This should be simple if it's possible, but how can I find the intersection of $y=x^3$ and $y=x^2 + x$? I factor an $x$ out of the second equation, then divide both sides by $x$ to obtain $x^2 = x + 1$ when I set them equal to each other. I get stuck there.
@user19405892 No. For some reason I forgot that finding the roots of that was the same as finding the intersection. And I have a calc II test tomorrow. I hope my brain isn't as fried then. (I've been cram-studying for 4 hours)
Thanks. I've got a solids of revolution test tomorrow and I'm trying to find the hardest problems I can so I'll be extra prepared... do you happen to know any good ones?
In a space, let $B$ be a sphere (including the inside) with radius of 1. Line $l$ intersects with $B$, the length of the common part is the line segment with the length of $\sqrt{3}$. Find the volume of the solid generated by rotating $B$ about $l$.
So it's a chord that intersects the sphere. I have to find a line rotated about a sphere. I'm not sure if I've got that level of knowledge yet; I've been using the disc/washer/shell method. I've heard of a cylinder method, but I don't know if that would help. I've been rotating about lines parallel to the x or y-axis, which would be a cylindrical body, I suppose. I guess I'd need something like $\dfrac{4 pi}{3}\int$stuff?$^3$. Is that close-ish?
I'm trying to prove that if $g \circ f$ (where $f: A \to B$ and $g: B \to C)$ is surjective, then $g$ is surjective.
We must prove that for any $y \in C$ there exists $x \in B$ such that $g(x) = y$. So let $y \in C$. Then since $f \circ g$ is surjective, there is $z \in A$ such that $g \circ f(z) = g(f(z)) =y. $ Letting $x = f(z) \in B$ we have $g(x) = y$. Therefore $g$ is surjective.
I meant "since $g \circ f$ is surjective" rather. Is it correct?
To find the distance from the center of the sphere, I was going to evaluate the semicircle $y = sqrt(1 - x^2)$ (from a 2D perspective) and solve for $sqrt(3)/2$. I got +/- $\dfrac{1}{2}$.
I just learned that when you said the sphere included the inside that it was a ball rather than just the surface area. Hmm. This is an interesting problem, but I might have to learn some more before I can tackle it.
It's more complicated if the 3-dimensional $c_1$ isn't torsion.
I mean this is the paper where he essentially developed Legendrian surgery and put Stein structures and tight contact structures on everything he could find.
@Mike
@MikeMiller The Milnor fiber has some nice facts about it that make this easier. I can write a similar proof for contact manifolds filled by a manifold with these facts, but $\Sigma (p,q,r)$ is pretty general (no idea if its true if you allow the contact structure to vary).
It's false for $\Sigma (2,2,2)$
Which is $\Bbb RP^3$ and is filled by the -2 trace on the unknot.
I don't have another Brieskorn example where its false.
each cycle is a function for instance (1,2,3) sends 1 to 2 ,2 to 3 , 3 to 1 and fixes 4 and 5. The multiplication is just composition. See what $\tau(i)$ is and what $\sigma(tau(i)$ is for each i between 1 and 5.
@PVAL My reasoning was that $\sigma = (1,2,3)(4,5),~ \tau = (1,5)(2,4)(3)$. So we wish to compute $\sigma \tau = (1,2,3)(4,5)(1,5)(2,4)$ since we can drop the $(3)$. Starting with the smallest number $1$ we have the first cycle sends $1$ to $2$, second and third fix $2$ and fourth sends $2$ to $4$. Next the first cycle fixes $4$, second sends $4$ to $5$, third sends $5$ to $1$ and fourth fixes $1$. So we close the bracket $(1,4)$ since we already have $1$. Is this wrong?
@PVAL Next, we pick the smallest number that isn't already in the disjoint cycle we have constructed. That's $2$. The first cycle sends to $2$ to $3$, second and third and fourth fix $3$. So we have $(2,3 \ldots)$. Next, the first cycle sends $3$ to $1$, second fixes $1$ , third sends $1$ to $5$. So we have $(2,3,5)$. Oops, so the answer is $(1,4)(2,3,5)$?
@PVAL I'm not asking you to check the computation. Just whether the answer I got using your method is correct (and I'll happily go back to the drawing board if it isn't).
Basically whether $(1,4)(2,3,5)$ and $(1,4,3)(2,5)$ are the same thing. (I'm a novice).
@MikeMiller: you said yesterday it's pretty obvious that the Laplacian is self-adjoint. did you really mean symmetric? I'm trying to show it's self-adjoint right now (in the manifold setting) and I'm comparing with what we've done in functional analysis (that was over $\mathbb{R}^n$) and it was quite a lengthy thing to do.
@MikeMiller: the proof we did required first knowing that the domain of the closure of the Laplacian is $H^2 \cap H_0^1$, we also need to know that under certain conditions $\| u \|_{H^{k+2}} \leq C \| f \|_{H^k}$ where $u \in H_0^1$ is the weak solution of the Dirichlet problem, we even required the trace operator. am I completely misunderstanding something here?
can anyone tell me what does that exactly mean by "function g is the convex envelop of the function f on a unit l_inf ball". I understand the part of "a function being the convex envelop of the other function" but what is the "on a $l_inf$ ball" means.
Consider the weighted undirected graph with $4$ vertices, where the weight of edge $\{i, j\}$ is given by the entry $W_{i, j}$ in the matrix $W$.
$$W =
\begin{bmatrix}
0&2&8&5\\
2&0&5&8\\
8&5&0&x\\
5&8&x&0\\
\end{bmatrix}
$$
The largest possible integer value of $x$, for which at least one short...
In a space, let $B$ be a sphere (including the inside) with radius of 1. Line $l$ intersects with $B$, the length of the common part is the line segment with the length of $\sqrt{3}$. Find the volume of the solid generated by rotating $B$ about $l$.
Any ideas about how to find the volume of this thing (I know what the figure looks like)
@user19405892 you should find an example of such a line, then show that (probably) every other line with this length is a rotation of this line, then calculate the volume with your sepcific example
@Huy: I think we're talking about self-adjointness in two different ways. I mean formally self-adjoint: in the $L^2$ metric on $C^\infty$ functions, we get something like $\langle \Delta f, g\rangle = \langle f, \Delta g\rangle$ rather trivially. When you're talking about self-adjointness I suspect you're talking about it with respect to the Sobolev inner products.
@MikeMiller: no. if you have a densely defined unbounded operator, you can define a densely defined adjoint operator. now an operator is self-adjoint, if it is its own adjoint AND the domain on which the adjoint is defined coincides with the domain on which it was originally defined. in general, the adjoint of a symmetric operator has a larger domain than the original one.
@MikeMiller: so what we did in functional analysis is was first to prove that one can extend the Laplacian defined on $C_c^\infty \subset L^2$ to $H_0^1 \cap H^2$ and then we had to prove that the adjoint of this extension again has domain $H_0^1 \cap H^2$
yes, I think formally self-adjoint is what we call symmetric
@Evinda No. Consider that argument for a circle $x^2+y^2=1$. The points $(1,0),(0,1)$ are in the line, but the line passing through those points isn't contained in the circle.
Does this stand only for groups of order $6$ ? Or do we have in general, for an even number $n$, that all the groups of order $n$ are the cyclic $\mathbb{Z}_n$ and $S_{\frac{n}{2}}$ ? @user19405892
Thinking about it again, $2i+bj$ is orthogonal to k for any b. This holds since i and j are both orthogonal to k , so also any linear combination of them, right? @DanielFischer
@MaryStar Basically the rule of classification of groups of order $pq$ a product of two distinct primes is this: If $p$ does not divide $q-1$, then there is only one isomorphism class of groups of order $pq$, namely, the cyclic group.
and
If $p$ divides $q-1$, then there are two possibilities: the cyclic group of order $pq$ and the semidirect product $\mathbb{Z_q} \cross \mathbb{Z_q}$ where $\mathbb{Z_q}$ is thought of as the additive group of integers mod $q$ and $\mathbb{Z_p}$ is identified with the subgroup of order $p$ in $\mathbb{Z_q}^*$, which is cyclic of order $q-1$.