NOTES Flashcards
VECTOR SPACE
- ∃0∈V : 0+u=u, ∀u∈V
- u+v=v+u, ∀u,v∈V
- u(v+w) = (u+v)+w, , ∀u,v,w∈V
- ∃z∈V : u+z=0, ∀u∈V
- 1.u=u, ∀u∈V
- a.b.u = ab.u, ∀u∈V, ∀a,b∈F
- a.(u+v) = (a.u)+(a.v), ∀u,v∈V, ∀a∈F
- u.(a+b) = (a.u)+(b.u), ∀u∈V, ∀a,b∈F
V “zero vector space”
V={0}
U is subspace of V (def.)
if U is subset of V that is a vector space with same vector addition and scalar multiplication as in V
U⊆V subpace of V
⟺
cu+v ∈U whenever u,v ∈U and c ∈F
LINEAR COMBINATION of v1,…,vr ∈V
the expression c1v1 + … + crvr
for given c1,…,cr ∈F
span(v1,..,vr∈V)
set of all linear combinations of v1,…,vr
:= {c1v1+…+crvr|c1,…,cr∈F} ⊆V
v∈span(v1,…,vn)
span(∅)
= {0}
PROPERTIES OF SPAN (thm.1.4.9,10)
let U,W ⊆ V
1. span U subspace of V
2. U ⊆ span U
3. U = span U ⟺ U is subspace of V
4. span(spanU) = span U
5. U ⊆W ⟹ span U ⊆ span W
spanning set of V
{v1,..,vr∈V} if every vector in V can be written as linear comb. of v1,..,vr
span(v1,..,vr) = V
span(U ∪ W) when U,W subspaces of V
= U + W
is subspace of V
DIRECT SUM
whenever U,W subspaces of V and U ∩ W = {0}
i.e. each vector in U+W can be expressed as unique sum of vector in U and vector in W
v1,…,vr LINEARLY DEPENDENT
if there are scalars c1,…,cr ∈F not all zero such that
c1v1+…+crvr=0
v1,…,vr LINEARLY INDEPENDENT
not linearly dependent
⟺
c1=…=cr=0
Thm.1.6.11
v1,…,vr linearly independent
then a1v1+…+arvr = b1v1+…+brvr
⟺ ai=bi each i=1,…,r
BASIS of vector space V
v1,…,vr∈V
if linearly independent and span(v1,…,vr)=V
MATRIX BASIS
Let A = [a1 … an] ∈ Mn(F) be invertible then a1,…,an is basis for Fn
REPLACEMENT LEMMA
- suppose β=u1,…,ur spans non-zero vector space V
- let nonzero v∈V be v= Σciui from i=1 to r
THEN - cj ≠ 0 for some j=1,…,r
- cj ≠ 0 ⟹ v,u1,…,u(^)j,…,ur (*) spans V
- β basis for V and cj ≠ 0 ⟹ (*) is basis for V
- r>=2, β basis for V and v∉span{u1,…,uk} for some k ∈{k+1,k+2,…,r} such that v,u1,…,uk,uk+1,…,u(^)j,…,ur is a basis for V
DIMENSION V
- {v1,…,vn} is basis of V
⟹ V dimension is n - V={0} ⟹ dimension 0
FINITE DIMENSIONAL
- V has dimension n integer
⟹ dimension denoted dimV
INFINITE DIMENSIONAL
- V not finite dimensional
DIMENSION MATRIX
Let A = [a1 … an] ∈ Mmxn(F) and β=a1,…,an in Fm.
then dim span β = dim col A = rank A
dim(U ∩ W) + dim (U + W) =
dim U + dim W
β-BASIS REPRESENTATION FUNCTION
- the function [.]_β :V->Fn defined by [u]_β = [c1…cn]^T
where β = v1,…,vn is basis for finite-dim. V and u∈V is any vector written as (unique) linear comb. u= c1v1+…+cnvn - c1,…,cn are “coordinates of u” w.r.t. basis β.
- [u]_β is “β-coordinate vector of u”
LINEAR TRANSFORMATION
T:V->W
T(cu+v) = cT(u) +T(v) ∀c∈F,∀u,v∈V
LINEAR OPERATOR
V=W
SET OF LINEAR TRANSFORMATIONS/OPERATORS
L(V,W)/L(V)
LINEAR TRANSFORMATION INDUCED BY A
T_A
T∈L(V,W) is one-to-one ⟺
ker(T) = {0}
LINEAR TRANSFORMATION PROPERTIES
- T(cv) = cT(v)
- T(0) = 0
- T(-v) = -T(v)
- T(a1v1+…+anvn) = a1T(v1)+…+anT(vn)
KerT
T:V->W
= {v∈V|T(v) = 0}
RanT
T:V->W
= {w∈W|∃v ∈V : T(v)=w}
SYLVESTER EQUATION
T(X) = AX+XB = C
β-γ change of basis matrix
γ[I]β = [[v1]γ … [vn]γ]
β = {v1,…,vn}
γ = {w1,…,wn} bases for V
- describes how to represent each vector in basis β as linear combination of vectors in basis γ
inverse of γ[I]β
β[I]γ = [[w1] β … [wn] β]
cor.2.4.11,12
- if a1,…,an is basis of Fn then A=[a1…an] ∈Mn(F) is invertible
- A∈Mn(F) invertible ⟺ rankA=n
A, B∈Mn(F) SIMILAR
if there is invertible S∈Mn(F) such that A = SBS^(-1)