annoying thing is that it was my family that had invented the popular indigestion tablet I'd probably be a millionaire :-)
Yeah. If its any consolation my surname is pretty jokeable too
More so, even
"Peel"
12:36
Since we have descended to making jokes about µFawads and indigestion, now seems a good time to head off and get lunch.
@JohnRennie careful you don't eat too much and earn yourself some heartburn
Emilio Pissant-y
@Phase yeah, you're definitely the first one to come up with that one
although that joke sounds harsher than I wanted
RIP sorry Emilio
@Phase that too
12:38
Emilio Pi-santa
there we go
that's more friendly
It's a nice feeling actually finally contributing to this site instead of just being a tumour and asking tumourous questions
oh my god
the brits can't even spell tumor right?
nice bait mate
nevermind
Im still a tumour
I wrote that you find the eigenvalue, and then you can find the eigenfunction with the schrodinger equation
but that isnt right is it
The eigenfunction is the eigenvector that goes with the eigenvalue
So what's the solution to the SE? Just an eigenfunction OF the SE?
@0ßelö7 please help I want at least one constructive post on this site
busy
@Phase which SE? TISE or TDSE?
@EmilioPisanty This is my answer
12:49
and why do you think there's "the" solution to the SE, as opposed to "one" solution of the SE?
Well the solution is a family of functions for the infinite well of a certain form
@Phase yeah, I saw that, mostly I thought the question was too puddly to have an answer to begin with
@Phase solution to which equation?
ill just delete it
Solution to the TISE
@Phase I don't think there was anything wrong in there
Yeah but if its not a question that belongs on the site there shouldn't be an answer I guess
12:51
@Phase I don't think it's bad enough that it needs to not get any answers
well now I am torn
if your answer isn't wrong and it helps OP then I say sure, w/e
Can answers be undeleted at any point or are they dropped after a certain time since deletion?
though then again this is a good bit of word salad
> Consider the infinite potential well, The solution to this gives you the complex probability amplitude function which can be multiplied with its conjugate to give you a real function describing the probability of finding the particle at various points in the well.
> The energy eigenvalue corresponding to some pure Energy state now also corresponds to some eigenfunction solution to the differential equation, so you now have functions describing the probability of finding the particle dependent on the Energy state it's in.
it is? I thought it was all defined terminology
my understanding of word salad is meaningless words thrown together, I was just trying to keep it concise and have all the words be there for a reason
:(
12:55
@Phase you can undelete at any time, but deleted answers can become undiscoverable after a set time. If you have the URL you can always see it and if you can see it you can undelete it (if you deleted it yourself) but it will only be listed in your profile for sixty (?) days. After 10k rep you can search for your deleted posts though.
Fair. whats word salad about it tho
@Phase Mostly, I don't think it's clear enough to be useful. I still can't quite work out what you're trying to say.
Well, that the solution to the SE gives you a complex valued function that represents the probability amplitude, and you take $\psi \psi *$ to get the real valued function $P(x)$
And the second paragraph refers to states where the state isn't a sum of eigenfunctions / is only composed of one eigenfunction, and that that function is a solution of TISE that is related to its own unique energy eigenvalue [as long as it's not degenerate]
and wrapping it up by saying that those functions then describe the probability of the particle as a function of where in the box it is

« first day (2512 days earlier)      last day (2713 days later) »