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A set S is a basis for V if
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1. S spans V
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2. S is LI.
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1. If S is a LI set of vectors in V, then S is a basis for V
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2. If S spans V, then S is a basis for V
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P[x]_B' = [x]_B
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[x]_B' = P-1 [x]_B
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[B B'] -> [ I P-1 ]
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[B' B ] -> [ I P ]
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if u = u1i + u2j + u3k
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AND
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v = v1i + v2j + v3k
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THEN
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u x v = (u2v3 - u3v2)i - (u1v3 -u3v1)j + (u1v2 - u2v1)k
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u + v is within V
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u+v = v+u
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u+(v+w) = (u+v)+w
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u+0 = u
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u-u = 0
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cu is within V
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c(u+v) = cu+cv
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(c+d)u = cu+du
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c(du) = (cd)u
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1*u = u
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length/norm ||v|| = sqrt(v_12 +...+ v_n2
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||cv|| = |c| ||v||
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v / ||v|| is the unit vector
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distance d(u,v) = ||u-v||
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Dot product u•v = (u_1v_1 +...+ u_nv_n)
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n cos(theta) = u•v / (||u|| ||v||)
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u&v are orthagonal when dot(u,v) = 0
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The scalar lambda(Y) is called an Eigenvalue of A when there is a nonzero vector x such that Ax = Yx.
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Vector x is an Eigenvector of A corresponding to Y.
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The set of all eigenvectors with the zero vector is a subspace of Rn called the Eigenspace of Y.
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1. Find Eigenvalues: det(YI - A) = 0
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2. Find Eigenvectors: (YI - A)x = 0
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If A is a triangular matrix then its eigenvalues are on its main diagonal
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1. B = {v1, v2, ..., vn}
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2. B' = {w1, w2, ..., wn}:
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w1 = v1
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w2 = v2 - projw1v2
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w3 = v3 - projw1v3 - projw2v3
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wn = vn - ...
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3. B'' = {u1, u2, ..., un}:
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ui = wi/||wi||
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B'' is an orthonormal basis for V
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span(B) = span(B'')
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Rn
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C(-inf, +inf)
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C[a, b]
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P
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P_n
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M_m,n
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||u|| = sqrt<u,u>
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d(u,v) = ||u-v||
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cos(theta) = <u,v> / (||u|| ||v||)
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u&v are orthagonal when <u,v> = 0
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proj_v u = <u,v>/<v,v> * v
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v is a linear combo of u_1 ... u_n
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.
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V & W are Vspaces. T:V->W is a linear transformation of V into W if:
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1. T(u+v) = T(u) = T(v)
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2. T(cu) = cT(u)
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T is one-to-one iff ker(T) = {0}
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T is onto iff rank(T) = dim(W)
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If dim(T) = dim(W) then T is one-to-one iff it is onto
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nullity(T) = dim(kernal)
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rank(T) = dim(range)
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range(T) + nullity(T) = n (in m_x n)
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dim(domain) = dim(range) + dim(kernal)
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1. u+v are in W
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2. cu is in w
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