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[Analysis] Various fixes and optimizations
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@@ -16,11 +16,18 @@ The homogeneous equation will then be all the elements of the set summed up.\\
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\shade{gray}{Inhomogeneous Equation}\rmvspace
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\begin{enumerate}[noitemsep]
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\item \bi{(Case 1)} $b(x) = c x^d e^{\alpha x}$, with special cases $x^d$ and $e^{\alpha x}$:
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$f_p = Q(x) e^{\alpha x}$ with $Q$ a polynomial with $\deg(Q) \leq j + d$, where $j$ is multiplicity of root $\alpha$ (if $P(\alpha) \neq 0$, then $j = 0$) of characteristic polynomial
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$f_p = Q(x) e^{\alpha x}$ with $Q$ a polynomial with $\deg(Q) \leq j + d$,
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where $j$ is multiplicity of root $\alpha$ (if $P(\alpha) \neq 0$, then $j = 0$) of characteristic polynomial
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\item \bi{(Case 2)} $b(x) = c x^d \cos(\alpha x)$, or $b(x) = c x^d \sin(\alpha x)$:
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$f_p = Q_1(x) \cdot \cos(\alpha x) + Q_2(x9 \cdot \sin(\alpha x))$,
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where $Q_i(x)$ a polynomial with $\deg(Q_i) \leq d + j$, where $j$ is the multiplicity of root $\alpha i$ (if $P(\alpha i) \neq 0$, then $j = 0$) of characteristic polynomial
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$f_p = Q_1(x) \cdot \cos(\alpha x) + Q_2(x) \cdot \sin(\alpha x))$,
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where $Q_i(x)$ a polynomial with $\deg(Q_i) \leq d + j$,
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where $j$ is the multiplicity of root $\alpha i$ (if $P(\alpha i) \neq 0$, then $j = 0$) of characteristic polynomial
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\item \bi{(Case 3)} $b(x) = c e^{\alpha x} \cos(\beta x)$, or $b(x) = c e^{\alpha x} \sin(\beta x)$, use the Ansatz
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$Q_1(x) e^{\alpha x} \sin(\beta x) + Q_2(x) e^{\alpha x} \cos(\beta x)$, agasin with the same polynomial.
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Often, it is sufficent to have a polynomial of degree 0 (i.e. constant)
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\end{enumerate}
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For inhomogeneous parts with addition or subtraction, the above cases can be combined.
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For any cases not covered, start with the same form as the inhomogeneous part has (for trigonometric functions, duplicate it with both $\sin$ and $\cos$).
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\rmvspace\shade{gray}{Other methods}\rmvspace
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\begin{itemize}[noitemsep]
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@@ -16,9 +16,10 @@
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We usually call $f : X \rightarrow \R^n$ (or sometimes $V$ a \bi{vector field}, which maps each point $x \in X$ to a vector in $\R^n$, displayed as originating from $x$.
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Ideally, to compute a line integral, we compute the derivative of $\gamma$ separately ($\gamma(t) = s$ usually, derive component-wise),
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limits of integration are start and end of section.
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\hl{Be careful with hat functions} like $|x|$, we need two separate integrals for each side of the center!
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\hl{Be careful with hat functions} like $|x|$, we need two separate integrals for each side of the center!\\
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Alternatively, see section \ref{sec:green-formula} for a faster way.
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For calculating the area enclosed by the curve, see there too.
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\bi{For computing}, we usually use the first integral in def \ref{all:4-1-1} (3).
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\setLabelNumber{all}{4}
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\compactdef{Oriented reparametrization} of $\gamma$ is parametrized curve $\sigma : [c, d] \rightarrow \R^n$ s.t $\sigma = \gamma \circ \varphi$, with $\varphi : [c, d] \rightarrow I$ cont. map,
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@@ -61,3 +61,7 @@ The center of mass of an object $\cU$ is given by $\displaystyle \overline{x}_i
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\rmvspace
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\shade{gray}{Dot product} For vectors $v, w \in \R^n$, we have $\displaystyle v \cdot w = \sum_{i = 1}^{n} v_i \cdot w_i$
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\rmvspace
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\shade{gray}{Matrix-Vector product} Given vector $v\in \R^m$ and matrix $A \in \R^{n \times m}$,
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we have $A \cdot v = u$ where $ \displaystyle u_j = \sum_{i = 1}^{m} v_i \cdot A_{j, i}$.
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