#linear-algebra
2 messages · Page 271 of 1
One out of 9 questions in a 2.5hr test.. just doing that one question is 30mins
try doing gram schmidt w/o a calculator...
especially when you get complex numbers and square roots
Nice
Hi, how do I show that $AA^{*}$ is a symmetric matrix?
I have to show $(AA^{})^{T} = AA^{}$.
So: $(AA^{})^{T} = A^{^{T}}A^{T} = \bar{A}A^{T}$
I am stuck here.
mate
Yeah, I am an idiot. Thank you.

17 a or 18a?
17 a
4-3=1
4 times 2 is 8, not 4
yeah realized that after typing it...
yes, 2R2+R1 goes to R1
ty
Yo
Consider the zero vector in R^n, the dot product of zero vector with v_i is 0, so less than or equal to 1.
@halcyon spindle we cant have zero vectors
v_i can’t be zero but your set can take any vectors that satisfy the inequality.
Yep.
Yep.
For the second problem consider make all the vectors the same and require it to be unit length.
So you end up dealing with just one set for the intersection.
Thanks for the help man i appreciate it. a) was so much simpler than i thought
Since norm(v_i) = 1, remember v_i • x = |v_i||x|cos(theta)= |x|cos(theta). The inequality says less than or equal to one so it must be |x| <= 1, so your set ends up being a unit disk or something. From that finding a bound for the set would be easy.
hey i m not verry familiar with sigma notation someone could help me to understand how he would change <x,y> in that form
Just realize that doesn’t really works
duchat
I'm trying to proof that the set of functions $${1,e^x,e^{2x},\dots}$$ is linearly independent on $C[0,1]$ without using the Wronskian. Our prof told us to prove it similarly to how it's proven for the set $${1,x,x^2,\dots}$$ She started by setting $$p(x) = a_0 + a_1x + \cdots + a_nx^n$$ and then factoring $p(x)$ into its roots, $x_1,x_2,\dots ,x_k$, with $k\leq n$ : $$p(x) =(x-x_1)(x-x_2)\cdots(x-x_k)q(x)$$ where $q(x)$ is a polynomial of degree less than $p(x)$ with no zeros on [0,1]. Since $p(x)$ has finitely many zeros, then $p$ is not identically the zero function on [0,1] , so ${1,x,x^2,\dots}$ is linearly independent.
duchat
however, how can I prove that $$p(x) = a_0+a_1e^x +a_2e^{2x}+\cdots + a_ne^{nx}$$ has finitely many zeros on [0,1]?
duchat
I was thinking maybe taylor expanding each of the exp(nx) terms into polynomials, but you need an infinite amount of polynomial terms, so I'd be making hand-wavy arguments with infinite quantities
Suppose that $\sum_{j = 0}^n a_j e^{jx}$ is identically zero. This should hold for every $x \in [0, 1]$ (you can extend this to $\mathbb R$). Multiply both sides by $e^{-nx}$ and see what happens when you let $x \to \infty$.
opengangs
I guess you can show it holds on R
which means that it also holds on a subset of R
what does it mean to say b is a linear combination of a1 & a2?
b=c1·a1+c2·a2 for some scalars c1 and c2
looks like what I'd've done
Cheers!@
So I have a homework question that I am a little stuck on. Stating this so no one solves the thing for me, but I'm confused as to where I go from here.
It's probably the wrong way of going about it. I figure you cannot solve for s or t unless you reduce the augmented matrix down.
Unless I substitute the values that $$s=x_1-x_4$$ and $$t=2x_2+2x_2-4x_4$$ throughout the matrix initially and see what comes out?
MrMadium
it would first be best if you got it down to Reduced Row Echelon Form, then you are able to use simple checks to see what values of s and t will make the system consistent
Can anyone tell me what this symbol means ?
Thanks Khazali - I couldn't quite see if it were possible but I'll give it another crack to get it to RREF
$\begin{vmatrix} y_{1} & x & x & \dots & x \ x & y_{2} & x & \dots & x \ x & x & y_{3} & \dots & x \ \vdots & \vdots $ \vdots &\ddots & \vdots \ x & x & x & \dots & y_{n} \end{vmatrix}$
mate
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- Does anybody know how to fix my TeX? 2. Could somebody help me solve this determinant?
$\begin{vmatrix} y_{1} & x & x & \dots & x \ x & y_{2} & x & \dots & x \ x & x & y_{3} & \dots & x \ \vdots & \vdots & \vdots &\ddots & \vdots \ x & x & x & \dots & y_{n} \end{vmatrix}$
you've got a stray $ in the middle of your matrix code
remove it
$\begin{vmatrix}
y_{1} & x & x & \dots & x \\
x & y_{2} & x & \dots & x \\
x & x & y_{3} & \dots & x \\
\vdots & \vdots & \vdots &\ddots & \vdots \\
x & x & x & \dots & y_{n}
\end{vmatrix}$
here
mate
$\begin{vmatrix}
y_{1} & x & x & \dots & x \
x & y_{2} & x & \dots & x \
x & x & y_{3} & \dots & x \
\vdots & \vdots & \vdots &\ddots & \vdots \
x & x & x & \dots & y_{n}
\end{vmatrix}$
mate
Thank you very much, Ann! I am still a beginnee, so I apologize.
let $D(x; y_1, y_2, \dots, y_n)$ be the determinant you're looking for (with arbitrarily many arguments after the semicolon; the matrix will be sized accordingly)
Ann
$D(x; y_1, y_2, \dots, y_n) = \begin{vmatrix}
y_{1}-x & x & x & \dots & x \
0 & y_{2} & x & \dots & x \
0 & x & y_{3} & \dots & x \
\vdots & \vdots & \vdots &\ddots & \vdots \
0 & x & x & \dots & y_{n}
\end{vmatrix} + \begin{vmatrix}
x & x & x & \dots & x \
x & y_{2} & x & \dots & x \
x & x & y_{3} & \dots & x \
\vdots & \vdots & \vdots &\ddots & \vdots \
x & x & x & \dots & y_{n}
\end{vmatrix}$
Ann
$$\implies D(x; y_1, \dots, y_n) = (y_1-x) D(x; y_2, \dots, y_n) + \begin{vmatrix}
x & x & x & \dots & x \
0 & y_{2}-x & 0 & \dots & 0 \
0 & 0 & y_{3}-x & \dots & 0 \
\vdots & \vdots & \vdots &\ddots & \vdots \
0 & 0 & 0 & \dots & y_{n}-x
\end{vmatrix}$$
Ann
$D(x; y_1, \dots, y_n) = (y_1-x) D(x; y_2, \dots, y_n) + x(y_2-x)(y_3-x) \dots(y_n - x)$
Ann
and as the base case, $D(x; y) = y$ (a $1 \times 1$ matrix with $y$ as its only entry)
Ann
$D(x; y_1, y_2) = (y_1 - x) \cdot y_2 + x \cdot (y_2 - x) = y_1y_2 - x^2$
Ann
$D(x; y_1, y_2, y_3) = (y_1 - x) \cdot (y_2y_3 - x^2) + x \cdot (y_2 - x)(y_3 - x) \ = y_1y_2y_3 - xy_2y_3 - y_1x^2 + x^3 + xy_2y_3 - x^2(y_2+y_3) - x^3 \ = y_1y_2y_3 - x^2(y_1+y_2+y_3)$
Ann
hm...
Thank you so much, Ann! Could you briefly explain what did you do here?
applied linearity in first row and came up w/ a recurrence relation
thanks :)
How can I test to see if a system of equations has no solution?
I've gone through a number of iterations of substitution and the like and I just cannot figure out how to solve $$x_1, x_2, x_3, x_4$$
MrMadium
Running through my calculations above, I just cannot see what I am doing wrong, other than running some kind of check to see if there is in fact no solution.
Unless $R_4$ (the bottom row) being all 0's means that there is an infinite amount of solutions?
MrMadium
why do authors keep inventing symbols
wdym, everyone knows the Lasagna operator
more seriously, maybe lagrangian, if these are like adjacency mats
but you'd have to read the text around it to know for sure
Conciseness of notation
Is there some standard definition of what it means for a polynomisl to be invariant under some kernel?
context?
In Hemker's paper on the order of prolongation and restriction operators for multigrid there's a part where he states that invariance implies
$P_k(x_k) = \sum_j c_j P_k(x_{k-j})$
criver
where P_k is a polynomial of degree <= k, c_j are the kernel coefficients, x_k is supposedly kh, where h is a constant
Is this definition standard or is it something that Hemker came up with
I am not sure whether his definition is equivalent to the above or whether the above is just a consequence of the invariance
That is, I want to find a rigorous definition of this invariance property
Hello, I have an equation here that I'm confused about
so in the last part it says exp{(-1/2)z'z}
what does the ' symbol mean on z'?
transpose probably
my guess is transpose like in matlab
but also this looks like statistics rather than linear algebra
You get the dot product
you get the dot product of z with itself yeah
@spare widget im looking at your paper and i cant find the equality youre mentioning
It's in the proof
There's a proof towards the middle/end
Where the author proves the relation between the high/low orders and the degree of the polynomials kept invariant
ctrl+f: If the restriction stencil
If the restriction stencil [c_j] leaves all polynomials...
hmm
criver
Which would imply what the author has (i.e. the special case x = x_k)
I have no idea though because I haven't seen this terminology used elsewhere
Even the multigrid books and articles I have read, so I thought it may be something from linear algebra (e.g. function being invariant wrt some linear operator)
For instance something like
$f = \sum_j c_j T_{-jh}(f)$
criver
The reason I am trying to figure this out is because I am trying to derive restriction/prolongation operators on irregular grids and with high order
So I thought it would be best if I understood the regular grid low-order case first
I guess a more general question would be:
Given offsets h_j are there coefficients c_j such that for any polynomial of degree <=k and any x it holds
$P_k(x) = \sum_{j}c_j P_k(x - h_j)$
criver
Sounds very similar to requiring a basis/frame
I still don't get it either
If the above is true though (provided enough coefficients) then my problem is probably solved
$a_1x + a_0 = c_1(a_1(x-h_1) + a_0) + c_2(a_1(x-h_2)+a_0) \ a_1 = c_1a_1 + c_2 a_2 \implies \sum_j c_j = 1 \
a_0 = (c_1 + c_2) a_0 - c_1h_1 - c_2h_2 \implies \sum_j c_jh_j = 0$
criver
Seems correct for linear as long as these conditions hold
Hopefully it generalizes to higher degrees
$a_2x^2 + a_1x + a_0 = \sum_{j=0}^{2}c_j(a_2(x-h_j)^2+a_1(x-h_j)+a_0) \
a_2 =\sum_j c_j a_2 \implies \sum_j c_j = 1 \
a_1 =\sum_j c_j(-2a_2h_j+a_1), , a_2 \ne 0 \implies \sum_jc_j h_j = 0\
a_0 = \sum_j c_j(a_2h_j^2 - a_1h_j + a_0) \implies \sum_j c_j h_j^2 = 0$
criver
I actually remember some criterion like that in the proof in Hemker's paper, so it likely generalizes to:
$\sum_j c_j = 1 \ \sum_j c_j(h_j)^i = 0, , i \in {1, \ldots, k}$
criver
criver
I think those equations can also be derived by trying to equate all derivatives
what are some examples to infinite dimensional vectorspaces?
sequence space, function space
C[0,1]
all infinite dimensional vector spaces are isomorphic to K^X where K is some field and X is some infinite set.
Doesn't this depend on the flavour of infinity of X?
e.g. countably vs uncountably infinite
infinite dim vs has way more flavour thn finite dim ones
okay then what's L^2[0,1] isomorphic to
what cardinality is your X
Let B be a basis for L²[0,1]. (Such basis can be shown to exist using Zorn's Lemma). Then the cardinality of X is the cardinality of B.
oh yeah and how are you going to work with that monster of a basis lol
i won't
Is a more explicit characterization of this cardinality known to be independent of ZFC? Or is that unknown?
L² is hilbert space of dim ℵ_0
since you can find an isometric isomorphism from L²[0,1] to l²(ℤ)
R is a vector space over Q with a dimension of א if im not mistaken
uncountable dim, yes
aleph? which one?
Cardinality of R (my professor just used א for it, I guess it's supposed to be א_1?)
aleph1 sounds more like it
yeah makes sense
Wrong
Cardinality of R is not necessarily aleph1
look up continuum hypothesis
is the matrix for an orthogonal projection in R² onto y = -2x
$\begin{bmatrix}\frac{1}{5} && -\frac{2}{5} \\ -\frac{2}{5} && \frac{4}{5}\end{bmatrix}$
/
Alison40
oh so
Sorry it not neat, I had a pencil crisis that time.
i see
i mean
hm
not sure where i went wrong
probably mixed up the simultaneous equations
tbh
Yeah maybe.
When we have a vector space V with a inner product <,> defined, we can define a metric from this just by f(x,y) = \sqrt{<x-y,x-y>}, but there doesn't seem to be a way to reverse this and define a inner product off a metric. I think this is because of the added 'structure' that inner products give a set (bc of linearity?) but I don't know how to show this formally. not v clear on it either tbh would appreciate an explanation of why this is (lmk if this isn't appropriate for this channel)
you should be able to come up with a counterexample, i.e. make a metric that does not satisfy the definition of an inner product
for example, the inner product is linear
but a metric like d(x,y) = 0 if x=y, 1 otherwise
does not satisfy linearity
@gilded ivy
oh I was thinking discrete metric lol
but doesn't this leave open the possibility that we could define smth off the metric (like we did w the inner product) and get something that's linear?
yes, but it also shows that in general this is not possible
some metrics may have this property arbitrarily, but in general they don't
giving a counterexample proves the statement was false
the social distancing metric
shoulda been 1.5 then

if your metric satisfies
\begin{itemize}
\item $d(x+z, y+z) = d(x,y) \quad\forall x,y,z\in V$
\item $d(cx, cy)=|c| d(x,y) \quad \forall x,y\in V \qq{and} c\in K$
\end{itemize}
then it can work as a norm
what
what IS that
wtf is happening
$\qq\forall$
Ann
Compile Error! Click the
reaction for more information.
(You may edit your message to recompile.)
$a \qquad \forall$
Ann
it should be z instead of c in the first line, ryu
but why 4 ∀s 
hm is that translation invariance and scaling
idk what the second one is called
in addition to that, if your metric satisfied trapezoidal eq then it can also be used as an inner product
something like positive homogeneity
ye maybe
(try proving them
)
positive homogeneity of degree 1?
what's K here? a field?
that's kinda the thing, it's homogeneous when c is real and +ive
but in general it isn't homogeneous
at least i THINK that's what the def means
yes R or C
I'll look at this a bit more after I finish this problem set ty
@lavish jewel absolute homogeneity
makes sense, idk why i had never seen the term
Guys is there a method to reduce a third degree polynomial?
Oh thats interesting. I didnt know that. Thank you!
find exact solution to equation thnx
$$\begin{bmatrix} 7 &11 &9 &0 &158\ -67 &13 &11 &1 &32\ 0 &i &\pi &6 &\frac 9 7\ 2 &3 &3 &0 &17767\end{bmatrix} X = \begin{bmatrix} 6\ 1-i\ 0\ 7-2i\end{bmatrix}$$
Carla_
Can’t you just do row reduction on it?
Ok I see, let me grab my paper.
thank you ^w^
@wintry steppe are you trolling rn or what
Wolfram gives exact
sus
Also the matrix looks invertible. You could use Cramers rule
the matrix is literally 4 by 5
,rotate @wintry steppe I got it into REF, the rest should be easy for you.
omg thank you so much 💆♀️
bruv
im just impressed
carla is always trolling just so you know
never not a troll
that's insane
i admire your dedication
I would’ve factored a 7 out of R1 i think
I assume the inner product is just the classic dot product
which in fact becomes ez
Because orthogonality depends on the choice of the inner product, right?
The Hermitean dot product, but yeah.
show that the entries of AA* can be written in terms of inner products in the canonical basis
and yeah, as tropo says, it'd be v*u
oh yea
it might help to note that AA* is a hermitian matrix
it's just $\sum_{k=1}^n a_{i,k}\overline{a_{j,k}}$
remove the space before the second $
I was just a bit confused because it didn't specify the choice of inner product, but I realized it should of been obvious
Croqueta
which is basically multiplying the row vectors with the dot product.
already matrix mult can be interpreted so that the entries of the resulting matrix are inner products of rows from the left matrix and cols from the right matrix
just use that and play around with complex conjugates
Does Linear combination mean that two or more vectors are "Linearly combinable", meaning that if you multiply them with scalars and then add the vectors, you can get any vector by doing that.
no. linear combo simply refers to the result of those operations
if each vector in a given space can be written as a linear combo of a given set of vectors then the set is said to span the space
Then why do people say that any vector in R3 och R2 can be constructed, i keep hearing that.
R2 and R*
constructed in terms of what?
idk two vectors that are what i call "linearly combinable"
Those two can then form any other vector by simply first multiplying, and then adding them together
i think theres missing info
take the set of vectors {(1,0),(0,1)}
each vector in R^2 is a linear combo of these vectors
ie the set spans R^2
Ok so two vectors can span a smaller area than R2?
yes, like (1,0),(2,0)
what is their span
the x axis
And a span can be thought of as a plane in space right?
That is the set of all linear combinations of two vectors
if by plane u mean 2 dimensional space then no. the last example shows that spans can possibly be 'degenerate'. (1,0),(2,0) spans the x axis, a line
in 3d, depending on the vectors in a set, it can span either the origin, a line, a plane, or all of 3d space
in 3d, spans can either be the origin, a line, or all of 2d space
Thanks
no prob
What are all possible inner products of the vector space R over Q?
wait
I realized inner products are only defined for vector spaces over R or C (I think, or at least those are the interesting ones)...
the same definition can work for over subfields of C tho, idk if its interesting tho
There's ordinary multiplication of reals, and that multiplied by a positive constant, and then there are wild things that depend on the axiom of choice for their existence.
I ask because if we define a function $f\colon \mathbf{R}\to \mathbf{R}$ by $f(x)=\langle x,y\rangle$ where $y\in\mathbf{R}$ and where $\langle ,\rangle$ is an inner product then $f$ satisfies Cauchy's functional equation
Cauchy's functional equation being $f(x+y)=f(x)+f(y)$
Croqueta
So I was wondering if there were some funny solutions
(If you want a rational output from the product, I think there's only the wild things).
output need not be rational, but if it's rational it's still fun I suppose
I know over the reals there are weird solutions to Cauchy's which LA can tackle, but the ones I've seen are just some hamel basis manipulations, with the aid of maximum principle and so on, which I guess you can interpret with inner products anyway
Croqueta
I think the properties of an inner product basically forces it to have that form (i.e. Hamel basis shenanigans).
btw I meant inner product, not linear product xD
probably but I don't know tbh
I'm not really sure how crazy Hamel basis shenanigans can get
They're basically all crazy. The solutions to Cauchy's functional equation that are not simply multiplication by a real constant, all have graphs that are dense in R^2.
dense means that if you were to represent the graph in a plane then the whole plane would be covered by ink?
There'd be ink arbitrarily close to every point in the plane, yes.
uhm
there are solutions which involve Hamel bases which are more friendly I think. Let B be a basis for R over Q. Let $x,y\in B$, $x\neq y$ and define $f\colon B\to R$ by $f(x)=y$ and $f(y)=x$ and $f(z)=z$ otherwise. Then find a linear map $\phi$ (which exists with some work) such that $\phi(u)=f(u)$ for all $u\in B$
Croqueta
Even phi restricted to the span (over Q) of {x,y} will have a dense graph.
ohhh gocha
Basically we have phi(a)=ay/x when a is a rational multiple of x and phi(a)=ax/y when a is a rational multiple of y. These two lines grow far from each other for large a, and each has a domain that is dense in the real line. So if we want to find an a close to 0 where phi(a) is about 1000000, just find the place where the two lines have a vertical distance of 1000000, pick rational multiples of x and y close to that point, and subtract them.
And we can do that whenever there is a pair of x and y such that phi(x):phi(y) are not in the same ratio as x:y.
Question on infinite-dimensional vector spaces: let $V$ be an intinite-dimensional vector space and let $S={s_1,\dots}$ be an infinite subset of $V$. We say $S$ is linearly independent if and only if, for any finite set $M\subset\mathbf{N}$, $\sum_{k\in M} c_ks_k=0$ where $c_k$ are scalars, implies $c_k=0$ for each $k\in M$, right?
Croqueta
Right.
thanks
Your formulation assumes that S is countably infinite, but you can repeat the same thing for uncountable sets to ask if they're lineary independent. Just index the c's by the basis members themself instead of by numbers.
Right
Yeah true
Since you have touched on uncountable sets, does the concept of a conditionally convergent but not absolutelly convergent series over an uncountable set makes sense at all? @fringe fjord
Let $X$ be an uncountable set and let $f\colon X\to R$ be a function. A sum $\sum_{x\in X} f(x)$ which is conditionally convergent but not absolutelly
Croqueta
probably the wrong channel to ask this, idk
No, I'd say "conditionally convergent" doesn't make much sense unless the index set is specifically N.
that's what I was thinking
You need to be able to speak of partial sums.
It is very problematic, because the elements of X are not listable and because Riemman's theorem on conditionally convergent sums
If the sum is absolutelly convergent it makes sense though, because there are at most countably infinite non zero terms in the series
In general, unless f is zero on all except countably many inputs, all bets on giving it a sum will be off.
Yes.
by "off" you mean going to infinity?
No, I mean in the everyday sense of "all bets are off" = "there's no hope at all".
yeah
it's crazy
In fact ^
(related to the previous discussion)
oh although finitness is assumed
Everything is nice in finite dimension. :-)
very nice
this doesn't work in the context of infintie dimensional spaces?
probably not
Suppose $V$ is a vector space over $C$, $B$ an orthonormal basis for $V$ and $g\colon V\to C$ a linear map. Let $y=\sum_{b\in B} \overline{g(b)}b$. Take $x=\sum_{b\in B}c_b b\in V$. Then [ \langle x,y\rangle =\langle x,\sum_{b\in B}\overline{g(b)}b\rangle =\sum_{b\in B}g(b)\sum_{q\in B}c_q\langle q,b \rangle=\sum_{b\in B} g(b)c_b=g(x) ]
What is wrong about this when V is infinite-dimensional?
Croqueta
@dapper gorge there's a few problems
One of them might be the assumptions that B exists and that y is in V
-
existence of an orthonormal basis in infinite dimensions (not sure how big a problem this is, but gram-schmidt won't suffice)
-
y is not well-defined (are you trying create some infinite sum here?)
if V is infinite then that's an infinite sum, sure
infinite sums of vectors are not defined
addition is an operation you can apply only finitely many times. You can't talk about infinite sums of vectors without some notion of convergence
since you have a basis, you just need to keep track of the coefficients of the basis vectors in the partial sums, and then apply typical real analysis stuff
you can define them in this way I suppose
but it is still problematic
btw, there is a generalization of this to infinite dimensions. idk much about it, but its called riesz representation theorem. I don't think its quite a one-to-one generalization of the finite dim case. You need something like a hilbert space iirc
Wait, I might not have understood you. What you were saying is that if we have an infinite basis $B$ for a vector space $V$ and if we fix scalars $c_k$ for eack $k\in B$ then $\sum_{x\in B} c_xx \not\in V$ if infinitely many of the $c_k$'s are non zero ?
Croqueta
right, its just not defined. addition is an operation that we only know how to iterate finitely many times inside a vector space
I see
Like the polynomial space is infinite dimensional but $\sum_{n=1}^\infty x^n$ is definitely not a polynomial
yep exactly
Thanks
npnp
Croqueta
Guys, what's the correct notation to indicate that I am referring to the matrix in it's row reduced form?
There's no generally understood symbolic notation for that. Say it with words.
HeyMilkshake
ref A
i don't think that's like super standard notation, but everyone will know what you mean if you write ref A or rref A
Has anyone seen this before to represent it?
HeyMilkshake
i haven't. I prob wouldn't use that on a hw assignment unless your professor also uses that notation. A grader wouldn't be able to figure out what you are talking about as easily as with ref/rref
I just saw it in some book that I can't remember
but yea
maybe ref / rref is the most understandable thing to write
determine whether the set is a
subspace of the appropriate Rn.
it says subspace, but i get not subspace
How do you get that?
It's impossible to tell what you're doing wrong unless we can see what you're actually doing.
can you tell me how to go about solving it
pls show how u got 'not subspace'
A subset of a vector space is a subspace iff it is closed for linear combinations
is there a resource to practice proofs involving determinants? cant seem to find many resources online
@peak plinth still here?
Just take a random linear algebra book and try to prove every theorem about determinants yourself before reading the proof
Guys what is an example of scalar product which is non the classical scalar product? I know that scalar product is define as tX * y but what is an example of scalar product which is non the classical scalar product
Do you want it to be in R^3 or in any vector space?
Well can you do both or it is a problem?
You can define it like that for example in a space of continuois functions
And this is another possibility for R^3
You can also define a dot product on R^3 by stating which 3 vectors form an orthonormal basis
Perhaps it will also help to know that in english they call the standard scalar product "dot product" and the generalised scalar product "inner product"
Well i'm trying to understand and i am studying vocabulary to do this subject in english and i'm sorry but i come from italy
Thank you guys
Yes I wrote it because I suspected you didn't know ot and though you will find it useful :). I'm from slovenia and I also have a hard time learning english vocabulary at times
how do I find [T]^B_E?
the way I tried was doing T(b1)
and then trying to find [T(b1)]_E
but wouldn't it just always be the same?
because its the standard base?
or am I doing something wrong?
Hi, guys, the bijection betwen linear map from V to V and matrices exists only when i fix the bases of V? If I do not fix the bases, then there is no bijection between linear map and matrices?
yes
I won't say NO, but to define a isomorphism, you do need a fixed basis
otherwise it makes zero sense
Thanks!
how the standard of basis E of R3 is (1, 1, 1)?
oh not R^3
Is this a viable real vectorspace?
check it satisfies the vector space axioms
I'm confused by the first statement
what about it troubles you?
which real number lambda has this property
no no, they are telling you this is how scalar multiplication works in this set
so for any lambda, that is what it will do
yes, i know
forget about usual multiplication
wait what
they are telling you all scalar multiplication behaves this way here
this is not any set you have ever worked with
they made it up for this example
scalar multiplication and vector addition don't work the way you are used to, they are defined in this new, special way
e.g. if lambda = 5 and we want to compute 5*[x;y], we will get [5x, y/5]
ok got it
and so on
cool
1.5.19 a
Correct me if I'm wrong but we know that the set of invertible matrices is open
So isn't this question trivial?
Also, the sequence $A_n=\frac{n-1}{n}I$ can do for approximating I since we know $I-A_n$ is invertible and $(I-A_n)^{-1}=n \times I$
DarQ
Yes, mostly trivial. You should probably appeal explicitly to the fact that A \mapsto I-A is a continuous mapping.
which might depend in subtle ways on how you've defined a topology on Mat(2,2)
Could I get a quick sanity check? A skew symmetric matrix has identical row and column spaces right?
sorry for interrupting
Yes, since each row is minus some column, and vice versa.
Thanks 🙂
Hi everyone, stupid question: I have a casio calculator and im trying to do 1-cos(0.04), the calculator is prompting with 2.136*10^-7 instead of 0.00079 ? Any ideas why is giving me the wrong answer?
thanks!
What to do when I don't have free variables to calculate a basis?
What are you trying to do with that that matrix?
I want to find a basis
For what? A matrix is not something that in and of itself has a basis.
Probably something involving the rank-nullity theorem.
Unless you already know that the rank of a matrix and its transpose are equal. (But then there's not much to prove at all).
Hey everyone, any book recommendations on Numerical Linear Algebra apart from Golub and Van Loan? Something that covers well: SVD, LU, QR... these classical matrix decompositions... thanks!
(hope that's ok to ask, I got no answer in #book-recommendations )
I don't think it is @brittle gyro
You can repeat your question in #book-recommendations tho
Please try staying on topic as much as possible
I am learning linear algebra on my own. I don’t know where to start in order to solve the matrix. It feels a bit like trial and error. Is this normal?
It’s as if im doing random operations without any logical reason
I don’t know where to start
Turn it into upper triangular
Why is this not a subspace?
Look up row reduction, getting that augmented matrix in row echelon form.
We have the zero in R^3 is not in there.
MrMadium
Once you're done with the first column and only the first row has a value in it, move onto the second column etc.
Thus, reduced row form (as @halcyon spindle said)
I'm going to ask a stupid question:
Is x1 and x2 in the formula below both 1? I'm doing my first diagonalisation and my brain is failing me at the current second.
Thus:
(x_1 = \begin{bmatrix}1\1\end{bmatrix})
MrMadium
x_1 being the eigenvector, not the solution variable.
Anyone? Would really appreciate the second pair of eyes on it. I am soooo sleep deprived!
Any vector (after getting the matrix to parametric vector form) that is, after plugging in lambda, is considered a eigenvector. For a matrix A of size n, there should be n eigenvectors.
A combination of those eigenvectors can then be represented as a eigenspace, if each eigenvectors is linearly independent.
can anybody help explain this to me?
my text book doesn't explain this lesson well, for a vecto to span a set, the linear combination must be a consistent system?
if i may ask?
span is just the set of all linear combinations
Yes, but to tell if a vectors spans a set, there must be a solution in that case?
solution to ..?
the matrix of the linear combination, sorry I am not referring to this question, just in general
linear combination = (c1v1+c2v2+...+cnvn)
notice that in your problem, you can rewrite x_1 as a linear combination of y and x2, ... , x_k
since you are given that a_1 cannot be 0
yes, y can be written as a linear combination of a1x1 + a2x2 + .. + akxk
im confused, how does a1/=0 come into this equation?
well you can rewrite it as y - a2x2 - ... - akxk = a1x1
see where i'm going? (y - a2x2 - ... - akxk)/a1 = x1
yest, so you substitute positions
it shows that x_1 can be written as a linear combination of this
now use that to show that the spans are the same
becauyse a spannning set is the set of all linear combinations
yes
given that matrices and the algebra defined form a vector space, how can one explain the set of basis matrices
matrices with 1s in a single entry and 0s elsewhere
those form a nice basis
@granite wolf
and it’s M x N dimensional?
right
okay thank you :)
more specifically: a basis for $M(m\times n, F)$ is ${E_{i,j} : 1 \leq i \leq m, 1 \leq j \leq n}$, where the $(k,l)$-entry of $E_{i,j}$ is $1$ if $i=j,k=l$, and $0$ otherwise
TTerra
is the relationship between a linear operator and its expression with a matrix in some basis that you just defined analogous to the relationship between an arbitrary vector and it’s expression in some basis
somewhat
does there exist an operator that acts on matrices then ?
like matrices do on vector spaces
well i mean yes
$F^{m \times n}$ is a vector space in its own right so it is very much possible to define linear operators to and from it
Ann
one example of a \textit{named} linear operator would be trace, which acts on $n \times n$ matrices and returns the sum of the diagonal entries
Ann
oo okay okay
but that maps from the matrix to the real numbers
matrices turn vectors into other vectors
well i guess linear operators do technically
idk it’s late
@granite wolf matrices can represent linear maps but thats separate from this
i think it’s pretty closely related
@granite wolf im saying not to conflate that with this bc it seems ur switching between viewing matrices as vectors & matrices as map representations
the set of matrices forms a vector space
with their scalar multiplication and addition properties
matrices are elements of a set that, when defined with certain operations, form a vector space structure. they also have a basis subset of this space where any arbitrary element in the larger space is a linear combination of that basis
i just wonder what a linear operator acting on this vector space would look like
there is no one way to do this. the most compact way would be to define the linear transformations using einstein notation
alternatively, you could build something isomorphic to what you want, e.g. vectorize the matrices (unwrap into a single long vector) and multiply these vectorized matrices by a huge matrix that represents the transformation acting on the original matrix you vectorized
and then matricize back
u mentioned matrices (as map reps) as if the idea contradicted smth about trace acting on matrices
the way the transformation itself looks is not really important, and you could anyway represent it via sums
trace is a function that takes in a real matrix and spits out a real number right?
yes
that doesn’t sound like the same kind of mapping that is a linear operator
its a linear map R^nxn to R
it's pretty easy to do so by vectorizing the mat, for example
you vectorize it, multiply by a diagonal matrix with a 1 every m diagonal entries
and then add the elements up
which is a product by a vector of 1s
something like 1^T D vec{M}
(it's the same as a vector length m*n that has 1s every m elements)
so the linear operator is still represented by a matrix?
you CAN if you want
but you'd more succinctly just use sums
in einstein notation, Tr{A} = a_ii
equivalent to the double sum over i and j of a_ij b_ij, where b_ij = 1 if i=j and 0 otherwise
or something like that
any linear map between finite dimensional spaces has a matrix representation
oo neat i didn’t know that
ive typed a bit about it before so ill copypaste
okay ty 
for a vector x & basis B, (x)_B denotes the coordinates of x in B (written as a tall matrix)
thisll get bracket heavy. i didnt tex it
Let V & W be finite dimensional vector spaces over the same field where dim(V)=n. Pick a basis of V, which will have n vectors, B={b_1,...,b_n}, and pick a basis C of W. The matrix of a linear map A:V->W wrt B & C, denoted (A)^B_C, is constructed by placing (Ab_i)_C as the i'th column for i=1,...,n. Note that by construction, (Ax)_C=(A)^B_C (x)_B for all vectors x in V.
u can use this to write the matrix rep of trace wrt the usual basis of R^nxn & the basis {1} of R
do the same for any linear map R^n->R^m, wrt the usual bases, to check it agrees w/ how u usually think of matrix reps
the main equation is texd for some comfort
$$(Ax)_C=(A)^B_C(x)_B$$
RokettoJanpu
Guys what is the matrix associate to a dot product for R^2 and for R^3?
you mean the matrix of the standard dot product?
pretty sure that'd just be the identity
does the space of all real polynomials include the space of all formal power series?
it seems totally reasonable to me, but it seems funky to call it just the space of real polynomials then (like it does in this exercise).
does the space of all real polynomials include the space of all formal power series?
it's the other way around, no?
{polynomials} ⊆ {formal power series}
what's stopping me from saying "take the basis of the space of polynomials and add them?"
are infinite sums not acceptable here?
in general only finite sums make sense in a vector space
if you wanna talk about infinite sums you need to introduce some kind of topology
neat, and thanks
would you be willing to expand on that though at least on a surface level? Maybe it's just my unfamiliarity with topology though
well topology essentially is what lets you determine which sequences in your space are convergent, and where they converge to
because if you're talking about an infinite sum you really are talking about a sequence: the sequence of partial sums
ah that makes sense, thanks
i've never actually seen sequences defined in topology instead of metric spaces, so ig I'll have to look into that, thanks a ton! 🧡
Let $V$ be a vector space. Why is the natural correspondence between $V$ and $V^{**}$ important?
Croqueta
Where $V^{**}$ is the double dual of $V$
because of tensor products
Croqueta
also they play important role in harmonic analysis
you may not be able to appreciate them now
K
I was planning to study a little on tensor products today (I have read about them before, though I just know what they are)
Does anyone have any insight into why the unit vector uses the convention of i and j? I get the actual letters are arbitrary, but there's usually some reason why convention settles on specific letters, even if it's just because someone published a famous paper that used those letters, and the letters were chosen because the author had 2 cats named Igor and John.
you can probably blame hamilton for that
he introduced i, j and k for the three imaginary unit quaternions
Do you know why he started with i? m for matrix, n for natrix because m was already taken by a different matrix, then when he needed those vectors, just went with the next 3 letters?
i was already in use for the imaginary unit of complex numbers
not using i,j,k also makes "way too much sense"
Is this exactly correct? Doesn't this assume that the field is regarded as a vector space over itself?
I just realized that if $T\colon V\to W$ is a linear transformation then $(T^t)^t$ maps from $V^{}$ to $W^{}$
Croqueta

can any body help me here? I am kind of lost, i know i need to write both as a linear combination, but where do i go from there?
i need to write both as a linear combination,
maybe make it more concrete what you actually mean by that?
a1u+a2v+a3v=a1(u+v)+a2(u+w)+a3(v+w)
I could be worng, but that is what i am understanding
as written this isn't a true statement in general.
they are subsets of each other
i think you're suffering from a case of omitted detail
yes, you want to show that the spans of {u,v,w} and {u+v, u+w, v+w} are subsets of each other.
one way to do so is to show that:
- u is a linear combination of {u+v, u+w, v+w}
- v is a linear combination of {u+v, u+w, v+w}
- w is a linear combination of {u+v, u+w, v+w}
- u+v is a linear combination of {u,v,w}
- u+w is a linear combination of {u,v,w}
- v+w is a linear combination of {u,v,w}
three of these are obvious, the other three are kind of obvious but less so
okay, ty
it makes sense now
how do i show it is a linear combination now, it is so confusing with multiple variavles?
what is "it", and linear combination of what?
"it" refers to the 6 statements you wrote
which of the six statements are you confused at?
if multiple or all of them, which one would you like me to explain first?
can you explain 1
statement 1 reads:
u is a linear combination of {u+v, u+w, v+w}
to prove it, you need to show the existence of three scalars $a, b, c$ such that $a(u+v) + b(u+w) + c(v+w) = u$
Ann
well you could try to not let the abundance of symbols frighten you
and perhaps you could expand this and collect "like terms"
THis part isn't clicking at all
how does this even work after you expland and collect
well why don't you do it and then we'll talk
maybe it'll jump out at you even if you don't see it now
thing is ive looked at it last night, and this morning and still dont get it 😭
you have been unable to expand and collect like terms in a(u+v) + b(u+w) + c(v+w)?
is that what you're saying?
no i did
Let $A$ and $B$ be matrices, not necessarily square nor with equal dimensions. We label their respective components as $A^i_{;j}$ and $B^k_{;l}$. Now I want to consider their direct sum $A \oplus B$. How do I write the components $(A \oplus B)^r_{;s}$ in terms of the components $A^i_{;j}$ and $B^k_{;l}$ in index notation?
Siupa
My writing is terrible don’t mind
your v looks like r
but okay so like
you see that you have:
(a+b) * u + (a+c) * v + (b+c) * w = u
so now, how can you ensure that there is no v term on the left-hand side?
i.e. how can you make the (a+c) * v term go away?
don't overthink it
same thing, i figures it out now, thank you!
I am now stuck on this P is the set of polynomials, but im unsure how p(a)/=0
assume every p_i(a) = 0 and derive a contradiction, maybe

if $p_i(a) = 0$ for all $i$ then $1 \notin \mathrm{span}{p_1(x), p_2(x), \dots, p_k(x)}$
Ann
The points A = (-2,6-1), B = (118, -34, 19) and the point P lay on a line. The distance from A to P is 4 times larger than the distance between B and P. Determine the two possible positions for the point P. My solution so far:
OP = OA + 4AB/5
AB = OB - OA
OP = OA/5 + 4OB/5
I put in OA and OB and then I get 1/5(-474 142 -77) (edited)
Is this correct? If so, good. If not, how do I go about it then? If it is right, how do I find the second solution?
originB - originA
OA is the distance from origin to a
i just wrote it out for you
Yes, so all i would need would be a counter example correct?
i dont get it
do you know the distance formula?
i understand what the individual components mean but not how it relates to my question
my question was whether not my method was correct
what are you attempting to solve?
the question is stated
Question: The points A = (-2,6-1), B = (118, -34, 19) and the point P lay on a line. The distance from A to P is 4 times larger than the distance between B and P. Determine the two possible positions for the point P. My solution so far:
OP = OA + 4AB/5
AB = OB - OA
OP = OA/5 + 4OB/5
I put in OA and OB and then I get 1/5(-474 142 -77) (edited)
Is this correct? If so, good. If not, how do I go about it then? If it is right, how do I find the second solution?
AP/BP = 4
right
yes, so rearrange and you get AP=4BP
thats the relation
and you know they lie in the same line
if we have a basis for a vector space consisting of matrices and we are to find the dual of this basis
is using a trace function the way to do so?
meaning the dual will consist of trace functions
cause its the only linear functional i know of that can go from a matrix space to a field F
correct me on anything im misunderstanding ,bit rusty with my algebra 
what other linear functionals go from the space of nxn matrices with entries in R to R?
First entry multiplied by scalar for example
how does tensor product multiplication work like i have $(A\otimes B)(C\otimes D)$
what is this equal to
2217
What kind of things are A, B, C, D there?
matrices @fringe fjord
it would still be defined as a trace tho ? how else would you arrive at R
Then the tensor products are probably https://en.wikipedia.org/wiki/Kronecker_product
thanks!
having difficulty on this one. the problem wants me to solve using gaussian jordan elimination
This is my work
,rotate
I was trying to put it in reduced echelon form but idk how
The answer key only gives me the final answer they don’t show what the matrix should look like so I don’t know if I’m going in the right direction
hi guys, just needed a hand with this ex. , thanks
<@&286206848099549185>
hey guysss , i m not very familiar with sigma notation i didn't understand how we obtain this expression and also i didn't understand how to interpret it thanks for help
hey guys
quick question
in order to find pivot positions/columns in a matrix
should it be in REF?
I have to say writing vector coordinates with ψ and λ is not common. so in the first what is happening is the inner product is being distributed using linesrity
since $\ip{ \psi_i \vb{b}_i, \lambda_j \vb{b}_j}= \psi_i \lambda_j \ip{ \vb{b}_i, \vb{b}_j}$
but this is done over the sum
in third it's matrix notation,
,texw where \begin{gather*}
\hat{x}=\m{\psi_1 \ \vdots \ \psi_n} \
\hat{y}=\m{\lambda_1 \ \vdots \ \lambda_n} \
(A)_{ij}=\ip{\vb{b}_i, \vb{b}_j}
\end{gather*}
WHen getting an augmented matrix to Strict Triangular Form, or goal is to get 0's in for the dotted red right?
what's "strict triangular form"?
right
that's what i would call 'upper-triangular with nonzero diagonal'
but anyway, this definition should answer your own question
Sort of but I get confused with the extra 0's after we do this
Now there are two leading zeroes in the **second **row, does this mean we have to have three leading zeros for the **third **row?
@dusky epoch
no, it means you cannot put this system into strict triangular form at all
because your system is singular
this coefficient matrix is not even square so it cannot be put in strict triangular form no matter its content
Oh okay ty! I think I can comfortably move on to the other section now 🙂
Hi all!
I need to find (lim_n \rightarrow \infty M^n)
MrMadium
This is what I have done thus far:
Am I right in thinking that once I have calculated XD^nX^-1 that if the coefficient to the element is a fraction, it comes down to 0 and if it is a scalar, the element is a 1?
Or have I lost my mind?
I have no idea.
what is this?! what are you calling scalar and fraction?
I have no idea, man. My course notes and tutor haven't even explained it and it's part of the assessment. I have no idea.
also $(XD^nX^{-1})_{11} = \frac 1 2 \cdot 1^n$
the way you have written it makes it look like $(1/2)^n
I literally have no idea what you've written down 😄
I'm gonna go find some other resources then - thank you for trying to help out
I'm just missing something in my brain bits.

what part of it you don't understand
like you are doing such complex matrix manipulation but ...
this refers to the last line of your derivation
what's the easiest way to see that $$\det(I + tX) = 1 + tr(X)t + O(t^2)?$$
kxrider
$\det(I + tX) = t^n \chi_X(-t^{-1})$
Ann
probably something along those lines
btw about your question. stack exchange has a chat room, bunch of professors and grads reside there. they are probs closer to your level than most peeps here
i do not have a stackexchange account, so
Hii guys
I would like some idea on why taylor expansion could be use to prove linear independent
Where is this from? It's got so many grammatical errors I doubt its math
Yea that's just a bad answer. I'd ignore it
I have this problem and wonder if I could use taylor expansion
Dunno if this is correct or not
Can you calculate the Wronskian easily?
so what they did is essentially the same
by taking the taylor expansion, they automatically get derivatives of the functions
and then they exploit that the terms of different orders in the taylor exp are lin indep
thankk you so much hmmm i get this part but the sigma not for the notation 😆
Let $V$ be a vector space over $\mathbb{K}$ and $\varphi \in \operatorname{End}(V)$. $\varphi$ is called a projection if $\varphi^2 = \varphi \circ \varphi = \varphi$. I've already shown that the following holds:
$$ V = \operatorname{ker}(\varphi) + \operatorname{im}(\varphi) \text{ and } \operatorname{ker}(\varphi) \cap \operatorname{im}(\varphi) = {0}$$
Now what I'm struggling with is the following: \
An endomorphism $\varphi \in \operatorname{End}(V)$ is a projection if and only if there exists a basis $\mathcal{B} = b_1, \ldots, b_n$ of $V$ such that for the matrix presentation:
$${ }{\mathcal{B}} M{\mathcal{B}}^{\varphi}=\left(\begin{array}{cc}
E_{r} & 0 \
0 & 0
\end{array}\right) \in \mathbb{K}^{n \times n}$$
where $E_{r}=\left(e_{i j}\right) \in \mathbb{K}^{r \times r}$ is the matrix with $e_{ii} = 1$ for all $1 \leq i \leq r$ and $e_{ij} = 0$ for $i \neq j$ otherwise.
go on*
just take a basis of im(phi) and pad it with a basis of ker(phi)
isn't that what i suggested?
like if you already have the basis then isn't it clear?
do i need to specifically choose a basis
what i have rn is just
say that b_1, ..., b_k is a basis of im(phi)
say $v_j$ is a basis vector of $im(\phi)$ then there is a $y$ s.t. $\phi y = v_j$, now $\phi v_j = \phi^2 y = \phi y = v_j$
so the coordinate is just (0, 0, .., 1(j'th pos), 0, ..)
so wrt any basis of Im(phi), the matrix representation is the Identity
could you expand on this
wrt your choosen basis $\mathcal{B} := { v_j }$ the coordinate of $v_j$ is $\m{0 \ \vdots \ 1\ \vdots \ 0}$
oh since we are mapping from B to K^n again?
so the coordinate of the basis vector v_j
would just be e_j
yes
i see
rest clear or do I need to explain?
maybe go through it with me, im a little unsure
do you see why $\varphi(v_j) = v_j$?
you explained it, no?
I did, just reassuring
if $v_j$ is a basis vector of the $\operatorname{ker(\varphi)}$, we get that $\varphi(u_j) = 0$
yes, but call it u_j maybe because v is already in use
lewis
now it's just a matter of writing out the matrix of the transformation
now, what would that mean for the coordinate
which is pretty routine
$\varphi(v_j) = 0\cdot v_1 + 0\cdot v_2 + \cdots + 1\cdot v_j + \cdots + 0\cdot v_k + 0\cdot u_1 + \cdots + 0\cdot u_l$
can you pick up the coordinates from here?
0, 2, ..., 1 (j-th position), ..., 0
my bad should be 0
that's just e_j?
yeah
yes
also
the reason for the three 0's
in the right hand corner
that's due to
the kernel being non-empty, right?
or actually...
what if we were to choose all $n$ vectors from the image of $V$
lewis
does that even work
you can't unless the dim is itself n
there aren't even enough LI vectors to choose from
If Im(phi) has dim n, then yes
then wouldn't M just be the identity matrix
yes
with notations like this, yeah
and let's not talk about real analysis
because using that notation
it seems like
those 0's are fixed
$\left[\varphi\right]_{\mathcal{B}}^{\mathcal{B}}$
takes this much to write it out,
ye
it's much better, also you can just ignore B's
unless we're considering that the dimension of the kernel is not actually 0
anyway..., i thank you sm for clarifying 

How do you call the space of all eigenvectors?
don't think there's a term for that
"eigen space of all eigen vectors"
hello!
i am trying to understand how one can say in a matter of seconds that the following symmetric system of equations has the solution x^2 = y^2 = some constant.
the system is:
8x^2 - 17y^2 + 3 = 0
8y^2 - 17x^2 + 3 = 0.
I mean, besides the obvious "sure it works to check if x^2 = y^2 = some constant works" lol and then to consider "x^2 different from y^2" xD.
I guess if you imagine subtracting the second from the first you're gonna get C*(x^2-y^2)=0 and C != 0, so...
idk if that's a bit too much of a stretch to see there are two terms x^2-y^2 and factor it out like that mentally
Hmmm. Could be the case!
I was wondering more along the lines of the general theory for symmetric systems of equations or about quadratic forms.
Hell, maybe just the good old matrix for solving systems of equations 😂
How to draw a curly brace?
There is a nice isomorphism between $\textup{Hom}(V,W)$ and $V^V\otimes W$. Let $T\in\textup{Hom}(V,W)$ and $S\in\textup{Hom}(W,V)$. I was wondering what relations are there between $V^V\otimes W$, $W^W\otimes V$ and $\textup{Hom}(W,W)$ when considering compositions $T\circ S\in \textup{Hom}(W,W)$ (besides looking at the coefficients).
Croqueta
V and W are vector spaces *
that dual space notation hurts me
wdym
Could someone give me a rundown on the essential principles of finding the intersection basis of the sum of 2 vector subspaces?
Do you mean Grassmann's theorem?
I doubt it would have a name
just the simple method of finding the intersection basis
or rather the idea behind it
Well you have two subspaces am I wrong?
So I think that you have a vector space upper them
Now if you follow that you can conclude that the dimension of this two subspaces is the same. Now Grassmann says that
dim(V+W)=dim(V)+dim(W)-dim (w,v intersection) Now, if you have v and w subspaces it's easy to find the dimensions of them. After that you find dim(v+w) and then you solve the equation where x is your dim(w,v intersection).
Another method is to put the equation of V and W in a system together and then find the solution of this system. I hope I have been clear enought.
so grassman's theorem is just the dimension theorem for the sum of spaces? Oh we weren't given this name for it
the 1st paragraphs merely describes how to find the size of the basis of the intersection right?
it looks very similar to kramer's rule if that helps
could you post a wider picture?
how such a system is supposed to look like?
what does the notation in d and f mean exactly
i have never seen such a question
oh i think i got it
does it mean we multiply the matrices in the parentheses then multiply the result by the outer matrix
but wouldn't the result of the multiplication be undefined (in question d)...
brackets signify order of multiplication
so in d we should multiply AC first?
yes
but if we do that the end result would be undefined
and according to the book's answer
it's defined and it's a 5X2 matrix
maybe they mean (EA)C ?
why do you say E(AC) is undefined?
AC generated a 4X2 matrix
do note that E(AC) and (EA)C are the same thing, by the way
you can't multiply that by E which is a 5X4 matrix
are you sure?
(5x4) times (4x2)


