SEHH1069 Last minutes Linear System Consistent: Have solution(s) -Unique solution (Independent) -Infinitely many solution (Dependent) -Homogeneous 0 solution = trivial sol non-0 solution = non-trivial sol Inconsistent: -No solutions Elementary row operations - Interchange row π π β· π π 1 - Multiply and divide element of a row ππ π → π π π π π → π π (π ≠ 0) - Add and subtract row to another row ππ π + π π → π π To be: row echelon form (REF) (Gaussian Elimination) 1 ∗ (0 1 0 0 reduced row echelon form (RREF) (Gauss-Jordan Elimination) ∗ ∗ ∗| ∗) 0 0 1 (0 0 0 ∗ ∗ 1 ∗| ∗ ) 0 0 0 Requirement of row echelon form: ο· Non-0 rows are above any 0 rows ο· First non-0 entry(left->right) in row is 1 (Leading 1) ο· All entries below leading 1 are 0 Requirement of reduced row echelon form: ο· It is in REF ο· Each leading 1 is the only non-0 entry in its column Matrix Algebra Row/Column = Horizontal/Vertical (π[πππ€π ] × π[ππππ’πππ ] πππ‘πππ₯) Row/Column matrix (1 × π πππ‘πππ₯)/(π × 1 πππ‘πππ₯) Null(0) matrix All element are 0 Square matrix (π × π πππ‘πππ₯) Diagonal matrix A square matrix in which all the entries off the main diagonal are zero. π e.g., π΄ = (0 0 0 π 0 0 ππ π 0),Note that π΄ = ( 0 π 0 0 ππ 0 0 0 ) , π ∈ β€+ . ππ Identity Matrix(Ι) = a diagonal matrix with all diagonal element = 1. Triangular matrix -Lower triangular -Upper triangular ∗ ∗ 0 0 π΄ = (∗ ∗ 0) π΄ = (0 0 ∗ ∗ ∗ ∗ ∗ ∗ ∗) 0 ∗ Transpose of a matrix π (π π π π β π π π π ) = (π π π (π΄π )π = π΄ π π π π β) π (π΄ ± π΅)π = π΄π ± π΅ π (ππ΄)π = ππ΄π (π΄π΅)π = π΅ π π΄π Trace of a matrix (for square matrix) π π΄ = (π π π π β π π ) , π‘π(π΄) = π + π + π π π‘π(π΄ + π΅) = π‘π(π΄) + π‘π(π΅) π‘π(ππ΄) = ππ‘π(π΄) π‘π(π΄) = π‘π(π΄π ) π‘π(π΄π΅) = π‘π(π΅π΄) π‘π(π−1 π΄π) = π‘π(π΄) Inverse of a matrix (for square matrix) πΌπ π΄π΅ = π΅π΄ = πΌ, π΄−1 = π΅ πππ π΅ −1 = π΄ Invertible = non-singular : det π΄ ≠ 0 Not invertible = singular : det π΄ = 0 π π π΄=( π ) π π΄−1 = 1 π ( ππ − ππ −π (π΄π΅)−1 = π΅ −1 π΄−1 π΄−π = (π΄−1 )π = (π΄π )−1 (π΄π )−1 = (π΄−1 )π (ππ΄)−1 = π −1 π΄−1 Inversion Algorithm (π΄|πΌ)~(πΌ|π΅) Adjoint Method π΄−1 = det(π΄)−1 πππ(π΄) Cramer’s rule π π π π π π π |π π π | |π |π π π | π π π π₯1 π π π π π (π π π) (π₯2 ) = (π) π₯1 = π β π π₯2 = π₯3 = π π π π π π π π₯3 π β π π |π π π | |π π π | |π π β π π β π π Determinants det(π΄π ) = det(π΄) det(ππ΄) = π π det(π΄) πππ π × π πππ‘πππ₯ π΄ 1 det(π΄π΅) = det(π΄) det(π΅) det(π΄−1 ) = det(π΄) π π΄ = |π π π |π π π π β π π β π π| π ππ |π π ππ π β ππ π | = ππππ‘(π΄) π π + ππ π π | = − det(π΄) | π π π π + ππ π β π + ππ π | = det(π΄) π π π β π π β π π| π π π| π −π ) π Adjoint Matrix π π 2×2π΄ =( π π 3×3π΄ =( π π΄−1 = π ) π π π β π −π πππ(π΄) = ( −π ) π π | β π π ) πππ(π΄) = − |π β π π | ( π 1 πππ(π΄) det(π΄) adj(π΄) = det(π΄) π΄−1 det(πππ(π΄)) = det(det(π΄) π΄−1 ) πππ‘(πππ(π΄)) = det(π΄)π × det(π΄)−1 πππ‘(πππ(π΄)) = det(π΄)π−1 adj(π΄) = det(π΄) π΄−1 (πππ(π΄)) (πππ(π΄)) −1 −1 = (det(A) π΄−1 )−1 = = 1 det(πππ(π΄)) π΄ det(π΄) πππ(πππ(π΄)) πππ(πππ(π΄)) = det(πππ(π΄)) π΄ det(π΄) πππ(πππ(π΄)) = det(π΄)π−2 π΄ Symmetric Matrix π΄ = π΄π Skew symmetric Matrix π΄ = −π΄π π π π π π π | −| | | | π β π π π π π π π π | |π π | − | | π β π π π π π π | − |π π | | | π π π ) Function [open intervals] including border (closed intervals) excluding border Inverse function y = π(π₯) ~ π₯ = π −1 (π¦) ~ π¦ = π −1 (π₯) Limit - Simplification - Rationalization (sqrt) - 0 ±∞ π ′ (π₯) π(π₯) L'Hospital's Rule (0 \ ±∞) lim π(π₯) = lim π′ (π₯) π₯→π π₯→π Continuity lim π(π₯) = π(π) π₯→π Differentiation Differentiable Continuity and no “corner” at π₯ → π Chain rule ππ¦ ππ₯ = ππ¦ ππ’ β ππ’ ππ₯ Implicit Differentiation Inverse function theorem (π −1 )′ (π₯ ) = 1 π ′ (π−1 (π₯)) Logarithmic Differentiation π¦ = π₯π ln π¦ = π ln π₯ 1 ππ¦ π ln π₯ β =π π¦ ππ₯ ππ¦ Increasing/Decreasing π ′ (π₯) > 0 / π′(π₯) < 0 Critical/Maximum/Minimum Point π ′ (π₯) = 0 Convex/Concave π ′′ (π₯) > 0 / π′′(π₯) < 0 Point of inflexion π ′ ′(π₯) = 0 SAsymtotes o Vertical Asymptote lim π(π₯) = ±∞ ππ lim π(π₯) = ±∞ π₯→π+ π₯→π− o Horizontal Asymptote lim π(π₯) = πΏ ππ lim π(π₯) = πΏ π₯→+∞ π₯→−∞π Integrals - Partial Fractions - Substitution Part ∫ π(π₯)π′ (π₯)ππ₯ = π(π₯)π(π₯) − ∫ π(π₯)π′(π₯) ππ₯ - FTC o FTC I π₯ πΉ(π₯) = ∫ π(π‘)ππ‘ πππ π ≤ π₯ ≤ π π π₯ π [∫ π(π‘)ππ‘] = π(π₯) πππ π ≤ π₯ ≤ π ππ₯ π o FTC II π ∫ π(π₯) ππ₯ = ∫ π(π)ππ₯ − ∫ π(π) ππ₯ π - Area/Volume π o Area ∫π [π(π₯) − π(π₯)]ππ₯ Formulas and Identities(Provided/Learnt) sin θ 1 1 1 sec π = csc π = cot π = cos θ cos π sin π tan π 2 2 2 2 2 sin π + cos π = 1 1 + tan π = sec π 1 + cot π = csc 2 π sin(π ± π) = sin π cos π ± cos π sin π cos(π ± π) = cos π cos π β sin π sin π tan θ = tan(π ± π) = tan π ± cos π 1 β tan π tan π sin π₯ cos π¦ = sin(π₯ − π¦) + sin(π₯ + π¦) 2 cos π₯ cos π¦ = cos(π₯ − π¦) + cos(π₯ + π¦) cos(2π₯) = 2 cos 2 π₯ − 1 = 1 − 2 sin2 π₯ 2 sin π₯ sin π¦ = cos(π₯ − π¦) − cos(π₯ + π¦) 2 sin(2π₯) = 2 sin π₯ cos π₯ 1 1 sin πΌ ± sin π½ = 2 sin (πΌ ± π½) cos (πΌ β π½) 2 2 1 1 cos πΌ + cos π½ = 2 cos (πΌ + π½) cos (πΌ − π½) 2 2 1 1 cos πΌ − cos π½ = −2 sin (πΌ + π½) sin (πΌ − π½) 2 2 1 n lim (1 + ) = e n→∞ n π(x) c x r 1 lim (1 + π)π = π π→0 π ′ (x) 0 rx r−1 ax ax ln π sin π₯ cos π₯ cos π₯ − sin π₯ tan π₯ sec 2 π₯ cot π₯ − csc 2 π₯ sec π₯ sec π₯ tan π₯ csc π₯ − csc π₯ cot π₯ π −1 sin (ππ₯) cos−1 (ππ₯) tan−1(ππ₯) √1 − (ππ₯)2 π − √1 − (ππ₯)2 π 1 + (ππ₯)2 π(x) ∫ π(x)ππ₯ 1 π₯ ln|π₯| ππ₯ (π > 0 πππ π ≠ 1) ππ₯ ln π π₯π sin π₯ π₯ π+1 π+1 − cos π₯ cos π₯ sin π₯ 2 sec π₯ tan π₯ csc 2 π₯ − cot π₯ sec π₯ tan π₯ sec π₯ csc π₯ cot π₯ 1 − csc π₯ √1 − (ππ₯)2 1 1 + (ππ₯)2 1 −1 sin (ππ₯) π 1 tan−1(ππ₯) π ∫ ln π₯ ππ₯ ∫ tan2 π₯ ππ₯ 1 = ln(π₯) π₯ − ∫ π₯ ( ) ππ₯ π₯ = ∫ sec 2 π₯ + 1 ππ₯ = π₯ ln(π₯) − ∫ ππ₯ = π₯ ln(π₯) − π₯ + πΆ sin π₯ ππ₯ cos π₯ = −∫ 1 π cos π₯ cos π₯ = − ln|cos π₯| + πΆ = ln|sec π₯| + πΆ ∫ sec π₯ ππ₯ = ∫ sec π₯ × ∫ sec 2 π₯ ππ₯ = π‘ππ π₯ + πΆ ∫ tan π₯ ππ₯ =∫ = tan π₯ + π₯ + πΆ sec π₯ + tan π₯ ππ₯ sec π₯ + tan π₯ (sec 2 π₯ + sec π₯ tan π₯) ππ₯ sec π₯ + tan π₯ 1 =∫ π(sec π₯ + tan π₯) sec π₯ + tan π₯ ∫ sin−1 π₯ ππ₯ = ∫ 1 × sin−1 π₯ ππ₯ = π₯ sin−1 π₯ − ∫ π₯ × 1 ππ₯ √1 − π₯ 2 1 1 = π₯ sin−1 π₯ − ∫ π(1 − π₯ 2 ) 2 √1 − π₯ 2 1 1 = π₯ sin−1 π₯ − × 2 × (1 − π₯ 2 )2 + πΆ 2 = π₯ sin−1 π₯ − √1 − π₯ 2 + πΆ =∫ = ln|sec π₯ + tan π₯| + πΆ ∫ tan−1 π₯ ππ₯ = ∫ 1 × tan−1 π₯ ππ₯ = π₯ tan−1 π₯ − ∫ π₯ × ∫ sin2 π₯ ππ₯ 1 cos 2π₯ =∫ − dx 2 2 = x 1 − ∫ cos 2π₯ ππ₯ 2 2 = x 1 1 − × ∫ cos 2π₯ π2π₯ 2 2 2 = x sin 2π₯ − +C 2 4 1 ππ₯ 1 + π₯2 1 1 = π₯ tan−1 π₯ − ∫ π(1 + π₯ 2 ) 2 1 + π₯2 1 = π₯ tan−1 π₯ − ln(1 + π₯ 2 ) + πΆ 2