Conversation started Nov 10, 2016 at 6:22.
user116211
Nov 10, 2016 06:22
Anyways, I was reading about how the set of column matrices of an $n\times n$ invertible matrix over field $F$ spans all the column matrices $F^{n\times 1}\,.$
I'm not playing this game with you @SirCumference.
I'll just use the ignore feature, temporarily.
@DanielSank I'm not being pedantic
I just think it's going to die out soon enough on its own
@MAFIA36790 Yeah ok.
user116211
Nov 10, 2016 06:23
Let $P$ be the concerned invertible $n\times n$ matrix.
@MAFIA36790 ok
@MAFIA36790 Do you understand geometrically why that's true?
It's actually quite intuitive!
user116211
Then $P_1, P_2,\ldots,P_n$ forms the basis of the concerned vector space.
user116211
$P_i$ is the $i$th column of $P\,.$
user116211
@DanielSank Well, the author proceeded to prove it but mentioned no geometrical significance, I fear.
user116211
Anyways, then he wrote the product $PX$ where $X$ is a column matrix as $$PX = x_1P_1 + \ldots + x_nP_n\,.$$
user116211
Nov 10, 2016 06:27
This is what I'm not getting.
user116211
Won't the product be $P_1x_1 + \ldots+ P_nx_n\,?$
Hello. Does anyone know why people (even physicists) refer to Weak interaction as the fourth type of interaction along with Gravitational, Electromagnetic, and Strong? I mean isn't the electro-weak unification a standard established piece of today;s Physics?
user116211
What is going is this:
user116211
$$\begin{bmatrix}P_1 & \ldots& P_n\end{bmatrix}\cdot \begin{bmatrix}x_1 \\ \vdots \\ x_n\end{bmatrix}\,.$$
user116211
@DanielSank, any insight?
Nov 10, 2016 06:32
@MAFIA36790 How does that differ from the author's expression?
user116211
hmm.
user116211
I don't know but why he would write in that way.
@Dvij History. Lots of terminology used in science is very stupid if you think about it, but people use it because of history.
@MAFIA36790 How is $x_1 P_1$ different from $P_1 x_1$?
Scalar multiplication is commutative.
user116211
Okay!
user116211
I forgot $x$ is scalar.
Nov 10, 2016 06:36
@MAFIA36790 let me know if you want to talk about the geometrical way of thinking about matrices.
user116211
@DanielSank, Isn't every element of a matrix an element of a field? I mean field of complex numbers; they are scalars; aren't they?
@MAFIA36790 Yes.
user116211
Suppose $AX = Y\,.$ Then $y_i = A_{i1}x_1 + \ldots+ A_{in}x_n\,.$
user116211
You can't write $y_i = x_1A_{i1} +\ldots+ x_n A_{in},$ can you?
@MAFIA36790 Of course you can.
$$A = \left( \begin{array}{cc} 3 & 5 \\ 1 & -1 \end{array} \right)$$
$$X = \left( \begin{array}{cc} 2 & 4 \\ 8 & 16 \end{array} \right)$$
$$y_1 = 3 \cdot 2 + 5 \cdot 8 = 2 \cdot 3 + 8 \cdot 5$$
@MAFIA36790 Wait a second.
What does $y_i$ mean?
Your notation is inconsistent.
user116211
Nov 10, 2016 06:47
$i$th row of $Y\,.$
user116211
@DanielSank Sorry, I should have mentioned that.
What is x_1?
user116211
$i$th row of $X\,.$
user116211
@JohnRennie morning.
Morning
Nov 10, 2016 06:49
The statement to remember is $$Y_{nm} = \sum_i A_{ni} X_{im}$$
user116211
@DanielSank Correct.
That defines matrix multiplication.
user116211
yes.
soooo
I don't understand your question.
user116211
In a nutshell, I'm surprised as the author switched the position like saying $Y_{nm} =\displaystyle \sum_i X_{im}A_{ni}\,.$
user116211
Nov 10, 2016 06:57
Matrix multiplication is not commutative, as everyone knows.
@MAFIA36790 If that's all the author did, it's just silly, but not wrong.
$$X_{im} A_{ni} = A_{ni} X_{im}$$
user228700
Man, I do not get springs >.<
[Example of circular logic] I want the feeling of hopelessness to feel the pain of the feeling of hopelessness itself, so it will stop bothering me by making me to feel hopeless, which is painful.
user116211
@DanielSank okay.
@Kaumudi Hi.
Bonjour, Monsieur LeRennie.
That "R" sound is just delicious.
user116211
Nov 10, 2016 07:12
@DanielSank yes, I would surely love to; but let me complete what the author has to say.
user228700
@DanielSank Ello :-)
user116211
Got it; that's easy.
user116211
If you have time @DanielSank, you can go.
user116211
They first proved, the set is linearly independent; then they showed why it spans $F^{n\times 1}\,.$
@Kaumudi Hookes law? You've done much harder stuff than that ...
Nov 10, 2016 07:21
@MAFIA36790 Imagine you live in a 2D plane.
user116211
done.
On that plane there is a set of coordinate axes.
user116211
okay.
user228700
@JohnRennie Hooke's law isn't so bad. It's when I've to deal with springs attached to blocks, performing S.H.M >.<
Those axes could be thought of as a set of vectors $$\left( \begin{array}{c} 1 \\ 0 \end{array} \right) \qquad \left( \begin{array}{c} 0 \\ 1 \end{array} \right)$$
user116211
Nov 10, 2016 07:23
okay.
@Kaumudi SHM is easy, and the spring is just an excuse to introduce the type of force required for SHM.
Now, suppose you have a matrix $A$ with components $A_{ij}$.
What do you get if you act $A$ on the first coordinate (basis) vector?
user228700
@JohnRennie Yeah, but I'm finding it difficult to internalize everything that's happening when there are multiple springs and blocks and what not.
@MAFIA36790 you dead?
user228700
It's very interesting and all, but it's a little difficult :-|
user228700
Nov 10, 2016 07:31
@JohnRennie: Are u especially busy at the moment? (Or are u just drinking coffee and chilling? :-P)
user116211
@DanielSank sorry, connectivity interruption.
user116211
@DanielSank Order of $A\,?$
@Kaumudi no. Are you still perplexed by springs? :-)
@MAFIA36790 huh?
user116211
I mean $m\times n\,.$
user228700
Nov 10, 2016 07:33
Yep yep yep. I've an actual problem (and a crappy solution :-|) Maybe it will help to see how it should be approached..? (By superhuman geniuses like urself :-P)
@MAFIA36790 $2 \times 2$.
user116211
okay.
Ok let's see the problem ...
0
Q: Is it possible for $\nabla f=y\mathbf{i}-x\mathbf{j}$

ddjygdcis it possible for a function $f(x,y)$ satisfying $\nabla f=y\mathbf{i}-x\mathbf{j}$ ? Since $\frac{\partial^2 f}{\partial x\partial y}=-1$ and $\frac{\partial^2 f}{\partial y\partial x}=1$, thus $f$ should be singular. I find a similar answer in wikipedia "Symmetry of second derivatives", $f(...

Off to MSE with you
@MAFIA36790 I'm going to sleep, unless you want to go through this now.
user116211
Nov 10, 2016 07:37
$(A\textrm{Basis}_1)_{11} = A_{11}\cdot 1 + A_{12} \cdot 0 $
user228700
That looks straightforward ...
user116211
$\begin{bmatrix}A_{11}\\ A_{21}\end{bmatrix}$
user228700
Of course :-P
The system is symmetrical about the mid point, so you need only consider the motion of one block.
user228700
Nov 10, 2016 07:39
( ^ Sarcasm)
Anonymous
@JohnRennie did you mean centre of mass ?
Anonymous
or literally mid point ?
The mid point is the centre of mass
user116211
Am I right @DanielSank?
user228700
But $m_1≠m_2$
Anonymous
Nov 10, 2016 07:40
@JohnRennie But the masses are different
@S007 Oops, well spotted, I assumed the masses were identical :-)
Anonymous
@JohnRennie :-)
@Kaumudi as S007 says, find the centre of mass and put your origin at that point.
@MAFIA36790 Yeah
Right. What about for the second basis vector?
@Kaumudi I have something to do for the next ten minutes or so, but if you don't mind waiting I can go through the detail.
user228700
Nov 10, 2016 07:43
@JohnRennie I'll try and wrap my head around it while I wait...
user116211
$\begin{bmatrix}A_{12}\\ A_{22}\end{bmatrix}$
Very good.
user228700
Perhaps we should continue later...I need to do something else in 15 mins :-|
Notice this simple fact: The $i^\text{th}$ column of a matrix is simply the vector you get by acting that matrix on the $i^\text{th}$ basis vector.
user116211
yes!
Anonymous
Nov 10, 2016 07:45
@Kaumudi The question is simple....see this youtube.com/… will get it
Ok, so, think about what happens if we act $A$ on our pair of basis vectors.
We get two new vectors.
user116211
The sum of which is ....
Don't worry about the sum.
user116211
okay.
The point is that we start with two orthogonal vectors, and we wind up with two new vectors.
user116211
Nov 10, 2016 07:45
yes.
Now, what does it mean for $A$ to be invertible?
user116211
$A$ is row-equivalent to $2\times 2$ identity matrix?
$A$ is arbitrary.
If $A$ is invertible, then given any vector $v$ in the 2D plane, there is some vector $u$ such that $Au = v$.
@MAFIA36790 No, $A$ is not the identity.
user116211
yes.
$A$ is something arbitrary.
user116211
Nov 10, 2016 07:47
gotcha.
Ok, now...
Let's call the two basis vectors $e_1$ and $e_2$.
user116211
okay.
Suppose $v$ can be written as a sum of $Ae_1$ and $Ae_2$.
So, e.g. $v = \alpha A e_1 + \beta A e_2$.
user116211
yeh.
In that case, can you tell me what the inverse of $v$ is?
Uh, not the inverse... I mean the thing that $A$ turns into $v$.
"Inverse" is the wrong word.
user116211
Nov 10, 2016 07:51
$\alpha e_1 + \beta e_2\,?$
Exactly
So, it seems like we can always find some $u$ such that $Au = v$. All we do is write $v$ in terms of $Ae_1$ and $Ae_2$, and then the value of $u$ is obvious.
Right?
user116211
yeh, sure.
Ok! Now if that were true that we could always do this, then every matrix $A$ would be invertible.
user116211
yes, there is always a $u$ for which the relation, above, is true.
However, what happens if, for some $v$ we cannot write $v$ as a sum of $Ae_1$ and $Ae_2$?
For example, what if $Ae_1$ and $Ae_2$ are parallel?
Then there is a direction in which we could point $v$ such that $v$ cannot be expressed as a sum of $Ae_1$ and $Ae_2$.
...and so our strategy fails.
user116211
Nov 10, 2016 07:55
Then our assumption should be wrong.
user116211
@DanielSank yes.
So we see the following: we can't invert $A$ if $A$ takes the two basis vectors and makes them parallel.
Think of $e_1$ and $e_2$ as cutting out a square in the 2D plane.
user116211
yes.
Another way to say what I said above just now is "If the shape cut out by $Ae_1$ and $Ae_2$ has nonzero area, then $A$ is invertible".
Mew
Mew
@heather, what is it?
@S007, let me know when you're going to behave sensibly and we can chat
Nov 10, 2016 07:58
@Mew Yeah, that's a useful tone which is likely to encourage everyone to get along and make progress.
Mew
Mew
@DanielSank, he spammed the new site with foul language and offensive posts
most of it has been hidden by moderators
@Mew ok.
Mew
Mew
I don't think I need to be polite to him when he's showing this behaviour
Still not seeing how sarcasm is going to help.
@Mew I strongly disagree. This site has a "be nice" policy.
Mew
Mew
@DanielSank, even to those who are trying to destroy it?
Nov 10, 2016 08:00
This site's rules don't care about users' activities on other sites.
user116211
@DanielSank cutting a square? I'm failing to visualise :(
@Mew Yes.
Mew
Mew
well we aren't on the site are we and i'm not being mean
Mew
Mew
I'm just saying when he starts being sensibly, we can chat
behaving*
Nov 10, 2016 08:00
@MAFIA36790 see picture
Mew
Mew
and clearly he isn't behaving sensibly
user116211
@DanielSank got it.
Ok, so we've established that if the shape cut out by the transformed basis vectors has zero area, then the matrix is not invertible.
user116211
@DanielSank Yes, when they are parallel.
Another way to see why is like this: If the transformation enacted by the matrix squashes the basis vectors together, then there's no way to invert because a point on the squashed vectors could have come from either $e_1$ or $e_2$.
Let me know if that makes sense. It's a critical thing to understand.
user116211
Nov 10, 2016 08:02
Okay, I'm seeing what you wanted to mean by the geometrical significance.
Ok, @MAFIA36790 now there's one last point to make that's very interesting.
user116211
tell tell.
This whole reasoning works in any dimension. If we take a 3x3 matrix, then we could act it on the x, y, and z basis vectors.
user116211
yes.
user116211
That's very true.
Nov 10, 2016 08:04
If the action of the matrix turns the xyz cube into something with zero volume, then the matrix is not invertible.
Ok so far?
user116211
@DanielSank okay.
Now to the final point: do you know what a determinant is?
user116211
yes from high school; but haven't read it rigorously now.
user116211
It is in chapter 5 in Hoffman, Kunze.
user116211
And I'm in chapter 2: Vector Spaces.
Nov 10, 2016 08:05
ok ok
There is a particular number associated to each matrix called its determinant. Never mind how you compute it for now.
Here's the important thing to remember:
user116211
okay.
The determinant of a matrix is the volume/area/whatever of the geometrical object produced by acting that matrix on the set of basis vectors.
user116211
okay!
user116211
This is new to me!
SO! If the determinant of a matrix is zero, the matrix is not invertible!
If the determinant of the matrix is not zero, the matrix is invertible.
user116211
Nov 10, 2016 08:07
Yes, I know that.
But now you know why. It's because the determinant is the volume of the transformation.
user116211
Singular matrices has no inverse matrix.
If the transformation squashes the volume, then you can't find an inverse for any point in the squashed area.
user116211
@DanielSank yes, I didn't know about the geometrical motivation behind it; now I got the whole point.
 
Conversation ended Nov 10, 2016 at 8:08.