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@ -83,7 +83,7 @@ Clearly the $\sin(x)$ inside the exponential is an issue. If we let $u(x) = \sin
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$$
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\int_0^2 u\prime(x) e^{u(x)} dx =
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\int_0^{\pi/2} u\prime(x) e^{u(x)} dx =
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\int_{u(0)}^{u(\pi/2)} e^x dx = e^x \big|_{\sin(0)}^{\sin(\pi/2)} = e^1 - e^0.
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$$
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@ -100,7 +100,7 @@ In the above problem, $\int_0^{\pi/2} \cos(x) e^{\sin(x)} dx$, we might just ren
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$$
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\int_0^{\pi/2} \cos(x) e^{\sin(x)} dx = \int_0^{\pi/2} e^{\sin(x)} \cdot \cos(x) dx = \int_{u(0)}^{u(\pi)} e^u du.
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\int_0^{\pi/2} \cos(x) e^{\sin(x)} dx = \int_0^{\pi/2} e^{\sin(x)} \cdot \cos(x) dx = \int_{u(0)}^{u(\pi/2)} e^u du.
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$$
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---
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@ -131,14 +131,14 @@ $$
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---
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Consider $\int_0^{\pi} \cos(x)^3 \sin(x) dx$. The $\cos(x)$ function inside the $x^3$ function is complicated. We let $u(x) = \cos(x)$ and see what that implies: $du = \sin(x) dx$, which we see is part of the question. So the above becomes:
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Consider $\int_0^{\pi} \cos(x)^3 \sin(x) dx$. The $\cos(x)$ function inside the $x^3$ function is complicated. We let $u(x) = \cos(x)$ and see what that implies: $du = -\sin(x) dx$, which we see is part of the question. So the above becomes:
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$$
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\int_0^{\pi} \cos(x)^3 \sin(x) dx = \int_{u(0)}^{u(\pi)} u^3 du= \frac{u^4}{4}\big|_0^0 = 0.
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\int_0^{\pi} \cos(x)^3 \sin(x) dx = \int_{u(0)}^{u(\pi)} -u^3 du= -\frac{u^4}{4}\big|_1^{-1} = 0.
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$$
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Changing limits leaves the two endpoints the same, which means the total area after substitution is $0$. A graph of this function shows that about $\pi/2$ the function has odd-like symmetry, so the answer of $0$ is supported by the plot:
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Changing limits leaves the two antiderivative values of endpoints the same, which means the total area after substitution is $0$. A graph of this function shows that about $\pi/2$ the function has odd-like symmetry, so the answer of $0$ is supported by the plot:
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```{julia}
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@ -177,20 +177,20 @@ For example, consider the "hat" function $f(x) = 1 - \lvert x \rvert$
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when $-1 \leq x \leq 1$ and $0$ otherwise. The area under $f$ is just $1$ - the graph forms a triangle with base of length $2$ and height $1$. If we take any values of $c$ and $h$, what do we find for the area under the curve of the transformed function?
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Let $u(x) = (x-c)/h$ and $g(x) = h f(u(x))$. Then, as $du = 1/h dx$
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Let $u(x) = (x-c)/h$ and $g(x) = (1/h) \cdot f(u(x))$. Then, as $du = 1/h dx$
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\begin{align*}
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\int_{c-h}^{c+h} g(x) dx
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&= \int_{c-h}^{c+h} h f(u(x)) dx\\
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&= \int_{c-h}^{c+h} \frac{1}{h} f(u(x)) dx\\
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&= \int_{u(c-h)}^{u(c+h)} f(u) du\\
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&= \int_{-1}^1 f(u) du\\
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&= 1.
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\end{align*}
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So the area of this transformed function is still $1$. The shifting by $c$ we know doesn't effect the area, the scaling by $h$ inside of $f$ does, but is balanced out by the multiplication by $h$ outside of $f$.
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So the area of this transformed function is still $1$. The shifting by $c$ we know doesn't effect the area, the scaling by $h$ inside of $f$ does, but is balanced out by the multiplication by $1/h$ outside of $f$.
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##### Example: Speed versus velocity
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@ -203,7 +203,7 @@ As mentioned previously, position is the integral of velocity, as expressed prec
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$$
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x(t) = \int_0^t v(u) du - x(0).
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x(t) = \int_0^t v(u) du + x(0).
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$$
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What is the integral of speed?
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@ -244,7 +244,7 @@ $$
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\int_{-2}^1 \lvert u^3/3 - 4u/3 \rvert du.
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$$
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But $u^3/3 - 4u/3 = (1/3) \cdot u(u-1)(u+2)$, so between $-2$ and $0$ it is positive and between $0$ and $1$ negative, so this integral is:
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But $u^3/3 - 4u/3 = (1/3) \cdot u(u-2)(u+2)$, so between $-2$ and $0$ it is positive and between $0$ and $1$ negative, so this integral is:
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@ -353,7 +353,7 @@ f(x) = 1/(x*log(x))
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integrate(f(x), (x, sympy.E, sympy.E^2))
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```
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(We used `sympy.E)` - and not `e` - to avoid any conversion to floating point, which could yield an inexact answer.)
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(We used `sympy.E` - and not `e` - to avoid any conversion to floating point, which could yield an inexact answer.)
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The antiderivative is interesting here; it being an *iterated* logarithm.
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@ -455,7 +455,7 @@ Let's see some examples where a trigonometric substitution is all that is needed
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Consider $\int 1/(1+x^2) dx$. This is an antiderivative of some function, but if that isn't observed, we might notice the $1+x^2$ and try to simplify that. First, an attempt at a $u$-substitution:
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Letting $u = 1+x^2$ we get $du = 2xdx$ which gives $\int (1/u) (2x) du$. We aren't able to address the "$2x$" part successfully, so this attempt is for naught.
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Letting $u = 1+x^2$ we get $du = 2xdx$ which gives $\int (1/u) (1/2x) du$. We aren't able to address the "$2x$" part successfully, so this attempt is for naught.
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Now we try a trigonometric substitution, taking advantage of the identity $1+\tan(x)^2 = \sec(x)^2$. Letting $\tan(u) = x$ yields $\sec(u)^2 du = dx$ and we get:
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@ -484,7 +484,7 @@ integrate(1 / (a^2 + (b*x)^2), x)
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##### Example
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The expression $1-x^2$ can be attacked by the substitution $\sin(u) =x$ as then $1-x^2 = 1-\cos(u)^2 = \sin(u)^2$. Here we see this substitution being used successfully:
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The expression $1-x^2$ can be attacked by the substitution $\sin(u) =x$ as then $1-x^2 = 1-\sin(u)^2 = \cos(u)^2$. Here we see this substitution being used successfully:
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@ -558,7 +558,7 @@ Letting $\sin(u) = x/a$ gives $a\cos(u)du = dx$ and an antiderivative is found w
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$$
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4 b \int_0^a \sqrt{1 - x^2/a^2} dx = 4b \int_0^{\pi/2} \sqrt{1-u^2} a \cos(u) du
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4 b \int_0^a \sqrt{1 - x^2/a^2} dx = 4b \int_0^{\pi/2} \sqrt{1-\sin(u)^2} a \cos(u) du
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= 4ab \int_0^{\pi/2} \cos(u)^2 du
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$$
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@ -601,7 +601,7 @@ radioq(choices, answ)
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###### Question
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For $\int \tan(x)^4 \sec(x)2 dx$ what $u$-substitution makes this easy?
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For $\int \tan(x)^4 \sec(x)^2 dx$ what $u$-substitution makes this easy?
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```{julia}
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@ -715,7 +715,7 @@ choices = [
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"``a=0,~ b=0``",
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"``a=1,~ b=1``"
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]
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answ = 1
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answ = 2
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radioq(choices, answ)
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```
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@ -804,7 +804,7 @@ The integral $\int dx / (a^2 + x^2)$ lends itself to what substitution?
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#| hold: true
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#| echo: false
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choices = [
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"``\\tan(u) = x``",
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"``a\\tan(u) = x``",
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"``\\tan(u) = x``",
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"``a\\sec(u) = x``",
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"``\\sec(u) = x``"]
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Loading…
Reference in New Issue
Block a user