In mathematics, specifically in the calculus of variations, a variation δf of a function f can be concentrated on an arbitrarily small interval, but not a single point.
Accordingly, the necessary condition of extremum (functional derivative equal zero) appears in a weak formulation (variational form) integrated with an arbitrary function δf. The fundamental lemma of the calculus of variations is typically used to transform this weak formulation into the strong formulation (differential equation), free of the integration with arbitrary function. The proof usually exploits the possibility to choose...
@EmilioPisanty yes, it could still go in lots of different ways. BoJo wants to call a general election, but that needs to be agreed by parliament and the opposition have said they'll vote against it.
Plus as I understand it the motion was to ask for another three month extension in the event of no deal being approved, but the EU may not agree to another extension on the grounds nothing will change in three months.
But it's still good to see that mendacious scumbag get a kicking :-)
If I'm not fucking up, the final transformed action is something along the lines of $$S[\Phi(x)] = \int_{\Phi(t_a)}^{\Phi(t_b)} \dot{\alpha}(\alpha^{-1}(s)) \left[ (f'(x, s))^2 \dot{x}^2 + 2 \dot{x} f'(x, s) \dot{f}(x, s) + \dot{f}^2(x,s) \right] ds$$
And the end result should be $$\int_{\Phi(t_a)}^{\Phi(t_b)} \dot{\alpha}(\alpha^{-1}(s)) \left[ (f'(x, s))^2 \dot{x}^2 + 2 \dot{x} f'(x, s) \dot{f}(x, s) + \dot{f}^2(x,s) \right] ds = \int_{\Phi(t_a)}^{\Phi(t_b)} \dot{x}^2 ds $$
Obviously this works all fine for $f'$ a Galilean transformation and $\alpha$ a time translation
But showing that these are the unique transformations seems tricky
Wait is it even correct for a Galilean transformation
@EmilioPisanty It's because the fear is that BoJo will drag the election out to leave not enough time to sort out what to do before the Oct 31st deadline.
I wonder where on earth the negative sign in the third step comes from?!. The anticommnutation relations implies a positive sign since we have pair anticommutations
@JMac Sure, but there's a possibility of the OP clarifying that. Whereas if it is off-topic, then no amount of clarification or other editing will help.
@Slereah I tend to agree. OTOH, you could say the same about most questions asking about the various interpretations of QM. ;)
I'm solving a quantum mechanical problem, and the quantization condition requires me to solve the equation
$$
U\left(\frac12(\ell+1-E), \ell+1, r^2\right) = 0,
$$
where $U(a,b,z)$ is the confluent hypergeometric function of the second kind, $r>0$ is a fixed positive real number, and $\ell\geq0$ i...
@PM2Ring Right, but if I can't even really understand if question relates to physics, it's hard to actually say it is off topic, and not just a poorly worded physics question.
The last time I was here I had some funky Bessel function combinations and this package saved me. I'm afraid that with this one I won't be quite as lucky.
@EmilioPisanty This is way out of my league, but I suspect that if Mathematica can't handle it, things may be grim. Does it help if you use more precision? In Python, I use mpmath for arbitrary precision maths. It's got some good root solvers, and it supplies a bunch of hypergeometric functions. mpmath.org/doc/current/functions/hypergeometric.html
If the charge conjugation is defined as $Ca_pC = b_p ; Cb_pC = a_p$
How to prove that $\overline{\psi} \gamma^{0} \psi$ substracts the infinite constant that appears from anticommutation relations of creation and annihilation operators?
@Slereah in Landau they say that Galileo is the most general "additive" symmetry group (I assume this means linear), but no comment on non-linear and I highly doubt they are not in there!
What it means is that charge conjugation sends $\psi$ into $\overline{\psi}$ (i.e. interchanges particles and anti-particles) but in bilinears it does not interchange the order of creation and annihilation operators, so it wont force you to correct any expressions using anti-commutators the way you do around 3.113 when you get that infinite constant. What it then says is that if you defined your fields initially so that this constant never appeared, it will not suddenly appear
@JohnRennie I think I've turned it into a mania :(
I want to find the most unique, good name, that there isn't anything similar to it, but I guess it's not possible.
@JohnRennie My father's words.
I thought of a few other names but there are similars to them as well.
I've read in sites that it's important for me to be happy with the name, but I feel like I'll never be happy as long as there are similar names to mine. What do I do? :(
in appealing to that, I have in mind: fix some $r$ and $l$ (say, $r$ in the vicinity in the zone of bad behavior and $\ell=0$) and see how $U$ varies with $E$
@enumaris makes sense. I do think mathematica is running into trouble because its numerics are not able to properly approximate HypergeometricU in that regime due to it being oscillatory with growing amplitude
Dividing by 1/Gamma should tame that, but it doesn’t seem to work
i nevertheless think that’s the right thing to do. It just may be necessary to do some more massaging to get that ratio in a form which Mathematica is numerically comfortable with
Hence why I was looking at some of the transformation properties. But finding info about U(a,b,z) for integer b is remarkably annoying
I've talked to some guys on an entrepreneur forum and I'm proud to say that I've settled on Anastir. I really shouldn't put so much time and energy on the name, when I actually have a unique, easy to write, easy to say and not-taken one.
@JohnRennie I bought coin holders and put water with NaOH and TiO2 particles but the particles seem to stick to the container and I can't see what's going on. What do I do?
@JohnRennie How can I test for a magnetic field storing another magnetic field in the form of a magnetic field inside itself? I am wanting to carry out an experiment to test for that.