Chapter 2: Vector spaces

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Presentation transcript:

Chapter 2: Vector spaces Vector spaces, subspaces, basis, dimension, coordinates, row-equivalence, computations

A vector space (V,F, +, .) F a field V a set (of objects called vectors) Addition of vectors (commutative, associative) Scalar multiplications

Examples Other laws are easy to show This is just written differently

The space of functions: A a set, F a field If A is finite, this is just F|A|. Otherwise this is infinite dimensional. The space of polynomial functions The following are different.

Subspaces V a vector space of a field F. A subspace W of V is a subset W s.t. restricted operations of vector addition, scalar multiplication make W into a vector space. +:WxW -> W, :FxW -> W. W nonempty subset of V is a vector subspace iff for each pair of vectors a,b in W, and c in F, ca+b is in W. (iff for all a,b in W, c, d in F, ca+db is in W.) Example:

is a vector subspace with field F. Solution spaces: Given an mxn matrix A Example x+y+z=0 in R3. x+y+z=1 (no) The intersection of a collection of vector subspaces is a vector subspace is not.

Span(S) Theorem 3. W= Span(S) is a vector subspace and is the set of all linear combinations of vectors in S. Proof:

Sum of subsets S1, S2, …,Sk of V If Si are all subspaces of V, then the above is a subspace. Example: y=x+z subspace: Row space of A: the span of row vectors of A. Column space of A: the space of column vectors of A.

Linear independence A subset S of V is linearly dependent if A set which is not linearly dependent is called linearly independent: The negation of the above statement

Basis A basis of V is a linearly independent set of vectors in V which spans V. Example: Fn the standard basis V is finite dimensional if there is a finite basis. Dimension of V is the number of elements of a basis. (Independent of the choice of basis.) A proper subspace W of V has dim W < dim V. (to be proved)

Example: P invertible nxn matrix. P1,…,Pn columns form a basis of Fnx1. Independence: x1P1+…+xnPn=0, PX=0. Thus X=0. Span Fnx1: Y in Fnx1. Let X = P-1Y. Then Y = PX. Y= x1P1+…+xnPn. Solution space of AX=0. Change to RX=0. Basis Ej uj=1, other uk=0 and solve above

Infinite dimensional example: V:={f| f(x) = c0+c1x+c2x2 + …+ cnxn}. Thus the dimension is n-r: Infinite dimensional example: V:={f| f(x) = c0+c1x+c2x2 + …+ cnxn}. Given any finite collection g1,…,gn there is a maximum degree k. Then any polynomial of degree larger than k can not be written as a linear combination.

Theorem 4: V is spanned by Then any independent set of vectors in V is finite and number is  m. Proof: To prove, we show every set S with more than m vectors is linearly dependent. Let be elements of S with n > m. A is mxn matrix. Theorem 6, Ch 1, we can solve for x1,x2,…,xn not all zero for Thus

This defines dimension. dim Fn=n. dim Fmxn=mn. Corollary. V is a finite d.v.s. Any two bases have the same number of elements. Proof: B,B’ basis. Then |B’||B| and |B||B’|. This defines dimension. dim Fn=n. dim Fmxn=mn. Lemma. S a linearly independent subset of V. Suppose that b is a vector not in the span of S. Then S{b} is independent. Proof: Then k=0. Otherwise b is in the span. Thus, and ciare all zero.

Theorem 5. If W is a subspace of V, every linearly independent subset of W is finite and is a part of a basis of W. W a subspace of V. dim W  dim V. A set of linearly independent vectors can be extended to a basis. A nxn-matrix. Rows (respectively columns) of A are independent iff A is invertible. (->) Rows of A are independent. Dim Rows A = n. Dim Rows r.r.e R of A =n. R is I -> A is inv. (<-) A=B.R. for r.r.e form R. B is inv. AB-1 is inv. R is inv. R=I. Rows of R are independent. Dim Span R = n. Dim Span A = n. Rows of A are independent.

Theorem 6. dim (W1+W2) = dim W1+dimW2-dimW1W2. Proof: W1W2 has basis a1,…,ak. W1 has basis a1,..,ak,b1,…,bm. W2 has basis a1,..,ak,c1,…,cn. W1+W2 is spanned by a1,..,ak,b1,…,bm ,c1,…,cn. There are also independent. Suppose Then By independence zk=0. xi=0,yj=0 also.

Coordinates Given a vector in a vector space, how does one name it? Think of charting earth. If we are given Fn, this is easy? What about others? We use ordered basis: One can write any vector uniquely

This sets up a one-to-one correspondence between V and Fn. Thus,we name Coordinate (nx1)-matrix (n-tuple) of a vector. For standard basis in Fn, coordinate and vector are the same. This sets up a one-to-one correspondence between V and Fn. Given a vector, there is unique n-tuple of coordinates. Given an n-tuple of coordinates, there is a unique vector with that coordinates. These are verified by the properties of the notion of bases. (See page 50)

Coordinate change? If we choose different basis, what happens to the coordinates? Given two bases Write

Example {(1,0),(0,1)}, {(1,i), (i,1)} X=0 iff X’=0 Theorem 7,Ch1, P is invertible Thus, X = PX’, X’=P-1X. Example {(1,0),(0,1)}, {(1,i), (i,1)} (1,i) = (1,0)+i(0,1) (i,1) = i(1,0)+(0,1) (a,b)=a(1,0)+b(1,0): (a,b)B =(a,b) (a,b)B’ = P-1(a,b) = ((a-ib)/2,(-ia+b)/2). We check that (a-ib)/2x(1,i)+ (-ia+b)/2x(i,1)=(a,b).