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Add sixth semester Ecuaciones Diferenciales II notes
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--- | ||
type: 🏫 | ||
tags: | ||
- MAC/6/ED2 | ||
--- | ||
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# Integral Transforms | ||
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An [[Integral Transform|integral transform]] is an operator that takes a set, a function to be operated and another _specific_ function (called the integral kernel), returning one more function that's obtained through integration. It's basically just integrating the product of a function by the integral kernel over a given set. | ||
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## Laplace Transform | ||
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The [[Laplace Transform|Laplace transform]] is an integral transform whose integral kernel is $e^{-st}$ and integration interval is $[0, \infty)$. | ||
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We can obtain the [[Laplace Transform of Simple Functions|Laplace transform of varios simple functions]] to facilitate other more complex transforms. Similarly, there are several [[Fundamental Theorems of the Laplace Transform|fundamental theorems]] that we can also use to our convenience. We can use one of them to easily obtain the Laplace transform of a piecewise function after having it [[Expressing a Piecewise Function with Shifted Unit Step Functions|rewritten in terms of shifted unit step functions]]. | ||
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We can guarantee the existence of a Laplace transform by [[Laplace Transform Conditions of Existence|means of the consequences of two theorems]]. | ||
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Mathematics/Expressing a Piecewise Function with Shifted Unit Step Functions.md
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--- | ||
date: 2024-02-13 | ||
type: 🧠 | ||
tags: | ||
- MAC/6/ED2 | ||
--- | ||
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**Topics:** [[Piecewise Function]] | ||
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--- | ||
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_**(theorem)**_ | ||
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Let $f(t)$ be a [[Piecewise Function|piecewise function]] of the following form: | ||
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$$ | ||
f(t) = | ||
\begin{cases} | ||
g(t) & \text{if } 0 \leq t < a \\ | ||
h(t) & \text{if } a \leq t < b \\ | ||
k(t) & \text{if } b \leq t | ||
\end{cases} | ||
$$ | ||
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We can write such a function as follows, by using the [[Shifted Unit Step Function|shifted unit step function]] $U$: | ||
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$$ | ||
\begin{align*} | ||
f(t) &= g(t) - g(t) U(t-a) + h(t) U(t-a) - h(t) U(t-b) + k(t) U(t-b) \\[0.5em] | ||
&= g(t) + [h(t) - g(t)] U(t-a) + [k(t) - h(t)] U(t-b) | ||
\end{align*} | ||
$$ |
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Mathematics/Fundamental Theorems of the Laplace Transform.md
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--- | ||
date: 2024-02-13 | ||
type: 🧠 | ||
tags: | ||
- MAC/6/ED2 | ||
--- | ||
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**Topics:** [[Laplace Transform]] | ||
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--- | ||
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_**(theorems)**_ | ||
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There are several theorems that prove to be fundamental when working with [[Laplace Transform|Laplace transforms]]: | ||
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$$ | ||
\begin{align*} | ||
\mathcal{L}\{f(at)\} &= \frac{1}{a} F \left( \frac{s}{a} \right) & \quad \text{(t. 9)} \\[1em] | ||
\mathcal{L}\{f^{n}(t)\} &= s^{n} F(s) - s^{n-1} f(0) - \dots - f^{n-1} (0) & \quad \text{(t. 10)} \\[1em] | ||
\mathcal{L}\{e^{at}f(t)\} &= F(s-a) & \quad \text{(t. 11)} \\[1em] | ||
\mathcal{L}\{f(t-a)U(t-a)\} &= e^{-as} F(s) & \quad \text{(t. 12)} \\[1em] | ||
\mathcal{L}\{t^{n}f(t)\} &= (-1)^{n} \frac{d^{n} F(s)}{ds^{n}}& \quad \text{(t. 13)} \\[1em] | ||
\mathcal{L}\{f(t)g(t)\} &= F(s) G(s) & \quad \text{(t. 14)} \\[1em] | ||
\end{align*} | ||
$$ | ||
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…where $U(t-a)$ is the [[Shifted Unit Step Function|shifted unit step function]]: | ||
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$$ | ||
U(t-a) = | ||
\begin{cases} | ||
0 & \text{if } 0 \leq t \leq a \\ | ||
1 & \text{if } t > a | ||
\end{cases} | ||
$$ | ||
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> [!info]- Theorem Numbering | ||
> The theorems are numbered according to my [[Ecuaciones Diferenciales II]] course. |
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--- | ||
date: 2024-02-01 | ||
type: 🧠 | ||
tags: | ||
- MAC/6D | ||
--- | ||
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**Topics:** [[Integral Transform]] | ||
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--- | ||
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An **integral transform** is an [[Operator|operator]] that is derived from other [[Function|functions]] though a [[Definite Integral|definite integral]]. They allow us to switch from a reference system to another, with the advantage of being able to go back to the original system (this ability being the inverse transform). | ||
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Instances of integral transforms include the [[Laplace Transform|Laplace transform]]. | ||
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_**(definition)**_ | ||
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Formally, an **integral transform** is an operator that associates a new function to a given [[Set|set]] through integration with respect to a given parameter: | ||
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$$ | ||
T\{f(t)\} = F(s) = \int_{a}^{b} K(t,s) f(t) \ dt | ||
$$ | ||
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…where: | ||
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- $K(t,s)$ is the _integral kernel_ of the transform | ||
- $(a,b)$ is the interval that is commonly infinite | ||
- $F(s)$ is the _transform_ of the function $f$ | ||
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Do note that integral transforms are [[Linear Transformation|linear transformations]]. |
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--- | ||
date: 2024-02-19 | ||
type: 🧠 | ||
tags: | ||
- MAC/6/ED2 | ||
--- | ||
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**Topics:** [[Laplace Transform]] | ||
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--- | ||
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Concerning [[Laplace Transform|Laplace transforms]], we can guarantee their existence by means of the consequences of the following theorems. | ||
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_**(theorem, 8)**_ | ||
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Note that, as $t$ increases, the growth of the [[Complex Number Module|module]] of the function $f(t)$ is not greater than that of an [[Exponential Function|exponential function]]. That is, there exists $M > 0$ and $s_{0} \geq 0$ such that, for every value of $t$: | ||
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$$ | ||
\left| f(t) \right| < Me^{s_{0}t} | ||
$$ | ||
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We call $s_{0}$ the _growth exponent_ of the function $f(t)$. This condition guarantees the existence of the Laplace transform. | ||
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_**(theorem)**_ | ||
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If $f(t)$ is [[Piecewise Continuous|piecewise continuous]] in every finite set $0 < t < M$ of exponential order $s_{0}$ for $t > M$, then the Laplace transform $F(s)$ exists as long as $s_0 > 0$. |
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--- | ||
date: 2024-02-06 | ||
type: 🧠 | ||
tags: | ||
- MAC/6/ED2 | ||
--- | ||
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**Topics:** [[Laplace Transform]] | ||
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--- | ||
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_**(theorems)**_ | ||
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The [[Laplace Transform|Laplace transform]] of simple functions like $f(t) = c, f(t) = t$, etc. is as follows: | ||
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$$ | ||
\begin{align*} | ||
\mathcal{L}\{c\} &= \frac{c}{s} & s>0 & \qquad \text{(theorem 1)} \\[1em] | ||
\mathcal{L}\{t^n\} &= \frac{n!}{s^{n+1}} & s>0 & \qquad \text{(theorem 2)} \\[1em] | ||
\mathcal{L}\{\sin(at)\} &= \frac{a}{s^{2} + a^{2}} & s>0 & \qquad \text{(theorem 3)} \\[1em] | ||
\mathcal{L}\{\cos(at)\} &= \frac{s}{s^{2} + a^{2}} & s>0 & \qquad \text{(theorem 4)} \\[1em] | ||
\mathcal{L}\{e^{at}\} &= \frac{1}{s-a} & s>0 & \qquad \text{(theorem 5)} \\[1em] | ||
\mathcal{L}\{\sinh(at)\} &= \frac{a}{s^{2}-a^{2}} & s>0 & \qquad \text{(theorem 6)} \\[1em] | ||
\mathcal{L}\{\cosh(at)\} &= \frac{s}{s^{2}-a^{2}} & s>0 & \qquad \text{(theorem 7)} | ||
\end{align*} | ||
$$ | ||
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> [!info]- Theorem Numbering | ||
> The theorems are numbered according to my [[Ecuaciones Diferenciales II]] course. |
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Mathematics/Sample Statistic.sync-conflict-20240214-080921-LPBDAHD.md
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--- | ||
date: 2024-02-19 | ||
type: 🧠 | ||
tags: | ||
- MAC/6/ED2 | ||
--- | ||
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**Topics:** [[Unit Step Function]] | ||
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--- | ||
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_**(definition)**_ | ||
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The **shifted [[Unit Step Function|unit step function]]** is defined as: | ||
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$$ | ||
U(t-a) = | ||
\begin{cases} | ||
0 & \text{if } t \leq a \\ | ||
1 & \text{if } t > a | ||
\end{cases} | ||
$$ | ||
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As the name suggests, it's just a unit step function that has been shifted from $0$ to $a$. |
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--- | ||
date: 2024-02-19 | ||
type: 🧠 | ||
tags: | ||
- MAC/6/ED2 | ||
--- | ||
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**Topics:** [[Function]] | ||
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--- | ||
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_**(definition)**_ | ||
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The **unit step function** is defined as: | ||
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$$ | ||
u(t) = | ||
\begin{cases} | ||
0 & \text{if } t \leq 0 \\ | ||
1 & \text{if } t > 0 | ||
\end{cases} | ||
$$ | ||
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In other words, the unit step function is a [[Function|function]] that returns $0$ when its argument is non-positive, and $1$ when it is positive. Sometimes $<, \geq$ are used instead of $\leq, >$. | ||
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We can [[Shifted Unit Step Function|shift this function]] so that it's centred around a number other than $0$. |