#linear-algebra
2 messages · Page 127 of 1
if you equip the endomorphisms on some vector space with the addition of linear maps and the function composition as multiplication
then they form a unital ring
so all the definitions above apply
we can construct a polynomial ring End(V)[X]
oh okay, I see
so now the polynomials are certain sequences where the elements are endomorphisms
we can do this for any ring
endomorphisms are the ring elements
basically, view the definitions from the beginning but replace $R$ with $(End(V), +, \circ)$
Flow:
nothing changes
In summary, a polynomial is a sequence of finite support, where these elements could form a polynomial ring, with the operations of addition and multiplication. We could evaluate polynomials from elements in the unital ring, namely by substitution. Since the set of endomorphisms equipped with the correct operations results in a ring as well, the above apply and we obtain polynomials of operators right ?
essentially yes
yep
and then you can evaluate this polynomial by substituting in a linear operator
and then the evaluated polynomial will be a sum of compositions of linear operators
which is again a linear operator
so the only question that remains is "why can we plug an operator into a polynomial over the field F"
and i tried to give that answer in my last remark
the answer, imo, is that the most obvious way to do so (with the slight caveat of interpreting the constant term as a multiple of the identity operator) behaves almost as you would expect
yea
that's basically what i wrote as well xd
we can map elements of the field to an operator by $\lambda \mapsto \lambda \id_V$
Flow:
that's how we get from polynomials over the field to polynomials over operators
and then we can just evaluate as usual there
so the remark is basically saying that if we create a mapping between the field F and the set of endomorphisms, the map is actually a ring homomorphism as it satisfies the conditions. Thus, this map implies that the polynomial over F is sufficient to take in elements from End(V) ?
yea, we can always plug an operator into a polynomial over F if we identify each field element $\lambda$ with the operator $\lambda \id$
Flow:
is that some sort of trick involved ?
no, that's straight forward
so this suggests that every field has an identity operator ?
no
we have a field F and a vector space V over F and the ring of endomorphisms End(V) whose unity is the identity operator on V
Is $\vec{r}-\cos(\varphi)\vec{r}=\vec{r}(1-\cos(\varphi))$?
Anton S.:
Yes
ignore my stupid message just know. Instead it works because if we map each element to its identity operator we essentially have a ring homomorphism, therefore we can evaluate the polynomial of an operator. Rephrasing the remark, take the inclusion map to bring each term of the polynomial to an operator, then take the evaluation map to show that the sum itself is a operator as well right ?
evaluate as in "calculating the substitution" ?
uh i guess?
evaluate as in plug an operator into the polynomial to get an operator as a result
map each field element to a multiple of the identity operator, then use the evaluation map for polynomials over rings
as usual
oh so you map first, then plug
ahhhhhhh okay, now I know what the evaluate do LOL
thank you so much for your time 😹
i can give you an example i guess, maybe that helps
so if you start if a polynomial in F[X] like 1 + 2X + 3X²
then you first map it to the polynomial in End(V)[X]: (1 id) + (2 id)X + (3 id)X²
and then you evaluate it by plugging an operator T in
$(1 \id)\circ T^0 + (2 \id) \circ T^1 + (3 \id) \circ T^2$
Flow:
note that $T^0 = \id$ and $T^2 = T \circ T$
Flow:
so the inclusion maps the polynomial $a_i$ while the evaluation maps $X$
Otoro:
with your example then kinda yeah ?
good, i think that should be enough for now, since you didnt have ring theory and the book you read doesnt need it either
the inclusion map i defined does not map between the polynomials
it maps between the field and the endomorphisms
but i can map between the polynomials by applying the inclusion map element-wise
i think the main problem is that all my definitions need justifications and proofs and i left them out
i just claimed that a bunch of functions are homomorphisms
So from the book, the $a_i$'s in p is different from $a_i$'s in p(T) right ?
Otoro:
idk
i didnt read enough of the books to know how he defines polynomials
if its a polynomial function, then the a_i are the same
if its a formal polynomial then they are technically different, but it doesnt matter for how you use them
@old flame no, they're the same a_i
@dusky epoch is it because the $a_i$ is scalars in this case ?
Otoro:
Thank you very much
i think the main problem is that all my definitions need justifications and proofs and i left them out
@spiral star maybe once I start learning ring theory, the definitions would start to make more sense and I may try to prove them with enough tools
I guess this is quite an interesting introduction sort of to rings lol
I have the solutions but I can’t make sense of it
Can someone help me out.... how did they determine which was the hard and soft earth
@thick kite soft earth is the blue area
How did you know that though??
it says as B is hard
You know how in the solutions when calculating the total cost they times 100 by CE
When did they considered just CE as soft
Why not the whole thing
I think thats a typo, it should be 100 times x
cause it should be AC + CB
and btw @thick kite this question should be in #calculus
Ahhhh okayy makes sense now
My bad I avoided posting there since they were in the middle of a discussion... didn’t wanna interrupt
ah I see, no worries
I need help in proving that the given set of basis is a spanning set for the vector space of polynimials(degree <= 3).
I need help in proving that the given set of basis is a spanning set for the vector space of polynimials(degree <= 3).
@wintry steppe V is the vector space of polynimials (deg <=3)
You mean you have to prove the given set is a basis?
You mean you have to prove the given set is a basis?
@native rampart yes
I don't kmow how to show that the set spans the space.
I've proved that it is linearly independent
Show 1,x,x^2,x^3 are in the span
oh
So you mean to say that represent 1, x, x^2, x^3 as a linear combination of the elements of the give basis
I hope I didn't ask a stupid question
@native rampart
Actually,You get 4 independent vectors,right
They span a subspace of the required space
So,They should be a basis
@wintry steppe
Actually,You get 4 independent vectors,right
@native rampart yes
So,They should be a basis
@native rampart oh
Clever
Look up Lagrange polynomials
This is clever because it tells you that to define a polynomial,you just need outputs at n+1 different points
This is clever because it tells you that to define a polynomial,you just need outputs at n+1 different points
@native rampart 👍 got it. Thanks again.
Kinda stuck on showing this. Any tips or help?
hello people
I need help with some math and idk if im wrong or not
Determine the degree of the polynomial and the coefficients
I know the degrees
thx
alef0:
$\begin{equation}
\begin{aligned}
&\operatorname{If} M \in M_{n \times n}(K) \text { and } A \text { y } B \text { are square } M=\left[\begin{array}{cc}
A & 0 \\
0 & B
\end{array}\right] \text { then }\\
&\det (M)=\det(A)\det(B)
\end{aligned}
\end{equation}
I try this \det(M)=\det(\begin{bmatrix}
A & 0 \\
0 & B
\end{bmatrix})=a_1\det(B)=\det(A)*\det(B) $
```Compile error! Output:
! LaTeX Error: Bad math environment delimiter.
See the LaTeX manual or LaTeX Companion for explanation.
Type H <return> for immediate help.
...
l.54 $\begin{equation}
Your command was ignored.
Type I <command> <return> to replace it with another command,
or <return> to continue without it.
I try this
alef0:
For 2x2 matrix $\det(M)=\det(\begin{bmatrix}
A & 0 \
0 & B
\end{bmatrix})=a_1\det(\begin{bmatrix}
A_{11} & 0 \
0 & B
\end{bmatrix})+(-1)^{3}a_2\det(\begin{bmatrix}
A_{12} & 0 \
0 & B
\end{bmatrix})=a_1a_4\det(B)-a_2a_3\det(B)=\det(B)(a_1a_4-a_2a_3)=\det(B)\det(A)$
alef0:
I have to do induction on the size of matrix A and im stuck to prove it is valid for a matrix $A_{s+1\times s+1}$
alef0:
<@&286206848099549185>
@spiral star quick question, whats the difference between the left and the right side ?
Apparently it's a good idea to put my question from #help-5 here
I want to find the transpose of this:
The two 'outer' terms for C are orthogonal matrices
I tried this and:
- switched Sigma_X and Sigma_Y
- switched ^-1/2 for ^1/2
Looking at a known calculation, it appears that my second change was incorrect
However, I can't see any issues with what I've done
Oh and we know have Sigma_XY^T of course
@native rampart well the book asked me to verify that $(pq)(T)=p(T)q(T)$ and Im not sure how
Otoro:
does it make sense to talk about normed and inner product spaces over some arbitrary field rather than R or C?
i guess the field needs to have some analogue of the absolute value/modulus
I think the only other thing that your arbitrary field needs is a partial order
As you need to somehow define positive definiteness in your field
So i am just suppose to show that it doesnt satify one of the 3 conditions for being an inner product space correct?
which are 1. linearity 2. Symmetric 3. Positive Definite
that's right
I forget to put I have to prove it by induction on size of Matrix A
Im assuming it doesnt satisfy linearity because it works for the other two
Provide a counter-example
any negative scalar should work right?
thanks lol
@wintry steppe this should go in algebra/prealgebra i can help you there
ok ty
quick question about determinants
i have a 3x3 matrix and i have a 0 in the bottom rightmost element,so i wanna switch columns so its on the left
i would have to 2 permutations and multiply the determinant by (-1)² right?
yes
ty!
swapping any two rows or columns changes the sign
so swapping twice multiplies by (-1)^2
you are right
i can only swap adjacent rows or columns right?
they do not have to be adjacent, but it certainly makes computations easier (and maybe longer) if you do thay
there's something to be said more generally about the determinant as an alternating multilinear function of the columns (or rows) of your matrix, but i can't tex it rn
So, I was thinking about determinants the other day.
Let V be an n-dimensional vector space, let 𝛬ⁿ(V) denote the vector space of alternating n-linear forms on V and let F : V -> V be an endomorphism
Then F induces a pullback Fᵀ : 𝛬ⁿ(V) -> 𝛬ⁿ(V) given by, for 𝜔 ∈ 𝛬ⁿ(V) and v₁, ..., vₙ ∈ V, as
(Fᵀ𝜔)(v₁, ..., vₙ) = 𝜔(Fv₁, ..., Fvₙ)
Now Fᵀ is a linear map and 𝛬ⁿ(V) is 1-dimensional, so we can ask about the eigenvalue of Fᵀ. This eigenvalue is then the determinant of F (I haven't verified, was busy brushing my teeth when I came up with this, should hopefully be correct).
Over the complex numbers, we have this cool identity which says that the determinant of an endomorphism is equal to the product of its eigenvalues
But this obviously does not work over arbitrary fields
I wonder, is there a way of constructing some similar identity by considering the pullbacks on the vector spaces of multilinear alternating k-forms?
The older editions of Axler had this construction for the determinant of an endomorphism over the reals, where he factored the characteristic polynomial to a product of one and second degree polynomials and then proclaimed that the determinant is the product of the constant terms
ugh sorry this is being a pain in the ass, when i fix my latex i'll post this
@wintry steppe Yes indeed. The nice thing about the construction I did is that it can be done in a basis-independent way.
But it might just be shifting the mess elsewhere
Likely to the part where 𝛬ⁿ(V) is 1-dimensional needs to be proven
𝛬^k(V) for V n-dimensional has dimension n choose k
...so 𝛬ⁿ(V) is a 1-dimensional space.
shifting the mess elsewhere
not sure what this means. proving that 𝛬^k(V) has dim n choose k isn't that bad
I guess not. Still nicer than constructing the determinant of a matrix first and then showing that it is actually basis-independent and thus a property of the parent linear map.
Hmm, apparently the Cramer's rule can be proven this way
tbh this is the best defn of the determinant
Yes indeed. I am almost afraid to guess as to why most textbooks do not take this route.
because developing exterior algebra is way too much work for the definition of the determinant most people use
it's my favorite definition, but for having a working definition of the determinant, you can go with easier
What do people actually use the determinant for?
I guess computing the characteristic polynomial
defining the special linear group
the determinant is also a useful invariant in things like checking whether matrices are similar
computing-with-numbers things it seems
namington is more knowledgeable than me so i will leave this to them
it is true that many of the determinant's applications are more computational, yes
however there are some nice more "pure" framings
continuity of the determinant function is an important theoretical one iirc
@limber sierra But, computing the determinant for large-ish matrices is infeasible anyway
it's very fast for computers
and oftentimes determinants are more "heuristics"
like computing the exact value of a determinant may be annoying
but determining, say, its sign
might be easier
Computers compute the determinant by factoring the matrix involved though
So if you like, need to check for linear independence, you do not have to do the final step
if you want a less computational example, let $\mathbb{F}, M(\mathbb{F})$ be monoids under $\cdot$ in $\mathbb{F}$; then every homomorphism $M(\mathbb{F}) \to \mathbb{F}$ can be written as $\varphi \circ \det$ for some monoid homomorphism $\varphi\colon\mathbb{F} \to \mathbb{F}$
Namington:
this means that every monoid homomorphism from square matrices to their scalar field "factors into determinant"
algebraically this is a very handy propery as it makes the determinant, in some sense, a "canonical" homomorphism
at least multiplication-wise
when extracting scalars from matrices
Interesting. I should probably study some more abstract algebra sometime.
note however that for n * n matrices where n > 1
there is no ring homomorphism from this space of matrices back into F
If you guys are done, I have a question..
ie theres no way to get a homomorphism compatible with both addition and multiplication
unless of course n=1, since then you have 1x1 matrices
and the identity map (converting matrices to scalars) does the trick
also, the leibniz definition of the determinant hints at some group theoretic connections (ie permutation groups)
which may be worth exploriing
@main widget go ahead
I'm stuck with this problem. I've recalculated it like 3x even using online calculator for cross product and still somehow get it wrong. Any idea?
Basically the way I did it was first to cross the two intersecting plane to get a vector parallel to the intersecting line. Then, find one point from the two plane equation laying somewhere in the intersection line. After we get that, we now have the vector going the same direction as the intersecting line (from cross product of the two planes) and we can find the other vector from connecting the point that's given to the one in the intersecting line. After that, I cross both vectors to get the normal vector perpendicular to the plane that we're trying to find. Once I get that, I just use the general A(x-x0) + B(y-y0) + C(z-z0) = 0 formula.
<@&286206848099549185>
yo can anyone help me out with algebra 1 hw rn? <@&286206848099549185>
where at?
#prealg-and-algebra maybe, or one of the question channels
is this a good place to ask for matrices
Sure
alright needed just to be sure rn no specific question tho aside from what do matrices really mean
i get they express how i j k and other base vectors will transform into a specific way
but need to do some more learning
@versed topaz Do you agree with me, if an determinant of an marix is 0, it has an area 0
Matrices don't have areas
but thats' what is determinant, so far what I understand
So like, if think of all the columns as vectors in space, they form a paralleliped, and the volume of that is the determinant
( 1 0
0 3
) this means you multiply x with y which will get you 3 which means this matrice has the area of 3
3bluebrown1 is really good at explaining this, so the yellow is represented to be the area.
so when a matrice has a determinant 0, i hat and jhat overlap which means they dont have any solutions apperantly.
3 blue 1 brown is god of linear transformation
Or infinite solutions
?
x+y=2
2x+2y=4
if ihat and jhat is pararell then I think there are no solutions tho?
Solutions means there is a change to the plane ?
no solutions with 3d space, means khat doesn't do any change on its axis
there is no change in 3d space
it is infinite
WTH
how is that possible?
but if you gonna do gausselimination with that system equation
You will just get 0 = 2 which is a contradiction?
no
you will get
0 = 0
in the last row
you will only get x + y = 2 which is infinite solution yeyeyeyye
@native rampart but are you saying that a matrice that has det 0 can be both have no solutions and have infinite solutions?
Either no solutions or infinite
ye but it doesn't make any sense, DET 0 just means they overlapp
Don't rely on geometric intuition,in places where there are none. You would have to abstract at some point
You can
Hey I have this problem, I'm hoping to get some ideas on how to solve it
There's a 4x14 rectangle and I need to find how many ways there are to fill it entirely with 1x2 rectangles (the solution is preferrably using matrices, but without matrices is fine too)
@native rampart how would you do it?
There's this thing called Row reduced echleon form
Given a system Ax=b you mutliply both sides with P,such that C=PA is row reduced echleon
Cx=Pb is simple to solve,and you can check the number of soultions with that
And if the det is non zero A is invertible,and C will be Identity
and if cx = pb is false then it has no solutions+
Yes
I've done Row reduced echleon form
but
I was thinking perhaps you could perhaps use determinant eithweay
You can use row reduced echelant form adn then multiply the diogonal and get the determinant
If Invertible,Cx=Pb will always be true for a particular value of x
The process doesn't preserve determinants
wdym ?
If you take 2I and row reduce it you get I
Determinant of original is 2^n and latter is 1
are you saying upper triangle method doesn't work in all cases?
Ok, You could do that
oh I see, we missunderstood each other.
Row reduce and find the determinant of the row reduced form
Is that what you mean?
Well,If you do a few more steps you would get row reduced form
is this method aka gauss method ?
A part of gauss
and gauss jordan is like total obliteration
idk why you would use gauss over gauss Jordan
sometimes gauss jordan will end up using a lot of fractions
depends
gauss jordan fs is more useful
but might be unpractical
May I ask how is at least one j not injective ?
If all were injective,The only vector that would be sent to 0 would be 0
So, Atleast one has to be non injective,since a non zero v gets sent to 0
so for the final line, could we treatt the factors with operators function composition ? or whats going on witht the factors with v
So it is a composition, where we apply the transformation $(T-\lambda_1) \circ (T-\lambda_2) \circ \cdots \circ (T-\lambda_m) (v)$ right ?
Yes
so one of them lets say j would be zero, $(T-\lambda_j I)v=0$ ? so it corresponds to $Tv=\lambda_j v$ hence the existence of one eigenvalue $\lambda_j$
Otoro:
Yes
ok thank you
oh whats wrong
The composition of other operators put the vector into the null space of $(T-\lambda_i)$
so following the usage of the jth term, as the jth composition produces zero, this puts the previous compositions in null(T-\lambda_j I) ?
Yes
so this shows that $(T-\lambda_j I)$ is not injective right ?
Otoro:
since $null (T-\lambda_j) \neq {0}$
Yes, because it has a nullspace
Otoro:
then how can we conclude it has eigenvalue ?
DrunkenDrake:
so its just using the fact that it has some non-zero vector that maps to 0, then just rearrange and done ?
Yes
thanks
I dont understand why they remove row 2 so it becomes 3x3 matrice
ah it's a determinant calculation
ye
looks like the minors method
why did they remove row 2
they remove column 3
and multiply by -1
look up the minors formula, also called the laplace expansion
lmao im braindead
forgot that straight bars on a matrix denotes determinant sometimes
det is invariant wrt row/col operations, and a tip is to laplace expand along a row/col with many 0s
to expand on what rokabe and smh were saying, if you expand along the third column, the result will be -1 * det(matrix with second row and third column deleted)
which is what happened
But that is because 1 is -1 in that scheeme
did you google laplace expansion formula?
ah, schemes, everyone's favorite LA topic
Yes
Using the definition of the determinant, the following expression was derived in Example 5:
I I didn't know you could do it in this way,
but apperantly you can do that
I think you it is fine using laplace expansion with 4x4 but if you have more than 5x5 then I you are being better of just using gausselimination / upper triangle method.
if you have a 5x5 matrix or larger you use wolframalpha
Im just speaking general
Anyone have an idea on how to solve this problem. need some help!
Can someone help with the very last question after d?
I feel like it's not possible for a square matrix to satisfy b)
Can someone help me understand this proof? A is a lin operator A (V->V), detA=/=0 then det A* =/=0. Proof : we assume detA*=0 , then there is such y, y=/=0, Ay=0, we multiply by x from the left side <x,Ay>= <x,0> or <Ax,y>=0. But since A is a regular operator, ImA=V, so there is such vector x that Ax= y, so from before we get <y,y>=0, y=0. Contradiction, detA*=/=0
why does y=0 cause a contradiction here?
Can you use latex pls.
What is A*
y = 0 causes a contradiction because you assumed y is non-zero
A* is the adjoint of A
Never learned what that was in my LA class
do you know inner products?
unique linear operator with <Ax, y> = <x, A^*y> for all x,y
iirc
sniped
wait
you deleted it
it's whatever you got it 1st
ayy thanks got it now
btw \* to avoid error
il go through latex next time
don't feel peer pressured to latex
i like this
You like not being able to read?
i read it just fine
im allready begging for help, might as well make it easier for people to help me
see that's the spirit
If L is a subspace defined as $ L = { A + A^{T} : A \in R^{2x2}}$
how would a basis of said subspace look like?
Lonac:
$ span{ \begin{pmatrix}
2 & 0\
0 & 0
\end{pmatrix} \begin{pmatrix}
0 & 1\
1 & 0
\end{pmatrix} \begin{pmatrix}
0 & 1\
1 & 0
\end{pmatrix}\begin{pmatrix}
0 & 0\
0 & 2
\end{pmatrix} }$
can someone help me determine if (2a, b, a+1) is a subspace of R3
@errant wyvern I think your second matrix isn't in the subspace
Lonac:
ayyy i wrote it
@charred nacelle the channel is occupied, so you should ask one of the help channels. that said, this should be straightforward. just check the vector space axioms and see if they work. i think that one of them fails
Yeah that looks better, but when you write the basis no need to include the second matrix twice
But otherwise that works as a basis. Do you need to prove it is a basis?
Im supposed to check if Linear operator of orthogonal projection on $L^{\perp}$ is a unitary operator
Lonac:
I'm guessing you are using the standard inner product from R^4
uuu thats got me thinking, yeah the inner product isnt defined, so is there a list of standard inner products based on the space its performed in?
I mean the problem isn't well defined unless they give you an inner product
My guess is that they want the standard inner product like dot product from R^4
$x=\begin{pmatrix}
x_1 & x_2\
x_3 & x_4
\end{pmatrix} ; y=\begin{pmatrix}
y_1 & y_2\
y_3 & y_4
\end{pmatrix} then $$\langle x,y\rangle$$ = x_1*y_1 + x_2*y_2+x_3*y_3+x_4*y_4$
use _ for subscripts/indices
and \langle \rangle for inner product brackets
e.g. \langle x_{test}, y_3 \rangle
TTerra:
why does x3*y3 show as x3 "x" y3
i typed it the same way as every other multipliction
I don't know actually
Lonac:
Wait unitary means that it preserves the inner product right?
$U*U^{*}= I$
Lonac:
which is equivalent to what vman said
$\langle Ux, Uy \rangle = \langle x, y \rangle $
Lonac:
Right, so in particular it should preserve lengths/the norm. Try to show that the norm of some matrix changes after applying the projection
could you elaborate?
Sure
So if the projection was unitary, it should preserve the norms of all vectors.
But I'm saying the projection changes the norm of some vectors
So to show that the projection is not unitary it is enough to find some vector (matrix) that has its norm change after applying the projection
ah i see, so i can just pick a vector, apply the projection in it and show that the norm is different after the projection
Yeah
Well some vectors will have the same norm
But as long as you find one whose norm changes you're good
Ok while still on this topic for said L how would i find $L^{\perp} $
Lonac:
There are two approaches I know of
The easiest might be to find an orthogonal basis for L and then extend it to an orthogonal basis for all of V = R^{2 x 2}. The basis vectors not in L should be a basis for the perpendicular subspace
oh so when we did a simmilar task we would create a matrix from the vectors that span L and then for that matrix find ker, and it would be the orthogonal complement, but i couldnt do that here because my vectors are in matrix form themselves right?
No, you can use the same thing
But you need an orthogonal set of vectors that span L
I think
im confused, how would the matrix created from the vectors that span L as i found above look like?
You treat the matrices like vectors in R^4 and then the projection map would be represented by a 4 by 4 matrix
For example if I wanted to represent the transposition map on 2x2 matrices, I can choose a basis like
$$\Bigg{\begin{bmatrix}1 & 0 \ 0 & 0\end{bmatrix}, \begin{bmatrix}0 & 0 \ 1 & 0\end{bmatrix}, \begin{bmatrix}0 & 1 \ 0 & 0\end{bmatrix}, \begin{bmatrix}0 & 0 \ 0 & 1\end{bmatrix}\Bigg}$$
The_Vman:
And then transposition with would be represented by
$$\begin{bmatrix}1 & 0 & 0 & 0 \ 0 & 0 & 1 & 0 \ 0 & 1 & 0 & 0 \ 0 & 0 & 0 & 1\end{bmatrix}$$
The_Vman:
In the chosen basis
As transposition exchanges the 2nd and 3rd basis vectors while keeping the others the same
$\begin{pmatrix}2 & 0 & 0 & 0 \ 0 & 1 & 0 & 1 \ 0 & 0 & 0 & 2\end{pmatrix}
Lonac:
Compile Error! Click the
reaction for details. (You may edit your message)
so the matrix would look like this ?
You are trying to represent the projection to L?
im trying to get a matrix of L so i can find kerL to get vectors that span $L^{\perp}
yeah i guess
So if you want to find the space perpendicular to L, you can't just take any map the goes into L, you need the orthogonal projection to L. I believe to find the orthogonal projection you first need an orthogonal basis for L, which the one you have is, but then the map isn't simply putting that basis in the columns
I think the orthogonal projection onto the space spanned by an orthogonal basis ${v_1, \dots, v_k}$ is given by
$$P(x) = \sum_{i = 1}^k \frac{\langle x, v_i\rangle}{|v_i|^2} \cdot v_i$$
The_Vman:
So if you want to represent the orthogonal projection onto L you need to find where the basis vectors
$$\Bigg{\begin{bmatrix}1 & 0 \ 0 & 0\end{bmatrix}, \begin{bmatrix}0 & 0 \ 1 & 0\end{bmatrix}, \begin{bmatrix}0 & 1 \ 0 & 0\end{bmatrix}, \begin{bmatrix}0 & 0 \ 0 & 1\end{bmatrix}\Bigg}$$
go when you apply $P$.
The_Vman:
It is a bit of a process
But the first and last basis vectors are conveniently already in L so they should be kept the same. That means you only need to compute P of the second and third basis vectors
And there two of the inner products you have to take will be zero so that should make the computation easier
ok
You can do it if you want the practice, but otherwise the Gram-Schmidt should be easier
Ayy while reading and writting this on the side i did what u said first
Oh nice
Found that for x thats all ones
like $x=\begin{pmatrix}1 & 1 \ 1 & 1 \end{pmatrix}
Lonac:
Compile Error! Click the
reaction for details. (You may edit your message)
that its norm is different when i apply the orthogonal projection operator on it then its own
so eyy that works
Awesome
I will still try to do but if you dont mind entartaining me let me attempt to clear this up in my own head
I was just gonna say that since the projection is onto a lower dimensional space, the projection has a non-zero kernel and so can't preserve the norm
so we had a simmilar example to this in our notebooks, so im wandering if we have vectors that are written as 2x2 matrices, how would their form look like when written as a matrix, like in the picture above they littelarly put the vectors that span W into a matrix to form it
Yeah you should be able to put the matrices as a row vector with 4 entries
Like you did above
I think I got a bit mixed up thinking about the projection map
It does make sense now that I think about it
So like
$$\begin{pmatrix}2 & 0 & 0 & 0 \ 0 & 1 & 1 & 0 \ 0 & 0 & 0 & 2\end{pmatrix}$$
The_Vman:
No problem
So if i have vectors x= 1-3t^2 and y=0, how do i find d(x,y)?
how's d defined
im not sure how to extrapolate that from the exercise im trying to figure out so let me get the exercise
In space of polynomials with degree equal or lesser then 3, we are given some scalar product, matrix B=f', subspace L=span {1,t^2} and we need to figure out based on the scalar product matrix A thats orthogonal projection on L. Task is given to us to find the distance between B(A(f)) and A(B(f)) for f=1+t-t^3
so i calculated B(A(f)) and A(B(f)) i just need the way to get the distance between them and i forgot how you do that
oh yeah scalar product is inner product or dot product in english litterature
the problem or your book should define a metric on such spaces
$\begin{bmatrix}1//2//3\end{bmatrix}$
Resident Tracksuit Advisor:
using the wrong slash
\\ not //
\ /
oh
Resident Tracksuit Advisor:
Compile Error! Click the
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$\begin{bmatrix}1\2\3\end{bmatrix}$
RokettoJanpu:
$\begin{bmatrix}1\\2\\3\end{bmatrix}$
no prob
in the past we used $d(x,y) = \sqrt{ (x_1-y_1)^2+...+(x_n-y_n)^2}
that's a usual metric on R^n but this is a different space
if you got an inner product then that defines a usual norm by ||x||=sqrt(<x,x>) which in turn defines a usual metric by d(x,y)=||x-y||
ohh so id need to find ||x-y||
ight gonna go do that quick, we were given an inner product in the exercise it self
thx
you're welcome
Why am I wrong? I have tried multiple ways of putting it in. Please help.
3, 6, 15
0, 0, 0
you messed up signs
uh sure np
why are there two points labelled C
also this might belong in #geometry-and-trigonometry instead of here
ah sorry, ill move it there than
$\delta\left(\begin{array}{c}
V_{1} \
\vdots \
V_{s-1}\
U+kV \
\vdots \
V_{s+1}\
\vdots \
V_n
\end{array}\right)= \delta\left(\begin{array}{c}
V_{1} \
\vdots \
V_{(s-1)} \
U\
\vdots \
V_{s+1}\
\vdots \
V_{n}
\end{array}\right)+k\delta\left(\begin{array}{c}
V_{1} \
\vdots \
V_{s-1}\
V \
\vdots \
V_{s+1}\
\vdots \
V_{(n)}
\end{array}\right)$
alef0:
This is the def of a n-linear function
What are all 1-linear functions of $\delta(M_{1x1}(K) to\ K$
alef0:
alef0:
what is delta(M_{1x1}(K))?
are you just asking what the linear maps from M_{1 x 1}(K) to K are?
if that is the case then you are right
$\delta\left(\begin{array}{c}
V_{1} \
\vdots \
V_{s-1}\
U+kV \
\vdots \
V_{s+1}\
\vdots \
V_n
\end{array}\right)= \delta\left(\begin{array}{c}
V_{1} \
\vdots \
V_{(s-1)} \
U\
\vdots \
V_{s+1}\
\vdots \
V_{n}
\end{array}\right)+k\delta\left(\begin{array}{c}
V_{1} \
\vdots \
V_{s-1}\
V \
\vdots \
V_{s+1}\
\vdots \
V_{(n)}
\end{array}\right)$ the domain of this all Matrix nxn and the functions that they comply with that are called n-linear functions
alef0:
Oh thank you!
if T : M_{1 x 1}(K) -> K is linear, then it's equal to scalar multiplication by T(1)
where, if you want to be pedantic, that 1 denotes the 1x1 matrix containing a 1
is the fact that a vector space being closed under addition an axiom in itself, or is it derived from sth else?
it's part of how the operation of vector addition is defined
its usually not considered "its own axiom" so to speak
its just
when you say $+$ is a function from $V \times V \to V$
Namington:
this requires closure
otherwise it wouldnt be a function into V
the key takeaway: you do need to check that your vector space is closed under vector addition (and scalar multiplication) unless it's obvious
thanks, that's a really good explanation
as an aside, it will usually be "obvious" that a vector space constructed "directly" from a field is closed under +
like we know R the real numbers are closed under addition
so of course R^n will be
since vector addition in R^n is just adding up real numbers repeatedly
the most common case where closure "isn't obvious" is when we're trying to verify whether something is a subspace
let A, B be two nxn matrices both with positive determinant. is it true that det(tA + (1-t)B) > 0 for any t in [0,1]?
wait no
obviously not

Hi. I've been thinking about how invariant subspaces of diagonalizable linear operators (over finite dimensional real and complex vector spaces) look like. Does an invariant subspace of a diagonalizable operator necessarily have a basis of eigenvectors?
@crystal oracle The restriction of the linear operator to the subspace is itself diagonalisable (prove this) and therefore there exists a basis of eigenvectors
@fallen sigil I know that being diagonalizable is the same as having a basis of eigenvectors.
Anyway, I've resolved my question for arbitrary field thanks to https://math.stackexchange.com/a/78106
Are all symmetrical matrixes invertibles?
You're welcome!
One more thing I've a doubt with: Is the transposed of the inverted equal to the inverted of the transposed? Sorry by mistakes or conventions, I speak spanish.
@split heart you can try proving this
I haven't go through proves yet 😟
you can do it if you know properties of transpose & definition of inverse. take an invertible matrix A, prove (A^T)^-1=(A^-1)^T
Alright, I'll try
Does anyone have an nice proof of showing that the nonzero rows of a row reduced echelon form a matrix are linearly independent?
It says it's clearly true in my book and if you look at any examples of a RREf it's clear that the nonzero rows are linearly independent but I was wondering if there was a way to prove it really nicely.
I may just take it's word for it.
in every nonzero row there's exactly one 1 and all other 0s, and that's the only 1 in its column
so if you took a linear combination equal to 0, all the coefficients would have to be zero
kind of handwavy, maybe you can use induction or something to do it properly
nvm that deleted message is super wrong, ill have to take a second to phrase it properly
Anyone available to help me get started on this?
just check the definition of a vector space
there should be a list of things to check to see if that set is a vector space
Okay, thanks
To show subspaces you just gotta show it's closed under addition and scaling not all the axioms of a vector space
doesnt matter. you can pick any 2 variables as free and express the other two in terms of those
i think choosing x and z as free makes it very easy to generate a basis
I have a question about triple cross products. Suppose u and v are vectors in 3–space where u = (u1, u2, u3) and v = (v1, v2, v3). Evaluate u × v × u
and v × u × u.
It's not said what part of the cross product is to be done first. So no brackets.
Do i then assume v x u x u = (v x u) x u and u x v x u = (u x v) x u ?
Because what i think this question wants me do is expand both u × v × u
and v × u × u to show their not equal?
Just for clarity's sake
i don’t think you can do anything beside mark this as a badly written question
Do i then assume v x u x u = (v x u) x u and u x v x u = (u x v) x u ?
@gritty sapphire
I think i'll just to this
Because it's 10 marks of a 50 mark assignment
or ask the prof to clarify
Could I ask how is $T-\lambda I$ not surjective ?
Otoro:
Since $\lambda$ is an eigenvalue of $T$, $T$ sends some nonzero vector $v$ to $\lambda v$. But then $T - \lambda I$ sends $v$ to $0$.
The_Vman:
Do you see why that makes T not surjective?
If this is the standard matrix of a linear transformation, how do you describe what the transformation does? Is it just nothing?
@rose coral so therefore, there is at least one v that maps to 0, hence the mapping cannot cover the entire space V itself right ?
But why does sending some nonzero vector to zero mean it's not surjective?
@rose coral Is it because T and $(T-\lambda I)$ is technically the same ? cause its just an rearrangment
Otoro:
Compile Error! Click the
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No, we're not thinking about $T$ really just the map $T - \lambda I$, which we could rename $S$. The question now is just about a generic linear map $S$ on a finite dimensional space which sends a nonzero vector to 0
The_Vman:
And we want to say S can't be surjective
is this related to the null ?
Is it because $null (T-\lambda I) \neq {0}$ since T is an operator, it is not injective and hence not surjective ?
Otoro:
ah alright, cause I recall theres a theorem about an operator being injective is the same as not being injective and not inveritble thank you so much
No problem, just wanted to make sure you knew which theorem the text was referencing
I didn't thought of it at first, but then suddenly rmb that $(T-\lambda I)$ is an operator as well lol, thanks
Otoro:
Glad I could help
@spare hornet Being very technical I wouldn't say the transformation "does nothing." But that's being kinda technical. I would say that it's adding a dimension to the space you are talking about.
@rose coral thanks for the answer! My homework asks me to "describe the transformation". Would it be accurate to say that it adds a dimension to the vector?
It maps the vector to a vector space, whose dimension is greater than the original one by 1
thanks!
Prove it however you would prove the kernel of any other linear transformation.
Let $ f \in ker(T)$. $T(f(x)) = \int_{0}^{x} f(t) dt = 0$ ; this is what it means for $f \in ker(T)$.
TheDon:
Think about the fundaemntal theorem of calculus, and that should help you.
Gas:
Seems right to me.
That's it.
Just the the set of continuous functions such that F(x) = F(0)
where F is the antiderivative of f(x)
Is the underlined part a typo ? is it suppose to be $span(v_1,...,v_{k-1})$ if its not a typo, could you explain why ?
Otoro:
the representation of Tv_k in the basis {v_1, v_2, ..., v_n} is just the k'th col of that matrix, is it not?
yes
Otoro:
so is it because $\lambda_k=0$, then the transformation of the kth basis vector is just the combination of vectors $v_1,...,v_{k-1}$ ?
lambda_k=0
Otoro:
sorry I typed wrong lol
yes...
I don't get how to deduce that last iff (T* being the adjoint here)
@old flame reading Linear Algebra Done Right?
@prisma cairn yeah you ?
seems like you're way ahead of me though lol
oh lol, thanks Ann
If you have a parabola with a focal point in (1+sqrt(3), -1+1/sqrt(3), -2/sqrt(3)) and line (translation said scroll?) (1, -1, 0) (that is the direction of the line ) and throug point q (-1-7/sqrt(3), 1-3*sqrt(3), 8/sqrt(3))
How do i create the coordinatematrix
Cause i remember using 2 focal points to create its direction vector to have it "appointed" as z axis
For an ellips
Then finding a vector thats orthogonal to it
Abd then last orthogonal to previous two
But how do i start here?
I am trying to show that a particular transformation is linear if and only if b=c=0. The transformation is as follows:
T(x,y,z) = (2x-4y+3z+b,6x+cxyz)
My attempt was to write out:
T(x1+y1,x2+y2,x3+y3) = T(x1,x2,x3) + T(y1,y2,y3)
In this form it is easy to show that b = 0 because one side has b and the other has b + b; however, I am unsure how to show that c = 0. Using the second term in the transformation gives the statement:
c((x1+y1)(x2+y2)(x3+y3)) = c(x1)(x2)(x3) + c(y1)(y2)(y3)
This is ignoring the "6x" in the second term. I do not know how to show from here that c must be 0.
I solved it. Homogeneity property makes c = 0 easy to show.
Anyone know where I can get the strang book for free
@lucid cedar Easiest way would be to make sure that T(0)=0
That tells you immediately that b=0
By inspection we can see that cxyz makes it nonlinear as well
That is the path that the solution manual took
i did not really follow it
the c part i mean
then we can probably just do something easy like show T(1,1,1)+T(1,1,1) is not equal to T(2,2,2) to show c=0
how did the solution manual do it?
or better yet, show that kT(x,y,z) is not T(kz,ky,kz)
that was how i did it
kT(x) =/= T(kx)
The solution manual I have did T(1,1,0) + T(0,0,1) and showed c = 0
maybe im stupid but wouldnt both of those inputs make the c term zero?
looking back at it, I do get what they did, but i just dont see how that method is a reliable skill. What if the example that reveals c = 0 is rather difficult to find with a more complicated Transformation
This is the solution for reference:
oh now i get it
T(1,1,1)=T(1,1,0)+T(0,0,1)
i thought you meant just looking at the right side
yea sorry i left part of it out
This sort of solution just feels cheap because it seems like its difficult to generalize this process to any transformation. I tend to feel this way when specific vectors are used rather than general ones. What if for thousands of examples the property holds but for only a few it breaks? It could very well be possible that I am missing something about the nature of linear algebra that should lead me to, intuitively, find solutions like this or that this method is more powerful than I give it credit for.
I guess a good question I should ask myself is "Can a non linear transformation appear linear for some number of specific examples?"
@lucid cedar Well, unless it's obnoxiously obvious, I think it's possible to find an infinite number of examples that make a nonlinear transformation look linear. It's probably not easy but it's probably possible.
I mean unless you're a computer, an algorithm to determine if a transformation is linear is a waste of time. With some practice you can look at a nonlinear transformation and show it's not linear in one or two steps.
The way in which it is nonlinear makes certain properties easier to prove than others.
If a constant is being added, just show that T(0) is not 0
if terms are multiplied then homogeneity may be the fastest way
showing that T(a+b) is not T(a)+T(b) may be faster in some cases though
with a lot of these upper level math things, you have to assess the situation and pick the best tool. You're not in elementary algebra where every single problem has the same easy 5 step solution anymore. some tools make some problems nearly trivial and others obnoxiously computational. it really depends.
That's true. Thanks for talking me through it.
@wintry steppe If it helps put your mind at ease, here's a plot.
I'm self banned from anything linear algebra, due to none competence or I'd try and help
You could probably take an arbitrary element in W1, an arbitrary element in W2 and apply the definition of their sum. Given this new element, take another element of that set and apply vector addition. Then take a scalar and apply vector multiplication. And then check the 0 vector exists. And probably containment.
it's not really clear what you're doing. did you mean "suppose W_1, W_2 ⊂ V" ? what does WNTS mean? why are you considering x, y like that? what are a,b,c,d? (presumably elements of W_1, W_2, but you should spell this out)
alright
your end goal is to prove that W_1 + W_2 is a subspace of V
so it should be "WNTS W_1 + W_2 is a subspace of V"
your next step should be to go right to the definition of a subspace
there are a few things, then, that you have to check about W_1 + W_2
- it's a subset of V (no one will ever do this, practically, but for the sake of following definitions i include it)
- it's closed under vector addition (presumably this is what you were trying to do in the picture)
- it's closed under scalar multiplication. that is, if v is in W_1 + W_2 and c is a scalar, then cv is in W_1 + W_2
you can check all of these by using the definition of W_1 + W_2 given in the picture. some might say that you should verify that the zero vector of V is also in here, but that follows from (2)
it might make it easier to split your proof into three steps, each verifying the three things i listed above
so my book is telling me to consider the geometric interpretation of this parametric system but im not really clear on what they mean
how do you look at something like this and interpret it geometrically?
is that too general and bad of a question to ask
i wasnt sure what to ask
x is in the form r+x3*v where r,v are vectors. this matches the form of position vector tracing a line
is the intuition that this is tracing a line built through doing a bunch of these examples or is there a standard table or something of forms people consult
It just comes out of the geometric interpreation of vector addition.
You usually learn about it either in this class or multivariable calculus.
hmm
its like
you fix a vector (-2,1,0)^T
and change the parameter x3
in the direction of the other one
youre scaling the vector being summed by the parameter
I have solved part a) i)
But I am completely unsure as how to approach part a) ii) and the intuitive reasoning behind it. I would very much appreciate an explanation.
you've found the time $t_0$ at which the altitude is 60 meters in part (a)(i)
Ann:
you now need to find the angle between $\mathbf{r}(t_0)$ and the $xy$ plane
Ann:
Most definitely 🙂 I'm struggling with the application of finding the angle itself @dusky epoch I've been thinking to find the dot product between r(t0), and r(t0) without the k component, but I'm not too sure if that's the case, and why it is.
there are two possible routes
either you find the angle between r(t0) and k, then subtract it from pi/2
or you project r(t0) onto the xy plane, and find the angle between that and r(t0)
What's the logic behind subtracting the angle with the k unit vector from 90o?
Ohhhhh
I think i get it, that's very smart 😄
Is it because the entire angle from the k axis to the xy plane constitutes pi/2? @dusky epoch And so, we subtract to find the remaining angle
yes
I'm not too sure about how to project it onto the x-y plane, though
I know vector projections involve multiplying twice by the unit vector in a specific direction
Wait a second, would we find the dot product between r(t0) and r(t0) in the x-y plane (so just remove the k component). If so, that now makes a lot of sense, as that would give the line of the vector without it's altitude. @dusky epoch
Thank you for provoking my thought-process btw, instead of simply giving me the answer.
How would we do part b)
I made the i component equal to 0, and i got an invalid solution
The i component of r(t) @dusky epoch
why
Should it have been velocity?
yes of course it should've been velocity
what you found is when the particle touches the y axis
or goes through
Completely right. Thank you.
I'm quite confused about parts a) and b). I used constant acceleration formulas, but I don't think I was close to showing it.
@harsh parrot dude you there?
Anyway, you got it wrong, the speed at which the car took off the top of the cliff doesn't matter at all in the first part. While you're considering vertical motion you gotta consider initial velocity in vertical direction i.e. y-axis which is 0 in this case. So all you gotta do is :
Ignore the top couple lines
@wintry steppe thank you :)
I'm assuming for part b, we can just multiply the initial speed by the time (4 seconds)
Given it is in the horizontal direction
No need to thank mate. We're here to help each other out right?
Of course, I appreciate that man.
Yeah you can take t = 4 in the second part too since it won't be travelling horizontally after bumping into the ground ;)
Thanks again mate, I hope you get the same help I just did when you need it.
Anytime mate :)
well, it's not linear algebra
just because it's a university course doesn't mean it can't go in the "pre-university" channels
aii
where did you get your numbers from?
the number of columns that are not pivot columns
no, thats what it means to be a free variable
basic variables are variables that are not free
so columns that are pivot columns
Hi! I have quite the trouble understanding generalized vector spaces. Could anyone tell me why the objects inside a generalized vector space are called vectors but don't actually requires to be vectors?
Why not call them Sets or something that doesn't have anything to do with vectors?
ignoring what a vector space is
what is a vector, to you?
i ask because you say "objects inside a generalized vector space are called vectors but don't actually requires to be vectors"
For me vectors are a quantity with a direction, or a segment with direction
okay
But in my textbook (Advanced engineering mathematics, by Greenberg)
They say that a vector can be anything
like a matrix or a function
well you need to understand a vector space before that
so
among other things, vectors can be added and multiplied by scalars in ways that obey certain laws (associativity, commutativity, etc.)
the idea of a vector space takes this and generalizes it
the definition of vector space lets one see objects beyond boxes of pointy arrows as vector spaces all the same with the similar structure we like from the original boxes
I understand pretty well the concept of vectors in higher dimensions which can't be represented as arrows, so could I say that the set of vectors of 4 dimensions is a vector space?
nope we're not restricting our talk to R^n
yes, but if you want to understand the idea of an abstract vector space, you should completely forget the idea of vectors as a thing with direction and magnitude
anyways i am going to leave this to rokabe because i know he doesn't like having multiple people in one channel
So as long as any mathematical objects follows the properties of vector addition and scalars multiplication can be called a vector?
it can be called*
we have the so called vector space axioms which is basically a list of criteria for a set, with given definitions of addition & scaling of elements in that set, to qualify as a vector space
after all that, elements of that vector space can be called vectors
So, if I understand,the set of all 2D vectors, is 1 particular Vector Space
and same for the set of all 3d vectors
etc...
but Anything else which satisfies these axioms is also a vector space
since we're talking of the definition of vector space, i'm going to ask you to specify how you're defining addition & scaling on those spaces, and what you mean by 2d
Ahhh we call the 2d arrows vectors because they are part of a vector space
I think my mind was going the other way around
So, if I understand,the set of all 2D vectors, is 1 particular Vector Space
there are gaps in what you said, namely
i'm going to ask you to specify how you're defining addition & scaling on those spaces, and what you mean by 2d
Additon is when you take a vector, add it to another vector
and the result is a vector
it is commutative and associative
1st clarify wym 2d
Well I mean the 2d arrows, like U = (u1, u2)
you don't have to talk of them visually as arrows
by 2d space you mean the set of all ordered pairs with real entries?
Yeah I guess
the set of all pairs (x,y) where x,y are real numbers
Yeah
we call that R^2 which is shorthand for RxR, a cartesian product of R with R
now how do you like to define adding pairs ie (a,b)+(c,d)=?
how about scaling a pair ie c*(a,b)=?
(ca, cb)
now keep your definitions of addition & scaling on the side
have you seen the vector space axioms?
Yeah
have you proved smth is a vector space using em?
Yeah
I couldn't get into my head that matrices could be called vectors but I think I am starting to get it now
so this shouldn't be new. make sure R^2, along with how you define addition & scaling, satisfies all the axioms, then you can call R^2, with the same definitions of addition & scaling, and with scalars presumably coming from R, a vector space, and any element in R^2 can be called a vector
yes you can do the same thing with matrices, say the set of all n by m matrices with real entries, with addition & scaling defined the usual entrywise way, with real scalars. go through the axioms with that set, that's a vector space too
I think I'm stupid but how in the world do you graph this
draw lines
like just random lines on my paper?
no
each equation corresponds to a line in the plane
$x_1 + x_2 = 4$ to the line $x_2 = -x_1 + 4$, and $x_1 - x_2 = 2$ to the line...
TTerra:
once you find that second one you should be able to graph both lines
why subtract x1 instead of x2
because i am rearranging the equation $x_1 + x_2 = 4$ for $x_2$ in terms of $x_1$
TTerra:
when you guys are done would you mind if I asked a question
not sure if discussion is still ahppening
it is up to apollo
👍
if they don't respond in like, 10 minutes, then just ask
ok so lets say I want to solve for x2 for the 2nd equation, so it would be
$x_1 - x_2 = 2$ then $-x_2 = 2 - x_1$ then $x_2 = -2 + x_1$
Apollo:
yes
oh lol
and it would get me the same result regardless if i solved for x1 or x2
right?
the same solution, yeah
I am wondering if the solution set lies in a plane because we are confined to (b1 -1/2b2 + b3) = 0 or because we only have 2 pivots?
I feel the former makes more sense because if we have 3 pivots then b1, b2, b3 could be anything which allows for coverage of all of R^n
am I thinking of this right
Can anyone explain to me how I go about solving a question like this ? This linear algebra class literally makes no sense to me ☠️
I don’t even know what R3 means .. all real numbers cubed??
$\bR^3$ is the space of vectors with three real number elements
Namington:
Namington:
Just because it has 3 things on it ?
whereas $\begin{pmatrix}7\-3\-14.349034\0\end{pmatrix}$ is not, since it has 4 entries
Namington:
Ah ok
and $\begin{pmatrix}4+i\31.2\-i\end{pmatrix}$ is not, since $i$ is not a real number
Namington:
Namington:
each entry in the vector corresponding to one of the coordinates in (x, y, z)
So when the question asks to find two points that are not in the set ... does it mean like two separate r^3 sets or 2 individual things in the set (like x and y)
two things that are not in the set l
your image does not include what l is
so its pretty hard to answer that
but presumably l is a separate set, defined in the question or a previous part somewhere
So I already tried to solve for x and y and have z free , right ? At least I think that’s right , so from how I understand I can pick any point on z
So if I can just pick any point on z, why can’t I just pick any numbers for x and y that don’t match up to Z for the same number and that not be in the set
im not quite sure what you mean
you have free variables, which means that what you choose for z will affect the values of x and y, but it will do so in a predictable way
Yeah. So if I say z = 1 and that gives me a certain value for x and y , then I can say that perticular x and y does belong to L
So why can’t I say something along the lines of x and y being something else while z still being 0 then that set shouldn’t belong to L because it’s not true
for example, lets say i had the system:
[ x + y = 1 ]
[ y + z = 0]
then the solution vectors will look like $\begin{pmatrix}x\y\z\end{pmatrix} = \begin{pmatrix}z+1\-z\z\end{pmatrix}$
Namington:
where the value of z is chosen arbitrarily
for example, if i choose $z = 5$, then that particular solution is $\begin{pmatrix}6\-5\5\end{pmatrix}$
Namington:
i.e. x = 6, y = -5, z = 5
here the set l would represent the set of all possible vectors which we get by choosing any value of z
(naturally your set will look a bit different since your system is different, but the same ideas apply)
Ok so , since the question is asking to find something that does not belong to that
Can I say x = 7 , y = -4 , z = 5
I mean it doesn’t belong to the set , because x and y are wrong ?
so idk if that works
Yeah I mean for your example tho
right, then yeah
that would be an answer to #4
(well, one of the two vectors you need for an answer)
So all I have to do is pick numbers that are wrong ?
Ah okay awesome
at least that's what i'm assuming, you cut off some of the text in your image
And then for parellel lines , xD how do I do that lol ?
Uhhhhhhhhhh
Lemme think for a second lol
Isn’t it like the solution of 2 of them or something ?
Idk ☠️
Or can I just arbitrarily put in values for z and then maybe make a line out of the points ?
sorry, have to leave right away - hopefully someone else is available to help - but the key term to look up here is "vector equation of a line"
your textbook might have something on it
Ah okay, thanks for the help !
it’s about sub vector space, can somebody explain to me which of the following sets are subspaces of real numbers ^n, the rule: n element of natural numbers with n >= 2, i‘m a bit lost
do you know the definition of a subspace
this exercise is only a matter of applying that
only a bit
do you need me to remind you of it & take you through checking U and V against it?
I'm wondering what a 2D plane represent? Does it represent all combinations of vectors in a 2d plane? Or potential vectors?
A plane in the traditional sense is just a flat two-dimensional surface existing in $\mathbb{R}^3$ and has scalar equation $Ax + By + Cz = D$ and vector equation $ \langle a_1,a_2,a_3 \rangle + t\langle b_1, b_2, b_3 \rangle + s \langle c_1, c_2, c_3 \rangle$ $t, s \in \mathbb{R}$. A plane, in general, is a vector space having dimension 2. However, a hyperplane generalizes the concept of a plane. A hyperplane is a subspace of a vector space of dimension $n$ that has dimension $n - 1$. What we think of as a plane in the traditional sense, is a hyperplane of $\mathbb{R}^3$. All of $\mathbb{R}^2$ is a plane in the traditional sense, but if you want to think of what a plane is with respect to $\mathbb{R}^2$ then that's a hyperplane and it's any subspace that has dimension 1. Meaning that lines are "planes" i.e. hyperplanes in 2D spaces.
TheDon:
Hey guys
Once I was shown here a picture that talked about determinants and what its value mean
I was wondering if any of you know what picture I m talking about
The volume interpretation?
So if $$ \overrightarrow{c}= 3*\overrightarrow{m} + 3*\overrightarrow{n} and \overrightarrow{d} = \overrightarrow{m} - \overrightarrow{n} $$ then what is $$ |-1/2 \overrightarrow{c} \times \overrightarrow{d}| $$ equal to? $$\overrightarrow{n} & \overrightarrow{m}$$are unit vectors
Lonac:
