oh. but anyway, $H_1(X, A) \to \tilde{H_0}(A)$ is the map obtained from taking a class $[z]$ and mapping this to $[\partial z]$, the homology class in $H_0(A)$ of it's boundary
write down the short exact sequence of triples, apply $H_\bullet$ functors and extend to long exact sequence by snake lemma, and then set $(X, A, B) = (X, A, pt)$
In mathematics, general topology is the branch of topology that deals with the basic set-theoretic definitions and constructions used in topology. It is the foundation of most other branches of topology, including differential topology, geometric topology, and algebraic topology. Another name for general topology is point-set topology.
The fundamental concepts in point-set topology are continuity, compactness, and connectedness:
Continuous functions, intuitively, take nearby points to nearby points.
Compact sets are those that can be covered by finitely many sets of arbitrarily small size.
Connected...
for example, $C_n(X)$ are free abelian groups generated by the simplices in a simplicial complex $X$, and $H_\bullet(\mathcal{C})$ is a good topological invariant for the simplicial complex. just like that, $H_n(X^n, X^{n-1})$ are free abgrps generated by cells in a cell complex $X$, and $H_\bullet$ of the chain complex of $H_p(X^p, X^{p-1})$ also gives us a topological invariant for our space
the interesting bit is that we don't need a simplicial structure anymore : just knowing a good cell structure (which is generally by far easier) does the trick
spectral sequences are like books, where the first page is about homology, second page is about homology of homologies, third is about homology of homology of homolgies and so forth.
and that's what makes them good tools : you have pages of informations about something instead of just one big nasty long exact sequence
but of course, this is what i understand, and i haven't even read about serre spectral sequences.
In differential geometry, the jet bundle is a certain construction that makes a new smooth fiber bundle out of a given smooth fiber bundle. It makes it possible to write differential equations on sections of a fiber bundle in an invariant form. Jets may also be seen as the coordinate free versions of Taylor expansions.
Historically, jet bundles are attributed to Ehresmann, and were an advance on the method (prolongation) of Élie Cartan, of dealing geometrically with higher derivatives, by imposing differential form conditions on newly introduced formal variables. Jet bundles are sometimes called...
Let $V=C^1([a,b])$. If $J$ is a continuous functional for the norm $\|\cdot\|_\infty$ then it is continuous for the norm $\|\cdot\|_1:= ||y||_{\infty}+||y'||_{\infty}, y \in V$. But the converse is false.
In my book there is the hint that we can use the functional of arc length, in order to show...
We can break an alternating sum into the difference of the non-alternating sum and twice the sum of the even terms:
$$
\begin{align}
&\sum_{m=1}^{2^n}(-1)^{m-1}(b-a)2^{-n}f(a+m(b-a)2^{-n})\\
&=\sum_{m=1}^{2^n}(b-a)2^{-n}f(a+m(b-a)2^{-n})
-2\sum_{m=1}^{2^{n-1}}(b-a)2^{-n}f(a+2m(b-a)2^{-n})\\
&=\un...
@robjohn is the best nick that I know (we dont know if exist a person, an IA or whatever under it xDDD). He is my best and bigger ultrafriend :D (metafriend is legit too)
In analysis it is just like saying that if i take two roads which are supposed to meet at a point and do actually meet then we will call that whole road continuous at that point@robjohn
But in topology we think in terms of open balls which are basically collection of points and if the value of the function in that ball is the subset of a ball with the center which is the function value at that point@robjohn
@Agawa001 Ah... just because I have a chat window open (which puts my avatar on the avatar bar) does not mean that that window is on top (so that I can see all questions). And if I see a question that is not posed directly to me that I can't answer at the time, I usually won't butt in :-)
@Rememberme Yes, and that is just the same thing as in the analysis definition. They are the same once you define the balls using a metric.
@Agawa001 okay... I just don't want someone to think that I was ignoring them just because I didn't respond.
@Rememberme That is pretty much the topological definition (inverse image of an open set is an open set) written in a form that resembles the analysis definition.
@Rememberme Suppose that for all $\epsilon\gt0$ there is a $\delta\gt0$ so that if $|x-x_0|\le\delta$ then $|f(x)-f(x_0)|\le\epsilon$. Suppose that we have an open set $U$. Pick a point $x\in f^{-1}(U)$. That is $f(x)\in U$. Since $U$ is open, there is an $\epsilon\gt0$ so that $|y-f(x)|\lt\epsilon$ means that $y\in U$. Choose the $\delta\gt0$ we have assumed for this $\epsilon$, then if $|x-y|\le\delta$, $|f(x)-f(y)|\le\epsilon$. That is, $f(y)\in U$ and therefore, $y\in f^{-1}(U)$. QED
That is, all points within $\delta$ of $x$ are in $f^{-1}(U)$ so $f^{-1}(U)$ is open and $f$ is continuous by the topological definition.
Hi @DanielFischer Could you explain me why the existence interval of $ \tan x$ is $(-\frac{\pi}{2}, \frac{\pi}{2})$ and not the domain of the function that is $\mathbb{R}$ ?
@evinda $\cos$ has zeros at $\bigl(k+\frac{1}{2}\bigr)\pi$ for $k\in \mathbb{Z}$, so $\tan$ has poles there. So if you want an interval in $\mathbb{R}$ on which $\tan$ is finite, it must be contained in $\Bigl(\bigl(k-\frac{1}{2}\bigr)\pi, \bigl(k+\frac{1}{2}\bigr)\pi\Bigr)$ for some $k\in \mathbb{Z}$.
$\tan$ is only defined on all of $\mathbb{R}$ if you let it take values in the real projective line $\mathbb{R}\cup \{\infty\}$ [note that $\infty$ is glued to both ends of $\mathbb{R}$, unlike $+\infty$ and $-\infty$].
@DanielFischer With : $\tan$ has poles there , do you mean that there are values of x for which $\tan x$ is not defined? Also, is $\tan$ finite in intervals, at which it has no poles? Or have I understood it wrong?
The sequence A023042 on the OEIS website shows that a large percentage of $N^3$ are a sum of three positive cubes. OEIS lists only N<1770, but we can extend that:$$\begin{array}{|c|c|}
N&\text{%}\\
2000&85.8\text{%}\\
4000&89.8\text{%}\\
6000&92.1\text{%}\\
8000&93.3\text{%}\\
10000&94.2\text{%}\...
@DanielFischer I see... So are we looking for an interval at which it doesn't hold that $\cos x = 0$ for any $x$?
@DanielFischer If so, then the interval of existence is the smallest interval of the form $\Bigl(\bigl(k-\frac{1}{2}\bigr)\pi, \bigl(k+\frac{1}{2}\bigr)\pi\Bigr)$ , $k\in \mathbb{Z}$ so that $\cos x$ never gets the value $0$. Or am I wrong?
@evinda These intervals are all equally long. It is convenient to consider the one containing $0$, however, so unless specified otherwise, that one is assumed.
a quick question, I need confirm (or refutation if I did something wrong) that this diophantine equation have no solutions: $$a^2+b^2=c^2+d^2\ ,\ a\ne b\ne c \ne d$$
this means that you cant caracterize different vectors only with euclidian norm... at least vectors of 2 dimensions (vectors formed only with natural numbers)
I was wanting a way to characterize isomorphic vectors that are composed of entire quantities on its coordinates
but, maybe, if I use a norm of dimension greater than 2 it may work (or not :p)
Construct and draw the streamlines of the velocity field $u=az-bt, v=\frac{b}{4}z-cy, w=2(a-1)$. Calculate $c$ (as a function of the constants $a$, $b$) such that the flow field $\overrightarrow{u}=(u, v, w)$ represents the flow of an incompressible fluid. Find also the pathlines of the element o...
According to Clique Percolation Method as shown in Wikipedia
I could not understand why the result of Graph1 is Graph2 if we assign k to be=2,
According to the definition of CPM, then the cluster resulting from cliques must be 4 cliques not only 2, because also :{2,4,12} and {8,9,13} is also max...