#linear-algebra
2 messages · Page 52 of 1
The key is that you have P^(-1) and P next to each other when you write it
matrix multiplication in general isn't commutative so (AB)^n is not the same as A^nB^n
^
$PDP^{-1}PDP^{-1}PDP^{-1} = PD(P^{-1}P)D(P^{-1}P)DP^{-1}$
Ann:
holy shit
and you get the identity 1 thing
fucking brilliant
thank you
what property of upper triangular lets you skip the RREF and say that vectors are linearly independent?
to be more precise, the solution seems to be unfinished to me until you're able to put it into RREF
whenever the columns are linearly independent in REF. Basically, you can stop whenever its obvious that the columns are linearly dependent/independent.
(1,0,0) clearly can't be used to write (3, -2, 0) and same with the other vectors
i know the dependent thing is we just have to make a row with all 0s
but is there something special about stopping at the upper triangular matrix?
for A=PDP^inverse, when I find P, am i allowed to change one column of P to remove the fractions?
@north sierra when you find your eigenbasis, i think you are allowed to scale any vector by any amount you want, because they will be linearly dependent
in* but true
that's also true lol i mean dependent as in scaling any vector doesnt change much (you can go back to the original vector with fractions without any problems)
well scaling a column or whatever will change the inverse matrix
bruh how
that's a thing?
im so fucked
all these special properties i dont know about
when you're working with a basis only
then i guess its okay to scale it
but not when you combine other basis together
?
is this true
wat? scaling a basis gives you a different basis
yeah but you can still scale it
no if u mean basis and not eigen basis
the different basis matters
it's a different transformation
if a question said find the eigen basis, and i found it but it contained fractions couldn't i just scale it to remove it?
you can for that
and wouldn't it still be a basis
basis and eigenbasis are different
basis is kind of like.. how u change i, j, k and stuff
okok. So scaling eigenvectors is fine, but you have to make sure you are inverting the corrected matrix with the scaled columns and not the original.
brilliant
and just a hunch: any nice-ness you gain by scaling an eigenvector is probably lost when you invert the matrix for the sake of preserving determinant. i.e. if det(P^-1) = det(P)^-1
yeah i would leave my basis alone if i had to do inverse tho
${\vec{e_1}, \vec{e_2} \cdots \vec{e_n} }$
agentnola:
much better
it has 0s and just 1 one
alright time to take diffeq final 
good luck
gl
thanks for helping out
in a) how did they go from the identity matrix to saying showing its invertible, and in b) im confused about what's going on in general
oh
my god
they multiplied by A ^ -1
im such an idiot
If you have AB = I, then B is A's inverse by definition
i kept looking at some of the invertible matrix theorem rules
I wouldn't try multiplying by A^(-1) if you're not sure that the inverse exists
how does that "show" A is invertible?
Yeah that's why the questions seems more like "find an expression for A^-1"
than "show A is invertible"
I mean if you find a A^(-1) then A definitely has an inverse
But you shouldn't assume such a thing exists
how can they say the RREF of 1/2 (A - 3I) returns the identity matrix?
oh
beacuse it is invertible
it must be able to turn into the identity matrix
👌
How did they get rid of the 1/2 ?
But I don't see why that proves it has no eigens?
yeah...
If 1/2 A is invertible, then A is too
OH I see
how can they say no eigen basis
we need a null space to find an eigen basis?
ohh
What's det(A - 3I)?
not 0
So 3 is not an eigenvalue
Clever question I liked it
what does it mean by "complex conjugates" ?
ohh nvm i got it
they just made a typo in part of the answer
should be -1 - i
if $A \in \bR^{n \times n}$ is a real matrix and $v \in \bC^n$ is an eigenvector of $A$ with complex eigenvalue $\lambda$ then $A\overline{v} = \overline{\lambda}\overline{v}$
Ann:
Yes
Stay hydrated
Because 0v + 0u + 0w is in Span(v,u,w)
yeah I was just thinking maybe the constants not allowed to be 0 because you get a trivial solution
That has to do with linear independence lol but I know what you're talking about
wont lie i miss 🅱️ aynex ur handle was straight fire
Is this alright? Fair trade-off?
ur so awesome lol
Nah I'm on here teaching math. I clearly never got a life
nah kids like me out here passing thanks to people like u
hopefully
how come the geometric multiplicity is in terms of the # of free variables, not the basic variables?
What's the defn of the geo. mult, there's more than one
Probability that the charpoly splits
In this case you plug in the eigen values into the matrix and row reduce to find the eigen vector
well the geometric mult is the number of linearly independent eigenvectors associated to an eigenvalue
yes
Oh ic
now if you know how to construct a matrix from a basis, you'll understand that you need as many linearly independent eigenvectors as the geometric multiplicity
Then what do the basic variables mean? in terms of the row reduced matrix
what basic variables?
since we associate eigen vectors with the free variables, what do we associate with the basic variables?
yup sorry 1 sec im bad at explaining what I dont know
in the rref, what does "x1" mean conceptually?
x2 and x3 to me are the null space
that means that x_1 has to satisfy the equation
because we have x1 -3/2 x_2 + 1/3x_3 = 0
so we have two free variables right
x_2 and x_3
x_2 and x_3 completely determine x_1
yeah we write our basic variable in terms of the free variables
but our eigen basis is the null of that RREF
yes
sorry I think i realized
I dont know how to say what I dont know
i feel like an idiot
basically, the null space is determined by x_2 and x_3
which are free variables
so they can be whatever they want
yes exactly
but x_1 can be written in terms of x_2 and x_3
what space is determined by x1?
the column space?
and the row space?
i think that's what Im not getting
your column space of the matrix above is spanned by [1,0,0]
why not [3,3,0]
[3,0,0] is in the span of [1,0,0]
any scalar multiple of [1,0,0] is in the span
well I mean its impossible to have any non-0 variables in the second and third row

im bad at explaining
we have your matrix with 0's in all rows except the first row
I thought only for row space we use the row in RREF
but if we do Ax = b where A is that matrix, the first element of b is determined by your first row of A dot by the column of x
for column space we use the column before we reduced to rref
sry 1 sec

i am confused too
Anyways i have class now
i know one of the spaces we use the unreduced matrix row/col
I am taking linear algebra next semester and want to get a headstart over the break . I already am proficient in the basics(using augmented matrices to solve equations, etc), but have no real experience writing proofs which I know I will have to get good at. How do you learn to write a proof? I feel like I was never really taught how in previous math courses.
Is this room free to ask a question ?
I guess it is
Im doing geometry on algebra and got to find
Point D
So i tried finding point F
But when i check where it is on a 3D calculator
Im way off
Is my logic wrong here ? I made a point F thats on the BC line and the vector FA perpendicular to BC. Solved where it is, but its definitely not where its supposed to be
Any help will be super appreciated
Wait i messed up the input into geogebra, and some basic calculations ill be back in a sec to report
Ok its correct im just bad at inputting data lmao
So I was wondering if it’s possible to have a Q matrix which is orthogonal but not orthonormal (Q matrix from the QlambdaQ^T decomposition)
Find a vector $v$ in there and a number $a\in\bR$ such that $av$ is not in there
Icy001:
could i use the -1 scalar?
sure
i guess any <0 scalar would work right
Literally any nonzero scalar works
Since the line $y=ax$ and $y=x^2$ intersect at $x=a$ and $x=0$ and can't have any more intersection points
Icy001:
what the heck is a vector space
it's a set of objects called vectors where the objects satisfy the vector space axioms 
what are axioms
rules
For 1a, the solution Manuel is super confusing as to how to get the answer. Can someone help show me what I’m supposed to do?
Can someone explain how 11a is done
@silent dune you need to find an indépendant column vector which will not be a combination of the previous ones
In other words, I’d say complete the base
a cross product between the two should work
oh boy...what is this person writing
let the third column of A be x,y,z. consider any of the cofactors of the matrix entries not on the same column or row as the 0 entry (so a_12 or a_32) to find y
then just consider any other cofactors and solve x and z simultaneously with y
(then consider cofactors of x,y,z for unknown cofactors in C)
you can find nxn using gauss jordan
that's the beauty of linear algebra; things just generalize so easily and so naturally
Hello
so my professor wants me to take a huge amount of variables (36) in my dataset and turn it into linear regression?
I am so confused how would I do that? He did not give us an specific instructions
All i have done is this
@calm fulcrum looks awful lmfao
@calm fulcrum this should probably go in stat btw
and I think I can help with this
I know it looks terrible
My professor literally gave us no instructions on how to do any of this and was absent 2 weeks. @timber minnow any help would be amazing
let's talk in #probability-statistics
Okay going there now
The easiest proof I can think of is by contradiction
the subspace can't possibly have a basis which contains more independent vectors than the dimension of the vector space itself
What exactly is the eigenvalue of a conic or a quadric?
Geometrically
Like for linear functions we know that f(v) =lambda v, but for a conic?
I don't see how the zero space relates to this
Why does d hold true?
Why is it if and only if b=0?
is it "b=0 => set is a subspace" or "set is a subspace => b=0"
Why not 1 or 2?
which of these directions do you need clarified
"b=0 => set is a subspace" or "set is a subspace => b=0"
Both
ok well
alright
i think it might be helpful if we give our set a name
say W
so $W = { f : (0,3) \to \bR \mid f \text{ differentiable}; f'(2) = b }$
Ann:
@lone quail that ok?
Yes
we need to check that for all f, g ∈ W and constants c ∈ R, that f+g ∈ W and c*f ∈ W
As well as having 0
so if b=0
and we have f, g ∈ W
f and g are both differentiable
and f'(2)=g'(2)=0
then f+g is also differentiable
and (f+g)'(2) = f'(2) + g'(2) = 0 + 0 = 0
that's the definition of W that we were given
ok now
f ∈ W
and c ∈ R
(cf)'(2) = c * f'(2) = c * 0 = 0
so if b=0 then W is closed under addition and under scalar multiplication
and i will leave it to you to check that the zero function is a member of W
does this make sense so far
ok
so
does the other direction need to be clarified still
or in other words does it need to be clarified why W is NOT a subspace if b is NOT 0
Hmm 🤔
Is it because it wouldnt be closed linearly otherwise?
Iike if it was 1, then a scalar times 1 might not be in the set (0,3)?
Please correct me if im wrong
@dusky epoch
it's even simpler than that.
suppose b != 0
then W fails to even be closed under addition
(f+g)'(2) = 2b
and since b is not 0
2b is not equal to b
Ahhh ok thanks
Does anything good come from the fact that for some square matrices
AX = A = (X^T)A
?
any idea?
Why do matrices work in electrical circuits? I've been using them for over 4 years now to solve circuits and recently introduced myself to using them in the complex field as well (2x2 matrix for every value in the equation) but is there some proof that explains why it works? I'm super interested
and cuz my matrix knowledge isn't superb I guess
the way I use it with kirchoff's law of voltages and law of currents
I might need to ask this in the other discord, but I was wondering if some multi-knowledge people could help me understand why it works to convert the Kirchoff equations to a matrix then RREF them to find a solution.
Afaik, RREF is just to solve equations in general by manipulating the rows and such
but the conversion from Kirchoff equations -> matrix baffles me for some reason lol
Could be ultra simple- but I'm just interested 🙂
What are you using them for
The simplest application of matrices is to solve systems of eqns linear in each variable
Is that what you're doing?
Do you have a link to someone explains kirchoff as matrices
If it's pde stuff i probably can't help 😓
But maybe i can
Ooh
The ones for summing current or voltage?
No calculus?
Yes okay
@stone valve do you have an example I can use to demonstrate
do you know what an isomorphism is
no
When you're talking about Kirchoff's Laws, you're talking about forming a linear system of equations in terms of the currents and voltages?
do you know basic matrix arithmetic?
yes
yes
you're asking about how to convert from complex equations to 4 real equations, yes?
'Why it works to convert he Kirchoff equations to a matrix then RREF them to find a solution'
2x2 matrix per complex number I suppose as that's how I'm doing it now
^That is your main question?
so
I'm going to define two objects
$\mathbf 1$ and $\mathbf i$
and I'm going to write a complex number a+bi as
$a \mathbf 1 + b \mathbf i$
let me bold it
and I'm claiming that any complex number is going to satisfy
$(a \mathbf 1 + b \mathbf i) + (c \mathbf 1 + d \mathbf i) = $
gfauxpas:
$(a+b) \mathbf 1 + (c+d) \mathbf i$
gfauxpas:
gfauxpas:
as
uh let me make sure I dont make an arithmetic mistake here
$(ac-bd) \mathbf 1 + (ad+bc) \mathbf i$
gfauxpas:
this is just multiplication of complex numbers
make sense? just a fancy new notation you dont see the point of yet
follow?
this you can check will have all the expected properties like
$\mathbf i \times \mathbf i = - \mathbf 1$
gfauxpas:
$\mathbf 1 \times \mathbf i = \mathbf i$
gfauxpas:
did I lose you or do you follow
I'm following
oh I forgot to say a and b and c and d are real numbers
doing 4 thigns at once atm - sorry for being inresponsive
okay, are you sitting in a chair with arms
because this might surprise you so much you'll fall over
if I wanted to
I can create 1 and i with matrices
and get all the same results as with regular complex numbers
$\mathbf 1 = \begin{bmatrix} 1 & 0 \ 0 & 1 \end{bmatrix}, \mathbf i = \begin{bmatrix} 0 & -1 \ 1 & 0\end{bmatrix}$
gfauxpas:
yes I know this
so
found it through youtube
2 equations in 2 unknowns
with complex coefficients
become 2 equations in 4 unknowns with real coefficients
err
no
4 equations
yes
that's not enough to answer your question it sounds like
oh
'Why it works to convert he Kirchoff equations to a matrix then RREF them to find a solution'
it's just the way you transform the circuit info to the matrix
^This was the original question that baffled him
oh oops
Okay, the idea here is this
luddy was there he knows what im talking about
You understand that Kirchoff's Laws create a linear system of equations that are written in terms of the currents and voltages in a circuit?
yes lol
You introduce those currents and voltages as unknowns and then, you solve for them.
Now, the idea here is that any linear system of equations can be transformed into a matrix by dumping their coefficients into a rectangular array of numbers. That rectangular array is exactly what we call a matrix.
Yes
there's another way that works, but it
's not immediately obvious why it works
is to take the real parts of each equation and set them equal to each other
etc
anyway
The process of reducing the matrix to RREF is, in effect, solving the equations to obtain each variable's values.
thats not your question nm
The idea behind all of this is to convert a physics/engineering problem into a mathematical one.
just seemed weird that I can just slap this in a matrix and RREF this to get the actual current as I'm using the resistances and the voltage-
For example, if you consider the motion of a projectile, you will realize that it obeys a parabolic trajectory. The idea behind that is that we wish to reduce any kind of physical problem into a mathematical one. Once we can describe it using mathematical language, we can use mathematical solutions to describe something physical.
Well, RREF can be achieved through Gauss-Jordan Elimination and that's just a way to solve linear systems. For example, we would solve a linear system of 2 equations by eliminating one of the variables and solving for one of them first before solving for the other. It's the same idea here
I just feel like I'm posing a question that is either simple to answer or I'm completely missinterpretting what I'm doing
xD
I just don't see clearly on how I can say that a matrix of only resistances with the last collumn being voltages produces a unit matrix except for the last collumn consisting of currents
wait
no
fuck
NEVERMIND

I understand now
ignore my retardation
Thank you @cursive narwhal @vast torrent ❤️
not understanding something isn't a bad thing
as my tutor tells me
the answer to a question being obvious after you know the answer
doesn't at all mean you knew the answer or you should have known the answer
Hmm i may have misinterpreted your question. Apologies for that. I tend to do that sometimes.
Don't worry you both- did amazing to try to help
What did you ask?
Does anything good come from the fact that for some square matrices
AX = A = (X^T)A
?
oh, and A here is symmetric
and everything is in R
for all X or some X
for some
then nothing comes to mind
Ah, so we have $A = A^T$
$(AX)^T = X^T \cdot A^T = X^T \cdot A$
for some both of them
Abhijeet Vats:
yeah
we dont know A = A^T, how do we know that if it's only true for some X
^That's pretty general for all matrices A & X that are multiplicatively conformable.
oooh A is symmetric
because I said A is symmetric
missed that line
He said that A is symmetric
yeah
:X
Okay, but you also said that $AX = A$, for some matrix X.
Thus, we have:
$(AX)^T = A^T = A =X^T \cdot A$
Abhijeet Vats:
I think that's more of a specific thing rather than something general. Like, what I used to get to it is general because, for any two multiplicatively conformable matrices $A$ and $B$, we have:
$(AB)^T = B^T \cdot A^T$
mind that A is not invertible
or at least doesn't have to be otherwise its boring
Unless someone wants to come in and talk about a more general application of the relationship that you have, I don't think it's anything interesting
Oh hmm
Abhijeet Vats:
well
this actually was my conclusion from something
an original exercises asked me to prove that
$\forall X: A^TAX = A^T$ X is pseudoinverse to A
Dovahkiin:
Ah well, that doesn't seem like something i could assist with. I'm sorry 😦
So it's a statement for all X
for all X
for which that thing works
what I previously posted had different X
and was somehow related to this
but maybe it wasn't helpful
I decided to show the original task
anyone have a good tutorial on how to do svd
How can I find the new coordinates of (0,1,-1) if it is rotated by an angle of pi/3 about the line (1,1,1)
I have to find a matrix that rotates by pi/3 about the line 1,1,1
Now I found two vectors orthogonal to (1,1,1). I From this I calculated P. For the diagonal, by we have that the eigenvalue corresponding to (1,1,1) is 1. Setting the remaining eigenvalues as x and 1/x, I was able to calculate the matrix A = PDP-1 as a function of x. Now I just need the value of x.
You're best seeing what happens to the basis
Yeah to see that is why I asked what happens to (0,1,-1) when rotated by pi/3 around (1,1,1)
I tried using the face The matrix A has trace of 1+2cos theta and det(A) = 1 implies det(D) = 1 but to no avail
oof
cool this buut
I also did them
we can you know
compare our solutions or something)
Yeah just let me look through my notes real fast
Post it
$$A^TAX = A^T$$
$Im_A$ is orthogonal to $Ker_{A^T}$ -- since $\forall v, \forall w \in Ker_{A^T}, (Av,w) = (v, A^Tw) = 0$.
Another fact:
\begin{align*}
& (A^TA)(X) = A^T \
& A^T(AX - E) = 0
\end{align*}
meaning that we know $Im_{AX - E}$ is in $Ker_{A^T}$. Now, consider any vector $v$. We have:
$$u = (AXA - A)v = A(XA - E)v $$
and
$$u = (AXA - A)v = (AX - E)Av$$
Conclusion: -- $u$ is in $Im_{AX-E}$, but also $u$ is in $Im_A$, and they are orthogonal hence $u = 0 \Rightarrow AXA = A$.
Dovahkiin:
uu, smart bot
Yeah pretty neat @meager tinsel
Can't really do shit without geometry))
Part is a’s answer is 0.8
Also, I proved it, and then I forgot what was given and couldn't explain it to a friend for like 10 minutes
almost gone crazy haha
@meager tinsel another way to solve it
Wbich is do much simpler
You can just multiply by the inverse of the left side to both sides
(You can do that because At*A is a square matrix)
I will send it to you in a sec
I want that proff other parts I understand
But if you do it that way then you get the equation of the pseudo matrix on the right side
And thats finished
I mean
jsut take a 2x3 matrix with 1 in the (0,3) and 0 everywhere else
and
Yeah but theres a specific requirement for matrix A
Otherwise it doesnt even make any sense for it to have a pseusoinverse
what is it?
Nvm i did the pseudomatrices in a very specific context
in my exercise I had only A is mxn matrix and thats it
Yeah
It has to have max rank
Because generaly you use A for projections
And A is usually formed by the basis vectors of a space
So they have to be linearly independent
Which inplies that A has max rank
oh
yeah in that case yeah
its trivial then though
buuuut
I just
didn't assume anything
Yeah
@meager tinsel but how can you even say ImA when you just have a matrix
Dont you need a linear function
Yeah but then the orthogonality between imA and ker At doesnt apply
It does
Hmm alright, we didnt dive too dip into this area in my course
@violet field this channel is for linear algebra, which is very different from the algebra done at high school
I suggest you post in #❓how-to-get-help
Never did it so i cant help you with that sadly
how do you do projection with gram schmidt
@lone quail my fault it’s health econ, college Economics
Is there a section or similar discord you could push me to
As long as its about maths you can post in #❓how-to-get-help
Oh okay
@odd yarrow the theory behind gram shmidt
Is the following:
Lets say you are in R2
And have vectors, v1 and v2 which span the subspace of W
and what you want to do is find an orthogonal basis of W
then, by taking either v1 or v2 as a reference, you can remove the x or y components using gram shmidt
this is done by removing, for example, the projection of v1 on v2 from v1
so that the result is a vector having only the y-component (if v2 is parallel to the x axis)
what did orthogonal mean again
it means that their dot product is 0 (perpendicular)
so basically by removing the projection of v1 on v2, you are removing from it the component on the direction of v2
so, of course, they would become orthogonal to each other
how did you calculate span again
cos something right?
linear algebra will b the death of me
the span is the smallest set of vectors which fully describe a certain subspace
uh
said simply
that's more a basis
yeah the span is whats generated by the linear combination of said basis?
yeah but it wouldnt make any sense
of course it would
why would it
because the span is the set of all linear combinations of the vectors
yeah
nothing about the definition of span says you need to be spanning linearly independent vectors
okay but don't misdefine terms to do so :/
yeah, its just i have a but of trouble translating from time to time
we dont even have span here xd
ah
well, the span of a set of vectors is all possible linear combinations of the vectors
+1
the span of a set of vectors is always a subspace
@odd yarrow get it now?
just gonna try to make everything into a system of equations and solve it
lol
partial credit hail mary
what was the original question
how do you do projections with gram schmidt
okay. do you know what gram schmidt is
or what it's supposed to do
or when you use it
make it orthonormal
make what orthonormal?
to make a basis orthonormal
the formula for projection of one vector v on another vector u is
$\frac{\langle v, u \rangle}{\langle u, u \rangle} u$
gfauxpas:
where <u,v> means the dot product
if u is a unit vector, the formula is simpler
$\langle v, \hat u \rangle \hat u$
gfauxpas:
to project a vector v onto a unit vector u
yep, then the reasoning is what i told you earlier
you dot product v with u, and multiply that number by u
this only works if u is a unit vector
this simplified formula
Do we know how to calculate complex eigenvectors corresponding to a rotation
any idea how to input lambda into a calculator
just use L
uhh I dont think my cal has that
so use t or x or any other letter
Ended up doing this ffs.....
Any help with this?
Find a basis of the subspace H of R3 spanned by the vectors x1, x2, x3 and use the basis to determine the dimension of H.
x1 = [-1 0 1], x2 = [3 12 7], x3 = [3 6 2]
I think I'm suppose to turn x1, x2, x3 into a matrix H, then find the subsp of H?
@north sandal you can do it that way but there's a shortcut
if all 3 vectors are linearly independent the dimension is 3. otherwise the dimension is lower than 3. can you tell if any of the vectors are linear combinations of the others? can you prove that or disprove that just by looking at them?
how can i prove that this is linear
or show
or show that it isn't
without doing the zero vector trick
why
@north sierra ok so, to show that it is linear
It means that there exists a and b such that f(av+bu)=af(v)+bf(u)
Where a and b are in the real numbers
And v and u are vectors
Go through the axioms lol
just have to try to show one axiom
Try this:
T(av + bu) | aT(v) + bT(u)
|
|
|
|
With a line down the middle
Simplify both sides, and show they come to the same thing
Or that they dont
Exactly. Or, if it fails to, it should leave you with a nice counter example
you can even just do plain T(av)=aT(v) but I like how Kaynex is doing it too
okay i will try this when im home
@quartz compass no you need two vectors
Actually yeah that's not a bad idea split it into those two cases
Because you have to prove the sun too
no lol @lone quail
Sum
that is sufficient
Nope
sorry you're wrong
Show both T(av) = aT(v) and T(u + v) = T(u) + T(v)
no it doesn't, you should work it out yourself
Necessary but not sufficient
For T(av) = aT(v) to imply a vector space
Yes if it fails you can stop
It will fail lol but Elite doesn't know that
I'm saying T(av) doesn't equal aT(v)
But if it succeeds it doesnt tell you anything
which is why that's all you need to do
You need to prove the sum too
obviously, but it doesn't succeed
Yeah but sometimes its not obvious
You need to explain to him that he needs both conditions
Otherwise he will always do that and not know he needs the sum too
lol calm down already
wait is the sub space test and test to show a map is linear the same?
For subspace you have to show that the result of the addition and scalar multiplication is in the same subspace
i know
To show that a map is linear you have to show that it respects the addition and scalar multiplication
but are the same axioms?
The subspace test tests sets
Yes
oh okay
Same axioms but the proofs are just slightly different
A neccesary cond for T to be linear, btw, is T[0]=0'
T(x,y) fails that immediately
in my question right?
they did ask for some alternative to that though, at least that's what I assumed he meant by "without the 0 trick"
Yes
yeah i asked for alternative
Oh
i wanna get good with the other axioms thats why
The properties of a linear map aren't axioms,i wouldn't think of it that way
No, i mean
It's just a property some functions have
If i want to test whether a function is odd
I don't consider the axioms of oddness
Yeah but almost everything you do in linear algebra is based on the fact that said function is linear
So you always basically consider that fact even if you dont do it explicitly
But they're not called axioms, it's the wrong terminology
Yep agreed
You don't say a continuous function satisfies the axioms of continuity
lol true
It's just not the right wording
Anyways im not sure about english terminology so i leave that to you guys xd
property?
Properties
Yeah property sounds good
I'd use definition
okay
Okay perfect 👌
Group axioms...
Who wants a super tough linear algebra question?
I don't see the difference between a definition or axiom personally, but I don't care enough to argue about it
Not me
I know you want it 😉
Anyways for someone who feels confident about linear algebra this is the question
Determine the equation of the surface obtained by rotating the conic gamma in the plane xy, of equation x^2 -2xy+y^2-4x=0, around its principal axis. Classify the surface obtained and determine its geometric properties (axis of symmetry, planes of symmetry, centre and vertex) as well as writing its canonic form.
Tell me if anyone wants the worked out solution
diagonalize the symmetric matrix of coefficients to get the change of basis
Yeah but
although I think it's just a 45 degree rotation so I can do that regardless without doing that
What about the 4x
just let it chill outside
complete the square after rotation
or square(s) I should say
@quartz compass you are getting close but its not 45 degrees
$$x=\frac{u+v}{\sqrt{2}}$$ $$y=\frac{u-v}{\sqrt{2}}$$
You are right about diagonalosong tho
Merosity:
that'd be my guess
of course I'm right
but I'm not gonna work it out cause I am busy, but that guess probably works to remove the xy cross term then you should be good
which is a 45 degree rotation
Why complete after rotation
I'd be surprised if it didn't
And not before
doesn't matter
Hm
do whatever works
I'd do that and use vectors [x,y,1] to catch the constant terms, right?
wait which way are you doing it, to try to catch the constant terms inside the square
yeah, this is why I wouldn't bother with completing the square first
Id get it in the form u²+cuv+v²+constant, idk how else to do it
And use homogenous coordinates
T(av + bu)
nah
what is the b vector?
There's an easier way?
How do i diagonalize with the 4x there
just leave it outside the matrix
Okay
Hmm theres a specific matrix you have to use
So ill do that, then what
$f(x) = x^TAx + b^Tx +c$
Let me send you the matrix
Merosity:
Yes
Merosity:
So the radii stay the same size
that's your transformation
Of the diagonal matrix
$(Px)^T D(Px) + (Pb)^T Px +c$
Merosity:
Ooh
$u^TDu + v^T u +c$
I like it
Merosity:
then complete the squares
Anyways the matrix you gotta use is the one at the bottom of the page
And to transform in canonic form you also gotta do a translation
Idk what canonic form is
You do
Because it has to have centre in the orogin
Or vertex or whatever this conic is
I just explained why you don't
Idk what canonic form is
it's cute but I'm not arguing with you over something stupid a second time
you don't understand what you're talking about I'm afrais
Alright do what you like, do you want me to show you the textbook which explains you have to translate?
What is canonic form?
can someone help me with the linear question i had earlier maybe in another channel 😢
Its basically when the centre/vertex is in the origin
And you use canonic vectors
Im just saying you cant get to the right answer without a translation because thats not what canonic form is about
The canonic form of a conic is specific
For a conic to be in canonic form it has to have centre/vertex in the origin
@north sierra anyways go ahead
Whats the issue
hey
gonna post again
so like i wanna use the addition property
and test it
not sure how to start
Check this example
This is doing both at once but you should be able to extrapolate what to do
the thing that confuses me is the T(x,y)
idk i dont get that example
F(v+u)=f(v)+f(u) for addition
So that means take a generic vector v
x,y
And a generic vector u
x’,y’
so in my case what would the u vector be?
x’,y’
Any values
x`+5?
Like this
As you can see you cant go forward
@north sierra
Anyways im getting some sleep now its past 1am here
It feels very iffy because that's the second time I did the problem and my previous answer was different.
I think it's all good @wintry steppe
Had to cut my name out
lol
Yes, this is correct
Thanks @half osprey and @uneven bloom !
np
Is there a shorter way to get to the same (or even a slightly different) simplification?
A(A^2(BA)^(-1))^T=
A(AB^(-1))^T=
A(AB^T)^T=
ABA^T=
-ABA
Lol I made it so convoluted
As long as it’s valid, it’s fine
@north sierra
Still looking for it?
for what @half ice
T(x,y) = (x+1,y+1)
Try this:
T(v + u) | T(v) + T(u)
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Each are vectors in your space. You're working in R² right now
but what about T(x,y)?
T is a transformation that takes in a vector from R² and outputs a vector from R²
yeah
You can call such a vector (x,y). I called it v instead.
Well, any arbitrary vector can be represented as either (x,y) or v
or u
These are labels that are simply names for the object we're working with
Plus if I write them all as (x,y) it's gon get messy
Well, I suppose you have to.
so for addition we need to do something like $T((x1,y1)+(x2,y2))?$
The-Elite:
Yes exactly
ohh so instead of writing $T((x1,y1)+(x2,y2))?$ you let v = (x1,y1) because itll be messy?
The-Elite:
Can you write that without a T?
I write T(u + v) = T(u) + T(v) because it conveys the additive definition no matter what vector space we're actually working on
But fair, you need to put in (x1,y1) in order to simplify it
T[(x1, y1) + (x2, y2)]
= T(x1 + x2, y1 + y2)
= (x1 + x2 + 1, y1 + y2 - 1)
That simplifies to that
Follow how I applied the transformation?
ok
Can you do that one? It's not bad
okay
should i include the x1, x2 in the transformed one ?
T(x1,x2) = x1 + 1, y1 - 1
T(x2+x2) = x2 + 1, y2 - 1
?
or remove the 1,2 thing
Yes we want to work with these where they are not the same vector
oh ok
You should have T(x1,y1) and T(x2,y2) and yes include the 1 and 2
Yus, that's T(x1, y1) + T(x2, y2)
yeah and if it's a linear transformation that is supposed to equal T(x1+x2,y1+y2)
Well one of the steps atleast
But the other condition is alot easier to show
im confused on adding these
Remember when adding two vectors in R² you just add their components
$\begin{pmatrix}x1+1\ y1-1\end{pmatrix}+\begin{pmatrix}x2+1\ y2-1\end{pmatrix}$?
The-Elite:
Can also write them like that yeah
$\begin{pmatrix}x1+1\ y1-1\end{pmatrix}+\begin{pmatrix}x2+1\ y2-1\end{pmatrix}:=:\begin{pmatrix}x1+x2+2\ y1+y2-2\end{pmatrix}$
The-Elite:
earlier we had $\left(x1:+:x2:+:1,:y1:+:y2:-:1\right)$
The-Elite:
Now you're getting it
lol
T(u + v) ≠ T(u) + T(v)
like?
However, what we did could have proven T is a linear transformation
And counterexamples can't do that
(But T isn't a linear transformation here so the result is good)
