Theorem 2.4. For any connected smooth manifold, the following properties are equivalent: (1) M admits a Lorentz metric. (2) M admits a time-orientable Lorentz metric. (3) M admits a non-vanishing vector field X. (4) Either M is non-compact or its Euler characteristic is 0.
"(1) ⇒ (2) (The converse is trivial.) The time orientable double covering ( ̃M, ̃g), satisfies (3) and hence (4). So, the latter is satisfied obviously by M."
@0celo7 Well, the formal answer is, they aren't "defined" at all: A manifold is by definition a topological space that fulfills some extra conditions. But it is true that the topology is generated by the (pre)images of open sets in $\mathbb{R}^n$ under some chart.
Assume a certain action $S$ with certain symmetries, from which according to the Lagrangian formalism, the equations of motion (EOM) of the system are the corresponding Euler-Lagrange equations.
Can it happen that the equations of motion derived by this procedure have different kinds and/or numb...
"The antisymmetric part of the Christoffel symbols will not contribute here in any case, but the torsion will change the symmetric part (and thus invalidate the conclusion that extremal length paths are geodesics) if and only if $T_{cab} \neq T_{[cab]}$."
> The other is the source of the name (as I understand it): a “shortest possible path” between any two of its points (or more generally, an “extremal length path” between them). In the presence of torsion, these two concepts need no longer be equivalent
The contorsion tensor in differential geometry expresses the difference between a metric-compatible affine connection with Christoffel symbol and the unique torsion-free Levi-Civita connection for the same metric.
The contortion tensor is defined in terms of the torsion tensor as
where the indices are being raised and lowered with respect to the metric:
.
The reason for the non-obvious sum in the definition is that the contortion tensor, being the difference between two metric-compatible Christoffel symbols, must be antisymmetric in the last two indices, whilst the torsion tensor itself is...
OK, then. Someone who doesn't understand first semester basics about the centripetal force has been bothering us with endless questions about his efforts to overthrow the current understanding of large scale cosmology. Nice.
@0celo7 In the sense that your buddies, even casual ones, pass casual insults just for the hell of it. I don't know you well enough to hazard a guess about your inner self.
OK, then. Someone who doesn't understand first semester basics about the centripetal force has been bothering us with endless questions about his efforts to overthrow the current understanding of large scale cosmology. Nice.
The reason I said "not me" is because I thought the first few words were about me or something
@0celo7 Donald has been trying to overthrow big bang cosmology for the last few months. But it seems he would have struggled on the test I gave last week.
Of course, my class struggles, too. So he'd have been right at home.
Several times when you engaged in seemingly pointless rounds of minor insults with other users. Or should I have taken them seriously and move in with my moderator nightstick?
This is my problem: The bungee jumper jumps to the water from the bridge that is 24 metres high... First 12 metres of the fall the cord is not extended, it is only the free fall... The next 12 metres the cord is extended and the total fall is 24 metres, so the jumper falls in a way that he almost touches the water... The weight of the jumper is 60 kg. What is the maximum speed that the jumper attains during the fall?
The maxim speed is reached after falling more than 12 metres because the speed is growing as long as the downward force of gravity is greater than than the upward force of extension of the spring. F = m*a , m*g - k*Δx = m*a . The speed stops growing when a=0, when those two forces are equal. At this moment the jumper attains the maximum speed.
The thing is that I don't know how to calculate this maximum speed.
@bolbteppa : I know plenty of maths. IMHO what's important is to understand what the terms really mean. If you've ever seen any of my stuff you can see how I've looked hard at things like E and m and c and C. As for rotation and reflection, please provide a link and I'll comment.
I see 0celo on a downward spiral :\ linear algebra is a tough subject, would drive anybody down that road, even moreso if they had been studying string theory 2 months before
Well I did a math course so that the time would come when I could learn physics at the best level without math holding me back, so it's a good idea if you are willing to wait 2 years
But I did not go off studying string theory books without real analysis or linear algebra, which is like the biggest sin a student could commit in my eyes
@Secret I find it's very helpful at times, but I'm always conscious of that Feynman warning where he says math might ruin everything haha
@JohnDuffield your profile here science20.com/profile/john_duffield (not working for me at the moment for some reason) says you don't know much math, even the stand up physicist guy was admonishing you on that site, personally I would take it as a sign I may be doing something wrong hehe
@JohnDuffield But you say you've tried hard to understand energy $E$, do you know how to write down the energy in special relativity from a Lagrangian?
I'm not trying to catch you out, merely trying to convince you to study math more thoroughly, and better physics books than the ones you've read
"Something of an analyst and logician, well read on physics, but maths relatively weak and technically an amateur."
I am trying to illustrate the relationship when you add an odd number to an odd number, and even number to an even number and an odd umber to an even number
It's just something that pops up when I am procratinating because of being frustrated too much by some matlab code
we know that odd+odd=even even + even=even odd + even=odd
I am just jotting these out some some kind of map or graph or something
probably, I am just curious on what operations lead to where
Let's use a london subway map as an analogy, what I am doing above is trying to construct something like a guide so that I can see where and how I get to places
Becuase I have a tendency to like to make "roadmaps" of mathematical objects, and then start doing some extra things to it
I didn't say I have a clever analogy, I am just saying how I think about it. I don't force people to use them, and I am actually pretty dumb
or am I still making That Mistake?
I could have jsut say I want to make a map for mathemtical objects for myself to explore it, but I cannot say that because maths peopel here will think I am talkign about maps as defined in mathematics
Sometimes I just don't have enough volcabulary to express what I am trying to say