#linear-algebra
2 messages · Page 7 of 1
Ann:
so it has a dimension
ok
and from the fact that $\sum_{i=1}^{n-1} x_i v_i = u$ has a unique solution (this is taken straight from the problem statement), you can deduce right away that ${v_1, ..., v_{n-1}}$ is linearly independent, and so $\dim(\mathrm{span}{v_1, ..., v_{n-1}}) = n-1$
Ann:
ok
following you
ok its not a proof we have done yet but i can deduct it from a n+1xn matrix with a unique solution has a unique solution to every free variable.
uh i get what youre digging at
wait lemme type out what im thinking
$x_{1}v_{1}+ ...+x_{n-1}v_{n-1} = u$ has a unique solution, therefore $x_{1}v_{1}+ ...+x_{n-1}v_{n-1} + tw= u$ also has one unique solution t = 0, because it if had more it would imply a solution exists to $x_{1}v_{1}+ ...+x_{n-1}v_{n-1} = w$
lemme fix up the tex
kakamaika:
therefore they span the field
▮?
$x_{1}v_{1}+ ...+x_{n-1}v_{n-1} = u$ has a unique solution, therefore $x_{1}v_{1}+ ...+x_{n-1}v_{n-1} + tw= u$ also has one unique solution t = 0, because it if had a solution $t\neq 0$ we can do $\frac{1}{t}(x_{1}v_{1}+ ...+x_{n-1}v_{n-1} + u)= w$ and insert our unique solution to the first equation giving us a unique $x_{1}v_{1}+ ...+x_{n-1}v_{n-1} = w$
kakamaika:
I... think this is tight?
and then i just need to show a unique solution to that carries spanning the field since we havent proven that yet
man im dumb it cancels out when u moves sides
still works tho cus then it would imply t = 0 which we can easily show is not possible i guess
$\mathrm{span} { v_1, ..., v_{n-1} } \subsetneq \mathrm{span} { v_1, ..., v_{n-1}, w } \subseteq \bbR^n$
Ann:
$n-1 = \dim \mathrm{span} { v_1, ..., v_{n-1} } < \dim \mathrm{span} { v_1, ..., v_{n-1}, w } \leq \dim \bbR^n = n$
Ann:
@viscid apex $\dim \mathrm{span} { v_1, ..., v_{n-1}, w }$ is forced to be $n$, and that can be argued as above
Ann:
you really don't need any of those fussy arguments there lmao
kidna need it cus ithink your relying on proofs that we havent done yet. weve just touched spanning
huh?
i mean
$V \subseteq W$ implies $\dim V \leq \dim W$ for any vector spaces $V, W$
Ann:
that's really the most complicated thing i'm relying on
$\mathrm{span} { v_1, ..., v_{n-1} } \subsetneq \mathrm{span} { v_1, ..., v_{n-1}, w }$ follows immediately from the problem statement since $w \notin \mathrm{span} { v_1, ..., v_{n-1} }$
Ann:
i know and I understand the logic but if I put this on the exercise its gonna raise eyebrows a bit
how come
because its obviously not something I could have come up on my own
$n-1 = \dim \mathrm{span} { v1, ..., v{n-1} } < \dim \mathrm{span} { v1, ..., v{n-1}, w } \leq \dim \bbR^n = n$
kakamaika:
this is the part thats giving me troubles
we havent really defined dimensions properly yet and neither span (of vectors)
anyhow thanks
@dusky epoch
what would you define dimensions as
might have one and im not understanding the term
i know a span is all possible linear combinations
the dimension of a vector space is the number of vectors in its basis (over the base field)
nah we dont have that
...its a bad program dont tell me about it its not out of choice that im learning here
well probably go over all this in a month or ill go over it next week if i have time
thanks anyhow ill insert my fiddly answer for now
@dusky epoch what 's the diff between $A^T,A^\dagger,A^\ast$
flimflam:
idk if there's actually any T, might just be a truncated dagger
@jagged pendant
@tranquil ermine are these all adjoint notations
@evеryone
yeah i took a peek in the book this is all talked about in a month or so
applying the Gram Schmidt process is easy, but how do I check if the obtained set is orthonormal in a single matrix multiplication step, especially since the inner-product is not the standard dot product in R^n (and instead is the weighted inner-product) ?
(simply checking if the columns form an orthogonal matrix doesnt work in this case)
hang on, i think i've got it. we can check if E^T W E = Identity or not
Yep, the diagonal elements of EtWE are (ei,ei) and the other elements are (ei,ej)
You could also just calculate (ei,ei) and (ei,ej) separately instead
hey guys! how do you guys determine if vectors lie on a plane?
and how do guys determine if those vectors lie on a line?
ex.
v3 would lie on the plane formed by v1 and v2 if v3 is a linear combination of v1 and v2.
The vectors lie on a line if they are a linear combination of just one other vector.
as for actually finding out if they are linearly independent or not, I would just write v1,v2, v3 as column vectors in the matrix [v1 v2 v3] and put that matrix in row echelon form. That way, if there is any linear dependence, it will be nice and easy to see
@slow scroll so basically, if vectors are linearly dependant, it lies on a plane
or a line
and if v1 = cv2, it lies on a line?
yes
so u can have vectors that lie on planes but not on lines?
sure. cv1 + dv2 where c!=0 and d!=0 are all vectors that lie on planes but not lines
what is a way that i can say that those vectors do not lie on a line?
as in, since there are no scalar that can make v1 = v2, these vectors do not lie on a line
yea u could say that
v1 is not a linear combination of v2 or v3, and v2 is not a linear combination of v3, so none of the vectors are linear combinations of each other
if you put the the vectors in a matrix, and put the matrix in row echelon, one row will zero out if one of the vectors lie in the plane spanned by the other two vectors, and two rows will zero out if two of the vectors are linear combinations of each other (lie on a line) @wintry steppe
np
Hello guys, is II and III the correct statements?
if (II) is correct then (I) must be as well 😛
Since A is a square matrix of order 4, can I say that its row space has dimension 4?
4 different vectors
no, just because A is a square matrix of order 4 does not by itself mean its row space has dimension 4
because the row space is determined by the subspace?
what you just said is nonsensical
sorry im quite lost, not sure why if A is a square matrix of order 4, it doesn't by itself mean that row space has dimension 4
because the dimension of the row space of A is equal to the rank of A
what does rank of A means?
i mean ok that's kinda the definition really
the rank of A is defined as either the dim of its row space or the dim of its col space (those are always the same)
but like for example the row space of the zero matrix (of any size) is {0} and so has dimension 0
or for a less trivial example, the dimension of the row space of $\begin{bmatrix} -1 & 5 & 1 & 3 \ -1 & 5 & 1 & 3 \ -1 & 5 & 1 & 3 \ -1 & 5 & 1 & 3 \end{bmatrix}$ is 1
Ann:
is that why order 4 doesn't necessary mean dimension 4
unless we know the values of the entries, we can't tell the dimension base on the order correct?
beyond knowing that the dimension can never be greater than the order, yes, we cannot say anything
Thanks! For this question, what does orthogonality has got to do with subspaces?
Think R^3 first
check whether V, as defined in the problem, is a subspace of R^4
Maybe it will help you understand the problem from a geometric perspective
how do I check without knowing the values
Two vectors $u,v$ are orthogonal if their innerproduct $\langle u,v \rangle = 0$, if I remember correctly
markus:
yes
So you need to check if the set ${\mathbf{v} \in \mathbb{R}^4 : \langle \mathbf{u}, \mathbf{v} \rangle = 0}$ is a vector space
markus:
subspace*
to check whether something is a subspace you show that it satisfies the definition of a subspace
of R^4
if you don't know what a subspace is, go back and read your notes
or just check the easiest: If v and w is in V, is then v+w also in V? Why/why not?
See here for an example of subspace check, you are basicly just checking certain axioms. Many of them are inherited by V just being a subspace of some bigger vector space
subset
there are only two things to check for subspaces
closure under addition and closure under scaling
Show it is closed under addition.
Show it is closed under scalar multiplication.
Show that the vector 0 is in the subset.
you don't need the third thing
it follows from the other two
(and nonemptiness)
it's a good exercise to prove that
That the 0 vector is in V is very easy to verify here tho
it is, but it's extraneous to do so
Yeah ofc
Nice problem btw Ann ^
Or exercise, dunno if those words are synonyms or not in mathematics
how am I gonna check the conditions without knowing the exact values?
Take $u,v \in V$. What properties do they have?
markus:
dot product of u and v equals 0
Oh bad notation, because u is the vector everything in V is supposedly orthogonal to
so lets take v,w instead
yeah u is fixed
Yeah, so if $u+w$ is also supposed to be in V, what should you verify then?
markus:
v+w
dot product of v + w and u equals 0
Exactly
Now, how can you manipulate the expression $\langle v+w,u \rangle$ algebraicly?
markus:
(this comes down to one of the axioms of inner products)
how the dot product is defined?
yeah, like how do you for example calculate $u \cdot v$ if u and v is in R^2
markus:
Compile Error! Click the
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$ \left< x+y, z \right> = \left< x, z \right> + \left< y, z \right>$
Ann:
Now you’re giving it away 😦
u1 v1 + u2v2 = 0
Yes, correct
So why should the formula Ann wrote over be true
It says that $(v+w)\cdot u = v \cdot u + w \cdot u$
markus:
for vectors $v,w,u$ in some euclidean vector space
markus:
And what can you then say about the dot product of v+w and u using that formula?
You are very close!!
that the condition for it to be subspace is satisfied
Yes, or it is closed under addition
Now, the only thing left to prove is that $(av) \cdot u$ is in V
markus:
it doesn't satisfy the condition
markus:
dot product of v and u equals 0 as defined earlier
but if its av and u, it might not be 0
?
No, remember what $(a \overrightarrow{v}) \cdot \overrightarrow{u}$ actually means!
markus:
oh, v is not fixed
It is $av_1u_1 + av_2u_2 + \dots$. Now, factorize out $a$, what happens
markus:
?
yeah but how do we determine its dimension
Okay, R^4 is hard to think of geometrically, so to get a intuitition for what the dimension should be, lets first go down to R^2
If you’re given a vector in R^2, what does any orthogonal vector to it have as angle to that vector?
what is the angle between two orthogonal vectors in R^2?
90
Yes! So what do that vector span out?
R^2?
No, thats not quite right.
Imagine $u$ being the vector $u=(1,0)$. Then any orthogonal vector to u needs to be a vector on the form $(0,a)$. Agree?
markus:
okay, so what do all vector on the form $(0,a)$ span out in this case?
markus:
Where can you go by adding those?
straight line through origin
exactly
And what is a straight line to the origin
What vector space can we think of as that?
R^2?
No, what is a straight line?
Remember R^2 are tuples of two points
Remember, to span out a straight line you only need one basis vector. How many basis vector do R have, and how many do R^2 have?
R^2 has two basis vectors?
one
straight line
1
Perfect!
Okay, so know we know that in R^2 the vector space V consisting of orthogonal vectors to u have dimension 1.
Lets move up to R^3.
If $u=(1,0,0)$, and which form is the two other (linearly independent) orthogonal vectors to $u$?
markus:
Think geometrically of the axis
(0,1, 0) , (0, 0, 1)
markus:
R^2
Yes great job
wow
So what vectors are orthogonal to $(1,0,0,0)$ in R^4?
markus:
Compile Error! Click the
reaction for details. (You may edit your message)
Yes great job dude!
thank you!!! can I ask a few more questions? these are the ones where I'm not sure
go ahead
Just happy I could help @dull kettle
For this question, my answer is I is false, II is true but I'm not sure about III
what does it mean for u not to be in span(S)?
yes indeed I is false and II is true
in terms of linear dependence, I mean
what does it mean for "u does not belong to V"?
V is a subspace of a larger vector space
so you can have vectors which are in the larger space, ℝ⁵, but not in V
oh, is statement III true then? since you want span(S) which has dimension 3 and u which has dimension 1
@dull kettle $u \notin V$
Ann:
so what would span (S U {u}) be? 3?
span is not a number
it’s a space
the span of S union {u} is the set of all vectors you can get to by linear combination of those vectors in S union {u}
sorry i meant dimension of span (S U {u}))
well, that’s what we have to find out, right?
so, u is not in V
so u is not in Span(S)
(becasue V = Span(S) by definition of a basis)
right?
yes
so can u be linearly dependent with the vectors in S?
no
why?
its one of the condition for basis
yea but you don’t know if S union {u} is a basis yet
here’s a quick argument
let’s say S = {v1, v2, v3}, right?
ok
now, if {v1, v2, v3, u} was linearly independent
then you could find coefficients a1…a4 with
a1*v1 + a2*v2 + a3*v3 + a4*u = 0
by definition of linear dependence
agreed?
yes
now you can solve that for u, you’ll get
u = -a1/a4 v1 - a2/a4 v2 - a3/a4 v3
so u is actually in the span of S
but we know it’s not
contradiction
therefore, {v1, v2, v3, u} is linearly independent
and as such the basis of a 4-dimensional subspace
you mean "if {v1, v2, v3, u} was linearly dependent" instead of independent right?
yes
yes, sorry
how does u = -a1/a4 v1 - a2/a4 v2 - a3/a4 v3 shows that u is actually in the span of S?
what does u have to be for it not to be in the span of S?
0?
what does it mean for u to be in the span of S?
it was written above
u = -a1/a4 v1 - a2/a4 v2 - a3/a4 v3
so u is actually in the span of S```
no, forget about that. can you give me the definition of "u is in the span of S"?
it belongs to the span, so span(v1, v2, v3, u)
what is a span?
consists of all the linear combinations
so what does it mean that u belongs to the span of {v1, v2, v3}?
u consists of linear combination of v1,v2 and v3
and have you found such a linear combination?
yea sorry bad phrasing
u = (-a1/a4)v1 + (-a2/a4)v2 + (-a3/a4) v3
and yes there's such a linear combination
For this question, I and II is true but i'm unsure about III
Statements I and II are correct, am I correct?
does your course consider real/complex vector spaces only, or over arbitrary fields as well?
(if you don't know what i'm talking about it's likely the former)
former it is then
thanks! can you look at the question above the latest one, i'm tryna make sense of III
can't see how does random non zero vectors would give me basis for solution space of Ax = 0
yeah they might not even be LI
and if they aren't LI they aren't gonna make a basis for anything
okay, in the same question, for statement I, is it false? since say if the solution space is {v1, v2, v3} then v1 + v2 would be not in the solution space anymore
for \textbf{any} matrix $A \in \bbR^{m \times n}$, the set of solutions to $Ax = 0$ will \textbf{always} be a subspace of $\bbR^m$
Ann:
and you should check that
sorry but how do I check it?
use the definition lmao
let $x$ and $y$ be such that $Ax = 0$ and $Ay = 0$, and let $c$ be a constant.
Ann:
is it true that $A(x+y) = 0$? is it true that $A(cx) = 0$?
Ann:
yes and yes
voilà
thank you! @dusky epoch
oh btw @dusky epoch the reason you have to check 0 in a subspace is to ensure nonemptyness
A(0) = 0 o:
yea I know, but I listed three properties to check that sth is a subspace and ann complained that 0∈W is redundant
cause you can prove it from x-x
but what if there is no x
the empty set isn’t a subspace
fair fair o:
and I just remembered why you need it
so yea technically you don’^ have to check 0∈W, but you have to check something ∈ W
and 0 is usually the easiest anyway, so you might as well
yeah in linear algebra 1, our definition of a vector subspace was for it to be non-empty + other two
whereas in linear algebra 2, our definition of a vector subspace was for it to contain 0 + other two
which as you mentioned, are obviously equivalent
I wonder if there's any reason to why someone people prefer one over the other
our definition was “a subset which is a vector space with the same operations”
the other characterization was a theorem
I would have prefered that tbh, makes more sense chronologically o:
.> makes me wonder how many other 'definitions' I know are just conveniences
our definition for a matrix was “a rectangle with numbers”
lol
our definition for a matrix was "a map {1, ..., m} x {1, ..., n} -> R"
where R is the base ring
wait what
That's a way to formalize the same idea
The image of (i,j) is the i,j coordinate of the matrix
oh
yea, fair
did you do linalg over general rings?
ie did your linalg course just straight up do modules?
we started with modules yeah
well that’s certainly a curious approach
and then used that module theory to build our way up to JNF and all that jazz
Jordan form = trivial corollary of STFGMPID
at my school you only really study modules if you take commutative algebra
STFGMPID?
what an abbreviation
wehre we proved the classification theorem for finitely generated modules over PIDs
which may be STFGMPID come to think of it
Yup
what’s the S? structure?
Yeah
I’ve seen different versions of that interestingly
Lmao I love how I can just say that and people can guess what it means
the one we proved was that $$M \cong R^n \oplus R/(a_1) \oplus \dots \oplus R/(a_m)$$ where $a_i$ are neither units nor zero, and $a_1 \mid a_2 \mid \dots \mid a_m$ and $m, n, (a_i)$ are all unique
Sascha Baer:
the proof was really weird tho
and I couldn’t really follow it
it suddenly involved a bunch of linalg over PIDs, which we’d of course never done
Smith normal form?
he did a thing where he found some matrix representing a module homomorphism, and then did something akin to gaussian elimination to it
Yeah that's Smith normal form
It's where you have a "diagonal" matrix and a_{ii} divides a_{i+1 i+1}
@dusky epoch wait, you started linear algebra with modules? o.0
that sounds... really unconventional
we also had rings before groups 😛
in soviet russia 

tbh, we had fields before groups
but it's not like we talked about any real field theory, just field theory about the reals
... I'm sure that makes sense lol
Spivak chapter 1? 😛
we also had rings before groups
in Algebra
but we’d already seen both in linalg and analysis anyway
we just did ring theory first
Can anybody here explain what M-matrix and Stieljes matrix are? they confused me 😦
we had like…
in linalg:
-groups, rings and fields: definitions and most basic properties
-vector spaces
in analysis:
-ordered fields
in algebra:
-ring theory
-group theory
-field extensions and modules (only very brief intro each)
-galois theory (ongoing)
the linalg and analysis stuff was in parallel and took place within the first two weeks of the course
algebra was one semester, except galois theory which is algebra II
Can three vectors be LD in r4?
of course; even a set of one vector can be linearly dependent
@wintry steppe only if it's zero lol
@dense holly one salient point is ever pairing can be lin independent but the set as a whole can still fail to be linearly independent
matrices and vectors and all that shit
algebra
its algebra, but its linear
well a lot of LA is derived from the concept of creating linear functions between vector spaces. Linear functions are functions that satisfy f(ax_1 + bx_2) = af(x_1) + b(fx_2)
and those functions are the main link between most subfields of linear algebra
like matrices for example
.... and vector spaces are just sets along with the operations of scalar multiplication and addition. An analogy would be f(x) = x^2 + x as a function which takes a real number input under the operations of addition and multiplication. (Sets under multiplication and addition are called fields.)
Think of mathematical vectors and vector spaces as like a super generalization of physics vectors
Yeah a function is just something that assigns an input to a unique output
can i ask question here? i saw the almost full moon today. and i was wondering if there is a way to calculate where on earth i have to stand to look up and be directly under the moon when it's completely full. i'm sorry if i ask it in the wrong place. just really curious
sounds like #geometry-and-trigonometry
but als you would need the moon's ephemerides
i.e numerical data on where the moon is
the basic idea with spectral theorem is selfadjoint operators on a nice enough Banach space are unitarily similar to a diagonal operator?
for complex ips
@honest swift is this the gist of it?
or is it not that simple once you're not fdvs
It is not that simple. Without an inner product what is unitary? Are your operators bounded?
Even defining self-adjointness in general requires some care when operators are unbounded, as they often will be.
(Note that symmetric and self-adjoint are not interchangeable terms in this setting.)
does anyone know riemann notation for distance between 2 points in a non euclidean space?
take the infimum of the lengths of all smooth curves joining your points, with curve length being defined using the Riemannian metric and integration.
its some kind of ds=dx²+dy²+dz² but a liitle more complex with news terms
mb
@honest swift was gonna just assume compact operators, and you still have an inner product
You said Banach, not Hilbert.
Compact self-adjoint is the nicest case basically.
Banach with its specified norm induced by ip = Hilbert more precisely.
is the norm ever not ip induced
yes, not all banach spaces are hilbert spaces
thanks charles catto
oh ya

can you induce the supremum norm with an inner product?
nope, try to prove this.
🐱
You could use Riesz rep and say try to show it isn't reflexive
Wait actually actually LMAO
I have the best proof for this
Everyone get some popcorn
So, subspaces of reflexive spaces are reflexive, right?
Well, it turns out every separable Banach space embeds as a closed subspace of C[0,1]
So to show C[0,1] is not reflexive, we just have to show that some separable Banach space isn't. L^1
@honest swift what do you think?
Lol that's a good one.
It's definitely gonna be easier to use just the parallelogram law if you wanna show C[0,1] isn't Hilbert but is it easier to show that it's not reflexive?
I guess you can use Eberlein-Smulyan and ask whether the unit ball is weakly sequentially compact
i'm dumb someone please check #prealg-and-algebra
Please don't message channels other than the one you posted your question in
:(
Anyway I think the dual of C[0,1] is the space of signed Borel measures by Riesz rep? So we'd wanna find a sequence of functions f_n, let's say of sup norm 1, so that no subsequence converges weakly
Wait hmm so to converge weakly you need that every measure works, so let's be ballsy and say x^n with Lebesgue measure
Darisal:
Tbh this idea now that I think about it isn't too far off from embedding L^1 in it
Yeah will think about this another day @proper crescent , have just gotten home after 6 hours of grading hooman noobery.
Lmao, isn't this a break from that? 😛
But yeah I'm just thinking out loud more or less
Also wait I love how this is in linear algebra, some poor first year is gonna wonder what it's all about and then a barrage of words flying around
Haha kind of, but I don't want to look at any math for a little while :p.
Lmao yeah.
I don't like thinking of the dual of C[0,1] so I'm gonna try something else
Wait actually if C[0,1] were reflexive, then it would be separable + reflexive, so the dual would be separable as well
That would imply the unit ball of C[0,1] were weakly metrizable which feels very wrong, also I just don't think the space of signed Borel measures on [0,1] is separable
Oh wait a sec
LMAO
Just take dirac masses
Yeah gg
🐱 👍
is this where we deal with vectors?
i just wanna check if i'm doing some things right
Yeah there are vectors in linear algebra haha @warped sinew
A lot of the basis of linear algebra is based on vectors
yes the basis hAha
xddddddd
hey guys i have a question regarding eigenvalues
so my eignvalues are 2 and 3
and i got x1=1 and x2=1
but x2 is supposed to be negative one
<@&286206848099549185>
this is for my eigenvalue of 3
i got
,, \begin{pmatrix}-1&1\ 0&0\end{pmatrix}\cdot \begin{pmatrix}x_1\ x_2\end{pmatrix}=\begin{pmatrix}0\ 0\end{pmatrix}
0031:
idk
same
not me
i watched like 2 vids on this so idk
Doesn’t that mean the solutions are on a plane or something?
the set of solutions is a plane
i think
X1=x2 So V(3)=span of 1,1
do you ever care about the complex conjugate untransposed or the transpose not complex conjugated with complex matrices?
also is there any standard notation if so
I have two vectors D and N (direction & normal_of_collision)
I want to calculate a correction vector that is perpendicular to N and is based on the direction D points.
Does someone know how to do this?
ummm
you want a vector in direction orthoganal to N
but you also want it to be based on the way D points?
this seems contradictory my dooooood
Figured it out
project D onto N and subtract it from D
@lean aspen just like, $\overline{A}$ for conjugation
Sascha Baer:
Compile Error! Click the
reaction for details. (You may edit your message)
I don’t think you would care about it a lot, but I mean it can still be useful to have notation occasionally
conjugate-transpose doens’t have stnadard notation, I’ve seen at least three different notations
$A^*, A^H, A^\dagger$
Sascha Baer:
$\overline{A}^T$
Ann:

$\overline{A^T}$
Sascha Baer:


this is not linear algebra xd
multiply both sides by 7
More proof that "linear algebra" is an incredibly unfortunate name
Though I don't really have a better proposal
"matrix algebra" is too specific and obscures the motivations, while also not really being correct
they should just change the name of this channel to "vector space math" or something
Maybe "algebraic representations"? Nah nvm that sounds clunky af and too broad
Uhhh
Anyone have an idea how to do 1?
@wicked trellis
The left side is A¯¹b
So, you're given that
[1]
A¯¹b = [2]
[3]
Multiply on the left by A:
[1]
b = A[2]
[3]
And thus, that's your solution to Ax = b
Thanks 😃
Np. Feel free to ask if you have anything else!
So multiplying a matrix by its inverse will equal 1?
Oh ok
Hey guys I need some help on my hw, here is a picture of one of my many questions I’m confused about
Ok
Have the characteristic polynomial?
umm lol should that be given?
If you don't that's k we can find it
I don't know it
A - Ix =
[2-x 0 -3]
[-1 -1-x -3]
[1 3 6-x]
The characteristic polynomial is the determinant of that.
There we go. That's the polynomial
okay so from there where do we go in my problem?
Also going to need that
Now, I don't know what lemma 1 is. Your book must make a reference to it
Well, it's easy to check if these matrices satisfy the lemma, but I'm not sure where they come from lel
Let me look it up
Oh thank god Ann is here
@wicked trellis the identity matrix plays the role of 1 in the world of matrices
Know how to get E1 and E2 from the info above?
Makes sense :))))))
I have no idea
this class has put me in the fetal positions and kicked me to the point right before death
And as quickly as Ann arrives, she leaves. Mysterious
lol
Lel I'm jk of course
what are the E_i in Lemma 1?
We already have the partial fraction decomp, but I'm not sure how to use that to get E1 and E2
I've been trying to look that up but can't find it?

Im sorry guys it looks like I've stumped ya but thats what fun about math, right?
Of course! It's an interesting question and I've never seen the method before
I was able to understand this class until wk 9 but now i'm in week ten and completely lost
Yeah, if you have any name attached to this, it would make it ez to look up
strange
Does this help?
this is the best I got
I tried to look this up but I think my professor makes his own material
so is that what you needed?
oof sorry i don't have the energy to do this rn
thats okay can I come back later?
sure
okay thank you

For b) I can see that the matrix would have to have two columns, but its not really obvious to me whether such a matrix with these properties exists, and if so, how i would find it 
rank-nullity theorem
Okay then what?
rank = 1
nullity = 1
rank + nullity = 2
it seems like all rank-nullity can do here is tell me how many columns the matrix would have to have, not whether it exists or how to find it :/
yeah, and yet your matrix is supposed to be 3 by 3
why cant it be 3x2?
in other words, if my matrix is 3x2, the span of its columns is a subspace of R2? Im confused.
sorry, i mixed it up
i meant its nullspace
a 3x2 matrix represents a linear transformation from R^2 to R^3
Can gauss elimination have different solutions at the end or is there only one solution?
The rref form of a matrix is unique if that’s what ur asking
No, since rref is another ref
dam that's sound logic lol thanks
similarly, the inverse which you can compute via gaussian elimination is also unique
and LU-decomposition is unique if you force one of the matrices to have only ones on the diagonal, iirc
LDU decomp is unique if L and U are forced unitriangular then
big help pls
I subtracted lambda at diagonal
but I get scuffed polynomial
-λ^3 + 6λ^2 - 12λ + 8
when checked in calculator the eigenvalue is 3.26 which is weird
it doesnt distribute on linear components 
maybe I screwed up matrix B: I typed it as: first row(2,2,0), 2nd row(1,2,2), 3rd(0,-1,2)
yeah
and a matrix M
I made matrix psi in standard basis
first row(2,2,0), 2nd row(1,2,2), 3rd(0,-1,2)
and like to find Jordan matrix of B I would need like an eigenvalue
what's B
M(psi)st
never seen this
which basis, the only basis here is the canonical basis of R^3
yeah
M is just notation for matrix of transforamtion psi in these basis
what
its not a multiplication
then what does "and let M = ..." mean
yeah the notation here is scuffed, the other matrix should be named differently, its needed for another question
yes that seems correct
yeah, so it has only 1 eigen value 3.26
what are its roots?
that's not correct
Let V be a subspace of Rn. Suppose that B = (b1; ..., br) is an orthonormal basis of V . Prove that for all v, w ∈ V , [v]B * [ w]B = v * w.
how do? 
@wintry steppe split v and w into a linear combination of elements of B
then use orthonormality
and linearity of *
So I have one exercise where I need to determine whether there exists basis A, such that matrix of transofmation in that basis equals M(a given matrix). We also are given matrix of the transforamtion in standard basis, lets call it B. I checked that B and M have the same Jordan matrix, so there exists such basis A, but how do I find vectors of this basis? R3
Okay so on 7.14, it seems like it is obviously possible for complex matrices, since 7.13 serves as an example (assuming i did the question right), but I am having trouble with real matrices. If I can just find a symmetric matrix such that A^2 = 0, then this would be easy, but I can't come up with one nor prove that there can't be one. Any hints?
the set that contains all Mn that are invertible, has a null element? (n = nxn, n being a integer)
in (b) my immediate intuition is to claim that Qv = - reflV*reflV so Q(v)=-v
is that correct?
when 1 is not an eigenvalue of A
spec being the eigenvalues?
yes
hm, actualy, yea wait, that seems reasonable
so let’s assume A is diagonalizable first
then $A = Q^{-1}DQ$
Sascha Baer:
why not jordan it lol
fair actually. repalce D with J
$I - A = Q^{-1}(I - J)Q$
Ann:
and so $I - A = I - Q^{-1}JQ = Q^{-1}Q - Q^{-1}JQ = Q^{-1}(I - J)Q$, which is invertible iff J has no 1 on the diagonal
Sascha Baer:
indeed.
i mean there's a less nukey argument tho
A - I invertible iff det(A - I) != 0 iff 1 not in spec(A)
determinant doens’t play well with addition tho so how does that follow?
If you know that adding I increases the eigen value by 1, yot can say it nore elegantly without det
@broken hawk how does what follow
I don’t know how to show that without invoking JNF
the fact that det(A-I) != iff 1 not in spec(A)
aka adding identity changes all eigenvalues by 1
oh. right. and we just added another I in, so λ+1
Hi I'm doing linear independence, but I'm stuck on doing gauss jordan elimination when there's a variable involved... my vectors are (1, 1, 2, -4), (1, 2, k, -5), (1, 5, 3, -8), I made a matrix
[ 1 1 1 0]
[ 1 2 5 0]
[ 2 k 3 0]
[-4 -5 -8 0]```
Doing elemination until
[1 1 1 0]
[0 1 4 0]
[0 k-2 1 0]
[0 0 0 0]
``` but now I'm stuck
<@&286206848099549185>
try to make your matrix diagonal
you can for example subtract the first col from the second and from the third, thereby zeroing out the first row
and then zero out the second row by subtracting 4 * the second col from the third
you'll end up with $\begin{bmatrix} 1 \ & 1 \ & & 9-4k \ & & & 0 \end{bmatrix}$
Ann:
how does $a_{23}$ become 0
GyroW:
the one left of 9-4k that is
err
you're right sorry it doesn't
i messed up
well basically it all now hinges on whether 9 - 4k is zero or not
if it is zero then your vectors are LD bc the rank of this matrix is 2
if it is not zero then you can zero out a_23
moin
plus
I have an exam in which I'll have to compute some least-squares polynomial fits
that gives a linear system of equations
but I can only do that with a simple calculator that doesn't uhhh have much stuff tbh
is there an approximate method to solve such a linear problem?
something that I could do more or less easily with a simple calculator
HYPE, but uhmm wrong channel lmao
for any given nxn matrix, is the detA^TA always >0 ?
$\geq 0$
Tuong:
but not always >0
when would it be 0
When A isn't inversible
oh well yea mb, i was asking for whenever its invertible
can some1 help me find an example of this: a 3×3 invertible matrix A such that A^3=0
I don't think there exists any
me neither i cannot think of anything where this would work
if A is inversible and A³=0, then
A¯¹×A³=A¯¹×0
A²=0
A¯¹×A²=A¯¹×0
A=0
but 0 isn't inversible!
yes
ok, i just one more, im a little confused by the wording of the question: cant there be no determinant for an mxn matrix, what do they mean by working through m=1>?
There's no question in this
Do you have to prove the statement?
I've found a counter example
A = [0, 1]
with $A=[0\ 1],\ \ \det(A^TA)=\begin{vmatrix}0&0\ 0&1\end{vmatrix}=0\ \
\det(AA^T)=|1|=1$
Tuong:
but isn't there no determinant for mxn matrices anyways?
yeah yoiur counterexample makes sense
i just thought we could immediately say its false because its an mxn matrix, but i get it
AA' and A'A are always square
oh i see
Hey y'all, anyone able to help me out with this?
I managed to show that they commute but nothing more
Any help would be really appreciated :)
B = xI + yP
A = aI + bP
AB = (aI + bP)(xI + yP)
= (ax + by)I + (ay + bx)P
= x'I + y'P
So if two matricies are of the form aI + bP, then their product will be. Multiplication by A can be seen as a linear transformation:
[a b] [x] = [x']
[b a] [y] [y']
The inverse of that matrix can be seen as a multiplication by A¯¹
@ruby crow
OH. I don't know why I didn't factor by I and P lol. That's perfect thank you
Oh, and you need to recognize that I is of that form, that helps
Np. Feel free to ask if you have anything else

Hi guys, none of the statement is true, am I right?
how does i affect its orthonormality
but what if u1's coordinates consist of negative number
in this case yes, because c1 is positive
in general it has the same sign as c1
thanks!
@dull kettle $w \cdot u_1$ is literally equal to $c_1$
Ann:
wow
thanks @dusky epoch overlooked that part in my notes
how do I tell how many blocks will be in a jordan matrix? and also their size
oh
there's actually a really beautiful method to do that
so what i assume is that you've already fully factored your char poly
(and if you haven't you should bc the method makes use of that)
@winter reef are you here? this is gonna take a little while to fully explain so i want to make sure you're here
yep!
alright good
I remember it being about the rank
ohh so like rank of subspace of eigenvalue
so just to fix some notation, let $A$ be the $n \times n$ matrix whose jordan form you're interested in, let $\lambda$ be an eigenvalue of $A$, $s$ be $\lambda$'s algebraic multiplicity (i.e. its multiplicity as a root of the characteristic polynomial of $A$), and $B = A - \lambda I$
Ann:
we're going to be interested in the ranks of powers of B
so what you want to do now is make this table:
$\begin{array}{c|c} k & \operatorname{rk}(B^k) \ \hline 0 & n \ 1 & \ 2 & \ \vdots & \vdots \end{array}$
Ann:
and fill in its right column
you should get a descending sequence of numbers
and you should continue that until it stabilizes at $n - s$
Ann:
umm I remember doing similiar but with a kernel
this is basically using images instead of kernels but it's essentially the same just dualized
well you can brute-force it by just finding elements in the kernel of B^k until you can’t find any more
but it’s tedious and to get the change of basis matrices you have to find cycles
anyway, continuing with what i wrote, $\operatorname{rk}(B^{k-1}) - \operatorname{rk}(B^k)$ is the number of Jordan blocks of size at least $k$
Ann:
hmm so I kinda see, but using kernels we were multiplying the matrix by itself until it was a zero matrix, then take any vector and find a vector that is in kernel of the one before minus the kernel of the next one kinda
so I see the similiarity of your way
and why do we multiply the matrix until n-s?
ohh is it because then it will be a matrix diagonal on n-s x n-s and rest are zeroes?
not quite.
so here's the thing
if two matrices are similar (i.e. are related via a change of basis matrix), then their rank sequences are the same
and if you write out the jordan form of A, then the blocks corresponding to λ will take up s positions
and accordingly the jordan form of B will have s zeroes where A has λs
so that block of the jordan form of B will be nilpotent
but the other blocks will stay full-rank no matter what power you raise them to
and so won't give you any rank reduction
wait what does jordan form of B will be nilpotent mean?
you parsed my sentence incorrectly
i said that that block of the jordan form of B is what's going to be nilpotent
ohh ok I found it, I just didnt know the term 'nilpotent' but I see now
yeah kinda makes sense, I'm gonna have to think about it more to get it, but thanks for your time!
What do you mean n×n (0,1)?
Like a matrix over mod 2 arithmetic?
The determinant gives invertability of a system. So stuff breaks when matricies have zero determinants
As well, it's easy to find the determinant of a product of matricies, without even needing to compute the product itself, so you can reduce computation time with clever implementations
Np. I also have other examples lol. Matricies control a lot of computation
if A is an nxn invertible matrix with entries that are all integers, and its determinant is 1, does that mean all entries of the inverse matrix of A are also all integers? how do i show tht
There's a cofactor formula for the inverse
The idea is that you divide by the determinant, so if it's just +/- 1 you're fine
@proper crescent ik it works if its +-1, but here its just saying that its 1
its not including -
That's a special case
@formal knoll just ask your question and if someone can help they'll answer
let's say i have A dot B =C which are all in r3. And we have b and c, how would you solve for vector A?
A dot B is in R, not R^3
a and b are in r^3
Okay so, the next issue is that there's more than one vector A which works
No problem! 👍
Is there a extra problems floating around regarding college functions and models?
What's college functions and models?
Westchester Community College’s Course Catalog including course descriptions and academic program information
Yeah
So that question should go under #prealg-and-algebra instead
can anyone help me solve q13? not sure what i'm suppose to do here. ty
<@&286206848099549185> ^ sorry it's a pretty easy question
@wintry steppe still here?
ya hi n.n
So for 13a, do you notice something about these vectors?
Or actually better idea
Look at 13b as a hint
What does 2:00 have to do with 8:00?
aren't they opposite
8 is -2?
Yeah
(To avoid ambiguity we should write x:00 since 8 and -2 could be interpreted as scalars)
But alright, so now when we add all the vectors on the clock, if v appears, -v appears later, right?
i'm really not sure how to get them into vectors in the first place, really new to this, is 12 = (0, 1) and 3 = (1, 0), then 1 = (1/3, 2/3)
Yeah technically you'd get them in coordinates but for the sake of this problem the better thing is to just say that we know that if x:00 corresponds to some vector v, then (x+6):00 will correspond to -v, and that v+-v = 0
So this way we don't have to do 12 different computations, you know?
by x:00 what do you mean
x o'clock, what you call x
oh lol sorry
I don't like referring to 2:00 as 2 because the issue is that 2 is also technically a scalar and there's cause for confusion
Anyone able to help?
Chances are that won't become an issue for us here, but in any event yeah that's why I'm using the notation I'm using
@tall bridge we're in the middle of something here, and that's not linear algebra, ask in #prealg-and-algebra or a questions channel
oh i think i get it
Also for fuck's sake post in one channel and then stop
oh wait so the answer would just be the zero vector
Yup! 😄
🆙 | ronnie has given @proper crescent a reputation point!
😃
Somehow 😃 on discord looks more like :D than 😄
Anyway tackle 3b using the same geometric ideas
@proper crescent wait so with b), the reason it sums to 8:00 is there's no -8:00 (2:00) to negate it, and the rest of them sum to 0?
Exactly
👌 ty n.n
Now part c is basically asking the angle between the 12:00 vector and the 2:00 vector, right?
Close, remember the full circle is 2pi, not pi
but isn't 2:00 just 30 degrees?
It's a third of the way to 6:00, right?
i'm not sure I understand that part
My point is that it's gonna end up being 60 degrees instead of 30. Do you buy that the angle between 12:00 and 2:00 should be one third of the angle between 12:00 and 6:00?
What's the angle between 12:00 and 6:00?
180 is pi
omg sorry i'm being stupid tonight lol
It's fine, so now you're with me that 2:00 is (cos(pi/3), sin(pi/3))?
isn't that the angle between the horizontal and 1
Right right I was measuring off of 12:00 for some reason
You were right the first time
Sorry
Yup you're good
👌 great ty for all the help
hello, how can I prove that given a permutation matrix P, there exists a number k, so that P^k = Identity matrix?
how familiar are you with group theory
somewhat familiar
and have you encountered what are called permutation groups?
you mean cyclic permutations for example ?
Ann:
sound familiar?
yes that rings a bell, in matrix (3x3) permutation the group of all permutations has 3! matrices I believe
and I understand that if you apply one permutation over and over again, eventually you will end up at the starting position
or is this not always the case?
well i mean... it's a consequence of Lagrange's theorem in group theory that in a finite group G of order n, raising any element to the n'th power produces the identity
in your case, your group is the group of all permutation matrices, of order n!, which is of course still finite
I'm still not sure how I can prove this mathematically. I am attending an introductory linear-algebra course and I guess it should be quite simple



