#linear-algebra
2 messages · Page 21 of 1
after that
I take root
but I can take root this one
for example, if A^3 = P[27, 0; 0 27]P^-1 then A = P[3, 0; 0 3]P^-1
I forget that A is a real matrix
at first, I thought that A doesn't exist, but I didn't think that this one was easy
Can anyone help me with this question?
Explain Matrix Multiplication.
Especially for transforming polygons.
Do you know the correspondence between n x n matrices and linear maps on n-dimensional vector spaces?
A linear transformation is a function that maps a vector to another vector, such that:
-
For vectors u,v
f(u + v) = f(u) + f(v) -
And for a scalar α,
f(αu) = α f(u)
Any linear transformation has a matrix that represents it. That is, rather than applying the linear transformation onto a vector, multiply the vector by a matrix instead.
Multiplying two matricies is the same as composing the linear transformations they represent
I usually mess up the coordinates.
Like, I don't which coordinate comes first when you put the coordinates of the original polygon in a matrix.
For example, working entirely in R²:
Let A be a matrix that rotates a vector by 90 degrees.
Let B be a matrix that doubles the length of the vector.
Multiply them to get AB, AB is a matrix that doubles the length of the vector, then rotates by 90 degrees.
Can I send you a screenshot of the question?
Sure
Okay, give me a moment
It is still important that you understand what matrix multiplication is doing, even if your question doesn't pertain to it
Let's take the top point. That's the vector:
[0]
[4]
Right. That's the part where I get confused.
I don't know which coordinate comes first.
[x]
[y]
Sorry, not coordinate.
Ordered pair.
The purple is the original shape. By the way.
Oh lol fair enough
Yeah, is there some trick to it or something?
There's no purple dot at (4,1) or (4,0)
Yeah there's a dot at (3, 3)
My question is, why can't the first coordinate be (3,3)
When plugging into the matrix.
What's a "first" coordinate?
So, the matrix for purple is..
There's no order to them. They just each get sent somewhere
Okay. Each point can be assigned a vector.
Multiplying R by this vector tells you where the transformed vector goes
Right.
Ooh... I get it.
Yeah.
It just rung like a bell.
Got it.
Thanks, Kaynex.
Hopefully it helped! Feel free to ask if you need anything else
Sure.
Also, this is just about the linear algebra itself.
- Is Linear Algebra hard?
- What kind of mathematical knowledge should you have? Will you be fine with knowledge of Calc AB?
Because I am a high school student and I am quite intrigued by this course.
You don't need any prerequisite knowledge for linear algebra
The first question is subjective
It can be super hard for some people, but others can understand it intuitively easily
linear algebra is pretty different from any other math course i took in HS
I found portions of it intuitive and others a bit harder, some people found all of it hard
i mean, there is calculus in applications and examples. But cal AB should be all you need to understand them
do you really need calc AB? i was thinking and there's not too much of an overlap in subject matter, save for some of the mathematical maturity you would develop in calc
nah, I don't think you really need it.
aight im super duper confused fellas
how does one find an adjoint for a linear transformation from R^3 to R^3? My professor explained it very poorly and im not even well versed enough in this to do a proper search on the internet
what inner product are you using
actually, that doesn't matter much. the real question is
is your linear transformation represented with a matrix (which it most likely is)
and is the basis it's in orthonormal under your inner product
it is represented with a matrix
the question doesn't specify a special inner product so I'd assume its just the dot product
transpose the matrix and replace the entries with their complex conjugates.
so I have my
T(a,b,c) = [a,3b+6c,b+4c] <- transpose
so i'd take the transpose of that
[a,3b+6c,b+4c]?
yea. it might help to separate the matrix from the inputs tho
so get the matrix
[ 1 0 0 ] [ a ]
[ 0 3 6 ] [ b ]
[ 0 1 4 ] [ c ]
then transpose of that would be
xd
uh yeah is this better?
and your matrix is just $\begin{bmatrix} 1 \ & 3 & 6 \ & 1 & 4 \end{bmatrix}$
Ann:
blanks for 0 obviously
whoops that didn't work
[ 1 0 0 ]
[ 0 3 1 ]
[ 0 6 4 ]
im bad with that bot :/
@slow scroll so i took the transpose of my matrix
but why do you replace the elements with complex conjugates?
I guess I don't really understand
well its not obvious why you have to do it, but for a complex inner product space, that is the configuration that satisfies (Ax, y) = (x, A*y)
uhh no sorry
I'm kindof lost
how do you even get a complex conjugate here
The elements aren't complex numbers
thats right, so its just the transpose here
so that's just the adjoint?
That seems like... too simple?
so the adjoint of T: R^3 -> R^3
T(a,b,c) = [a,3b+6c,b+4c]^(transpose)
is just
[ 1 0 0 ]
[ 0 3 1 ]
[ 0 6 4 ]
?
That looks right.
hmmm to be clear, when ur talking about adjoint, you mean the hermitian adjoint, and not the matrix of minors adjoint, right?
i....
am actually not sure
It might actually be the matrix of minors
but like
I just searched for hermitian in our class notes
it doesn't have a mention of it
I can send the class notes I have on adjoint if that might help?
that might help i guess
oh okay, then yeah, this is right.
oh ok
cool
so the one with matrix of minors is usually referred to as adjugate right?
i think so. I've always known it as "the transpose of the cofactor matrix" personally, but these things can go by several names lol.
I had one case where something was called a name that I think literally only my professor used
I couldn't find it being referred to that name anywhere online
I don't remember what it was but it was very annoying
hmm strange
Can anyone give me just like a descriptions of what linear algebra is? Because I signed up for Applied Linear Algebra for my freshman year. Did I needed any introduction class like introduction to linear algebra?
please don't post across multiple channels
It's about solving equations
its about gauss jordan elims and nothing else. just bash numbers in a matrix
Always solve with Cramer's rule and the Laplace expansion
It's faster than the standard way of guess-and-check
cramers 🤢
Why use Cramer’s when you can use Wolfram
why use cramers when you can just invert the matrix
just guess and check
is there any characterization of nilpotent matrix to prove rank(A+A^2+A^3+...+A^2019) = rank(A) for A is a nilpotent matrix
why does A transpose times A have the same nullspace as A?
Well it's clear that the null space of A is contained in the null space as A^T A right
not really a linear algebra technique, but you could find $t_0$ such that $$\dv{t} \lVert P - L(t_0) \rVert = 0$$.
kxrider:
you could define a plane E that goes trough P and L is normal of it. Then you calculate the intersection point of E with L, that's Q, for the distance you can then simply evaluate the distance between Q and P
lmao
I figured it out right after I sent it
Why does this keep happening every time xD
Me with my non rigorous maf
linear algebra done right?
Yeah I just had a question but now I found out the answer
fuck man
i tried with it as like my first real math course i fucking sucked likle literally couldnt do any problem they were too hard
Axler? Its actually intended as a second course in linear algebra. That's probably why the problems seemed so hard
I’m working through it fight now and having taken LA once before, this book makes for a great supplement
One interesting thing is that the determinant is literally the last thing introduced in the book. So there are probably a lot of alternative explanations for stuff like the characteristic polynomial where determinant would normally be invoked.
Is {0} called the trivial vector space
yes
no it isnt
Yes linear algebruh is fun
no it isnt
but it is fun
Idk but I’m doing it now
Sometime after calculus or ODEs
ok
lol
okay
i guess the summer before college or sometime during winter break ill continue where i left off
which was like
LU decomp
kek
an orthogonal matrix can never be singular right?
Question. Is linear algebra mostly about matrices?
kind of not really
nu
no, not really
No not at all
They are also about Vectors, functional spaces and more things
That I am not literate enough to know.
Hm
I feel like I'd argue otherwise
Vector spaces by themselves are not very interesting objects, especially if you restrict yourself to finite-dimensional ones
So the real interesting stuff that happens is when you have linear transformations between spaces
And of course, these linear transformations are represented as matrices and so working with matrices really is most of linear algebra
Literally just got to first chapter on linear map
in R^3, $ker f = <(1, 1, 1), (0, 1, 2)>, Im f = <(1, 1, 1)>$, find $f$
Nguyễn Thành Trung:
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can anyone give me some suggestions for this problem?
So, we know that $f(1, 1, 1)=0, f(0, 1, 2)=0$
Element118:
It's $\mathbb{R}^3$, so you can find a third vector to complete the basis.
Element118:
$(1, 0, 0)$ works okay. $f(1, 0, 0) = k(1, 1, 1)$
Element118:
is f linear?
There is an infinite family of f, I think
f(1,0,1)=0 then
in R^3, $ker f = <(1, 1, 1), (0, 1, 2)>, Im f = <(1, 1, 1)>$, find $f$ as you said
dog:
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So, f(x, y, z)=k(-x+2y-z)(1, 1, 1) should work for any k not equal 0.
okay...
it's just one f satisfies
how?
f = (x1 - x2 + x3; x1 - x2 + x3; x1 - x2 + x3)
can you verify it?
before I post my solution
okay that works, but it's not unique
multiplying by any nonzero constant also works
but it should satisfies im f
oh no
I forgat
infinite f
f = k(x1 - 2x2 + x3; x1 - 2x2 + x3; x1 -2 x2 + x3)
yeah
nonzero
do you want to see my solution?
ah just drop it, I think that it's unnecesssary
The last sentence
Does that mean that T(v1), T(v2),..., T(vn) span T(V)?
@native lodge Im gonna straight up ping amphy
I can see that those vectors span T(V)
The a’s are scalars though
Oh i meant v1, v2
yes they do
Ok
The original v’s are a basis and then the outputs are then basis vectors for the output space
Really?
But what if the output space has lower dimension?
Then it can’t be a basis
oh, actually, yeah, you're right, it might not be a basis of course
I’ll have to read that chapter again, but I’m thinking it says something about the transformation being between the spaces of the same dimension
Oh, we say yes it is a basis if it is same dimension for both spaces
Ok
as you said, lets say dimV=n, dimW=k, n=/=k, T(v1),...,T(v_n) cant be basis of W
Between different dimensional spaces then that won’t hold
and no, even if its an endomorphism it may not be a basis
If T: V-> V is the zero transform then it can’t be a basis for either V nor T(V)
The last sentence
Does that mean that T(v1), T(v2),..., T(vn) span T(V)?
no it doesn't
it means that once you know the values of T(v_k) for 1 ≤ k ≤ n, you know the value of T(v) for any v ∈ V
this applies to any transformations, not just those from a space to itself
Well it you know any v in V then it means those vectors span the vector space
Ya but it implies span
Oh i see what you mean
I am kind of over thinking it
Is the null space of a transform $T$ just $T^{-1}({\mathbf{0}})$
Whoever:
yes
preimage of {0} under the transformation yes
0
the zero vector
at some point you stop having to use typographical stuff to mark the type of everythIng and you know when 0 is meant as the scalar and when as the vector
i think it was just a meme not a correction tbh
Maybe the wrong channel for this question, heck probably could ask it on another server too.
I need to calculate the vector of a refracted particle, but am having some trouble deciphering Snell's law's vector form. Hoping someone could shed some light
on this
im still a bit confused on how to find adjoints (inner product not matrix of minors)
I have T: P2 -> P2
T(a_0 + a_1 x + a_2 x^2) = (2a_1 - 2a_2) + (2a_0 + 3a_2)x + 3a_2 x^2
(I'm just going to call a_0, a_1, a_2... a,b,c because its easier to type)
I'd set it up like this, right?
<a+bx+cx^2, T*(a+bx+cx^2)> = <T(a+bx+cx^2), a+bx+cx^2>
?
and in this case it would be self-adjoint?
I think it makes sense but I just want to make sure I'm doing this right
the hermitian adjoint of an operator T, T^*, is defined as the operator that satisfies <Tu, v> = <u, T^*v> for all u, v
self-adjoint means that T = T^*
yeah. is that not the case here?
How do I find (a basis of the 3x3 matrices over R) consisting of invertible matrices?
consider determinant
uh
consider that the set of invertible 3×3 matrices isn't even a subspace of R^3×3
given that
yknow
the zero matrix isn't invertible
Anyone know linear programming?
$AB = A + B, rank(X) = 1, rank(A) \le n - 2$. Prove that $B+X$ isn't invertible
Nguyễn Thành Trung:
Nguyễn Thành Trung:
and I am trying to prove that
$rank(B) + 1 \le n - 1 \Leftrightarrow rank(B) \le n -2$
Nguyễn Thành Trung:
Nguyễn Thành Trung:
$\operatorname{rank}(B)$
DarK:
ahhhhh
I solved my problem
thanks for reading it
ahhh no
I misunderstand something
I haven't solved my problem yet
so we need to prove
r(B+X) <= n - 1
r(B+X) <= r(B) + r(X) = r(B) + 1 <= n - 1
<=> r(B) <= n - 2 is equivalent
Assume that r(B) = n
A+B = AB
<=> B = AB - A = A(B-I)
r(A) <= n - 2 => det(A) = 0 => det(B) = 0 => r(B) < n (wrong assumption)
Assume that r(B) = n - 1
B = A(B-I)
r(B) = r[A(B-I)]
<=> n - 1 = r[A(B-I)] <= min{r(A), r(B-I)}
but r(A) <= n - 2
so this is a wrong assumption too
so r(B) have to be < = n - 2
can you guys verify it for me please?
$AB = A + B, \operatorname{rank}(X) = 1, \operatorname{rank}(A) \le n - 2$. Prove that $B+X$ isn't invertible
Nguyễn Thành Trung:
Yeah, seems okay
Just that I'll clean up a bit more
$B=A(B-I)$, hence $\operatorname{rank}(B)\leq\operatorname{rank}(A)\leq n-2$. Hence $\operatorname{rank}(B+X)\leq\operatorname{rank}(B)+\operatorname{rank}(X)\leq n-2+1=n-1$ so B+X is not invertible.
Element118:
😮 wow, it's seem so smarter than my solution is
It is exactly the same
but phrased in a way such that the next bit follows from the previous bit
but can I know how rank(B) <= rank(A)?
Yeah, since A is a factor of B.
Bx=A(B-I)x
rank(B) is the dimension of all possible Bx.
rank(A) is the dimension of all possible Ax, which is greater than or equal to the dimension of all possible A[(B-I)x], which is rank(B).
Does this work?
😮 ok thank you so much 😄
😃
$A = \begin{bmatrix}1&\frac{2012}{n}\\frac{-2012}{n}&1\end{bmatrix}$. Find $\lim_{n\rightarrow \infty}\frac{1}{2012}(A^n-I)$
Nguyễn Thành Trung:
rotation?
It's almost that
you mean A.A^T? or something like that?
A rotation matrix tends to be $\begin{bmatrix}\cos{x}&\sin{x}\-\sin{x}&\cos{x}\end{bmatrix}$
Element118:
Yeah, that
Ah left hand system and right hand system
So, maybe we should divide by $\sqrt{1+\left(\frac{2012}{n}\right)^2}$
Element118:
To make it an actual rotation matrix
then, powers of A would be pretty easily written trigonometrically
I was thinking diagonalising until I realised it was a rotation matrix
$\frac{1}{\sqrt{...}} = \cos x$
Nguyễn Thành Trung:
yeah, we come up with what the angle x is and maybe that might help us along the way
Excuse me may I get help after?
and taking powers would be pretty easy too
@keen estuary You can try asking in a #❓how-to-get-help channel
Ok
so a rotation matrix
A^n = [cos(nx) sin(nx)...] right?
I just calculated it by hand
$\frac{\sqrt{1+\left(\frac{2012}{n}\right)^2}^n\left(\begin{bmatrix}\cos{nx}&\sin{nx}\-\sin{nx}&\cos{nx}\end{bmatrix}-I\right)}{2012}$
Element118:
something like this
yeah
similar to what I just did
but...
well
it makes the limit hard to be calculated
cos(nx) and sin(nx)
Well, now we have a closed form
don't have limit when n approches to inf
that's the good news
$x=\arccos{\frac{1}{\sqrt{1+\left(\frac{2012}{n}\right)^2}}}$
Element118:
We have sort of a closed form, so I guess we can continue with dealing with each of the parts
im pretty sure there is a nice formula for A^n, just input some values, notice the pattern and induction
I remember doing similiar
$\sqrt{1+\left(\frac{2012}{n}\right)^2}^n$ looks like some sort of $e^\frac{2012^2}{2n}$
Element118:
$\arccos \left(\frac{1}{\sqrt{1+\frac{2012^2}{n^2}}} \right) = \pi/2$
Nguyễn Thành Trung:
$\cos (nx) = \cos (n\pi/2)$ right?
Nguyễn Thành Trung:
Nope, arccos(near 1) should be about 0
$nx=n\arcsin{\frac{2012}{n\sqrt{1+\left(\frac{2012}{n}\right)^2}}}$ which should be near 2012 for n large enough
Element118:
so $\cos{nx}=\cos{2012}$, $\sin{nx}=\sin{2012}$ (radians)
Element118:
when n goes to infinity
Sorry but I think
$\sqrt{1+\left(\frac{2012}{n}\right)^2}^n$ looks like some sort of $e^\frac{2012^2}{n^3}$
Nguyễn Thành Trung:
n^3 but not 2n like you did
So, we start from $\left(1+\frac{a}{n}\right)^n$ goes to $e^a$
Element118:
yeah, ooops
yeah right
$\left(1+\frac{2012^2}{n^2}\right)^{n^2}$ goes to $e^{2012^2}$
Element118:
$\left(1+\frac{2012^2}{n^2}\right)^{n/2}$ goes to $e^\frac{2012^2}{2n}$
Element118:
that's how I got it
hm....
I think I'm right
let a = 2012^2
so
(1+a/n^2)^(1/n) = (1+a/n^2)^(n^2/n^3)
= (e^a)^(1/n^3)
It's (1+a/n^2)^(n/2) by the way
ok thank you 😃
$a \in (-1, 1), A \in M_n(\mathbb{R})$ satisfies $\det (A^4 - aA^3 - aA + I) = 0$
a) $n=2$, find $\det A$
b) find condition of $n$ for $A$ exists and then calculate $\det A$
Nguyễn Thành Trung:
hmm...
I don't get any further from this one
a in (-1, 1)
how about eigenvalues?
$\det(A^4 - aA^3 - aA + I) = 0 \Leftrightarrow \det(-(A^4-aA^3-aA) - I) = 0$
Nguyễn Thành Trung:
let $A=\begin{bmatrix}-2&1&1\-7&3&5\-1&1&1\end{bmatrix}$, calculate $\lim_{n\rightarrow \infty}\left(I+\sum_{k=1}^n\frac{A^k}{k} \right)$
Nguyễn Thành Trung:
here how I have done
I have diagnolized A
then we have A = PDP^(-1)
then
we have
Lol every time you send interesting problems @undone garnet
$P(\frac{D^1}{1}+\frac{D^2}{2}+\frac{D^3}{3}+...+\frac{D^n}{n})P^_{-1}$
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and get stuck here when calculate the limit
Your goal is to express A^k with a closed form
eigenvalues are (-1, 1, 2)
Seems like the problem is written incorrectly
Are you sure it's not k! on the bottom?
Which should be immediate if you've already gotten a diagonalization
pretty sure it's a typo, this sum doesn't converge
well I had thought so
because I have
(-1)^k/k, 1^k/k, 2^k/k for k from 1 to infty
I mean
1^k/k doesn't converge
$P=\begin{bmatrix}-1&1&1\-3&1&2\1&1&1\end{bmatrix}\
D=\begin{bmatrix}-1&0&0\0&1&0\0&0&2\end{bmatrix}\A=PDP^{-1}$
Nguyễn Thành Trung:
yeah I'd bet money that it's a typo
$\sum_{k=1}^n\frac{A^k}{k}=P\left(\frac{D^1}{1}+\frac{D^2}{2}+...+\frac{D^n}{n} \right)P^{-1} = P\Lambda P^{-1}$
Nguyễn Thành Trung:
inb4 it's some butchered typing of some matrix eponential shit
$\Lambda =\begin{bmatrix}\sum_{k=1}^n\frac{(-1)^k}{k}&0&0\0&\sum_{k=1}^n\frac{1^k}{k}&0\0&0&\sum_{k=1}^n\frac{2^k}{k}\end{bmatrix}$
Nguyễn Thành Trung:
correct
thank you 😃
Could one of you guys please critique my answer
I saw that most people online did this using matrix algebra, but I was wondering if it's also valid to do it this way
That looks fine
I have another proof
A^2 = 0 => det(A) = 0
moreover, det(A) = det(PDP^(-1) = det(D) = 0
So, D has to have at least one row equal 0
implies that at least one lambda = 0
That assumes that A is diagonalizable
Isn't it non-diagonizable if eigen=0
No
The matrix is singular, but still can be diagonalizable
The zero matrix is diagonalizable
Oh ok, thanks for clarifying
My linear class has been very poorly and loosely taught :p
Can you explain what it means to be singular?
it means determinant = 0
singular means you can't nicely undo it
or, formally, det(A) = 0 or equivalently that there exists no inverse
@ darkrifts & Nguyen, do you see any issues with what I posted above?
I'm concerned about the case where A is the zero matrix
no, I think it is correct
Then I can't take a non-zero column vector x
ah well, let me see
you can set independent case like
A = 0
then A has 0 eigenvalue
and then A not equal 0
so A has at least one column that not equal 0
and then like you did
yep, ok sure
it's from my final exam and annoyed I didn't think of this case while I was testing
bleh
oh well
hopefully my teacher is incompetent enough not to think of the case lol
$A = \begin{bmatrix}\cos{x}&\sin{x}\-\sin{x}&\cos{x}\end{bmatrix}$
Nguyễn Thành Trung:
angle addition identities
$A^2 = \begin{bmatrix}\cos{2x}&\sin{2x}\-\sin{2x}&\cos{2x}\end{bmatrix}$
Nguyễn Thành Trung:
but A^3 doesn't like what I hope cos(3x)
A is a rotation by an angle x.
A² is a rotation by an angle x twice.
ect.
from this could you form a hypothesis? and can you prove the hypothesis with induction?
it should be cos(3x)
also are we proving A^n over integers n or all real n
or just diagonalize it
and thats why i got a B in linear 
but how we can prove with induction?
$\cos (kx)\cos (x) - \sin (kx)\sin(x) = \cos ((k+1)x)$
Nguyễn Thành Trung:
yeah
so I'm trying to prove
$\cos (kx)\cos (x) - \sin (kx)\sin(x) = \cos ((k+1)x)$
Nguyễn Thành Trung:
use the cos(a+b) identity
thank you sigma
i dont know how to type matrices in latex tho...
$\begin{pmatrix} 1 && 2\ 3&&4\end{pmatrix}$
JohnDoeSmith:
$\begin{pmatrix} 1 && 2\\ 3&&4\end{pmatrix}$
that's a wide boi
$\begin{pmatrix} 1 & 1\ -i&i\end{pmatrix}$ $\begin{pmatrix} \cos(x)+i\sin(x)& 0\ 0& \cos(x)-i\sin(x)\end{pmatrix}$ $\begin{pmatrix} 1 & 1\ -i&i\end{pmatrix}$^{-1}
try using 1 &
oh right forgot we could make it less fat
Sigma:
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$\begin{pmatrix} 1 & 1\ -i&i\end{pmatrix} \begin{pmatrix} e^{ix}& 0\ 0& e^{-ix}\end{pmatrix} \begin{pmatrix} 1 & 1\ -i&i\end{pmatrix}^{-1}$
Sigma:
$A^3 = A + I$ prove $\det A > 0$
Nguyễn Thành Trung:
$A^3-A=I$, so $A(A^2-I)=I$. There, we found an inverse for A.
Element118:
Not done yet...
I think we should consider polynomial
1/det(A)=det(A^2-I)=det(A+I)det(A-I)=det(A^3)det(A-I)
So det(A)^-4=det(A-I)...
A(A^2-I) = I =>det(A^2-I) ≠ 0 => det(A-I) and det(A+I) ≠ 0
consider f(x) = det(A-xI)
obviously f(x) is continous
assume that f(-1)f(1) < 0
=> exists at least one x_0 such that f(x_0) = 0
=> x_0 is an eigenvalue of A
Cool!
=> g(x_0) = 0 with g(x) = x^3 - x - 1 = 0
but g(x) doesn't have any root in (-1, 1)
Oh, I forgot that x_0 in (-1, 1)
so this is not true
implies that
f(-1)f(1) > 0
=> det(A-I)det(A+I) = det(A^2-I) > 0
and
so, with det(A)^-4=det(A-I) we are done
whoa this is cool
never thought of that "consider f(x) = det(A-xI)
obviously f(x) is continous" before
we should share more problems
$\frac{1}{x-1}+\frac{1}{x-2}+\frac{1}{x-3}+\frac{1}{x-4} > 2015$
Nguyễn Thành Trung:
my friend said that this problem could be solve by using linear algbra
no, find x
find all x that satisfies the inequality
by algebra way
not calculus
could i have help with question 22.
if P is 2 dimen shouldnt the orthogonal complement also be 2?
i can't picture 4d but it seems theoretically the case
but the answer says its a line
you're really sure P is of dimension 2 though?
Gilbert strang book 
Gilbert strang book 
- no, the solution to 2t + 8 = 3 is not t = 2.5
- you're in the wrong channel, this goes in #prealg-and-algebra
can anyone tell me if LA(v1) is just Matrix vector product https://media.discordapp.net/attachments/440214120361492500/609104202668572672/unknown.png?width=1099&height=780
it is
Someone please helpppp I tried multiple times to find the basis of the intersection of two vector subspaces and I just can't😭
What's the question?
If the subspace is the null space of a matrix, then you can get the basis of the intersection by combining the matrices vertically and finding a basis for the resulting nullspace
Is there a good problens generator? There's wolfram alpha but it only generates problems like eigenvalues,inverses and determinants... I want things like finding the basis of a matrix, kernel, image, linear transformations etc... Do you know of anything like that?
Um
Do a quick google search
I don’t think there is a lack of problems like those
Hi Gilbert Strang @wintry steppe what do you think about John Gabriel
@pallid rampart I don't know who that is
Lolllllll
Yeah the are plenty of inverses, determinants etc but there are no wusstions aboust basis, kernel, image, linear transformatikns etc @pallid rampart
🤔
John gabriel is basically a guy who claimed to have create the one and only one rigorous calculus
And he shits on other people who tells him that his logic is wrong
Ah this youtube guy?
Yes he is on youtube
I didn't remember his name
He publishes calculus videos right?

As I like to say to my math majors: "I'm the sadist and you're the masochists"
Jk but my proffessor likes to say that
I'm a physics major tho
@proper yarrow that’s probably because they’re all just row reduction problems in disguise, and row reduction is pretty tedious to do by hand. I don’t know what you mean by image and linear transformation problems tho.

I dont know how to translate that into english
Um
Lol
Well, row reduction is approximately O(n^3), pretty slow to do by hand
I meant gaussian elimination
I mean... linear transformation problems
Well, there are a lot of linear transformation problems
Afterall, linear algebra is the study of linear transformation and vector spaces
Nope
Oof
@proper yarrow תגיד אתה צוחק עלי
כן
The questions he wants are as follows btw: 3.
Fo what values of A there exists a linear transformation T:R_2[x] -> R^3
such that Tv_i=w_i
For all values of a, find dim(ker(T)), dim(Im(T))
@wintry steppe yeah
For every a=1 find a bsis for ker(T), for the linear transformation you found before
For what values of a the transformation is invertible?
For what values for a there are more than one linear transformation?
Nope not good with linear algebra I just started it last week 
א. Find (the sign that is written there)
ב. Given (the sign written there) find (the sign written there)
ג. Find the basis B
@pallid rampart the questions he wants are advanced linear algebra imo
Yeah the letter א in Hebrew is also used for cardinality
I don't think there are any questions for those advanced things
just aleph not aleph null
second one btw is beth
א_0?
for cardinals of power sets
@wintry steppe yap but written from left to right
Yeah, א and ב are also letters in Hebrew
$\aleph_0$
Scientifica:
then there's this one
Whoever:
$\gimel$
Gilbert Strang:
Scientifica:
Oh god what is beth
ב is superior
א is for the tangible)?( numbers
How do you say that
Oh real numbers
nope
$\aleph_0\coloneqq\card\mathbb N$
Scientifica:
Compile Error! Click the
reaction for details. (You may edit your message)
card ..
Um
$$\aleph_0\coloneqq\text{card}\mathbb N$$
Scientifica:
and
@pallid rampart xD telling Gilbert Strang
Cardinality can’t equal to the set
?
cardinality is a set
the typical constructions make
$$\mathbb N=\aleph_0=\omega$$
Scientifica:
Um
thus the lovely joke
I don’t think that’s how it works
$$\aleph_0+1=1+\aleph_0$$
Scientifica:
Scientifica:
Scientifica:
bruh
I don’t think that’s how it works
What you mean?
The cardinality is a way to compare the size of sets
The cardinal number can’t equal to the set
$\text{card} \bbN=\aleph_0$
Whoever:
Whoever:
Compile Error! Click the
reaction for details. (You may edit your message)
Nope
The cardinality is a way to compare the size of sets
yup but the typical constructions makes them sets
you know this?
$$0=\emptyset$$
Scientifica:
$$n+1=n\cup{n}$$
Scientifica:
you know that natural numbers are cardinals themselves..
and that's a way to see them as sets
well the typical definitions there in ZFC
is that one defines ordinals
as sets satisfying smtgh
and then one defines a cardinal as the smallest ordinal of a fixed "size"
ordinals being sets, cardinals are sets as well
|(0,1)|=|R|=|0,0.0...1|=א
Isn't that ridiculous
what is | | ?
nope shouldn't be
It is the cardinality tho
It means cardinality
ok didn't understand your equation
|(0,1)|=|R|=|0,0.0...1|=א
R is IR right?
Lol
What even is 0,0.0...1
well you didn't specify which א though
not א_0 right?
Just א
א something for a certain ordinal? ok
aaah
lul
I read (0,1) as an ordered pair
but you mean the interval (0,1) right?
😂
Yeah
Btw can you remove my studying role?
The interval
and what is 0,0.0...1?
Same
The interval
Between 0 and 0.0...1 (... = 0000...)
@pallid rampart done
Thx
np
ah ic
yep more generally
|IR|=|(a,b)| for a<b in IR
Yeah
Isn't that ridiculous
I'm used to it so I don't really see it as ridiculous
I mean... It's infinity but...
yep the paradoxal is that a set strictly included in another set can still share its cardinality
Cantor theorem
what's with Cantor's theorem?
That's cantor (schröder bernstein) theorem
ah lol
don't just say "Cantor's theorem"
because that means |X|<|P(X)|
Ik
There are several of these
In my country we call everything just Cantor's theorem
lul
why?
Because he "invented" it all
xD
is your country Israel?
Yes
maybe it is more like what makes people choose, say, Picard–Lindelöf theorem vs Cauchy–Lipschitz theorem lul
Maybe
if I'm not mistaken Cantor was Jewish or of Jewish heritage?
Yes
yup
Scröder was also Jewish and bernstein was also Jewish
oh didn't know that
Schröder
thought it was like what makes some countries choose the name Cauchy-Lipschitz while others chose Picard-Lindelöf
Schröder and every laat name that ends with "stein" are Jewish last names
Lipschitz is also a Jewish last name
😮 didn't know that
Everything that ends with "stein"/"schitz"/"ger"/"baum"/"berg"/"wartz"/"feld"/"tzer"/"ern"/"mann" (for the most part)/"mer" (for the most part) is Jewish basically
Stein and schitz are suffixes coming from Yiddish
ic
There were a lot of Jewish mathmaticians basically😂
xD
Lol John Gabriel be like
Hope that never happens
Wtf he likes Hitler?
Is he aware of the fact that hitler would have him slaughtered for bejng Jewish
Idk
He is just one weird guy
He doesn’t accept anyone who says his argument is wrong
While saying that everyone else is wrong without saying why
😑
He is either a genius or a moron pretending to know something
Does he hold any academic position
@pallid rampart
Lol I watched his channel
He really has something against Gilbert Strang
Wtf when he sang the national anthem to prove that he doesn't hate Jews, he had a perfect Israeli accent😑
"on the feebleness of the jews" im fucking dead

OH SHIT
@wintry steppe HOLD UP LET ME INVITE YOU TO A SERVER JOHN GABRIEL IS ON
TRY AND TALK TO HIM
see how mad he gets holy fuck lmao
Alright
he's going to think you're actually gilbert strang and fly into a rage
i guarantee you
john gabriel is like terry davis but not contributing anything of value
i'm so ready for this kek
anyone
I have one problem that's quite hard
I have solution
but well I don't understand a lot
$X, B_0 \in M_n(\mathbb{R})$. We have $B_k = B_{k-1}X-XB_{k-1}, k\in \mathbb{N}^*$. Prove that if $X = B_{n^2}$ then $X = 0$
Nguyễn Thành Trung:
Hmm...
So X and B_0 are square matrices on the reals...
Let's try substituting in $k=n^2$ to make use of everything
Element118:
$X=B_{n^2}=B_{n^2-1}X-XB_{n^2-1}$
Element118:
my solution uses linear dependent to prove
$dim(M_n(\mathbb{R})) = n^2$, so $(B_0, B_1, ..., B_{n^2})$ is linear dependent
Nguyễn Thành Trung:
Yeah, you have that...
Okay, so we take some i as the minimum index with nonzero coefficient, and we eliminate the coefficients from there until we are left with a non-zero coefficient for $B_{n^2}$
Element118:
I think I had another problem with the same idea before
i is the minimum index with nonzero coefficient. We can hence transform it to: \
$B_i=t_{i+1}B_{i+1}+...+t_{n^2}B_{n^2}$ \
$B_iX-XB_i=t_{i+1}B_{i+1}X+...+t_{n^2}B_{n^2}X-Xt_{i+1}B_{i+1}-...-Xt_{n^2}B_{n^2}$ \
Rearranging and grouping: \
$B_{i+1}=t_{i+1}B_{i+2}+...+t_{n^2}B_{n^2+1}$ \
Note that $B_{n^2+1}=0$. So we can eliminate the last term, \
$B_{i+1}=t_{i+1}B_{i+2}+...+t_{n^2-1}B_{n^2}$ \
Repeating k times, we get: \
$B_{i+k}=t_{i+1}B_{i+1+k}+...+t_{n^2-k}B_{n^2}$ \
Now repeat until $i+k=n^2$, this gives us: \
$B_{n^2}=t_{i+1}B_{n^2+1}+...=0$ \
and we are done
Element118:
@undone garnet get this?
sorry but
I don't get
rearrraging and grouping
how B_{i+1} = t_{i+1}B_{i+2}+...
oh
I got this one
😄
hm....
okay 😄
that's a nice problem
thank you
$a \in (-1, 1)$ and $A \in M_n(\mathbb{R})$ satisfies $\det(A^4 - aA^3 - aA + I ) = 0$\
a) with $n = 2$, calculate $\det A$\
b) find condition of $n$ for $A$ exists, and then calculate $\det A$
Nguyễn Thành Trung:
do you know determinant of vandermonde matrix?
$k_1 < k_2 < ... < k_n$. Prove that $\frac{\det V_n(k_1, k_2, ..., k_n)}{\det V_n(1, 2, ..., n)} \in \mathbb{N}$
if you don't know
$\det V_n(a_1, a_2, ..., a_n) = \prod_{1 \le i < j \le n}(a_j-a_i)$
interesting questions
induction works well here
oh wait, I thought about showing the formula for that determinant
I'm pretty sure I saw it before, but I can't recall the proof
well well welll
To my surprise I realize there is a more general inner product beyond the "dot product" that goes like
$ \langle \vec{x},\vec{y}\rangle = (\vec{x})^T A \vec{y}$
If symmetry is defined as $\langle M\vec{x},\vec{y} \rangle = \langle \vec{x},M\vec{y} \rangle$, does the symmetry property of a matrix depend on what kind of [A] I define my inner product with?
上海:
Here's some relevant content

@sturdy scaffold this should answer your question
Oh I saw that
If you just use any matrix you get a bilinear form
I recall that they do a lot of this stuff in Lang, let me send a pic of that in a couple of minutes
:o
Sorry that I don't feel like rewriting this stuff lol, I just think it's well documented in other places
It's ok
I guess the only other thing I can say is I got this problem that asked me if a particular matrix is symmetric with respect to a non-standard inner product
So I'm curious if its the inner product that defines symmetricness or if it's something intrinsic to the matrix
If that's covered in Lang then Im eager to read
ty tho
I'm actually confused why the transpose would be dependent on the inner product
Can you send a picture of the question?
Chapter 13 in Lang 3rd edition, section 6 treats bilinear forms
Yee sure
Show that the linear mapping $M: R^2 \rightarrow R^2$ defined by the matrix
$M = \left(
\begin{array}{cc}
1 & 1 \
2 & 1 \
\end{array}
\right)$ is symmetric with respect to the non-standard inner product on $\mathbb{R}^2$ , that is:
$\langle x,y \rangle = (x)^T \left(
\begin{array}{cc}
2 & 1 \
1 & 1 \
\end{array}
\right) y$
上海:
The answer was staightforward :o Just write out explicitly:
LHS: $ \langle M(x),y \rangle = \left( \left(
\begin{array}{cc}
1 & 1
2 & 1
\end{array} x \right) \left(
\begin{array}{cc}
2 & 1
1 & 1
\end{array}
\right) y$
RHS: $ \langle x,M(y) \rangle = x \left(
\begin{array}{cc}
2 & 1
1 & 1
\end{array}
\right) \left( \left(
\begin{array}{cc}
1 & 1
2 & 1
\end{array} y \right)$
上海:
Compile Error! Click the
reaction for details. (You may edit your message)
What does symmettric wrt an inner product mean?
Oh, symmetry in my low level lin alg class means
$ \langle M(x), y \rangle = \langle x, M(y )\rangle$
上海:
So given this strange non-standard inner product, is this true for M
Oh I'm stupid, that is what symmetric means




