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Integration

1.4 Substitution

25 problems · hints, answers and solutions shown beside each one

Recall that we are using log⁡x\log x to denote the logarithm of xx with base ee. In other courses it is often denoted ln⁡x\ln x.

1Stage 1Conceptual

Do you understand the idea? Usually little or no calculation.

Q1Stage 1
  1. True or False: ∫sin⁡(ex)⋅ex dx=∫sin⁡(u) du∣u=ex=−cos⁡(ex)+C\displaystyle\int \sin(e^x)\cdot e^x\ \dee{x} = \left.\displaystyle\int \sin(u)\ \dee u\right|_{u=e^x} = -\cos(e^x)+C

  2. True or False: ∫01sin⁡(ex)⋅ex dx=∫01sin⁡(u) du=1−cos⁡(1)\displaystyle\int_0^1 \sin(e^x)\cdot e^x\ \dee{x} = \displaystyle\int_0^1 \sin(u)\ \dee u = 1-\cos(1)

Hint

One is true, the other false.

Answer

(a) true (b) false

Full solution

(a) This is true: it is an application of Theorem ? in the CLP-2 text with f(x)=sin⁡xf(x)=\sin x and u(x)=exu(x)=e^x.

(b) This is false: the upper limit of integration is incorrect. Using Theorem 1.4.6 in the CLP-2 text, the correct form is

∫01sin⁡(ex)⋅ex dx=∫1esin⁡(u) du=−cos⁡(e)+cos⁡(1)=cos⁡(1)−cos⁡(e).\displaystyle\int_0^1 \sin(e^x)\cdot e^x\ \dee{x} = \displaystyle\int_1^{e} \sin(u)\ \dee u = -\cos(e) + \cos(1) = \cos(1)-\cos(e).

Alternately, we can use the Fundamental Theorem of Calculus Part 2, and our answer from (a):

∫01sin⁡(ex)⋅ex dx=[−cos⁡(ex)+C]01=cos⁡(1)−cos⁡(e) .\int_0^1 \sin(e^x)\cdot e^x\ \dee{x}=\left[-\cos(e^x)+C\right]_{0}^1 = \cos(1)-\cos(e)\ .
Q2Stage 1

Is the following reasoning sound? If not, fix it.

Problem: Evaluate ∫(2x+1)2dx\displaystyle\int (2x+1)^2 \dee{x}.

Work: We use the substitution u=2x+1u=2x+1. Then:

∫(2x+1)2dx=∫u2 du=13u3+C=13(2x+1)3+C\begin{align*} \int (2x+1)^2 \dee{x}&=\int u^2\ \dee{u}\\ &=\frac{1}{3}u^3+C\\ &=\frac{1}{3}\left(2x+1\right)^3+C \end{align*}
Hint

You can check whether the final answer is correct by differentiating.

Answer

The reasoning is not sound: when we do a substitution, we need to take care of the differential (dx\dee{x}). Remember the method of substitution comes from the chain rule: there should be a function and its derivative. Here's the way to do it:

Problem: Evaluate ∫(2x+1)2dx\displaystyle\int (2x+1)^2 \dee{x}.

Work: We use the substitution u=2x+1u=2x+1. Then du=2dx\dee{u}=2\dee{x}, so dx=12du\dee{x} = \frac{1}{2}\dee{u}:

∫(2x+1)2dx=∫u2⋅12 du=16u3+C=16(2x+1)3+C\begin{align*} \int (2x+1)^2 \dee{x}&=\int u^2\cdot \frac{1}{2}\ \dee{u}\\ &=\frac{1}{6}u^3+C\\ &=\frac{1}{6}\left(2x+1\right)^3+C \end{align*}
Full solution

The reasoning is not sound: when we do a substitution, we need to take care of the differential (dx\dee{x}). Remember the method of substitution comes from the chain rule: there should be a function and its derivative. Here's the way to do it:

Problem: Evaluate ∫(2x+1)2dx\displaystyle\int (2x+1)^2 \dee{x}.

Work: We use the substitution u=2x+1u=2x+1. Then du=2dx\dee{u}=2\dee{x}, so dx=12du\dee{x} = \frac{1}{2}\dee{u}:

∫(2x+1)2dx=∫u2⋅12 du=16u3+C=16(2x+1)3+C\begin{align*} \int (2x+1)^2 \dee{x}&=\int u^2\cdot \frac{1}{2}\ \dee{u}\\ &=\frac{1}{6}u^3+C\\ &=\frac{1}{6}\left(2x+1\right)^3+C \end{align*}
Q3Stage 1

Is the following reasoning sound? If not, fix it.

Problem: Evaluate ∫1πcos⁡(log⁡t)tdt\displaystyle\int_{1}^{\pi} \dfrac{\cos(\log t)}{t}\dee{t}.

Work: We use the substitution u=log⁡tu=\log t, so du=1tdt\dee{u}=\frac{1}{t}\dee{t}. Then:

∫1πcos⁡(log⁡t)tdt=∫1πcos⁡(u)du=sin⁡(π)−sin⁡(1)=−sin⁡(1) .\begin{align*} \int_{1}^{\pi} \dfrac{\cos(\log t)}{t}\dee{t}&=\int_1^{\pi}\cos(u) \dee{u}\\ &=\sin(\pi)-\sin(1)=-\sin(1)\, . \end{align*}
Hint

Check the limits.

Answer

The problem is with the limits of integration, as in Question 1. Here's how it ought to go:

Problem: Evaluate ∫1πcos⁡(log⁡t)tdt\displaystyle\int_{1}^{\pi} \dfrac{\cos(\log t)}{t}\dee{t}.

Work: We use the substitution u=log⁡tu=\log t, so du=1tdt\dee{u}=\frac{1}{t}\dee{t}. When t=1t=1, we have u=log⁡1=0u=\log 1 =0 and when t=πt=\pi, we have u=log⁡(π)u=\log(\pi). Then:

∫1πcos⁡(log⁡t)tdt=∫log⁡1log⁡(π)cos⁡(u)du=∫0log⁡(π)cos⁡(u)du=sin⁡(log⁡(π))−sin⁡(0)=sin⁡(log⁡(π)).\begin{align*} \int_{1}^{\pi} \dfrac{\cos(\log t)}{t}\dee{t}&=\int_{\log 1}^{\log(\pi)}\cos(u) \dee{u}\\ &=\int_{0}^{\log(\pi)}\cos(u) \dee{u}\\ &=\sin(\log(\pi))-\sin(0)=\sin(\log(\pi)) . \end{align*}
Full solution

The problem is with the limits of integration, as in Question 1. Here's how it ought to go:

Problem: Evaluate ∫1πcos⁡(log⁡t)tdt\displaystyle\int_{1}^{\pi} \dfrac{\cos(\log t)}{t}\dee{t}.

Work: We use the substitution u=log⁡tu=\log t, so du=1tdt\dee{u}=\frac{1}{t}\dee{t}. When t=1t=1, we have u=log⁡1=0u=\log 1 =0 and when t=πt=\pi, we have u=log⁡(π)u=\log(\pi). Then:

∫1πcos⁡(log⁡t)tdt=∫log⁡1log⁡(π)cos⁡(u)du=∫0log⁡(π)cos⁡(u)du=sin⁡(log⁡(π))−sin⁡(0)=sin⁡(log⁡(π)).\begin{align*} \int_{1}^{\pi} \dfrac{\cos(\log t)}{t}\dee{t}&=\int_{\log 1}^{\log(\pi)}\cos(u) \dee{u}\\ &=\int_{0}^{\log(\pi)}\cos(u) \dee{u}\\ &=\sin(\log(\pi))-\sin(0)=\sin(\log(\pi)) . \end{align*}
Q4Stage 1

Is the following reasoning sound? If not, fix it.

Problem: Evaluate ∫0π/4xtan⁡(x2) dx\displaystyle\int_{0}^{\pi/4} x\tan (x^2) \ \dee{x}.

Work: We begin with the substitution u=x2u=x^2, du=2xdx\dee{u} = 2x\dee{x}:

∫0π/4xtan⁡(x2) dx=∫0π/412tan⁡(x2)⋅2xdx=∫0π2/1612tan⁡u du=12∫0π2/16sin⁡ucos⁡udu\begin{align*}\int_{0}^{\pi/4} x\tan (x^2) \ \dee{x}&= \int_{0}^{\pi/4} \frac{1}{2}\tan(x^2)\cdot 2x\dee{x}\\ &=\int_{0}^{\pi^2/16} \frac{1}{2}\tan u\ \dee{u}\\ &=\frac{1}{2}\int_{0}^{\pi^2/16} \dfrac{\sin u}{\cos u}\dee{u}\end{align*}

Now we use the substitution v=cos⁡uv=\cos u, dv=−sin⁡u du\dee{v}=-\sin u \ \dee{u}:

=12∫cos⁡0cos⁡(π2/16)−1vdv=−12∫1cos⁡(π2/16)1vdv=−12[log⁡∣v∣]1cos⁡(π2/16)=−12(log⁡(cos⁡(π2/16))−log⁡(1))=−12log⁡(cos⁡(π2/16))\begin{align*}&=\frac{1}{2}\int_{\cos 0}^{\cos(\pi^2/16)} -\dfrac{1}{v}\dee{v}\\ &=-\frac{1}{2}\int_{1}^{\cos(\pi^2/16)} \dfrac{1}{v}\dee{v}\\ &=-\frac{1}{2}\left[\log|v|\right]_{1}^{\cos(\pi^2/16)}\\ &=-\frac{1}{2}\left(\log\left(\cos(\pi^2/16)\right)-\log(1)\right)\\ &=-\frac{1}{2}\log\left(\cos(\pi^2/16)\right)\end{align*}
Hint

Check every step. Do they all make sense?

Answer

This one is OK.

Full solution

Perhaps shorter ways exist, but the reasoning here is valid.

Problem: Evaluate ∫0π/4xtan⁡(x2) dx\displaystyle\int_{0}^{\pi/4} x\tan (x^2) \ \dee{x}.

Work: We begin with the substitution u=x2u=x^2, du=2xdx\dee{u} = 2x\dee{x}:
If u=x2u=x^2, then dudx=2x\diff{u}{x} = 2x, so indeed du=2xdx\dee{u}=2x\dee{x}.

∫0π/4xtan⁡(x2) dx=∫0π/412tan⁡(x2)⋅2xdxalgebra=∫0π2/1612tan⁡u du\begin{align*}\int_{0}^{\pi/4} x\tan (x^2) \ \dee{x}&= \int_{0}^{\pi/4} \frac{1}{2}\tan(x^2)\cdot 2x\dee{x}&\color{red}\text{algebra}\\ &=\int_{0}^{\pi^2/16} \frac{1}{2}\tan u\ \dee{u}\end{align*}

Every piece is changed from xx to uu: integrand, differential, limits.

=12∫0π2/16sin⁡ucos⁡udutan⁡u=sin⁡ucos⁡u\begin{align*}&=\frac{1}{2}\int_{0}^{\pi^2/16} \dfrac{\sin u}{\cos u}\dee{u} &\color{red} \tan u = \frac{\sin u}{\cos u}\end{align*}

Now we use the substitution v=cos⁡uv=\cos u, dv=−sin⁡u du\dee{v}=-\sin u \ \dee{u}:

=12∫cos⁡0cos⁡(π2/16)−1vdv\begin{align*}&=\frac{1}{2}\int_{\cos 0}^{\cos(\pi^2/16)} -\dfrac{1}{v}\dee{v}\end{align*}

Every piece is changed from uu to vv: integrand, differential, limits.

=−12∫1cos⁡(π2/16)1vdvcos⁡(0)=1=−12[log⁡∣v∣]1cos⁡(π2/16)FTC Part 2=−12(log⁡(cos⁡(π2/16))−log⁡(1))=−12log⁡(cos⁡(π2/16))log⁡(1)=0\begin{align*}&=-\frac{1}{2}\int_{1}^{\cos(\pi^2/16)} \dfrac{1}{v}\dee{v}&\color{red} \cos(0)=1\\ &=-\frac{1}{2}\bigg[\log|v|\bigg]_{1}^{\cos(\pi^2/16)}&\color{red}\text{FTC Part 2}\\ &=-\frac{1}{2}\left(\log\left(\cos(\pi^2/16)\right)-\log(1)\right)\\ &=-\frac{1}{2}\log\left(\cos(\pi^2/16)\right)&\color{red} \log(1)=0\end{align*}
Q5Stage 1Past exam · 2016A

What is the integral that results when the substitution u=sin⁡xu= \sin x is applied to the integral ∫0π/2f(sin⁡x) dx\displaystyle \int_0^{\pi/2} f(\sin x)\,\dee{x}?

Answer

∫01f(u)1−u2 du\displaystyle\int_{0}^{1} \frac{f(u)}{\sqrt{1-u^2}}\,\dee{u}. Because the denominator 1−u2\sqrt{1-u^2} vanishes when u=1u=1, this is what is known as an improper integral. Improper integrals will be discussed in § 1.12 of the CLP-2 text.

Full solution

We substitute:

u=sin⁡x,du=cos⁡x dx,cos⁡x=1−sin⁡2x=1−u2,dx=ducos⁡x=du1−u2u(0)=sin⁡0=0u(π2)=sin⁡(π2)=1\begin{align*}u&=\sin x, \\ \dee{u}&=\cos x\,\dee{x}, \\ \cos x &= \sqrt{1-\sin^2 x}=\sqrt{1-u^2},\\ \dee{x} &=\dfrac{\dee{u}}{\cos x} = \dfrac{\dee{u}}{\sqrt{1-u^2}}\\ u(0)&=\sin 0 = 0\\ u\left(\frac{\pi}{2}\right)&=\sin\left(\frac{\pi}{2}\right)=1\end{align*}

So,

∫x=0x=π/2f(sin⁡x) dx=∫u=0u=1f(u) du1−u2\begin{align*}\int_{x=0}^{x=\pi/2} f(\sin x)\,\dee{x} &= \int_{u=0}^{u=1} f(u)\,\frac{\dee{u}}{\sqrt{1-u^2}}\end{align*}

Because the denominator 1−u2\sqrt{1-u^2} vanishes when u=1u=1, this is what is known as an improper integral. Improper integrals will be discussed in § 1.12 of the CLP-2 text.

Q6Stage 1

Let ff and gg be functions that are continuous and differentiable everywhere. Simplify

∫f′(g(x))g′(x) dx−f(g(x)).\int f'(g(x))g'(x)\ \dee{x} - f(g(x)).
Hint

What is ddx{f(g(x))}\diff{}{x}\{f(g(x))\}?

Answer

some constant CC

Full solution

Using the chain rule, we see that

ddx{f(g(x))}=f′(g(x))g′(x)\diff{}{x}\{f(g(x))\}=f'(g(x))g'(x)

So, f(g(x))\textcolor{red}{f(g(x))} is an antiderivative of f′(g(x))g′(x)\textcolor{red}{f'(g(x))g'(x)}. All antiderivatives of f′(g(x))g′(x)f'(g(x))g'(x) differ by only a constant, so:

∫f′(g(x))g′(x) dx−f(g(x))=f(g(x))+C−f(g(x))=C\begin{align*} \textcolor{red}{\int f'(g(x))g'(x)\ \dee{x}} - f(g(x))&=\textcolor{red}{f(g(x))+C}-f(g(x))\\ &=C \end{align*}

That is, our expression simplifies to some constant CC.

Remark: since

∫f′(g(x))g′(x) dt−f(g(x))=C\int f'(g(x))g'(x)\ \dee{t} - f(g(x))=C

we conclude

∫f′(g(x))g′(x) dt=f(g(x))+C\int f'(g(x))g'(x)\ \dee{t} = f(g(x))+C

which is precisely how we perform substitution on integrals.

2Stage 2Procedural

Practising the skill itself, until applying it is automatic.

Q7Stage 2Past exam · 2016Q2

Use substitution to evaluate ∫01xex2cos⁡(ex2) dx\displaystyle\int_{0}^{1} x e^{x^2} \cos (e^{x^2}) \,\dee{x}.

Hint

What is the derivative of the argument of the cosine?

Answer

12(sin⁡(e)−sin⁡(1))\dfrac{1}{2}\big( \sin(e) - \sin(1) \big)

Full solution

We write u(x)=ex2\textcolor{red}{u(x) = e^{x^2}} and find du=u′(x) dx=2xex2dx\textcolor{blue}{\dee{u} = u'(x)\,\dee{x}=2x e^{x^2}\dee{x}}. Note that u(1)=e12=eu(1)=e^{1^2}=e when x=1x=1, and u(0)=e02=1u(0)=e^{0^2}=1 when x=0x=0. Therefore:

∫01xex2cos⁡(ex2) dx=12∫x=0x=1cos⁡(u(x))u′(x) dx=12∫u=1u=ecos⁡(u) du=12[sin⁡(u)]1e=12(sin⁡(e)−sin⁡(1)).\begin{align*} \int_{0}^{1} \textcolor{blue}{x e^{x^2}} \cos (\textcolor{red}{e^{x^2}}) \,\textcolor{blue}{\dee{x}} &= \textcolor{blue}{\frac{1}{2}}\int_{x=0}^{x=1} \cos (\textcolor{red}{u(x)}) \textcolor{blue}{u'(x)\,\dee{x} }\\ &=\textcolor{blue}{ \frac{1}{2}}\int_{u=1}^{u=e} \cos(\textcolor{red}u)\,\color{blue}\dee{u}\\ &= \frac{1}{2}\bigg[\sin(u) \bigg]_1^e = \frac{1}{2}\big( \sin(e) - \sin(1) \big). \end{align*}
Q8Stage 2Past exam · 2001D

Let f(t)f(t) be any function for which ∫18f(t) dt=1\displaystyle\int_1^8 f(t)\,\dee{t}=1. Calculate the integral ∫12x2f(x3) dx\displaystyle\int_1^2 x^2 f(x^3)\,\dee{x}.

Hint

What is the title of the current section?

Answer

13\dfrac{1}{3}

Full solution

Substituting y=x3\textcolor{red}{y=x^3}, dy=3x2 dx\textcolor{blue}{\dee{y}=3x^2\ \dee{x}} :

∫12x2f(x3) dx=13∫18f(y) dy=13\begin{align*} \int_1^2 \textcolor{blue}{x^2} f(\textcolor{red}{x^3})\,\textcolor{blue}{\dee{x}} =\textcolor{blue}{\frac{1}{3}}\int_1^8 f(\textcolor{red}{y})\,\textcolor{blue}{\dee{y}} =\frac{1}{3} \end{align*}
Q9Stage 2Past exam · M121 2014A

Evaluate ∫x2(x3+1)101dx\displaystyle \int \frac{x^2}{{(x^3+1)}^{101}}\dee{x}.

Hint

What is the derivative of x3+1x^3+1?

Answer

−1300(x3+1)100+C-\dfrac{1}{300{(x^3+1)}^{100}} + C

Full solution

Setting u=x3+1\textcolor{red}{u=x^3+1}, we have du=3x2 dx\textcolor{blue}{\dee{u} = 3x^2\,\dee{x}} and so

∫x2 dx(x3+1)101=∫du/3u101=13∫u−101 du=13⋅u−100−100=−13×100u100+C=−1300(x3+1)100+C\begin{align*} \int \frac{\textcolor{blue}{x^2\,\dee{x}}}{{(\textcolor{red}{x^3+1})}^{101}} &= \int \frac{\textcolor{blue}{\dee{u}/3}}{\textcolor{red}{u}^{101}}\\ &=\frac{1}{3}\int u^{-101}\ \dee{u}\\ &=\frac{1}{3}\cdot\dfrac{u^{-100}}{-100}\\ &= -\frac{1}{3\times 100 u^{100}} + C\\ &=-\frac{1}{300{(x^3+1)}^{100}} + C \end{align*}
Q10Stage 2Past exam · 2016Q2

Evaluate ∫ee4dxxlog⁡x\displaystyle \int_{e}^{e^4} \frac{\dee{x}}{x\log x}.

Hint

What is the derivative of log⁡x\log x?

Answer

log⁡4\log 4

Full solution

Setting u=log⁡x\textcolor{red}{u=\log x}, we have du=1x dx\textcolor{blue}{\dee{u} = \frac{1}{x}\,\dee{x}} and so

∫ee4dxx⋅log⁡x=∫x=ex=e41log⁡x⋅1x dx=∫u=1u=41u du,\begin{equation*} \int_{e}^{e^4} \frac{\textcolor{blue}{\dee{x}}}{\textcolor{blue}x\cdot\textcolor{red}{\log x}} = \int_{x=e}^{x=e^4} \frac1{\textcolor{red}{\log x}} \cdot \textcolor{blue}{\frac{1}{x}\,\dee{x} } = \int_{u=1}^{u=4} \frac{1}{\textcolor{red}u}\,\textcolor{blue}{ \dee{u}}, \end{equation*}

since u=log⁡(e)=1u=\log(e)=1 when x=ex=e and u=log⁡(e4)=4u=\log(e^4)=4 when x=e4x=e^4. Then, by the Fundamental Theorem of Calculus Part 2,

∫141u du=[log⁡∣u∣]14=log⁡4−log⁡1=log⁡4.\begin{equation*} \int_{1}^{4} \frac{1}{u}\, \dee{u} = \Big[\log |u| \Big]_{1}^{4} = \log 4 - \log 1 = \log 4. \end{equation*}
Q11Stage 2Past exam · 2012A

Evaluate ∫0π/2cos⁡x1+sin⁡x dx\displaystyle \int_{0}^{\pi/2} \frac{\cos x} {1+\sin x}\,\dee{x}.

Hint

What is the derivative of 1+sin⁡x1+\sin x?

Answer

log⁡2\log 2

Full solution

Setting u=1+sin⁡x\textcolor{red}{u=1+\sin x}, we have du=cos⁡x dx\textcolor{blue}{\dee{u} = \cos x~\dee{x}} and so

∫0π/2cos⁡x1+sin⁡xdx=∫x=0x=π/211+sin⁡x cos⁡x dx=∫u=1u=2duu\begin{equation*} \int_{0}^{\pi/2} \frac{\textcolor{blue}{\cos x}} {\textcolor{red}{1+\sin x}} \textcolor{blue}{\dee{x} } = \int_{x=0}^{x=\pi/2} \frac{1}{\textcolor{red}{1+\sin x}}\, \textcolor{blue}{\cos x ~\dee{x} } = \int_{u=1}^{u=2} \frac{\textcolor{blue}{\dee{u}}}{\textcolor{red}u} \end{equation*}

since u=1+sin⁡0=1u=1+\sin 0=1 when x=0x=0 and u=1+sin⁡(π/2)=2u=1+\sin(\pi/2)=2 when x=π/2x=\pi/2. Then, by the Fundamental Theorem of Calculus Part 2,

∫u=1u=2duu=[log⁡∣u∣]12=log⁡2\begin{equation*} \int_{u=1}^{u=2} \frac{\dee{u}}{u} = \Big[\log|u| \Big]_{1}^{2} = \log 2 \end{equation*}
Q12Stage 2Past exam · 2016Q2

Evaluate ∫0π/2cos⁡x⋅(1+sin⁡2x) dx\displaystyle \int_{0}^{\pi/2} \cos x \cdot (1+\sin^2 x)\,\dee{x}.

Hint

cos⁡x\cos x is the derivative of what?

Answer

43\dfrac{4}{3}

Full solution

Setting u=sin⁡x\textcolor{red}{u=\sin x}, we have du=cos⁡x dx\textcolor{blue}{\dee{u} = \cos x~\dee{x}} and so

∫0π/2cos⁡x⋅(1+sin⁡2x)dx=∫x=0x=π/2(1+sin⁡2x)⋅cos⁡x dx=∫u=0u=1(1+u2) du,\begin{equation*} \int_{0}^{\pi/2} \textcolor{blue}{\cos x} \cdot (1+\textcolor{red}{\sin}^2 \textcolor{red}x)\textcolor{blue}{\dee{x} } = \int_{x=0}^{x=\pi/2} (1+\textcolor{red}{\sin}^2 \textcolor{red}{x})\cdot \textcolor{blue}{\cos x ~\dee{x} } = \int_{u=0}^{u=1} (1+\textcolor{red}{u}^2) \,\textcolor{blue}{\dee{u}}, \end{equation*}

since u=sin⁡0=0u=\sin 0=0 when x=0x=0 and u=sin⁡(π/2)=1u=\sin(\pi/2)=1 when x=π/2x=\pi/2. Then, by the Fundamental Theorem of Calculus Part 2,

∫01(1+u2) du=[u+u33]01=(1+13)−0=43.\begin{equation*} \int_{0}^{1} (1+u^2) \,\dee{u} = \left[u+\frac{u^3}{3} \right]_{0}^{1} =\left(1+\frac{1}{3}\right) -0 = \frac{4}{3}. \end{equation*}
Q13Stage 2Past exam · 2013A

Evaluate ∫13(2x−1)ex2−x dx\displaystyle\int_1^3(2x-1)e^{x^2-x}\ \dee{x}.

Hint

What is the derivative of the exponent?

Answer

e6−1e^6-1

Full solution

Substituting t=x2−x\textcolor{red}{t=x^2-x}, dt=(2x−1) dx\textcolor{blue}{\dee{t} = (2x-1)\,\dee{x}} and noting that t=0t=0 when x=1x=1 and t=6t=6 when x=3x=3,

∫13(2x−1)ex2−xdx=∫06et dt=[et]06=e6−1\begin{align*} \int_1^3 \textcolor{blue}{(2x-1)}e^{\textcolor{red}{x^2-x}}\textcolor{blue}{ \dee{x}} &= \int_0^6 e^{\textcolor{red}t}\ \textcolor{blue}{\dee{t} } =\big[e^t\big]_0^6 =e^6-1 \end{align*}
Q14Stage 2Past exam · 2016Q2

Evaluate ∫(x2−4)x4−x2 dx{\displaystyle \int \frac{(x^2-4)x}{\sqrt{4-x^2}}\,\dee{x}}.

Hint

What is the derivative of the argument of the square root?

Answer

13(4−x2)3/2+C\dfrac{1}{3}(4-x^2)^{3/2}+C

Full solution

We use the substitution u=4−x2\textcolor{red}{u=4-x^2}, for which du=−2x dx\textcolor{blue}{\dee{u}=-2x\,\dee{x}} :

∫x2−44−x2 x dx=∫12⋅4−x24−x2(−2x) dx=12∫uu du=12∫u du=12u3/23/2+C=13(4−x2)3/2+C\begin{align*} \int \frac{x^2-4}{\sqrt{4-x^2}}\,x\,\dee{x} &=\int \frac{1}{2}\cdot\frac{\textcolor{red}{4-x^2}}{\sqrt{\textcolor{red}{4-x^2}}}\textcolor{blue}{ ({-}2x)\,\dee{x}} \\ &=\frac{1}{2} \int \frac{\textcolor{red}u}{\sqrt{\textcolor{red}u}}\,\textcolor{blue}{\dee{u} }\\ &=\frac{1}{2}\int \sqrt{u}\,\dee{u} \\ &=\frac{1}{2}\frac{u^{3/2}}{3/2}+C\\ &=\frac{1}{3}(4-x^2)^{3/2}+C \end{align*}
Q15Stage 2

Evaluate ∫elog⁡x2xlog⁡x dx\displaystyle\int \dfrac{e^{\sqrt{\log x}}}{2x\sqrt{\log x}}\ \dee{x} .

Hint

What is ddx{log⁡x}\diff{}{x}\left\{\sqrt{\log x}\right\}?

Answer

elog⁡x+Ce^{\sqrt{\log x}}+C

Full solution
  • If we let u=log⁡x\textcolor{red}{u=\sqrt{\log x}}, then du=12xlog⁡x dx\textcolor{blue}{\dee{u}=\dfrac{1}{2x\sqrt{\log x}}\ \dee{x}}, and:

    ∫elog⁡x2xlog⁡x dx=∫eu du=eu+C=elog⁡x+C\begin{align*} \int \dfrac{e^{\textcolor{red}{\sqrt{\log x}}}}{\textcolor{blue}{2x\sqrt{\log x}}}\ \textcolor{blue}{\dee{x}}&=\int e^{\textcolor{red}u}\ \textcolor{blue}{\dee{u}}=e^u+C=e^{\sqrt{\log x}}+C \end{align*}
  • In Solution 1, we made a pretty slick choice. We might have tried to work with something a little less convenient. For example, it's not unnatural to think that u=log⁡x\textcolor{red}{u=\log x}, du=1x dx\textcolor{blue}{\dee{u}=\dfrac{1}{x}\ \dee{x}} would be a good choice. In that case:

    ∫elog⁡x2xlog⁡x dx=∫eu2udu\begin{align*}\int \dfrac{e^{\sqrt{\textcolor{red}{\log x}}}}{2\textcolor{blue}{x}\sqrt{\textcolor{red}{\log x}}}\ \textcolor{blue}{\dee{x}}&= \int \frac{e^{\sqrt{\textcolor{red}u}}}{2\sqrt{\textcolor{red}u}}\textcolor{blue}{\dee{u}}\end{align*}

    Now, we should be able to see that w=u\textcolor{orange}{w=\sqrt{u}}, dw=12u du\textcolor{purple}{\dee{w} = \dfrac{1}{2\sqrt{u}}\ \dee{u}} is a good choice:

    ∫eu2u du=∫ew dw=eu+C=elog⁡x+C\begin{align*}\int\frac{e^{\textcolor{orange}{\sqrt{u}}}}{\textcolor{purple}{2\sqrt{u}}}\ \textcolor{purple}{\dee{u}} &=\int e^{\textcolor{orange}w}\ \textcolor{purple}{\dee{w}}\\ &=e^{\sqrt{u}}+C\\ &=e^{\sqrt{\log x}}+C\end{align*}

3Stage 3Application

Further than practice: several ideas at once, or an unfamiliar situation.

Q16Stage 3Past exam · 2016A

Calculate ∫−22xex2 dx\displaystyle\int_{-2}^2 xe^{x^2}\,\dee{x}.

Hint

There is a short, slightly sneaky method — guess an antiderivative — and a really short, still-more-sneaky method.

Answer

00

Full solution
  • We use the substitution u=x2\textcolor{red}{u=x^2}, for which du=2x dx\textcolor{blue}{\dee{u}=2x\,\dee{x}}, and note that u=4u=4 for both x=2x=2 and x=−2x=-2:

    ∫−22xex2 dx=∫−2212ex2 2xdx=∫4412eu du=0\begin{align*} \int_{-2}^2 xe^{x^2}\,\dee{x} =\int_{-2}^2 \frac{1}{2}e^{\textcolor{red}{x^2}}\,\textcolor{blue}{2x\dee{x}} = \int_4^4 \frac{1}{2}e^{\textcolor{red}{u}}\,\textcolor{blue}{\dee{u}} =0 \end{align*}
  • We note that ddx{ex2}=2x ex2\displaystyle\diff{}{x} \left\{e^{x^2} \right\}= 2x\, e^{x^2}, so that 12ex2\dfrac{1}{2} e^{x^2} is a antiderivative for the integrand xex2x e^{x^2}. So

    ∫−22xex2 dx=[12ex2]−22=12e4−12e4=0\begin{align*} \int_{-2}^2 xe^{x^2}\,\dee{x} = \bigg[\frac{1}{2}e^{x^2}\bigg]_{-2}^2 =\frac{1}{2}e^4-\frac{1}{2}e^4=0 \end{align*}
  • The integrand f(x)=xex2f(x) = x e^{x^2} is an odd function (meaning that f(−x)=−f(x)f(-x)=-f(x)). So by Theorem 1.2.11 in the CLP-2 text every integral of the form ∫−aaxex2 dx\int_{-a}^a x e^{x^2}\,\dee{x} is zero.

Q17Stage 3Past exam · 2000D

Calculate lim⁡n→∞∑j=1njn2sin⁡(1+j2n2)\displaystyle\lim\limits_{n\rightarrow\infty}\sum\limits_{j=1}^n \dfrac{j}{n^2}\sin\left(1+\dfrac{j^2}{n^2}\right).

Hint

Review the definition of the definite integral and in particular Definitions 1.1.9 and 1.1.11 in the

CLP-2 text.

Answer

12[cos⁡1−cos⁡2]≈0.478\dfrac{1}{2}[\cos 1-\cos 2]\approx0.478

Full solution

The given sum is of the form

lim⁡n→∞∑j=1njn2sin⁡(1+j2n2)=lim⁡n→∞∑j=1nf(xj∗)Δx\begin{align*} \lim_{n\rightarrow\infty}\sum_{j=1}^n \frac{j}{n^2}\sin\Big(1+\frac{j^2}{n^2}\Big) =\lim_{n\rightarrow\infty}\sum_{j=1}^n f(x_j^*)\De x \end{align*}

with Δx=1n\De x=\frac{1}{n}, xj∗=jnx_j^*=\frac{j}{n} and f(x)=xsin⁡(1+x2)f(x)=x\sin(1+x^2). Since x0∗=0x_0^*=0 and xn∗=1x_n^*=1, the right hand side is the definition (using the right Riemann sum) of

∫01f(x) dx=∫01xsin⁡(1+x2) dx=12∫12sin⁡(y) dywith y=1+x2, dy=2x dx=12[−cos⁡(y)]y=1y=2=12[cos⁡1−cos⁡2]\begin{align*} \int_0^1 f(x)\,\dee{x} &=\int_0^1 x\sin(1+x^2)\,\dee{x} \\ &=\frac{1}{2}\int_1^2 \sin(y)\,\dee{y}\qquad\text{with }y=1+x^2\text{, }\dee{y}=2x\,\dee{x} \\ &=\frac{1}{2}\Big[-\cos(y)\Big]_{y=1}^{y=2} \\ &=\frac{1}{2}[\cos 1-\cos 2] \end{align*}

Using a calculator, we see this is close to 0.4780.478.

Questions 18 through 22 can be solved by substitution, but it may not be obvious which substitution will work. In general, when evaluating integrals, it is not always immediately clear which methods are appropriate. If this happens to you, don't despair, and definitely don't give up! Just guess a method and try it. Even if it fails, you'll probably learn something that you can use to make a better guess. (This is also pretty decent life advice.)

Q18Stage 3

Evaluate ∫01u3u2+1 du\displaystyle\int_{0}^1 \dfrac{u^3}{u^2+1}\ \dee{u}.

Hint

If w=u2+1w=u^2+1, then u2=w−1u^2=w-1.

Answer

12−12log⁡2\dfrac{1}{2}-\dfrac{1}{2}\log 2

Full solution

Often, the denominator of a function is a good guess for the substitution. So, let's try setting w=u2+1\textcolor{red}{w=u^2+1}. Then dw=2u du\textcolor{blue}{\dee{w}=2u\ \dee{u}}:

∫01u3u2+1 du=12∫01u2u2+1 2u du\begin{align*}\int_{0}^1 \dfrac{u^3}{u^2+1}\ \dee{u}&= \frac{1}{2}\int_{0}^1 \dfrac{u^2}{\textcolor{red}{u^2+1}}\ \textcolor{blue}{2u\ \dee{u}}\end{align*}

The numerator now is u2u^2, and looking at our substitution, we see u2=w−1\textcolor{red}{u^2=w-1}:

=12∫12w−1w dw=12∫12(1−1w)dw=12[w−log⁡∣w∣]w=1w=2=12(2−log⁡2−1)=12−12log⁡2\begin{align*}&=\frac{1}{2}\int_{1}^2 \dfrac{\textcolor{red}{w-1}}{\textcolor{red}{w}}\ \textcolor{blue}{\dee{w}}\\ &=\frac{1}{2}\int_{1}^2 \left(1 - \frac{1}{w}\right)\dee{w}\\ &=\frac{1}{2}\left[w - \log|w|\right]_{w=1}^{w=2}\\ &=\frac{1}{2}\left(2-\log 2 - 1\right)=\frac{1}{2}-\frac{1}{2}\log 2\end{align*}
Q19Stage 3

Evaluate ∫tan⁡3θ dθ\displaystyle\int \tan^3 \theta\ \dee{\theta} .

Hint

Using a trigonometric identity, this is similar (though not identical) to ∫tan⁡θ⋅sec⁡2θ dθ\int \tan \theta \cdot \sec^2 \theta\ \dee{\theta}.

Answer

12tan⁡2θ−log⁡∣sec⁡θ∣+C\frac{1}{2}\tan^2\theta -\log|\sec \theta|+C

Full solution

The only thing we really have to work with is a tangent, so it's worth considering what would happen if we substituted u=tan⁡θ\textcolor{red}{u=\tan \theta}. Then du=sec⁡2θ dθ\textcolor{blue}{\dee{u}=\sec^2\theta\ \dee{\theta}}. This doesn't show up in the integrand as it's written, but we can try and bring it out by using the identity tan⁡2θ=sec⁡2θ−1\tan^2\theta = \sec^2 \theta - 1:

∫tan⁡3θ dθ=∫tan⁡θ⋅tan⁡2 θdθ=∫tan⁡θ⋅(sec⁡2 θ−1)dθ=∫tan⁡θ⋅sec⁡2 θdθ−∫tan⁡θ dθ\begin{align*}\int \tan^3 \theta\ \dee{\theta}&= \int \textcolor{red}{\tan \theta}\cdot \tan^2\ \theta \dee{\theta}\\ &= \int \textcolor{red}{\tan \theta}\cdot \left(\sec^2\ \theta-1\right) \dee{\theta}\\ &= \int \textcolor{red}{\tan \theta}\cdot \textcolor{blue}{\sec^2\ \theta \dee{\theta}} -\int \tan \theta \ \dee{\theta}\end{align*}

In Example 1.4.17 of the CLP-2 text, we learned ∫tan⁡θ dθ=log⁡∣sec⁡θ∣+C\int \tan \theta \ \dee{\theta} = \log |\sec \theta|+C

=∫u du−log⁡∣sec⁡θ∣+C=12u2−log⁡∣sec⁡θ∣+C=12tan⁡2θ−log⁡∣sec⁡θ∣+C\begin{align*}&=\int \textcolor{red}{u}\ \textcolor{blue}{\dee{u}} -\log|\sec \theta|+C\\ &=\frac{1}{2}u^2 -\log|\sec \theta|+C\\ &=\frac{1}{2}\tan^2\theta -\log|\sec \theta|+C\end{align*}
Q20Stage 3

Evaluate ∫1ex+e−x dx\displaystyle\int \dfrac{1}{e^x+e^{-x}}\ \dee{x}

Hint

If you multiply the top and the bottom by exe^x, what does this look like the antiderivative of?

Answer

arctan⁡(ex)+C\arctan(e^x)+C

Full solution

At first glance, it's not clear what substitution to use. If we try the denominator, u=ex+e−xu=e^x+e^{-x}, then du=(ex−e−x) dx\dee{u}=(e^x-e^{-x})\ \dee{x}, but it's not clear how to make this work with our integral. So, we can try something else.

If we want to tidy things up, we might think to take u=ex\textcolor{red}{u=e^x} as a substitution. Then du=ex dx,\textcolor{blue}{\dee{u}=e^x\ \dee{x}}, so we need an exe^x in the numerator. That can be arranged.

∫1ex+e−x⋅(exex) dx=∫ex(ex)2+1 dx=∫1u2+1 du=arctan⁡(u)+C=arctan⁡(ex)+C\begin{align*} \int\dfrac{1}{e^x+e^{-x}}\cdot\left(\frac{e^x}{e^x}\right)\ \dee{x}&= \int\frac{\textcolor{blue}{e^x}}{\left(\textcolor{red}{e^{x}}\right)^2+1}\ \textcolor{blue}{\dee{x}}\\ &=\int \dfrac{1}{\textcolor{red}{u}^2+1}\ \textcolor{blue}{\dee{u}}\\ &=\arctan(u)+C\\ &=\arctan(e^x)+C \end{align*}
Q21Stage 3

Evaluate ∫01(1−2x)1−x2 dx\displaystyle\int_0^1 (1-2x)\sqrt{1-x^2}\ \dee{x}

Hint

You know methods other than substitution to evaluate definite integrals.

Answer

π4−23\dfrac{\pi}{4}-\dfrac{2}{3}

Full solution

We often like to take the “inside" function as our substitution, in this case u=1−x2\textcolor{red}{u=1-x^2}, so du=−2x dx\textcolor{blue}{\dee{u}=-2x\ \dee{x}}. This takes care of part of the integral:

∫01(1−2x)1−x2 dx=∫011−x2 dx+∫01(−2x)1−x2 dx\begin{align*}\int_0^1 (1-2x)\sqrt{\textcolor{red}{1-x^2}}\ \dee{x}&= \int_0^1 \sqrt{1-x^2}\ \dee{x}+\int_0^1 \textcolor{blue}{(-2x)}\sqrt{\textcolor{red}{1-x^2}}\ \textcolor{blue}{\dee{x}}\end{align*}

The left integral is tough to solve with substitution, but luckily we don't have to–it's the area of a quarter of a circle of radius 1.

=π4+∫10u du=π4+[23u3/2]u=1u=0=π4+0−23=π4−23\begin{align*}&=\frac{\pi}{4}+\int_1^0 \sqrt{\textcolor{red}{u}}\ \textcolor{blue}{\dee{u}}\\ &=\frac{\pi}{4}+\left[\frac{2}{3}u^{3/2}\right]_{u=1}^{u=0}\\ &=\frac{\pi}{4} + 0 - \frac{2}{3} = \frac{\pi}{4}-\frac{2}{3}\end{align*}
Q22Stage 3

Evaluate ∫tan⁡x⋅log⁡(cos⁡x)dx\displaystyle\int\tan x \cdot \log\left(\cos x\right) \dee{x}

Hint

tan⁡x=sin⁡xcos⁡x\tan x = \dfrac{\sin x}{\cos x}

Answer

−12(log⁡(cos⁡x))2+C-\frac{1}{2}\left(\log (\cos x)\right)^2+C

Full solution
  • We often find it useful to take “inside" functions as our substitutions, so let's try u=cos⁡x\textcolor{red}{u=\cos x}, du=−sin⁡x dx\textcolor{blue}{\dee{u} = -\sin x\ \dee{x}}. In order to dig up a sine, we use the identity tan⁡x=sin⁡xcos⁡x\tan x = \dfrac{\sin x}{\cos x} :

    ∫tan⁡x⋅log⁡(cos⁡x)dx=−∫−sin⁡xcos⁡x⋅log⁡(cos⁡x)dx=−∫1ulog⁡(u) du\begin{align*}\int\tan x \cdot \log\left(\textcolor{red}{\cos x}\right) \dee{x}&= -\int\frac{\textcolor{blue}{-\sin x}}{\textcolor{red}{\cos x}} \cdot \log\left(\textcolor{red}{\cos x}\right) \textcolor{blue}{\dee{x}}\\ &=-\int\frac{1}{\textcolor{red}u}\log(\textcolor{red}u)\textcolor{blue}{\ \dee{u}}\end{align*}

    Now, it is convenient to let w=log⁡u\textcolor{orange}{w=\log u}, dw=1u du\textcolor{purple}{\dee{w}=\frac{1}{u}\ \dee{u}} :

    −∫1ulog⁡(u) du=−∫w dw=−12w2+C=−12(log⁡u)2+C=−12(log⁡(cos⁡x))2+C\begin{align*}-\int\textcolor{purple}{\frac{1}{u}}\textcolor{orange}{\log(u)}\textcolor{purple}{\ \dee{u}} &=-\int \textcolor{orange}w\ \textcolor{purple}{\dee{w}}\\ &=-\frac{1}{2}w^2+C\\ &=-\frac{1}{2}\left(\log u\right)^2+C\\ &=-\frac{1}{2}\left(\log (\cos x)\right)^2+C\end{align*}
  • We might guess that it's useful to have u=log⁡(cos⁡x)\textcolor{red}{u=\log(\cos x)}, du=−sin⁡xcos⁡x dx=−tan⁡x dx\textcolor{blue}{\dee{u}=\dfrac{-\sin x}{\cos x}\ \dee{x} = -\tan x\ \dee{x}}:

    ∫tan⁡x⋅log⁡(cos⁡x)dx=−∫−tan⁡x⋅log⁡(cos⁡x)dx=−∫u du=−12u2+C=−12(log⁡(cos⁡x))2+C\begin{align*} \int\tan x \cdot \textcolor{red}{\log\left(\cos x\right)} \dee{x}&= -\int\textcolor{blue}{-\tan x} \cdot \textcolor{red}{\log\left(\cos x\right) }\textcolor{blue}{\dee{x}}\\ &=-\int \textcolor{red}{u}\ \textcolor{blue}{\dee{u}}\\ &=-\frac{1}{2}u^2+C\\ &=-\frac{1}{2}\left(\log(\cos x)\right)^2+C \end{align*}
Q23Stage 3Past exam · 2001A

Evaluate lim⁡n→∞∑j=1njn2cos⁡(j2n2)\displaystyle\lim\limits_{n\rightarrow\infty} \sum\limits_{j=1}^n \dfrac{j}{n^2}\cos\left(\dfrac{j^2}{n^2}\right).

Hint

Review the definition of the definite integral and in particular Definitions 1.1.9 and 1.1.11 in the

CLP-2 text.

Answer

12sin⁡(1)\half\sin(1)

Full solution

The given sum is of the form

lim⁡n→∞∑j=1njn2cos⁡(j2n2)=lim⁡n→∞∑j=1nf(xj∗)Δx\begin{align*} \lim_{n\rightarrow\infty}\sum_{j=1}^n \frac{j}{n^2}\cos\Big(\frac{j^2}{n^2}\Big) =\lim_{n\rightarrow\infty}\sum_{j=1}^n f(x_j^*)\De x \end{align*}

with Δx=1n\De x=\frac{1}{n}, xj∗=jnx_j^*=\frac{j}{n} and f(x)=xcos⁡(x2)f(x)=x\cos(x^2). Since x0∗=0x_0^*=0 and xn∗=1x_n^*=1, the right hand side is the definition (using the right Riemann sum) of

∫01f(x) dx=∫01xcos⁡(x2) dx=12∫01cos⁡(y) dywith y=x2, dy=2x dx=12[sin⁡(y)]01=12sin⁡1\begin{align*} \int_0^1 f(x)\,\dee{x} &=\int_0^1 \textcolor{blue}{x}\cos(\textcolor{red}{x^2})\,\textcolor{blue}{\dee{x}} \\ &=\textcolor{blue}{\frac{1}{2}}\int_0^1 \cos(\textcolor{red}{y})\,\textcolor{blue}{\dee{y} }\qquad\text{with }\textcolor{red}{y=x^2}\text{, }\textcolor{blue}{\dee{y}=2x\,\dee{x}} \\ &=\frac{1}{2}\Big[\sin(y)\Big]_0^1 \\ &=\frac{1}{2}\sin 1 \end{align*}
Q24Stage 3Past exam · 2001D

Calculate lim⁡n→∞∑j=1njn21+j2n2\displaystyle\lim\limits_{n\rightarrow\infty}\sum\limits_{j=1}^n \frac{j}{n^2}\sqrt{1+\frac{j^2}{n^2}}.

Hint

Review the definition of the definite integral and in particular Definitions 1.1.9 and 1.1.11 in the

CLP-2 text.

Answer

13[22−1]≈0.609\dfrac{1}{3}[2\sqrt{2}-1] \approx0.609

Full solution

The given sum is of the form

lim⁡n→∞∑j=1njn21+j2n2=lim⁡n→∞∑j=1nf(xj∗)Δx\begin{align*} \lim_{n\rightarrow\infty}\sum_{j=1}^n \frac{j}{n^2}\sqrt{1+\frac{j^2}{n^2}} =\lim_{n\rightarrow\infty}\sum_{j=1}^n f(x_j^*)\De x \end{align*}

with Δx=1n\De x=\frac{1}{n}, xj∗=jnx_j^*=\frac{j}{n} and f(x)=x1+x2f(x)=x\sqrt{1+x^2}. Since x0∗=0x_0^*=0 and xn∗=1x_n^*=1, the right hand side is the definition (using the right Riemann sum) of

∫01f(x) dx=∫01x1+x2 dx=12∫12y dywith y=1+x2, dy=2x dx=12[23y3/2]y=1y=2=13[22−1]\begin{align*} \int_0^1 f(x)\,\dee{x} &=\int_0^1 \textcolor{blue}{x}\sqrt{\textcolor{red}{1+x^2}}\ \textcolor{blue}{\dee{x}} \\ &=\textcolor{blue}{\frac{1}{2}}\int_1^2 \sqrt{\textcolor{red}{y}}\ \textcolor{blue}{\dee{y} }\qquad\text{with }\textcolor{red}{y=1+x^2}\text{, }\textcolor{blue}{\dee{y}=2x\,\dee{x}} \\ &=\frac{1}{2}{\left[\frac{2}{3}y^{3/2}\right]}_{y=1}^{y=2}\\ & =\frac{1}{3}[2\sqrt{2}-1] \end{align*}

Using a calculator, we see this is approximately 0.6090.609.

Q25Stage 3

Using Riemann sums, prove that

∫ab2f(2x)dx=∫2a2bf(x)dx\int_a^b 2f(2x)\dee{x} = \int_{2a}^{2b} f(x)\dee{x}
Hint

Find the right Riemann sum for both definite integrals.

Answer

Using the definition of a definite integral with right Riemann sums:

∫ab2f(2x)dx=lim⁡n→∞∑i=1nΔx⋅2f(2(a+iΔx))Δx=b−an=lim⁡n→∞∑i=1n(b−an)⋅2f(2(a+i(b−an)))=lim⁡n→∞∑i=1n(2b−2an)⋅f(2a+i(2b−2an))∫2a2bf(x)dx=lim⁡n→∞∑i=1nΔx⋅f(2a+iΔx)Δx=2b−2an=lim⁡n→∞∑i=1n(2b−2an)⋅f(2a+i(2b−2an))\begin{align*}\color{red}\int_a^b 2f(2x)\dee{x}&=\lim_{n \to \infty}\sum_{i=1}^n \Delta x \cdot 2f(2(a+i\Delta x))&\Delta x = \frac{b-a}{n}\\ &=\lim_{n \to \infty}\sum_{i=1}^n \left(\frac{b-a}{n}\right)\cdot2 f\left(2\left(a+i\left(\frac{b-a}{n}\right)\right)\right)\\ &=\lim_{n \to \infty}\sum_{i=1}^n \left(\frac{2b-2a}{n}\right)\cdot f\left(2a+i\left(\frac{2b-2a}{n}\right)\right)\\ \color{blue}\int_{2a}^{2b} f(x)\dee{x}&=\lim_{n \to \infty}\sum_{i=1}^n \Delta x \cdot f(2a+i\Delta x)&\Delta x = \frac{2b-2a}{n}\\ &=\lim_{n \to \infty}\sum_{i=1}^n \left(\frac{2b-2a}{n}\right) \cdot f\left(2a+i \left(\frac{2b-2a}{n}\right)\right)\end{align*}

Since the Riemann sums are exactly the same,

∫ab2f(2x)dx=∫2a2bf(x)dx\begin{align*}\color{red}\int_a^b 2f(2x)\dee{x}&= \color{blue}\int_{2a}^{2b} f(x)\dee{x}\end{align*}
Full solution

Using the definition of a definite integral with right Riemann sums:

∫ab2f(2x)dx=lim⁡n→∞∑i=1nΔx⋅2f(2(a+iΔx))Δx=b−an=lim⁡n→∞∑i=1n(b−an)⋅2f(2(a+i(b−an)))=lim⁡n→∞∑i=1n(2b−2an)⋅f(2a+i(2b−2an))∫2a2bf(x)dx=lim⁡n→∞∑i=1nΔx⋅f(2a+iΔx)Δx=2b−2an=lim⁡n→∞∑i=1n(2b−2an)⋅f(2a+i(2b−2an))\begin{align*}\color{red}\int_a^b 2f(2x)\dee{x}&=\lim_{n \to \infty}\sum_{i=1}^n \Delta x \cdot 2f(2(a+i\Delta x))&\Delta x = \frac{b-a}{n}\\ &=\lim_{n \to \infty}\sum_{i=1}^n \left(\frac{b-a}{n}\right)\cdot2 f\left(2\left(a+i\left(\frac{b-a}{n}\right)\right)\right)\\ &=\lim_{n \to \infty}\sum_{i=1}^n \left(\frac{2b-2a}{n}\right)\cdot f\left(2a+i\left(\frac{2b-2a}{n}\right)\right)\\ \color{blue}\int_{2a}^{2b} f(x)\dee{x}&=\lim_{n \to \infty}\sum_{i=1}^n \Delta x \cdot f(2a+i\Delta x)&\Delta x = \frac{2b-2a}{n}\\ &=\lim_{n \to \infty}\sum_{i=1}^n \left(\frac{2b-2a}{n}\right) \cdot f\left(2a+i \left(\frac{2b-2a}{n}\right)\right)\end{align*}

Since the Riemann sums are exactly the same,

∫ab2f(2x)dx=∫2a2bf(x)dx\begin{align*}\color{red}\int_a^b 2f(2x)\dee{x}&= \color{blue}\int_{2a}^{2b} f(x)\dee{x}\end{align*}

Looking at the Riemann sum in this way is instructive, because it is very clear why the two integrals should be equal (without using substitution). The rectangles in the first Riemann sum are half as wide, but twice as tall, as the rectangles in the second Riemann sum. So, the two Riemann sums have rectangles of the same area.

Figure from prob_s1.4, line 2

Figure from prob_s1.4, line 2

In the integral on the left, the variable is red x\textcolor{red}{x} and in the integral on the right, the variable is blue x\textcolor{blue}{x}. Red x\textcolor{red}{x} and blue x\textcolor{blue}{x} are not the same. In fact 2xi∗=xi∗2\textcolor{red}{x_i^*}=\textcolor{blue}{x_i^*}. (Not every substitution corresponds to such a simple picture.)

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From the UBC Math 101 open textbook project, © Joel Feldman, Andrew Rechnitzer, Elyse Yeager and others. Licensed CC BY-NC-SA 4.0; this HTML adaptation is released under the same licence. Full attribution.