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SEHH1069 Cheat Sheet (Autosaved)

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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 𝑅𝑖 ⟷ 𝑅𝑗
1
- Multiply and divide element of a row π‘˜π‘…π‘– → 𝑅𝑖
π‘˜
𝑅𝑖 → 𝑅𝑖 (π‘˜ ≠ 0)
- Add and subtract row to another row π‘˜π‘…π‘– + 𝑅𝑗 → 𝑅𝑗
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‘š[π‘Ÿπ‘œπ‘€π‘ ] × π‘›[π‘π‘œπ‘™π‘’π‘šπ‘›π‘ ] π‘šπ‘Žπ‘‘π‘Ÿπ‘–π‘₯)
Row/Column matrix (1 × π‘› π‘šπ‘Žπ‘‘π‘Ÿπ‘–π‘₯)/(π‘š × 1 π‘šπ‘Žπ‘‘π‘Ÿπ‘–π‘₯)
Null(0) matrix All element are 0
Square matrix (π‘š × π‘š π‘šπ‘Žπ‘‘π‘Ÿπ‘–π‘₯)
Diagonal matrix
A square matrix in which all the entries off the main diagonal are zero.
π‘Ž
e.g., 𝐴 = (0
0
0
𝑏
0
0
π‘Žπ‘›
𝑛
0),Note that 𝐴 = ( 0
𝑐
0
0
𝑏𝑛
0
0
0 ) , 𝑛 ∈ β„€+ .
𝑐𝑛
Identity Matrix(Ι) = a diagonal matrix with all diagonal element = 1.
Triangular matrix
-Lower triangular -Upper triangular
∗
∗ 0 0
𝐴 = (∗ ∗ 0) 𝐴 = (0
0
∗ ∗ ∗
∗ ∗
∗ ∗)
0 ∗
Transpose of a matrix
π‘Ž
(𝑑
𝑔
𝑏
𝑒
β„Ž
𝑐 𝑇
π‘Ž
𝑓 ) = (𝑏
𝑖
𝑐
(𝐴𝑇 )𝑇 = 𝐴
𝑑
𝑒
𝑓
𝑔
β„Ž)
𝑖
(𝐴 ± 𝐡)𝑇 = 𝐴𝑇 ± 𝐡 𝑇
(π‘˜π΄)𝑇 = π‘˜π΄π‘‡
(𝐴𝐡)𝑇 = 𝐡 𝑇 𝐴𝑇
Trace of a matrix (for square matrix)
π‘Ž
𝐴 = (𝑑
𝑔
𝑏
𝑒
β„Ž
𝑐
𝑓 ) , π‘‘π‘Ÿ(𝐴) = π‘Ž + 𝑒 + 𝑖
𝑖
π‘‘π‘Ÿ(𝐴 + 𝐡) = π‘‘π‘Ÿ(𝐴) + π‘‘π‘Ÿ(𝐡)
π‘‘π‘Ÿ(𝑐𝐴) = π‘π‘‘π‘Ÿ(𝐴) π‘‘π‘Ÿ(𝐴) = π‘‘π‘Ÿ(𝐴𝑇 ) π‘‘π‘Ÿ(𝐴𝐡) = π‘‘π‘Ÿ(𝐡𝐴) π‘‘π‘Ÿ(𝑃−1 𝐴𝑃) = π‘‘π‘Ÿ(𝐴)
Inverse of a matrix (for square matrix)
𝐼𝑓 𝐴𝐡 = 𝐡𝐴 = 𝐼, 𝐴−1 = 𝐡 π‘Žπ‘›π‘‘ 𝐡 −1 = 𝐴
Invertible = non-singular : det 𝐴 ≠ 0
Not invertible = singular : det 𝐴 = 0
π‘Ž
𝑐
𝐴=(
𝑏
)
𝑑
𝐴−1 =
1
𝑑
(
π‘Žπ‘‘ − 𝑏𝑐 −𝑐
(𝐴𝐡)−1 = 𝐡 −1 𝐴−1 𝐴−π‘˜ = (𝐴−1 )π‘˜ = (π΄π‘˜ )−1 (𝐴𝑇 )−1 = (𝐴−1 )𝑇 (π‘˜π΄)−1 = π‘˜ −1 𝐴−1
Inversion Algorithm (𝐴|𝐼)~(𝐼|𝐡)
Adjoint Method 𝐴−1 = det(𝐴)−1 π‘Žπ‘‘π‘—(𝐴)
Cramer’s rule
π‘Ž 𝑗 𝑐
π‘Ž
𝑗 𝑏 𝑐
|𝑑 π‘˜ 𝑓 |
|𝑑
|π‘˜ 𝑒 𝑓 |
π‘Ž 𝑏 𝑐 π‘₯1
𝑗
𝑔
𝑙
𝑖
𝑔
(𝑑 𝑒 𝑓) (π‘₯2 ) = (π‘˜) π‘₯1 = 𝑙 β„Ž 𝑖 π‘₯2 =
π‘₯3 =
π‘Ž 𝑏 𝑐
π‘Ž 𝑏 𝑐
π‘Ž
π‘₯3
𝑔 β„Ž 𝑖
𝑙
|𝑑 𝑒 𝑓 |
|𝑑 𝑒 𝑓 |
|𝑑
𝑔 β„Ž 𝑖
𝑔 β„Ž 𝑖
𝑔
Determinants
det(𝐴𝑇 ) = det(𝐴)
det(π‘˜π΄) = π‘˜ 𝑛 det(𝐴) π‘“π‘œπ‘Ÿ 𝑛 × π‘› π‘šπ‘Žπ‘‘π‘Ÿπ‘–π‘₯ 𝐴
1
det(𝐴𝐡) = det(𝐴) det(𝐡) det(𝐴−1 ) = det(𝐴)
π‘Ž
𝐴 = |𝑑
𝑔
𝑑
|π‘Ž
𝑔
𝑒
𝑏
β„Ž
𝑏
𝑒
β„Ž
𝑐
𝑓|
𝑖
π‘˜π‘Ž
|𝑑
𝑔
π‘˜π‘
𝑒
β„Ž
π‘˜π‘
𝑓 | = π‘˜π‘‘π‘’π‘‘(𝐴)
𝑖
π‘Ž + π‘˜π‘‘
𝑓
𝑐 | = − det(𝐴) | 𝑑
𝑖
𝑔
𝑏 + π‘˜π‘’
𝑒
β„Ž
𝑐 + π‘˜π‘“
𝑓 | = det(𝐴)
𝑖
𝑏
𝑒
β„Ž
𝑏
𝑒
β„Ž
𝑗
π‘˜|
𝑙
𝑐
𝑓|
𝑖
−𝑏
)
π‘Ž
Adjoint Matrix
π‘Ž
𝑐
2×2𝐴 =(
π‘Ž
𝑑
3×3𝐴 =(
𝑔
𝐴−1 =
𝑏
)
𝑑
𝑏
𝑒
β„Ž
𝑑
−𝑐
π‘Žπ‘‘π‘—(𝐴) = (
−𝑏
)
π‘Ž
𝑒
|
β„Ž
𝑐
𝑓 ) π‘Žπ‘‘π‘—(𝐴) = − |𝑏
β„Ž
𝑖
𝑏
|
( 𝑒
1
π‘Žπ‘‘π‘—(𝐴)
det(𝐴)
adj(𝐴) = det(𝐴) 𝐴−1
det(π‘Žπ‘‘π‘—(𝐴)) = det(det(𝐴) 𝐴−1 )
𝑑𝑒𝑑(π‘Žπ‘‘π‘—(𝐴)) = det(𝐴)𝑛 × det(𝐴)−1
𝑑𝑒𝑑(π‘Žπ‘‘π‘—(𝐴)) = det(𝐴)𝑛−1
adj(𝐴) = det(𝐴) 𝐴−1
(π‘Žπ‘‘π‘—(𝐴))
(π‘Žπ‘‘π‘—(𝐴))
−1
−1
= (det(A) 𝐴−1 )−1 =
=
1
det(π‘Žπ‘‘π‘—(𝐴))
𝐴
det(𝐴)
π‘Žπ‘‘π‘—(π‘Žπ‘‘π‘—(𝐴))
π‘Žπ‘‘π‘—(π‘Žπ‘‘π‘—(𝐴)) = det(π‘Žπ‘‘π‘—(𝐴))
𝐴
det(𝐴)
π‘Žπ‘‘π‘—(π‘Žπ‘‘π‘—(𝐴)) = det(𝐴)𝑛−2 𝐴
Symmetric Matrix 𝐴 = 𝐴𝑇
Skew symmetric Matrix 𝐴 = −𝐴𝑇
𝑇
𝑑 𝑓
𝑑 𝑒
𝑓
| −|
| |
|
𝑔 β„Ž
𝑔 𝑖
𝑖
π‘Ž
𝑐
π‘Ž 𝑏
𝑐
|
|𝑔 𝑖 | − |
|
𝑔
β„Ž
𝑖
π‘Ž 𝑐
𝑐
π‘Ž 𝑏
| − |𝑑 𝑓 | |
|
𝑓
𝑑 𝑒 )
Function
[open intervals] including border (closed intervals) excluding border
Inverse function y = 𝑓(π‘₯) ~ π‘₯ = 𝑓 −1 (𝑦) ~ 𝑦 = 𝑓 −1 (π‘₯)
Limit
- Simplification
- Rationalization (sqrt)
-
0
±∞
𝑓 ′ (π‘₯)
𝑓(π‘₯)
L'Hospital's Rule (0 \ ±∞) lim 𝑔(π‘₯) = lim 𝑔′ (π‘₯)
π‘₯→𝑐
π‘₯→𝑐
Continuity
lim 𝑓(π‘₯) = 𝑓(π‘Ž)
π‘₯→π‘Ž
Differentiation
Differentiable
Continuity and no “corner” at π‘₯ → π‘Ž
Chain rule
𝑑𝑦
𝑑π‘₯
=
𝑑𝑦 𝑑𝑒
βˆ™
𝑑𝑒 𝑑π‘₯
Implicit Differentiation
Inverse function theorem
(𝑓 −1 )′ (π‘₯ ) =
1
𝑓 ′ (𝑓−1 (π‘₯))
Logarithmic Differentiation
𝑦 = π‘₯π‘Ÿ
ln 𝑦 = π‘Ÿ ln π‘₯
1 𝑑𝑦
𝑑 ln π‘₯
βˆ™
=π‘Ÿ
𝑦 𝑑π‘₯
𝑑𝑦
Increasing/Decreasing 𝑓 ′ (π‘₯) > 0 / 𝑓′(π‘₯) < 0
Critical/Maximum/Minimum Point 𝑓 ′ (π‘₯) = 0
Convex/Concave 𝑓 ′′ (π‘₯) > 0 / 𝑓′′(π‘₯) < 0
Point of inflexion 𝑓 ′ ′(π‘₯) = 0
SAsymtotes
o Vertical Asymptote
lim 𝑓(π‘₯) = ±∞ π‘œπ‘Ÿ lim 𝑓(π‘₯) = ±∞
π‘₯→π‘Ž+
π‘₯→π‘Ž−
o Horizontal Asymptote
lim 𝑓(π‘₯) = 𝐿 π‘œπ‘Ÿ lim 𝑓(π‘₯) = 𝐿
π‘₯→+∞
π‘₯→−∞𝑆
Integrals
- Partial Fractions
-
Substitution
Part
∫ 𝑓(π‘₯)𝑔′ (π‘₯)𝑑π‘₯ = 𝑓(π‘₯)𝑔(π‘₯) − ∫ 𝑔(π‘₯)𝑓′(π‘₯) 𝑑π‘₯
-
FTC
o FTC I
π‘₯
𝐹(π‘₯) = ∫ 𝑓(𝑑)𝑑𝑑 π‘“π‘œπ‘Ÿ π‘Ž ≤ π‘₯ ≤ 𝑏
π‘Ž
π‘₯
𝑑
[∫ 𝑓(𝑑)𝑑𝑑] = 𝑓(π‘₯) π‘“π‘œπ‘Ÿ π‘Ž ≤ π‘₯ ≤ 𝑏
𝑑π‘₯ π‘Ž
o FTC II
𝑏
∫ 𝑓(π‘₯) 𝑑π‘₯ = ∫ 𝑓(𝑏)𝑑π‘₯ − ∫ 𝑓(π‘Ž) 𝑑π‘₯
π‘Ž
-
Area/Volume
𝑏
o Area ∫π‘Ž [𝑔(π‘₯) − 𝑓(π‘₯)]𝑑π‘₯
Formulas and Identities(Provided/Learnt)
sin θ
1
1
1
sec πœƒ =
csc πœƒ =
cot πœƒ =
cos θ
cos πœƒ
sin πœƒ
tan πœƒ
2
2
2
2
2
sin πœƒ + cos πœƒ = 1
1 + tan πœƒ = sec πœƒ
1 + cot πœƒ = csc 2 πœƒ
sin(π‘Ž ± 𝑏) = sin π‘Ž cos 𝑏 ± cos π‘Ž sin 𝑏
cos(π‘Ž ± 𝑏) = cos π‘Ž cos 𝑏 βˆ“ sin π‘Ž sin 𝑏
tan θ =
tan(π‘Ž ± 𝑏) =
tan π‘Ž ± cos 𝑏
1 βˆ“ tan π‘Ž tan 𝑏
sin π‘₯ cos 𝑦 =
sin(π‘₯ − 𝑦) + sin(π‘₯ + 𝑦)
2
cos π‘₯ cos 𝑦 =
cos(π‘₯ − 𝑦) + cos(π‘₯ + 𝑦)
cos(2π‘₯) = 2 cos 2 π‘₯ − 1 = 1 − 2 sin2 π‘₯
2
sin π‘₯ sin 𝑦 =
cos(π‘₯ − 𝑦) − cos(π‘₯ + 𝑦)
2
sin(2π‘₯) = 2 sin π‘₯ cos π‘₯
1
1
sin 𝛼 ± sin 𝛽 = 2 sin (𝛼 ± 𝛽) cos (𝛼 βˆ“ 𝛽)
2
2
1
1
cos 𝛼 + cos 𝛽 = 2 cos (𝛼 + 𝛽) cos (𝛼 − 𝛽)
2
2
1
1
cos 𝛼 − cos 𝛽 = −2 sin (𝛼 + 𝛽) sin (𝛼 − 𝛽)
2
2
1 n
lim (1 + ) = e
n→∞
n
𝑓(x)
c
x
r
1
lim (1 + 𝑛)𝑛 = 𝑒
𝑛→0
𝑓 ′ (x)
0
rx r−1
ax
ax ln π‘Ž
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‘Ž
−1
sin (π‘Žπ‘₯)
cos−1 (π‘Žπ‘₯)
tan−1(π‘Žπ‘₯)
√1 − (π‘Žπ‘₯)2
π‘Ž
−
√1 − (π‘Žπ‘₯)2
π‘Ž
1 + (π‘Žπ‘₯)2
𝑓(x)
∫ 𝑓(x)𝑑π‘₯
1
π‘₯
ln|π‘₯|
π‘Žπ‘₯
(π‘Ž > 0 π‘Žπ‘›π‘‘ π‘Ž ≠ 1)
π‘Žπ‘₯
ln π‘Ž
π‘₯π‘Ÿ
sin π‘₯
π‘₯ π‘Ÿ+1
π‘Ÿ+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 −
(π‘Žπ‘₯)2
1
1 + (π‘Žπ‘₯)2
1 −1
sin (π‘Žπ‘₯)
π‘Ž
1
tan−1(π‘Žπ‘₯)
π‘Ž
∫ ln π‘₯ 𝑑π‘₯
∫ tan2 π‘₯ 𝑑π‘₯
1
= ln(π‘₯) π‘₯ − ∫ π‘₯ ( ) 𝑑π‘₯
π‘₯
= ∫ sec 2 π‘₯ + 1 𝑑π‘₯
= π‘₯ ln(π‘₯) − ∫ 𝑑π‘₯
= π‘₯ ln(π‘₯) − π‘₯ + 𝐢
sin π‘₯
𝑑π‘₯
cos π‘₯
= −∫
1
𝑑 cos π‘₯
cos π‘₯
= − ln|cos π‘₯| + 𝐢
= ln|sec π‘₯| + 𝐢
∫ sec π‘₯ 𝑑π‘₯
= ∫ sec π‘₯ ×
∫ sec 2 π‘₯ 𝑑π‘₯
= π‘‘π‘Žπ‘› π‘₯ + 𝐢
∫ tan π‘₯ 𝑑π‘₯
=∫
= tan π‘₯ + π‘₯ + 𝐢
sec π‘₯ + tan π‘₯
𝑑π‘₯
sec π‘₯ + tan π‘₯
(sec 2 π‘₯ + sec π‘₯ tan π‘₯)
𝑑π‘₯
sec π‘₯ + tan π‘₯
1
=∫
𝑑(sec π‘₯ + tan π‘₯)
sec π‘₯ + tan π‘₯
∫ sin−1 π‘₯ 𝑑π‘₯
= ∫ 1 × sin−1 π‘₯ 𝑑π‘₯
= π‘₯ sin−1 π‘₯ − ∫ π‘₯ ×
1
𝑑π‘₯
√1 − π‘₯ 2
1
1
= π‘₯ sin−1 π‘₯ − ∫
𝑑(1 − π‘₯ 2 )
2 √1 − π‘₯ 2
1
1
= π‘₯ sin−1 π‘₯ − × 2 × (1 − π‘₯ 2 )2 + 𝐢
2
= π‘₯ sin−1 π‘₯ − √1 − π‘₯ 2 + 𝐢
=∫
= ln|sec π‘₯ + tan π‘₯| + 𝐢
∫ tan−1 π‘₯ 𝑑π‘₯
= ∫ 1 × tan−1 π‘₯ 𝑑π‘₯
= π‘₯ tan−1 π‘₯ − ∫ π‘₯ ×
∫ sin2 π‘₯ 𝑑π‘₯
1 cos 2π‘₯
=∫ −
dx
2
2
=
x 1
− ∫ cos 2π‘₯ 𝑑π‘₯
2 2
=
x 1 1
− × ∫ cos 2π‘₯ 𝑑2π‘₯
2 2 2
=
x sin 2π‘₯
−
+C
2
4
1
𝑑π‘₯
1 + π‘₯2
1
1
= π‘₯ tan−1 π‘₯ − ∫
𝑑(1 + π‘₯ 2 )
2 1 + π‘₯2
1
= π‘₯ tan−1 π‘₯ − ln(1 + π‘₯ 2 ) + 𝐢
2
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