#linear-algebra
2 messages ยท Page 215 of 1
i just can't make sense of the questions
Yeah my teacher just said to ignore the eignevalues ddef, and just find where the matrix in not invertible
bruh

well your teacher's definition is wrong lol
so you should definitely ignore it
yea i thought they did what you said R2T2, but whats going on with the 1+lambda there lol
imagine teaching a linear algebra class and messing up the definition of "eigenvalue" 
So then for part b does my work look good?
how did you get span (1, 1)?
That part I messed up on, it shouldn't be there
But besides for that is everything else good?
uh
part a is correct
part b is not
this is fine but i don't know how you went from this to span (1, 1)
Than what would the span be?
Idk how i would find the span from this
wait
i might be high
give me a moment to make sure im not lying to you lol

okay, nevermind, the image will indeed be span (1, 1). for the image is the span of the columns of A, and it's clear that that's span (1, 1)
i got my rows and columns mixed up, sorry
you're correct, but a few words of explanation of how you went from the picture i posted, to the span being span (1, 1), would help
Okay, ๐ how would I explain it though?
"the image is the span of the columns of A"
short and sweet
Also would I need work to show how I got span of [1,1]?
if you quote this then there's basically no work to be done
if you wanted to prove it directly
show that every Tx is a scalar multiple of (1, 1), and that every scalar multiple of (1, 1) is of the form Tx for some x
the amount of detail you should put into this really depends on what you've learned so far
ok thank you so much
no problem, and sorry about the confusion
i got my rows and columns mixed up earlier this week too 
Hi I am a beginner at vectors. I came across this problem
the answer says "|D| is the distance"
but distance from what?
it does not make sense to me.
I do not think that is true.
me neither, i'm checking it now
I mean a plane is (x-x0, y-y0,z-z0) dot (A,B,C)
so isn't d just -(Ax0 + By0 + Cz0)
what is "distance" the textbook is referring to?
$|D| = |(A, B, C) \cdot (x_0, y_0, z_0)|$, where $(A, B, C)$ is normal to the plane, and $(x_0, y_0, z_0)$ is some point of the plane. if $|(A, B, C)| = 1$ (for simplicity), then $|D|$ equals the length of the vector projection of $(x_0, y_0, z_0)$ along the normal $(A, B, C)$. hence, $|D|$ is the distance in which we have to move the plane through the origin $${Ax + By + Cz = 0}$$ in the direction of the normal $(A, B, C)$ to reach the original plane. (the sign of $D$ is meaningful, but here it's asking for $|D|$ so we can ignore that.)
R2T2 โ
it's been a really long time since i've thought about this kind of stuff
at least 3 years 
hmmmm, thank you very much
I will look over it
and I think you're right.
it makes sense! thanks
๐
this argument also works in two dimensions, if you replace plane by line
easier to draw convincing pictures then
i think this is it..?
Frank
oh, should have noted that omega(v', w' - w) = 0 by antisymmetry
is this tilde omega map basically the bilinear version of
they do be looking really similar
let me think about it
@spare crystal you have the right idea, but your middle line is a little off
i think
it doesn't feel right

but yeah, writing v as v' + v - v' and w as w' + w - w' is good
the terms with either v - v' or w - w' (or both) in the arguments of \omega vanish, leaving omega(v', w')
i wouldn't be too surprised if this was a special case of that, in a way. since $\omega\colon V \times V \to \bR$ is alternating and bilinear, it factors through $\wedge^2V$ to a linear map $\wedge^2V\to\bR$
R2T2 โ
maybe the kernel of this is related to the null space i defined earlier?
maybe not
how does one carry out a change of coordinates in the projective space?
specifically here
they move 1,1,1 to 1,0,0
not sure how
(X1, Y1, Z1) = (X, Y - X, Z - X)
I imagine. Then X = 1, Y = 1, Z = 1
Am I missing something because projective space? Haha
no
one sec
Is it just that we solve for all the m's
that would put them in terms of X' only?
or we choose coefficients for a convenient transformation?
can you explain me this
this fits better in #advanced-analysis
<@&286206848099549185> could someone help me out please?
what is the difference between a redundant system and a square system of linear equations?
someone else more qualified can correct me, but it looks like theyre doing a substitution x=Px'.
this is sometimes used to diagonalize things. like if A=PDP^-1 then the substitution x=Pu can turn x'=Ax into u'=Du once you multiply by P^-1.
cant say for sure though
what is a redundant system? like a system with linearly dependent equations?
according to google, it's a system in which at least one equation is "redundant", i.e. linearly dependent
idk what you call a "square system of linear equations" either
that's kinda weird terminology
redundant kind of makes sense i guess
square system of linear equations i assume means like Ax=b where A is square/nxn
maybe, yeah. but idk if they also imply that the system is solvable with that name
yea
so if i have a mxn system, there could be a redundant equation in there
yeah
good
theyre not mutually exclusive though
do you know what are fill ins in an upper triangular matrix?
after QR factoring the coefficient matrix and applying linear transformations to them, i'm supposed to get fill ins
but i have no idea of what they are
and how to reduce the amount of them in order to save computation time
sounds like it means it alters the structure
you start with an upper triang mat, but the decomposition can yield 2 dense matrices with all entries nonzero
they could be, yeah
what does that mean? being dense...
wait, lemme re read what structures QR uses
Q = orthogonal matrix (orthogonal to what?) R = upper triangular matrix
Orthogonal to nothing

Orthonormal matrix is also a term used for it
which linear transformations do you mean here?
applying transformations to Q and R as in multiplying them by some other generic matrices?
because multiplying R by another generic matrix will in general not be upper triangular
sorry
not linear transformations
i meant the fill ins that appear in the upper triangular matrix that is a product from the QR factoring of the coefficient matrix
coefficient matrix is a sparse matrix in it's augmented form
i have no idea what those 'fill ins' are
what do you mean by augmented form
i'm asked to symbolically determine the amount of fill ins in the upper triangular matrix.
i don't see how augmenting it would affect the sparsity, but ok
the matrices Q and R are in general not sparse
it doesnt
i'm saying the matrix A, which i want to QR factor, is sparse
yep
in general, Q and R aren't sparse
that's what they mean by "fill in"
and the opposite of a sparse matrix is a dense matrix
a matrix with all/almost all entries nonzero
but how to symbolically determine the amount of 'fill ins' in the R matrix?
i still don't understand what is meant by 'fill in'
it refers to nonzero entries in R that were originally zero in A
@lavish jewel do you know matlab scripting? i have a script here that would probably help me understand what i'm asking you if i were to understand what the script does
i do know matlab, but i'm about to go to sleep
ok
you can just read page 6 in that for a quick intro
but the idea is that A is sparse because it has a lot of zeros
THANK YOU
yep
fill in refers to the factor matrices having nonzeros where A or A^TA has zeros
ohhh
as to how exactly find the worst case fill in, i don't know the algorithms, but they should be a quick google search away for common decomps like QR, LU, and cholesky
this is exactly the type of answer i was looking for
assuming this is the matrix R
would inputting the command 'sparse(R)' reduce computational times?
it's the upper triangular matrix after applying Tinney-2 ordination
you'll have to read the flavors of sparse matrices in matlab
Is the MIT LA course by Gilbert strang recommended or is there something much better out there? I had a really bad lecturer this semester and honestly didn't understand anything.
wym flavors
some of them do sparsity by indexing rows or columns with nonzero elements
neither of those help here
why?
because all rows and columns have nonzero elements
i like strang's content myself
1.) that's why you look for a matrix representation that is not ONLY based on either row or column indexing, and 2.) that's still pretty small
you'll have to check what exactly matlab's sparse function is doing
the more common ones in python only throw away rows or columns, as far as i recall
i know it uses the incidence matrix to index the non-zero elements
is that right? lol
maybe, i don't remember lol
also
the size of the matrix is relative
for electrical engineering applications (my case) i need an application that can work in near real time with an updating coefficient matrix
so optimization is crucial
ah, real time stuff
yep
could someone explain why row operations don't change linear independence without using using the notion of rank?
row operations are the same as adding a quantity to both sides of an equation
Thanks for replying but I figured it out thanks
it's still the same relationship between both sides of the equation
suppose $A$ is an $m$ by $n$ matrix. Row operations on $A$ can be thought of as multiplication on the left by $m$ by $m$ invertible matrices, called elementary matrices. If $E$ is an $m$ by $m$ invertible matrix and $v_1,...,v_n$ are the column vectors of $A$, then $E(v_1),...,E(v_n)$ are the column vectors of $EA$. to keep things brief, if the first $r$ column vectors of $A$ are linearly independent, then $E(v_1),...,E(v_r)$ are also linearly independent (since injective linear transformations take linearly independent sets to linearly independent sets) thus preserving the linear independence of the column vectors of $EA$.
coycoy
thanks
how do i prove that these are not a system of generators of R^4?
put them as columns of a matrix and do gauss jordan?
reduce it to row echolon form
Or rows
if the rank <4 it doesn't span R4
you already asked this. a solution was given in the book #help-9 message
U can prove using any of this
๐
ez way is find det
if det is non zero it spans R4
depends on dimention
yeah, me no likey, but indeed, several ways to show it
I'm just saying there are multiple ways
do what's convinient for u
and don't mind my spellings
you don't need to do gauss jordan, gauss elimination will do
Not really, if you reduce a matrix to an upper triangular matrix, the determinant is just the multiplication of the elements of the main diagonal.
u just need it in row echolon form
don't need to reduce it to reduced row echolon?
oh nvm
in this case
det will reduce to a 3x3 sub matrix
Also ( correct me if Im wrong ) if the determinant of a submatrix ( so a matrix in the original matrix ) is 0 then the det of the main matrix is 0.
Im not sure about this tho.
I don't think so, but I'm unsure
I dont know how to search this up in google lmao
Yup
yeah
yeah, that sounds like you could apply it recursively
so any matrix with a 0 would have det 0
its just not even true in trivial cases. two by two identity matrix has two minors that have determinant zero while the two by two identity has determinant one. similar situation with any n by n identity matrix
wwhat does this mean
does it mean,
$\frac{\partial}{\partial x^{\mu}B_{\nu \rho}}$
?
LolLol
this notation is common in physics. i think it means $$\partial_\mu B_{\nu\rho} - \partial_{\nu\rho}B_\mu,$$ but i could be wrong
typo
TTerra
ah alright thanks bro
don't take my word for it
you should ask in the physics server
oh fair
differentiate wrt nu and then rho
ive seen this notation used in general relativity
Oh alright so its shorthand for $\partial_v\partial_p$
LolLol
im studying ssomething similar
im doing quantumgravity
im just not used to physics notations
the physicists will have an answer for you lol
cause im tryna use math for physics and it gives melike a panic attack
i just gave a wild guess as to what it means 
nah im sure ur answer is right
its for string theory
specifically quantum grav so u r correct
:p
check #old-network
physics server there
it's either that or some kind of sum of permutations of the indices on the brackets
Guys I'm new here and I have doubts in a specific question could someone help me?
just ask @marble sierra
I have this vector space
With the operations defined by
and need to determine the null vector of V
is that a vector space at all though?
it doesn't even look closed under addition
(0, -1) + (0, -1) = (0, 1) as defined here, and (0, 1) is not in V.
The exercise stated that it is a vector space that's what confused me
then the exercise lied to you and should be skipped and reported to your professor.
ok thank you very much i will talk to my teacher about
hello
i am trying to find the limit of a sequence
or to prove that a sequence has a limit, rather
i don't really understand how to do it
you're probably in the wrong channel then
more fitting channels would be #proofs-and-logic, #calculus, and #advanced-analysis
oh thanks
@solemn tusk $$\partial_{[\mu}B_{\nu \rho]} = \frac{1}{3!}\left(\partial_{\mu}B_{\nu \rho}+ \partial_{\rho}B_{ \mu \nu} + \partial_{\nu}B_{ \rho \mu} - \partial_{\mu}B_{\rho \nu } - \partial_{\rho}B_{\nu\mu } -\partial_{\nu}B_{\mu\rho} \right)$$
Timon
it's called the anti symmetric part of the tensor
part of Ricci calculus notation
(in case it's not clear $\partial_{\mu}B_{\nu \rho} = \frac{\partial}{\partial x^{\mu}}B_{\nu \rho}$)
Timon
is that it? what have you tried?
ty for the correction, i was close enough lol
i figured it was something like a commutator of indices but that makes sense too

how would u solve this?
Nothing. I'm not confident I completely understand this.
that's not linear algebra, unless you don't know how to compute linear maps
I know that the answer is no, but I don't know why
I'm probably just being stupid, though
what are the requirements for a subset of a vector space to be a subspace?
(ie what does subspace test say)
...
That's what my text says
Check that it's closed on addition and multiplication
and one more thing
I may be forgetting this
naive test:
- ?
- Closure under vector addition
- Closure under scaling
what special vector has to be in the set for it to be a subspace?
Oh. Zero vector?
yes
That's what I thought
What's the set? P2?
the set you're determining if it's a subspace or not
Or am I checking if it fulfills the condition?
${a_0+a_1t+a_2t^2|a_0+2a_1+a_2=4}$
Mosh
right
is 0 in that?
So you're asking me if 0 + 2(0) + 0 = 4?
yes
No
So it's not a subspace
yes
It's that simple?
yep
Right
but here it's simply 0 isnt in the set
Does the zero vector follow from being closed under multiplication?
?
we already know the existance of the 0 vector due to it being a subset of a vector space, so either 0 is included or not included in the subset
if it's not in the subset, we cant call that subset a subspace
yes, if the set were closed under multiplication, it would contain 0. for if x is any element of the set, then 0x = 0 must be in the set
actually checking that the space contains 0 is always unnecessary
but it's quick enough and usually works that it's included in "subspace tests" anyways
how do you change you're nickname on the server
have active role i think
how to obtain said role
be active
who determines how active i am lol
me
Tim O'Brien
So this is what I did
but I feel like this is too elementary
How would I solve this with a matrix?
I am trying pretty hard to stop using baby algebra
I tried doing it with matrix stuff and it was just complete nonsense
Well, you can look at the determinant of {1,h,3,6} when it is zero, the matrix is not invertible
Sorry I don't know determinant yet
I just started today
I am slow learning alone :(
your method works, so thatโs all that matters
what is R/2 ?
yeah but I could have done this with the normal algebra I learned this year
I want to do new stuff
I am pretty sure it means "the set of real numbers minus 2"
Like all real numbers except 2
should be $h \in \bR \setminus {2}$
111211211111221312211
Well, for this problem you canโt get too highbrow, but another way of looking at it maybe is that when the two coolumns of the matrix are linearly dependant, you canโt get every value when you multiply by some column vector, the answer will just be a constant times one of the column vectors of the matrix
Column, like the column of a matrix
I don't have the best understanding of this
But I will learn it I guess
I know linear dependence is when two vectors can only make one line
Yeah, i think it will make sense later
when multiplied by scalar
I am not picking up how columns work
I know rows are equations
The column of a matrix, say {1,3} in our case, is a vector
No donโt worry about this for now
When did you start linear alg?
Yes
I started like 1 week ago watching videos on khan academy
But there wasn't enough practice
so I downloaded a textbook pdf
that was today
I like the idea of matrices though
I see, then you donโt have to worry at all. This will all be there a little later. For now I guess you have to stick to the usual methods to do things though
OK got it
Something that excites me
I learned that you can put any data points in a matrix, like 3 variables describing one thing
and you can graph it to get a visual representation
that is super useful because a lot of times there are multiple variables that go into something, like damage, attack speed, and health in a video game
I hope I am not just saying nonsense; this is just waht I picked up today
yea linear algebra is really cool. im glad you're excited to learn about it. its one of my favorite subjects too
Not at all, this sounds like exactly the sort of thing linear algebra is good for
this is a question from my linear algebra course
mniip (owner) has a bot that tracks activity. it depends on the channel. for example, #chill messages count less towards the activity roles than questions channels
what about activity in #hentai
Tracked by god
Really?
I am doing Boolean Algebra for my Extended Essay over the summer
And I had no idea that it had something to do with matrices
I am just not a good researcher
Im pretty much terrible at everything I do XD
:c dont say that. ur doing great ๐ฅบ
wow. that is one fat raccoon
thanks!
is there a geometric interpretationof this @odd kite
pls ๐ฟ
like er for any
like what does the antisymmetric part MEAN.
I am supposed to find a Diagonalmatrix D and a Transformation Matrix P for the regular Matrix A for which I know all the Eigenvectors and Values
I know that I can use a matrix made up of the Eigenvectors with A = PDP^-1
but now i need to find one that fullfills A = PDP^T
so i gotta find P so that P^T = P^-1
define "regular matrix"?
inversible
just invertible, so all eigenvalues are nonzero, and that's it?
yup
hmm
i have a feeling that a decomposition into PDP^T may not always be possible, but don't quote me on this
ok so this is the thing https://cdn.discordapp.com/attachments/732592586803380314/856190750853562398/unknown.png
ah, so A is symmetric!
mb
then its eigenvectors for different eigenvalues will be orthogonal.
always? and for all eigenvectors?
yes. it can be proven by simple algebraic manipulation.
for P, all you need to do is normalize your eigenvectors so they have length 1.
and then i will have a matrix where P^-1 = P^T ?
hhhhm neat, I dont understand why but thats good enough
if you are ok waiting around 10 minutes i can walk you through the proof of what i mentioned
sure
another question. If I have a matrix with just orhogonal vectors in it I can do P^T = P^-1 always?
ok so length 1
My eigenvalues are 6 and 2
my iegenvectors are
$\vec{x}= \left(\begin{array}{c} 1\ 1 \end{array}\right)$
$\vec{x}= \left(\begin{array}{c} 1\ -1 \end{array}\right)$
Mergintaim
these should both be divided by sqrt(2) to normalize them
yeah was just about to say that
does the order play an importance?
lets say my d is
6 0
0 2
then the eigenvector for 6 would be at first column as well?
Yes
sweet
the order must match between P and D
Could someone explain Gauss reduction of quadratic forms to me ? In particular, I can't see the common point between the "classic version" (where you try to write q(x,y,z) as a sum of 3 or less squares) and the matrix version (where you basically do a gaussian elimination on both rows and columns on the matrix of the quadratic form)
It's bilinear algebra but I guess this is the right place anyway
thanks
Yo guys what is the point of linear transformations?
It took me a couple of re-reads to understand
But I fail to see how it's useful
wdym what's the point? you want like real world examples or something from the mathematical viewpoint?
Most (real) Systems of any kind, if you are into engineering
Schrodinger eqn in its simplest form
stuff like calculus operations and certain flavors of differential operators that show up differential eqs are linear
If you want to do physics or engineering, you will have to understand linear transforms
what is hodge star operator
Yes but how exactly?
Sorry to drag this on
Ask the physics people
And linear transformations
The important part
is the movement on the vectors righht?
it's not what happens to the xy plane
does that make sense?
xy plane is xy plane
I am watching a 3b1b video on it
and he keeps having the xy plane move with the vector
and it's lowkey confusing
the movement itself is not important
only where the vectors start and where they end
@forest quiver lets start super easy at an average level. Lets say you have some kind of Blackbox system that has 2 inputs and 2 outputs. If its linear you just need two Measurements to be able to formulate an equation for the relationship between the inputs and ouputs. This is because if you have linear systems you can use superposition because in the definition of linear it says f(x_1+x_2) = f(x_1)+f(x_2) and f(c *x)=x * f(x).
And superposition is every engineers wet dream. With this you can make a super complex problem insanely easy because you can just calculate the system for a specific input, then calculate for the next input and then just add them together.
lol this isnt starting "super easy"
Ok lets say you have this magic box
and lets say you put some voltage on the input
you will get some kind of output
and you do this again, for another set of inputs
So far you only know two pairs of inputs and outputs
But because the magic box is a linear system, or a linear transformation if you want to call it in math terms you actually have enough information to calculate the output for every possible input combination
imagine, if you will the inputs and outputs here as vectors
so for the inputvector (6,4) you get the output (2,-1), and for the inputvector (2,3) you get the output (3,2)
because we know this system is linear and the vectors (6,4) and (2,3) are linearily independant we actually have a base for our 2D-input space here
this is pretty neat because now we can write an equation for the output vector in the form of:
$a \cdot ( \begin{array}{c}6 \4 \end{array} ) + b \cdot ( \begin{array}{c}2 \3 \end{array} ) = \vec{O}$
Mergintaim
Before I get on my computer to get a better read at this, could you explain simply what exactly a linear system is?
A system that fullfiills these properties f(x_1+x_2) = f(x_1)+f(x_2) and f(c *x)=c * f(x)
And v_1 , v_2 are the base vectors of a vector ?
no v1 and v2 are just the inputs
Oh ok like a multi variable function
I see
6,4 and 2,3 are the base vectors of the linear transformation that is this system
the system is something "real" in the world. The linear transform is the mathematical model for it
yeah but for it to be linear it has to follow these rules. for example x^2 or e^x would not be a function that you would see in a linear system
Yeah and\
$\begin{bmatrix}
a\
b
\end{bmatrix}$\
Is where the vector ends up post-transformation right ?
Tim O'Brien
you can however pick a small part of x^2 and say its approxximattly linear in this sector with the approximation function blabla
a and b are just the scaling factors of the base vectors
you know how base vectors work?
Yeah
[ a b ] is the new vector
Let me read all this on my computer give me 10 mins
sure, [a,b] would be the new vector if you split the vectors to get the standard base vectors yes
so instead of $\begin{bmatrix}
6
4
\end{bmatrix}$\
Mergintaim
you would have
$\begin{bmatrix}
1
0
\end{bmatrix}$\
Mergintaim
This all makes adequate sense to me
Except for this part
The writing the equation
I think you mean c * f(x) ๐ญ
they wrote the O vector in terms of a different basis
that's all
since bases are not unique to the vector space
run through the axioms and find one that doesnt work
closure isnt a distinct axiom
o plus doesnโt have an identity

that was a lot of fun. you got any more?
is that sarcasm :(
probably not but thats just my guess
How would you go about proving that if W is orthocomplement of U then U is orthocomplement of W, where "orthocomplement" defined as:
orthocomplement $U^\perp := {\vec{v}\in\mathbb{R}^n\mid\vec{v}\cdot\vec{u}=0,,\text{ for all },,\vec{u}\in U}$ where $U$ is a subspace of $\mathbb{R}^n$
yes, that's where I'm lost
edit: wait no, W = U^perp by definition
I misread your answer
Commander Vimes
?
wait lol
Commander Vimes
Suppose $u \in U$. We want to show that for all $w \in U^{\perp}$ we have $\langle v, w \rangle = 0$
Commander Vimes
Commander Vimes
Commander Vimes
Commander Vimes
I can't use that, as that's what I need to prove next
in my problem
from U^perp^perp = U
@wintry steppe Let $V$ be an inner product space with inner product $\langle\cdot,\cdot\rangle$ and $\dim V=n$. Recall that if $U\subseteq V$ is a subspace of $V$, then $$U^{\perp}={v\in V:\forall u\in U:\langle u,v\rangle}$$ and $$(U^{\perp})^{\perp}={v\in V:\forall w\in U^{\perp}: \langle v,w\rangle=0}$$
If $u\in U$, then we have $\langle u,v\rangle =0$ for all $v\in U^{\perp}$, which by definition, implies $u\in (U^{\perp})^{\perp}$.
For the converse inclusion, let $\mathbf{u}=(u_1,\dots,u_r)$ be an orthonormal basis of $U$ (exists because of Gram-Schmidt). Extend this to an orthonormal basis $\mathbf{u}'=(u_1,\dots,u_r,u_{r+1},\dots,u_n)$ of $V$. Then consider the map $f:V\to V$ given by $$f(v)=\sum_{i=1}^{r}\langle v,u_i\rangle u_i$$
Hints would be to show that $U=\textnormal{im}(f)$ and $U^{\perp}=\textnormal{ker}(f)$. Then replace $U$ with $U^{\perp}$ and repeat the same process to get that $\textnormal{ker}(f)=(U^{\perp})^{\perp}$ and $\textnormal{im}(f)=U^{\perp}$. You should be able to conclude, with rank nullity that $\dim U=\dim (U^{\perp})^{\perp}$ and it should complete the proof, since $U\subseteq (U^{\perp})^{\perp}$.
coycoy
A represents a linear transformation that takes in component vectors w/r/t the standard basis for R^3 and gives out component vectors w/r/t the standard basis for R^3. I think [A]_B^B is the matrix that represents the same linear transformation but w/r/t the basis B you found.
So if f is the transformation,
$$[f(x)]_B = [A]_B^B [x]_B$$
Lunasong the Supergay
I might be talking shit, but idk what else it could be
so I just apply the transformation to basis B?
And then write the output in terms of B
I see thanks, I've only seen the notation with different basis
j-th column of matrix is image of j-th basis vector
Why is Option 2 correct, when it is clearly mentioned in the Question that Vector Space is non-zero.
Do you understand what a nonzero vector space is?
let a = 1.
- is true for any space tho
some off topic but I passed Lineal Algebra and wanted to shout out to everyone helping in this channel, you helped me a lot !
@delicate oxide nonzero vector space just means the vector space has nonzero vectors. It still has the zero vector. All vector spaces must have a zero vector.
Is the following true?
If a matrix $A$ is invertible, then it has an inverse matrix, $A^{-1}$.
Shen
isn't it part of the definition?
a matrix A is invertible if there exists a matrix B such that AB = BA = I
and B is referred to as A's inverse
I was just about sure this was the case, but I figured additional clarification would make me feel better - appreciate that
yes, existence of the inverse is the quintesential point of determining invertibility
that is the Tteppa
The matrix has columns T(1,0,0) T(0,1,0) T(0,0,1)
Yes?
Are you trolling me? 
Oh okay, dw
This works for any linear transformation
If T: V -> W and V has a basis {b1, ..., bm} and W has a basis W = {w1, ..., wn} then your matrix has columns [T(b_i)]_W where [ ]_W means the coordinate vector in terms of W
So here you just have the canonical basis
So you just check what each of the basis vectors get mapped to
T(1,0,0) = (2,0,0)
T(0,1,0) = (0,1,0)
T(0,0,1) = (0,0,1)
in the standard basis you can also think of this as multiplying T with the identity, and the resulting vectors are the columns of T*1
Then the matrix is
$$\begin{pmatrix} 2 & 0 & 0 \ 0 & 1 & 0 \ 0 & 0 & 1\end{pmatrix}$$
Lunasong the Supergay
To explain this, the i-th column of AB is A* i-th column of B. So let T be represented by matrix A. Then AI = A where I is the identity. So you can get the i-th column of AI (which is A) by multiplying A by the i-th column of I, which is the same as finding T(i-th basis vector)
I managed to do a
but in here, do I also have to prove that T is an isomorphism, or just that the inner products are equivalent, or both?
both. but bijectivity and linearity are almost immediate, so thereโs that
Be A nXn matrix , if A-3ฮป row are linear independant, what can you say about A?
is it Diagonalizable ? represent invertible matrix ? zero is not eigenvalue , or none of those?
what are you're thoughts on this ?
i think none
why do you say that ?
A - mu I is certainly invertible, where i just take mu = 3 lambda.
why?
its rows are linearly independent
oh wait it should be "represent invertible linear transformation "
i might be making myself look like quite an a**hole right now. you are right. it is none. sry about that
if i want to show that two vectors are parallel then i have to show that they are collinear right? i.e one has to be a multiple of the other, but for which a is this the case here? if i let k = -2, then i have that the first vector is equal to (2, -2a, 4), but this contradicts the other side
nah its my fault i forgot important note..
cannot read your writing
its k * (-1, a, -2) = (4a, 1, 4)
use cross product instead of scalar multiples
$a,b\in\mathbb{R}^3 \ a\parallel b \iff a\cross b =0$
Mosh
i dont think such an a exists. you have solved for k, since you have to have -2k=4 which gives k = -2. then from the second row you need -2a = 1 so a = -1/2. but from the first row you have 2=4a so a = 1/2...
yeah this is what i came across aswell
sorry, we didn't cover cross products yet
ok then yeah, check if you get a solution to those 3 equations, if not then no a exists
Is it possible to get a matrix representation for T here? I'm stumped on how to start with this one
V is infinite dimensional (most likely) so no
also it's not even obvious what a basis of V should be
what are you stumped on? can you recall the relevant definitions (linear, surjective, injective, and eigenvalue)?
I can recall the definitions, I'm just not sure how to solve this infinite dimensional
This is my first time encountering it
what about V possibly being infinit dimensional is stopping you from checking those things?
V would contain f(1) and I can't find a T(f)=f(1)
and i dont know how get eigenvalues if I can't make a determinant
eigenvalues still make sense even in settings where determinants don't
they're just scalars c such that Tf = cf for a nonzero f in V
you could probably assume that this is true, and use it to find out what the eigenvalues are
wait why? a basis would just consist of functions f_i: N->R where f_i(k) = 1 if k=i and 0 if else
lol
wait but this isn't a basis
f(n) = 1 for all n can't be expressed as a finite linear combination, for example
itโs an infinite dimensional vector space tho
ok
oh. it has to be a finite linear comb? even in an infinite dim setting?
this is the distinction between a "hamel basis" and a "schauder basis" iirc
oh. i will go research those then
ham
i realize i sort of threw words at you and didn't really address your question
if you only want to consider hamel bases then no, it's not a basis, but i guess that something similar to that would form a schauder basis
it is not injective because of the upper limit converging?
the moral of the story is that for infinite dimensional spaces you shouldn't work with bases
(at least if you're not in a banach/hilbert)
i was going to sayโฆ that isnโt entirely true. i could see some things getting messy with convergence of infinite series otherwise tho
its not injective because it has a non trivial kernel
im not sure what you mean
im going to make the question a lot easier for you and tell you that V is just the space of convergent real valued sequences, and that the linear map T is just the left shift
Yeah since they converge there's essentially f,g, f!=g such that T(f)=T(g)
you can make it simpler: T is injective if and only if Tf = 0 implies f = 0. can you think of a non zero f which gets sent to 0?
I'm not sure what a non zero f would even be, but I cannot think of one
T maps a sequence (a, b, c, ...) to (b, c, ...)
oh then (1,0,0,0,...) would be mapped to 0
so for surjective I need to prove that for every sequence (b,c,d,...) there exists (a,b,c,d,...)?
yea. so given a sequence a_n=a1,a2,โฆ, in V, we can define a new sequence b_1=1 and then b_k=a_k-1 for k>=2. then where does T map b_n to
Does anyone know how to find these eigenvalues? Or is more info needed
@warm kite try plugging in lambda = a
this should be a root of the characteristic polynomial of L - lambda I, so you can factor the cubic into a linear factor and a quadratic. the zeros of the quadratic along with 'a' will be the eigen values of L
@teal grotto why can I do that?
do what
Set lambda to a
the eigen values of L are the zeros of the polynomial you found
Yeah I know
if you evaluate that polynomial at lambda = a, you will get zero
Wait but why would I want that
because you can factor the polynomial to find the other two zeros, if they exist in the real numbers

um. this is called polynomial long division. if you have a polynomial p(x) and you know that p(a)=0 for some a, then there is a polynomial q(x) such that p(x)=(x-a)q(x)
basically, yes
by x - a
@wintry steppe have you slept yet lol
my disdain for do carmo's poor writing keeps me going
lmao, not to be creepy, but i saw that on mse. looks like a tough problem
it's not tough it's just stupid
lol
do carmo constantly dodges small technical points like the one im confused on
oh. well, it looks tough to me because i just dont understand anything that was written on the page
but that seems really irritating
what is your math background if i may ask?
it's a wonderful textbook to read if you want the idea of something, but if you want to get into the gritty technical details (i do) then it's not so great
just finished my third year of an undergraduate math degree
oh cool, i just finished my first year. you seem really knowledgeable tho
Sorry to bother but how do I solve this?
the quadratic equation ?
@teal grotto yeah, like how would I get values for lambda
well, use the quadratic formula of course
Oh wait I see
wait so what goes wrong, or are the key differences, if i use a schauder basis vs a hamel basis ?
other than not being able to write some vectors as a finite linear combination of basis vectors with the schauder basis, is there anything else that is different?
hamel basis makes sense for an arbitrary vector space, schauder basis is for a normed vector space and allows for infinite "linear combinations" provided they converge
axiom of choice implies that every vector space has a hamel basis
right. with zorns lemma
same thing xd
a concrete example of a hamel basis is {1, x, x^2, ...} for R[x]
as for schauder
right. so hamel basis can be infinite but each element can be written using only finitely many basis elements
yup
hmm. schauder basis for space of real sequences would just be the the one i provided above then
those feel like good examples to remember the distinction by then. thnx
for a concrete example of a schauder basis, consider \ell^2, the space of square summable sequences. then {e_1, e_2, ...} is a schauder basis that isn't a hamel basis
something like that
every hamel basis of a normed vector space is trivially a schauder basis, but as you've just seen the converse is false. that should make the distinctions a bit clearer
ig they give different conditions for linear independence and spanning as well
right, you have to be careful for schauder
you ask that every element of the space be representable uniquely as a convergent "infinite linear combination" of the basis vectors
that unique part in italics is the linear independence analogue ig
ah ok. cool
does anyone have any idea abt this
Hey guys Iโm stuck on a hw problem
Pls ping
For this I have an answer ^ just not sure
send it
Matrix 2 x 2
Top row 1 0
And 0 -1 bottom
Our textbook has it different in different spots
Also can u verify this bc I wasnโt sure if itโs 2 x3 or 3 x 2
2 rows, 3 columns. So a 2x3
So the way i have it is right?
yeh looks gud
One more question
If u donโt mind
for this matrix I got when h is not equal to -4 itโs consistent
m conflicted on if this is right or if itโs all values will make it consistent
Does anyone happen to know? ^
nvm not necessary^
does anyone wanna help me with Exponential Functions, Features of Exponential Functions and Graphs, Solving with Exponentials, Analyzing Quadratic Functions homework?
I will pay
It's for my course online and im struggling
You are requested not to offer money for getting your homework done. Read #rules .
Also, read #โhow-to-get-help to get help with these topics in an appropriate channel.
I am trying to derive this formula, but unsuccessful yet:
I understand it is to do with "determinants".
The numerator is the product of adjacent sides of the parallelogram, and the denominator is the "determinant" of the vectors of the parallel lines.
do you know the dot product?
i think cross product is what they're looking for
Anyways, got it. Thanks.
stuck on this question....
I don't think what I wrote in the middle paragraph is wrong....
But I am not sure how to do the last one since I am not given any explicit mapping? Would the last one also not have enough information in this case?
remind me what is it ?
norm of some kind
poorly typeset $\nrm{v}$ probably
Ann
ah probablly ty
here's a hint: think about geometric series
this might lead you to a formula for (I-A)^-1
Okay ty
Hello. Any $2 \times 2$ unitary matrix with determinant $1$ except $\pm I$ can be described as a nontrivial $3 \times 3$ rotation matrix?
MathPhysics
@dusky epoch can guide me?
Hint (1-x)(1+x)=1-x^2
If the column operations on matrix A are identical to row operations on A^T, why don't column operations preserve the rank?
they do preserve the rank. who's telling you they do not?
buncho dragons gave a hint.
Yeahh i got it thanks @dusky epoch and @native rampart
oh, the answers online xd
<@&286206848099549185> Hello. Any $2 \times 2$ unitary matrix with determinant $1$ except $\pm I$ can be described as a nontrivial $3 \times 3$ rotation matrix?
MathPhysics
T(0) != 0 therefore T isn't linear transformation. (is this true also in case of complex numbers above R and C like in this example?)
yes, any linear map should map 0 to 0
ty
Hi
How are you?
I'm studying linear algebra from zero
and right now I'm at the gaussian elimination part (and also Gauss-Jordan)
And I'd like to see a proof of that
Especifically, the case where you multiply a row by a number
I don't know why you can do that
And I'd like to know if there's a proof
Why do you think you shouldn't do that
No, it's not that
You want to know why elementary operations work?
Yeah
Especifically, the one where you multiply a row by a number
The book I'm reading says that it works because if we consider 3 elements $a,b,c$ from a field $K$, the idea is based on the fact that $a = b \Longleftrightarrow ac = bc$
Obamid
I don't understand how that proves that you can multiply a row by a number and then the 2 matrices are equivalent
Yes
Consider the following systems of linear equations:
2x+y+z=0
3x+2y+4z=0
5x+3y+z=0
and
2x+y+z=0
x+y+3z=0
5x+3y+z=0
These 2 should have the same solutions
Because you just subtracted equation 1 from equation 2 in 1 st system to get 2nd system
You say these 2 matrices are row equivalent
Because the corresponding linear systems can be converted to the other form by doing some perfectly legal operation(In our case system 1 -> system 2 Do eqn 2-> eqn 2- eqn 1
system 2-> system 1 Do eqn2 -> eqn2+ eqn1)
Elementary row operations are defined such that they convert a matrix into another row equivalent one
And when you multiply a row by a number?
Multiply by inverse to get back original system
That's assuming inverse exists
That's why multiplication by 0 is not elementary
So I can understand that with lines, yeah?
In Rยฒ, you would have that 2x + 4y = 5 is the same as 4x + 8y = 10, right?
Yed
So that's why in gaussian elimination you can multiply a row by any rational
Okay, thanks
:)
You can multiply a row with anything that has an inverse
So, if you were talking rings in general,that means you can multiply only with units
that's quite the definition
It means you can split the indices $1, \dots, m$ into two sets $S_1$ and $S_2$ such that any entry $a_{i, j}$ in the matrix where $i \in S_1$ and $j \in S_2$ is zero
Frank
at least i think lol
does this come with any examples?
The permutation just rearranges the indices so S_1 = 1, ..., k and S_2 = k, ..., m
I'm trying to prove that if $T$ is a linear operator over a complex vector space and has an orthonormal eigenbasis, then $T$ is normal (one direction of the complex spectral theorem). This stack exchange post says that if $v_1, \dots, v_n$ is an orthonormal eigenbasis of $V$ with eigenvalues $\lambda_1, \dots, \lambda_n$, then $T^*v_i = \overline{\lambda_i}v_i$. Does anyone know how I can show this?
Frank
any hints please
-
there's a typo in the displayed equation, the middle term should be |lambda_i|^2 v_i
-
show that |(T* - \bar{\lambda_i}I)v_i|^2 = 0
oh hmm lemme try that
i think that'd work
i think i have to somehow use the fact the v_i's are orthogonal because otherwise it wouldn't be true but im not exactly sure how to incorporate that
ah you're right probably. i thought about it a bit more and for my proof to work you need to assume T is normal (which is what you want to prove...)
you can probably show that the inner product of (T* - \bar{\lambda_i}I)v_i with each v_j is zero
ohhh wait I think I can show the inner product of T*v_i with each v_j is zero
0 = <lambda_j v_j, v_i> = <Tv_j, v_i> = <v_j, T*v_i>
Which means v_i is an eigenvector of T* which I think is most of the work
yeah i think that works
the first equality isn't necessarily true
but v_1, ..., v_n is orthonormal
TTerra
if i = j the first equality won't necessarily hold
oh right, but if it holds for all j โ i then that shows that T*v_i is orthogonal to all v_j where j โ i, which is all you need
oh this is a nice way too
to finish your argument off, $T^*v_i = cv_i$ for some scalar $c$. since $\langle v_i, v_i \rangle = 1$, $c = \langle T^*v_i,v_i\rangle=\bar{\lambda_i}$
TTerra
Wait, I know this is probably wrong but donโt we immediately get T to be normal just by saying that is is diagonal wrt to the basis {v_i}?
you'd have to know that the adjoint of T has matrix equal to the conjugate transpose of that of T (wrt orthonormal basis) and the proof of that fact probably follows from exactly the same work done here
T* is the adjoint of T. with respect to an orthonormal basis, it's matrix is the conjugate transpose of that of T
if one knows this already then there's no work to be done, as you say
oh i was trying to show it without this, yes if you use that its immediate
wrt any basis, not just orthonormal right?
no it has to be an orthonormal one
take the identity operator, and write it as a matrix w.r.t. something thats not orthonormal. you get something that's not symmetric
Oh yeah, thatโs true
wait i don't get it. the matrix of the identity operator with respect to any basis is going to be the identity matrix
LOL oops yeah thats not a valid example


I suppose you can take something like $$\begin{bmatrix}1 & 0 \ 0 & 2\end{bmatrix}$$ and write it with respect to some other basis
Frank
a random example i pulled out of my ass is T(x, y) = (x + y, y) and the basis (1, 0), (1, 1)
i just wrote down the first operator i could think of lol
ah thats easier. for some reason i was trying to come up with a normal operator
there's a tiny bit of computation to be done so it's not immediately clear that this example works
or if it works i could have made a computation error 
i think it works, I got the original operator has the identity matrix but the adjoint doesn't have the identity
if the original operator had the identity matrix then it'd be the identity operator on C

that'd be correct
what about $$\begin{bmatrix}1 & 1 \ 0 & 1\end{bmatrix}$$ for $T$ and $$\begin{bmatrix}0 & -1 \ 1 & 2\end{bmatrix}$$ for $T^*$
Frank
that's what i got
ok whew i can still do math
Anyway, thanks for the clarification, I figured I was going wrong somewhere
is it true that every invertible matrix with entries in {0,1} have a real eigenvalue?
was curious because I came across a problem which asked to show that an n by n invertible matrix with entries in {0,1} can have at least n ones and at most n(n-1)+1 ones.
the number n(n-1)+1 happens to be the dimension of the space of n by n matrices with v_0 as an eigen vector for some non-zero v_0 in R^n
Hello. Any $2 \times 2$ unitary matrix with determinant $1$ except $\pm I$ can be described as a nontrivial $3 \times 3$ rotation matrix?
MathPhysics
<@&286206848099549185>
what did you try?
I have no idea about it.
well lets start by explicitly writing out what elements of 2x2 unitary matrices with determinant 1 look like?
[a b \ -b* a*] with |a|^2 +|b|^2=1
about what axis?
any
(a better way to talk about this btw would be using quaternions, are you familiar with those?)
Only definition
i see, so unit quaternions are precisely rotations in 3d
i.e things of the form a+bi+cj+dk with a^2+b^2+c^2+d^2 = 1
now heres the hint, can you think of a way to represent i,j,k as 2x2 complex matrices?
(its related to unitary matrices)
[i 0 \ 0 -i], [0 1 \ -1 0], [0 i \ i 0]
mhm, now use this idea to write your SU(2) matrices (the 2x2 unitary matrices with det=1) as unit quaternions
How?
Break the SU(2) matrices as linear combination of those matrices and the identity
A linear combination of unit quaternions is a nontrivial 3 * 3 rotation matrix?
It must not be true; their ranks are different.
The unit quaternions are the rotations in R^3
the 3x3 matrices are just a way to write them
so if you show each element of SU(2) can also be written as a unit quaternion then you have shown its a rotation in R^3 and you are done
Anyhow notice
Why are unit quaternions rotations in R^3?
oh let me find a good source on it
try reading this @broken sun , rotations in 3d are almost always written as unit quaternions
@torn hornet Thanks. So, to answer my original question, I have to first show that rotations are quaternions, which is somewhat complicated?
I think you could go without it, but those would probably be disgusting algebra bashing with 3x3 rotation matrices. This is probably better and would help intuition
Ok. Thanks.
(btw if you want some good detailed expositions on this, John Stillwell's "Naive Lie Theory" chapter 1 is very good to explain this)
Does swapping rows during elementary row change the sign of a matrix?
if you mean the sign of its determinant
yes
each "swap performed" multiplies the determinant by -1
you can verify this by computing the determinant of a permutation matrix P [it'll be -1 if its just a single swap] and recalling that det(AP) = det(A)det(P)
is there a quick way to check whether A and B are diagonalizable matrices ?
you'll have to check the eigenvalues and eigenvectors
i can't think of a faster way than trying to do it
alright wanted to make sure I dont miss anything
they are not btw
well B isnt*
basically you know the eigenvalues are 1,1,2 right, you just need to confirm 1 has geometric multiplicity 2
yea
i thought u can just check if they are symmetric

