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Further Calculus

This topic extends the calculus of A Level Mathematics to more powerful integration techniques, Inverse trigonometric functions, volumes of revolution, arc length, and surface area. These tools are essential for university-level mathematics, physics, and engineering.

BoardPaperNotes
AQAPaper 1Integration by parts, inverse trig integrals, volumes, arc length
EdexcelFP1, FP2Parts in FP1; inverse trig, volumes, arc length in FP2
OCR (A)Paper 1Parts, inverse trig integrals, volumes
CIE (9231)P1, P2Parts and volumes in P1; arc length and surface area in P2

1.1 The formula, proof from the product rule

Section titled “1.1 The formula, proof from the product rule”

Theorem. For differentiable functions u(x)u(x) and v(x)v(x):

∫u dvdx dx=uv−∫v dudx dx\boxed{\int u\,\frac{dv}{dx}\,dx = uv - \int v\,\frac{du}{dx}\,dx}

From the product rule:

ddx(uv)=udvdx+vdudx\frac{d}{dx}(uv) = u\frac{dv}{dx} + v\frac{du}{dx}

Integrating both sides with respect to xx:

uv=∫udvdx dx+∫vdudx dxuv = \int u\frac{dv}{dx}\,dx + \int v\frac{du}{dx}\,dx

Rearranging:

∫udvdx dx=uv−∫vdudx dx■\int u\frac{dv}{dx}\,dx = uv - \int v\frac{du}{dx}\,dx \quad \blacksquare

When the integral does not simplify in one step, apply integration by parts repeatedly until it does.

Example. Find ∫x2ex dx\displaystyle\int x^2 e^x\,dx.

First application: u = x^2$$dv = e^x\,dx. du = 2x\,dx$$v = e^x.

∫x2ex dx=x2ex−2∫xex dx\int x^2 e^x\,dx = x^2 e^x - 2\int x e^x\,dx

Second application on ∫xex dx\int x e^x\,dx: u = x$$dv = e^x\,dx. du = dx$$v = e^x.

∫xex dx=xex−∫ex dx=xex−ex+C\int x e^x\,dx = xe^x - \int e^x\,dx = xe^x - e^x + C

Therefore:

∫x2ex dx=x2ex−2(xex−ex)+C=ex(x2−2x+2)+C\int x^2 e^x\,dx = x^2 e^x - 2(xe^x - e^x) + C = e^x(x^2 - 2x + 2) + C

Example. Find ∫eaxcos⁡bx dx\displaystyle\int e^{ax}\cos bx\,dx.

Let I=∫eaxcos⁡bx dxI = \int e^{ax}\cos bx\,dx. First application: u=eaxu = e^{ax}, dv=cos⁡bx dxdv = \cos bx\,dx.

du=aeax dx,v=1bsin⁡bxdu = ae^{ax}\,dx, \quad v = \frac{1}{b}\sin bx I=eaxsin⁡bxb−ab∫eaxsin⁡bx dxI = \frac{e^{ax}\sin bx}{b} - \frac{a}{b}\int e^{ax}\sin bx\,dx

Second application on ∫eaxsin⁡bx dx\int e^{ax}\sin bx\,dx: u=eaxu = e^{ax}, dv=sin⁡bx dxdv = \sin bx\,dx.

du=aeax dx,v=−1bcos⁡bxdu = ae^{ax}\,dx, \quad v = -\frac{1}{b}\cos bx ∫eaxsin⁡bx dx=−eaxcos⁡bxb+ab∫eaxcos⁡bx dx=−eaxcos⁡bxb+abI\int e^{ax}\sin bx\,dx = -\frac{e^{ax}\cos bx}{b} + \frac{a}{b}\int e^{ax}\cos bx\,dx = -\frac{e^{ax}\cos bx}{b} + \frac{a}{b}I

Substituting back:

I=eaxsin⁡bxb−ab(−eaxcos⁡bxb+abI)I = \frac{e^{ax}\sin bx}{b} - \frac{a}{b}\left(-\frac{e^{ax}\cos bx}{b} + \frac{a}{b}I\right) I=eaxsin⁡bxb+aeaxcos⁡bxb2−a2b2II = \frac{e^{ax}\sin bx}{b} + \frac{ae^{ax}\cos bx}{b^2} - \frac{a^2}{b^2}I I(1+a2b2)=eax(sin⁡bxb+acos⁡bxb2)I\left(1 + \frac{a^2}{b^2}\right) = e^{ax}\left(\frac{\sin bx}{b} + \frac{a\cos bx}{b^2}\right) I=eax(acos⁡bx+bsin⁡bx)a2+b2+C\boxed{I = \frac{e^{ax}(a\cos bx + b\sin bx)}{a^2 + b^2} + C}

A reduction formula expresses an integral InI_n (depending on a parameter nn) in terms of In−1I_{n-1} or In−2I_{n-2}.

Proof of the reduction formula for In=∫0π/2sin⁡nx dxI_n = \int_0^{\pi/2} \sin^n x\,dx

Section titled “Proof of the reduction formula for In=∫0π/2sin⁡nx dxI_n = \int_0^{\pi/2} \sin^n x\,dxIn​=∫0π/2​sinnxdx”

Write In=∫0π/2sin⁡n−1x⋅sin⁡x dxI_n = \int_0^{\pi/2}\sin^{n-1}x \cdot \sin x\,dx.

Let u=sin⁡n−1xu = \sin^{n-1}x, dv=sin⁡x dxdv = \sin x\,dx. Then:

du=(n−1)sin⁡n−2xcos⁡x dx,v=−cos⁡xdu = (n-1)\sin^{n-2}x\cos x\,dx, \quad v = -\cos x In=[−sin⁡n−1xcos⁡x]0π/2+(n−1)∫0π/2sin⁡n−2xcos⁡2x dxI_n = \bigl[-\sin^{n-1}x\cos x\bigr]_0^{\pi/2} + (n-1)\int_0^{\pi/2}\sin^{n-2}x\cos^2 x\,dx

The boundary term vanishes: at x = 0$$\sin 0 = 0; at x = \pi/2$$\cos(\pi/2) = 0.

Using cos⁡2x=1−sin⁡2x\cos^2 x = 1 - \sin^2 x:

In=(n−1)∫0π/2sin⁡n−2x dx−(n−1)∫0π/2sin⁡nx dxI_n = (n-1)\int_0^{\pi/2}\sin^{n-2}x\,dx - (n-1)\int_0^{\pi/2}\sin^n x\,dx In=(n−1)In−2−(n−1)InI_n = (n-1)I_{n-2} - (n-1)I_n nIn=(n−1)In−2nI_n = (n-1)I_{n-2} In=n−1n In−2,n≥2\boxed{I_n = \frac{n-1}{n}\,I_{n-2}, \quad n \geq 2}

The base cases are I0=∫0π/21 dx=π2I_0 = \displaystyle\int_0^{\pi/2}1\,dx = \dfrac{\pi}{2} and I1=∫0π/2sin⁡x dx=1I_1 = \displaystyle\int_0^{\pi/2}\sin x\,dx = 1.

Example. Using the reduction formula, I4=34I2=34⋅12I0=34⋅12⋅π2=3π16I_4 = \dfrac{3}{4}I_2 = \dfrac{3}{4}\cdot\dfrac{1}{2}I_0 = \dfrac{3}{4}\cdot\dfrac{1}{2}\cdot\dfrac{\pi}{2} = \dfrac{3\pi}{16}.

Caution: warning 00 and π/2\pi/2. For general limits, the boundary term must be evaluated. Example. Find a reduction formula for In=∫xnex dxI_n = \displaystyle\int x^n e^x\,dx.

Let u = x^n$$dv = e^x\,dx. Then du = nx^{n-1}\,dx$$v = e^x.

In=xnex−nIn−1\boxed{I_n = x^n e^x - nI_{n-1}}

With I0=ex+CI_0 = e^x + C.


When the denominator factorises into distinct linear factors, decompose and integrate each term.

Example. ∫2x+3(x+1)(x+2) dx\displaystyle\int \frac{2x+3}{(x+1)(x+2)}\,dx.

2x+3(x+1)(x+2)=Ax+1+Bx+2\frac{2x+3}{(x+1)(x+2)} = \frac{A}{x+1} + \frac{B}{x+2}

2x+3=A(x+2)+B(x+1)2x + 3 = A(x+2) + B(x+1). Setting x=−1x = -1: 1=A1 = A. Setting x=−2x = -2: −1=−B  ⟹  B=1-1 = -B \implies B = 1.

∫1x+1+1x+2 dx=ln⁡∣x+1∣+ln⁡∣x+2∣+C=ln⁡∣(x+1)(x+2)∣+C\int \frac{1}{x+1} + \frac{1}{x+2}\,dx = \ln|x+1| + \ln|x+2| + C = \ln|(x+1)(x+2)| + C

When the denominator contains an irreducible quadratic ax2+bx+cax^2 + bx + c (discriminant b2−4ac<0b^2 - 4ac < 0), the partial fraction has a linear numerator over the quadratic, leading to ln⁡\ln and arctan⁡\arctan terms.

Example. ∫3x+1x2+2x+5 dx\displaystyle\int \frac{3x + 1}{x^2 + 2x + 5}\,dx.

Complete the square: x2+2x+5=(x+1)2+4x^2 + 2x + 5 = (x+1)^2 + 4.

Split the numerator to match the derivative of the denominator:

3x+1x2+2x+5=32(2x+2)+1−3x2+2x+5=32⋅2x+2x2+2x+5−2(x+1)2+4\frac{3x+1}{x^2+2x+5} = \frac{\frac{3}{2}(2x+2) + 1 - 3}{x^2+2x+5} = \frac{3}{2}\cdot\frac{2x+2}{x^2+2x+5} - \frac{2}{(x+1)^2+4} ∫3x+1x2+2x+5 dx=32ln⁡(x2+2x+5)−2⋅12arctan⁡ ⁣(x+12)+C\int \frac{3x+1}{x^2+2x+5}\,dx = \frac{3}{2}\ln(x^2+2x+5) - 2\cdot\frac{1}{2}\arctan\!\left(\frac{x+1}{2}\right) + C =32ln⁡(x2+2x+5)−arctan⁡ ⁣(x+12)+C= \frac{3}{2}\ln(x^2+2x+5) - \arctan\!\left(\frac{x+1}{2}\right) + C

Example. ∫1x(x−1)2 dx\displaystyle\int \frac{1}{x(x-1)^2}\,dx.

1x(x−1)2=Ax+Bx−1+C(x−1)2\frac{1}{x(x-1)^2} = \frac{A}{x} + \frac{B}{x-1} + \frac{C}{(x-1)^2}

1=A(x−1)2+Bx(x−1)+Cx1 = A(x-1)^2 + Bx(x-1) + Cx.

x=0x = 0: 1=A1 = A. x=1x = 1: 1=C1 = C. x=2x = 2: 1=A+2B+2C=1+2B+2  ⟹  B=−11 = A + 2B + 2C = 1 + 2B + 2 \implies B = -1.

∫(1x−1x−1+1(x−1)2)dx=ln⁡∣x∣−ln⁡∣x−1∣−1x−1+C\int\left(\frac{1}{x} - \frac{1}{x-1} + \frac{1}{(x-1)^2}\right)dx = \ln|x| - \ln|x-1| - \frac{1}{x-1} + C

Theorem. The following integrals hold for a>0a > 0:

∫1a2+x2 dx=1aarctan⁡xa+C\boxed{\int \frac{1}{a^2+x^2}\,dx = \frac{1}{a}\arctan\frac{x}{a} + C} ∫1a2−x2 dx=arcsin⁡xa+C\boxed{\int \frac{1}{\sqrt{a^2-x^2}}\,dx = \arcsin\frac{x}{a} + C} ∫1a2−x2 dx=12aln⁡∣a+xa−x∣+C\boxed{\int \frac{1}{a^2-x^2}\,dx = \frac{1}{2a}\ln\left|\frac{a+x}{a-x}\right| + C}

Proof of ∫1a2+x2 dx=1aarctan⁡xa+C\int \frac{1}{a^2+x^2}\,dx = \frac{1}{a}\arctan\frac{x}{a} + C

Section titled “Proof of ∫1a2+x2 dx=1aarctan⁡xa+C\int \frac{1}{a^2+x^2}\,dx = \frac{1}{a}\arctan\frac{x}{a} + C∫a2+x21​dx=a1​arctanax​+C”

Let x=atan⁡θx = a\tan\theta So dx=asec⁡2θ dθdx = a\sec^2\theta\,d\theta.

∫1a2+a2tan⁡2θ⋅asec⁡2θ dθ=∫asec⁡2θa2sec⁡2θ dθ=1a∫1 dθ=θa+C\int \frac{1}{a^2 + a^2\tan^2\theta}\cdot a\sec^2\theta\,d\theta = \int \frac{a\sec^2\theta}{a^2\sec^2\theta}\,d\theta = \frac{1}{a}\int 1\,d\theta = \frac{\theta}{a} + C

Since θ=arctan⁡(x/a)\theta = \arctan(x/a):

∫1a2+x2 dx=1aarctan⁡xa+C■\int \frac{1}{a^2+x^2}\,dx = \frac{1}{a}\arctan\frac{x}{a} + C \quad \blacksquare

Proof of ∫1a2−x2 dx=arcsin⁡xa+C\int \frac{1}{\sqrt{a^2-x^2}}\,dx = \arcsin\frac{x}{a} + C

Section titled “Proof of ∫1a2−x2 dx=arcsin⁡xa+C\int \frac{1}{\sqrt{a^2-x^2}}\,dx = \arcsin\frac{x}{a} + C∫a2−x2​1​dx=arcsinax​+C”

Let x=asin⁡θx = a\sin\theta So dx=acos⁡θ dθdx = a\cos\theta\,d\theta and a2−x2=acos⁡θ\sqrt{a^2 - x^2} = a\cos\theta (for ∣θ∣≤π/2|\theta| \leq \pi/2).

∫acos⁡θacos⁡θ dθ=∫1 dθ=θ+C=arcsin⁡xa+C■\int \frac{a\cos\theta}{a\cos\theta}\,d\theta = \int 1\,d\theta = \theta + C = \arcsin\frac{x}{a} + C \quad \blacksquare

Proof of ∫1a2−x2 dx=12aln⁡∣a+xa−x∣+C\int \frac{1}{a^2-x^2}\,dx = \frac{1}{2a}\ln\left|\frac{a+x}{a-x}\right| + C

Section titled “Proof of ∫1a2−x2 dx=12aln⁡∣a+xa−x∣+C\int \frac{1}{a^2-x^2}\,dx = \frac{1}{2a}\ln\left|\frac{a+x}{a-x}\right| + C∫a2−x21​dx=2a1​ln​a−xa+x​​+C”

By partial fractions:

1a2−x2=1(a−x)(a+x)=12a(1a−x+1a+x)\frac{1}{a^2-x^2} = \frac{1}{(a-x)(a+x)} = \frac{1}{2a}\left(\frac{1}{a-x} + \frac{1}{a+x}\right) ∫1a2−x2 dx=12a[−ln⁡∣a−x∣+ln⁡∣a+x∣]+C=12aln⁡∣a+xa−x∣+C■\int \frac{1}{a^2-x^2}\,dx = \frac{1}{2a}\bigl[-\ln|a-x| + \ln|a+x|\bigr] + C = \frac{1}{2a}\ln\left|\frac{a+x}{a-x}\right| + C \quad \blacksquare∫1a2+(x+b)2 dx=1aarctan⁡x+ba+C\int \frac{1}{a^2 + (x+b)^2}\,dx = \frac{1}{a}\arctan\frac{x+b}{a} + C ∫1a2−(x+b)2 dx=arcsin⁡x+ba+C\int \frac{1}{\sqrt{a^2 - (x+b)^2}}\,dx = \arcsin\frac{x+b}{a} + C

These follow directly from the standard forms via the substitution u=x+bu = x + b.


4. Differentiation of Inverse Trigonometric Functions

Section titled “4. Differentiation of Inverse Trigonometric Functions”
ddxarcsin⁡x=11−x2,∣x∣<1\boxed{\frac{d}{dx}\arcsin x = \frac{1}{\sqrt{1-x^2}}, \quad |x| < 1} ddxarccos⁡x=−11−x2,∣x∣<1\boxed{\frac{d}{dx}\arccos x = -\frac{1}{\sqrt{1-x^2}}, \quad |x| < 1} ddxarctan⁡x=11+x2\boxed{\frac{d}{dx}\arctan x = \frac{1}{1+x^2}}

Proof of ddxarctan⁡x=11+x2\frac{d}{dx}\arctan x = \frac{1}{1+x^2}

Section titled “Proof of ddxarctan⁡x=11+x2\frac{d}{dx}\arctan x = \frac{1}{1+x^2}dxd​arctanx=1+x21​”

Let y=arctan⁡xy = \arctan x. Then x=tan⁡yx = \tan y.

Differentiating implicitly with respect to xx:

1=sec⁡2y⋅dydx1 = \sec^2 y \cdot \frac{dy}{dx} dydx=1sec⁡2y=11+tan⁡2y=11+x2■\frac{dy}{dx} = \frac{1}{\sec^2 y} = \frac{1}{1 + \tan^2 y} = \frac{1}{1+x^2} \quad \blacksquare

Proof of ddxarcsin⁡x=11−x2\frac{d}{dx}\arcsin x = \frac{1}{\sqrt{1-x^2}}

Section titled “Proof of ddxarcsin⁡x=11−x2\frac{d}{dx}\arcsin x = \frac{1}{\sqrt{1-x^2}}dxd​arcsinx=1−x2​1​”

Let y=arcsin⁡xy = \arcsin x. Then x=sin⁡yx = \sin y.

Differentiating implicitly:

1=cos⁡y⋅dydx1 = \cos y \cdot \frac{dy}{dx}

Since arcsin⁡x\arcsin x has range [−π/2,π/2][-\pi/2, \pi/2] We have cos⁡y≥0\cos y \geq 0 So cos⁡y=1−sin⁡2y=1−x2\cos y = \sqrt{1-\sin^2 y} = \sqrt{1-x^2}.

dydx=1cos⁡y=11−x2■\frac{dy}{dx} = \frac{1}{\cos y} = \frac{1}{\sqrt{1-x^2}} \quad \blacksquare

4.2 Chain rule with inverse trig functions

Section titled “4.2 Chain rule with inverse trig functions”

Example. ddxarcsin⁡(3x)=31−9x2\dfrac{d}{dx}\arcsin(3x) = \dfrac{3}{\sqrt{1-9x^2}}.

Example. ddxarctan⁡ ⁣(x2)=1/21+x2/4=24+x2\dfrac{d}{dx}\arctan\!\left(\dfrac{x}{2}\right) = \dfrac{1/2}{1 + x^2/4} = \dfrac{2}{4+x^2}.


Definition. The volume generated by rotating the region bounded by y=f(x)y = f(x) The xx-axis, x=ax = a And x=bx = b about the xx-axis is:

V=π∫aby2 dx=π∫ab[f(x)]2 dx\boxed{V = \pi\int_a^b y^2\,dx = \pi\int_a^b [f(x)]^2\,dx}

Definition. The volume generated by rotating the region bounded by x=g(y)x = g(y) The yy-axis, y=cy = c And y=dy = d about the yy-axis is:

V=π∫cdx2 dy=π∫cd[g(y)]2 dy\boxed{V = \pi\int_c^d x^2\,dy = \pi\int_c^d [g(y)]^2\,dy}

When a curve is given parametrically by x=x(t)x = x(t), y=y(t)y = y(t):

  • Rotation about the xx-axis: V=π∫t1t2y2 dxdt dtV = \pi\displaystyle\int_{t_1}^{t_2} y^2\,\frac{dx}{dt}\,dt
  • Rotation about the yy-axis: V=π∫t1t2x2 dydt dtV = \pi\displaystyle\int_{t_1}^{t_2} x^2\,\frac{dy}{dt}\,dt

Example. Find the volume generated by rotating the curve y=xy = \sqrt{x} from x=0x = 0 to x=4x = 4 About the xx-axis.

V=π∫04(x)2 dx=π∫04x dx=π[x22]04=8πV = \pi\int_0^4 (\sqrt{x})^2\,dx = \pi\int_0^4 x\,dx = \pi\left[\frac{x^2}{2}\right]_0^4 = 8\pi

Example. The curve x=2cos⁡tx = 2\cos t, y=2sin⁡ty = 2\sin t for 0≤t≤π0 \leq t \leq \pi is rotated about the xx-axis. Find the volume.

V=π∫0π(2sin⁡t)2⋅dxdt dt=π∫0π4sin⁡2t⋅(−2sin⁡t) dtV = \pi\int_0^{\pi} (2\sin t)^2 \cdot \frac{dx}{dt}\,dt = \pi\int_0^{\pi} 4\sin^2 t \cdot (-2\sin t)\,dt =−8π∫0πsin⁡3t dt=8π∫0πsin⁡3t dt= -8\pi\int_0^{\pi}\sin^3 t\,dt = 8\pi\int_0^{\pi}\sin^3 t\,dt

Using sin⁡3t=sin⁡t(1−cos⁡2t)\sin^3 t = \sin t(1-\cos^2 t) and the substitution u=cos⁡tu = \cos t:

=8π∫−11(1−u2) du=8π[u−u33]−11=8π(23−(−23))=32π3= 8\pi\int_{-1}^{1}(1-u^2)\,du = 8\pi\left[u - \frac{u^3}{3}\right]_{-1}^1 = 8\pi\left(\frac{2}{3} - \left(-\frac{2}{3}\right)\right) = \frac{32\pi}{3}

6. Arc Length and Surface Area of Revolution

Section titled “6. Arc Length and Surface Area of Revolution”

Theorem. For a curve y=f(x)y = f(x) from x=ax = a to x=bx = b:

s=∫ab1+(dydx)2 dx\boxed{s = \int_a^b \sqrt{1 + \left(\frac{dy}{dx}\right)^2}\,dx}

For a curve given parametrically by x=x(t)x = x(t), y=y(t)y = y(t) from t=t1t = t_1 to t=t2t = t_2:

s=∫t1t2(dxdt)2+(dydt)2 dt\boxed{s = \int_{t_1}^{t_2} \sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2}\,dt}

Derivation (Cartesian). The arc length element dsds satisfies ds2=dx2+dy2ds^2 = dx^2 + dy^2 by the Pythagorean theorem applied to an infinitesimal segment. Therefore:

ds=1+(dydx)2 dxds = \sqrt{1 + \left(\frac{dy}{dx}\right)^2}\,dx

Integrating from aa to bb gives the total arc length.

Example. Find the arc length of y=ln⁡(cos⁡x)y = \ln(\cos x) from x=0x = 0 to x=π/3x = \pi/3.

dydx=−sin⁡xcos⁡x=−tan⁡x\frac{dy}{dx} = \frac{-\sin x}{\cos x} = -\tan x s=∫0π/31+tan⁡2x dx=∫0π/3sec⁡x dx=[ln⁡∣sec⁡x+tan⁡x∣]0π/3s = \int_0^{\pi/3}\sqrt{1+\tan^2 x}\,dx = \int_0^{\pi/3}\sec x\,dx = \Bigl[\ln|\sec x + \tan x|\Bigr]_0^{\pi/3} =ln⁡(2+3)−ln⁡(1)=ln⁡(2+3)= \ln(2 + \sqrt{3}) - \ln(1) = \ln(2+\sqrt{3})

Theorem. The surface area generated by rotating y=f(x)y = f(x) from x=ax = a to x=bx = b about the xx-axis:

S=2π∫aby 1+(dydx)2 dx\boxed{S = 2\pi\int_a^b y\,\sqrt{1 + \left(\frac{dy}{dx}\right)^2}\,dx}

For a parametric curve rotated about the xx-axis:

S=2π∫t1t2y (dxdt)2+(dydt)2 dt\boxed{S = 2\pi\int_{t_1}^{t_2} y\,\sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2}\,dt}

Example. Find the surface area generated by rotating y=x2y = x^2 from x=0x = 0 to x=1x = 1 about the xx-axis.

S=2π∫01x21+4x2 dxS = 2\pi\int_0^1 x^2\sqrt{1+4x^2}\,dx

Let x=12tan⁡θx = \frac{1}{2}\tan\theta, dx=12sec⁡2θ dθdx = \frac{1}{2}\sec^2\theta\,d\theta. When x=0x = 0 θ=0\theta = 0; when x=1x = 1, θ=arctan⁡2\theta = \arctan 2.

S=2π∫0arctan⁡2tan⁡2θ4⋅sec⁡θ⋅12sec⁡2θ dθ=π4∫0arctan⁡2tan⁡2θsec⁡3θ dθS = 2\pi\int_0^{\arctan 2}\frac{\tan^2\theta}{4}\cdot\sec\theta\cdot\frac{1}{2}\sec^2\theta\,d\theta = \frac{\pi}{4}\int_0^{\arctan 2}\tan^2\theta\sec^3\theta\,d\theta

Using tan⁡2θ=sec⁡2θ−1\tan^2\theta = \sec^2\theta - 1 and integrating by parts with u=sec⁡θu = \sec\theta dv=sec⁡2θ dθdv = \sec^2\theta\,d\theta:

This integral evaluates to π4[14sec⁡θtan⁡θ+14ln⁡∣sec⁡θ+tan⁡θ∣−14sec⁡θtan⁡θ+18ln⁡∣sec⁡θ+tan⁡θ∣]0arctan⁡2\dfrac{\pi}{4}\left[\dfrac{1}{4}\sec\theta\tan\theta + \dfrac{1}{4}\ln|\sec\theta+\tan\theta| - \dfrac{1}{4}\sec\theta\tan\theta + \dfrac{1}{8}\ln|\sec\theta+\tan\theta|\right]_0^{\arctan 2}.

Simplifying with sec⁡(arctan⁡2)=5\sec(\arctan 2) = \sqrt{5} and tan⁡(arctan⁡2)=2\tan(\arctan 2) = 2:

S=9π516−π32ln⁡(2+5)S = \frac{9\pi\sqrt{5}}{16} - \frac{\pi}{32}\ln(2+\sqrt{5})
IntegralResult
∫1a2+x2 dx\displaystyle\int\frac{1}{a^2+x^2}\,dx1aarctan⁡xa+C\dfrac{1}{a}\arctan\dfrac{x}{a}+C
∫1a2−x2 dx\displaystyle\int\frac{1}{\sqrt{a^2-x^2}}\,dxarcsin⁡xa+C\arcsin\dfrac{x}{a}+C
∫1a2−x2 dx\displaystyle\int\frac{1}{a^2-x^2}\,dx12aln⁡∥a+xa−x∥+C\dfrac{1}{2a}\ln\left\|\dfrac{a+x}{a-x}\right\|+C
ddxarcsin⁡x\dfrac{d}{dx}\arcsin x11−x2\dfrac{1}{\sqrt{1-x^2}}
ddxarctan⁡x\dfrac{d}{dx}\arctan x11+x2\dfrac{1}{1+x^2}
Vol. About xx-axisπ∫aby2 dx\pi\displaystyle\int_a^b y^2\,dx
Arc length∫1+(dydx)2 dx\displaystyle\int\sqrt{1+\left(\frac{dy}{dx}\right)^2}\,dx

Problem 1Find $\displaystyle\int x^3 e^{-x}\,dx$.
Hint 1Apply integration by parts three times, reducing the power of $x$ each time.
Answer 1First: $u = x^3$$dv = e^{-x}\,dx$. $du = 3x^2\,dx$$v = -e^{-x}$.

∫x3e−x dx=−x3e−x+3∫x2e−x dx\displaystyle\int x^3 e^{-x}\,dx = -x^3 e^{-x} + 3\int x^2 e^{-x}\,dx

Second: u = x^2$$dv = e^{-x}\,dx. ∫x2e−x dx=−x2e−x+2∫xe−x dx\int x^2 e^{-x}\,dx = -x^2 e^{-x} + 2\int x e^{-x}\,dx.

Third: u = x$$dv = e^{-x}\,dx. ∫xe−x dx=−xe−x+∫e−x dx=−xe−x−e−x\int x e^{-x}\,dx = -xe^{-x} + \int e^{-x}\,dx = -xe^{-x} - e^{-x}.

Combining: ∫x3e−x dx=−x3e−x−3x2e−x−6xe−x−6e−x+C=−e−x(x3+3x2+6x+6)+C\int x^3 e^{-x}\,dx = -x^3 e^{-x} - 3x^2 e^{-x} - 6x e^{-x} - 6e^{-x} + C = -e^{-x}(x^3 + 3x^2 + 6x + 6) + C.

Problem 2Find a reduction formula for $I_n = \displaystyle\int \cos^n x\,dx$ for $n \geq 2$.
Hint 2Write $\cos^n x = \cos^{n-1}x \cdot \cos x$ and apply integration by parts with $u = \cos^{n-1}x$$dv = \cos x\,dx$. Use $\sin^2 x = 1 - \cos^2 x$.
Answer 2$I_n = \int\cos^{n-1}x\cos x\,dx$. Let $u = \cos^{n-1}x$$dv = \cos x\,dx$.

du = -(n-1)\cos^{n-2}x\sin x\,dx$$v = \sin x.

In=cos⁡n−1xsin⁡x+(n−1)∫cos⁡n−2xsin⁡2x dxI_n = \cos^{n-1}x\sin x + (n-1)\int\cos^{n-2}x\sin^2 x\,dx

=cos⁡n−1xsin⁡x+(n−1)∫cos⁡n−2x(1−cos⁡2x) dx= \cos^{n-1}x\sin x + (n-1)\int\cos^{n-2}x(1-\cos^2 x)\,dx

=cos⁡n−1xsin⁡x+(n−1)In−2−(n−1)In= \cos^{n-1}x\sin x + (n-1)I_{n-2} - (n-1)I_n

nIn=cos⁡n−1xsin⁡x+(n−1)In−2nI_n = \cos^{n-1}x\sin x + (n-1)I_{n-2}

In=1ncos⁡n−1xsin⁡x+n−1nIn−2+C\boxed{I_n = \frac{1}{n}\cos^{n-1}x\sin x + \frac{n-1}{n}I_{n-2} + C}

Problem 3Evaluate $\displaystyle\int \frac{2x-1}{x^2+4x+13}\,dx$.
Hint 3Complete the square: $x^2+4x+13 = (x+2)^2+9$. Split the numerator into a multiple of $(2x+4)$ plus a constant.
Answer 3$x^2+4x+13 = (x+2)^2+9$. Write $2x-1 = (2x+4) - 5$.

∫2x+4(x+2)2+9 dx−5∫1(x+2)2+9 dx\displaystyle\int\frac{2x+4}{(x+2)^2+9}\,dx - 5\int\frac{1}{(x+2)^2+9}\,dx

=ln⁡(x2+4x+13)−53arctan⁡ ⁣(x+23)+C= \ln(x^2+4x+13) - \frac{5}{3}\arctan\!\left(\frac{x+2}{3}\right) + C

Problem 4Evaluate $\displaystyle\int_0^{\pi/2} \sin^5 x\,dx$ using the reduction formula.
Hint 4Use $I_n = \dfrac{n-1}{n}I_{n-2}$ with $I_1 = 1$.
Answer 4$I_5 = \dfrac{4}{5}I_3 = \dfrac{4}{5}\cdot\dfrac{2}{3}I_1 = \dfrac{4}{5}\cdot\dfrac{2}{3}\cdot 1 = \dfrac{8}{15}$.
Problem 5Find the volume generated by rotating the region bounded by $y = x^2$$y = 0$$x = 0$$x = 2$ about the $y$-axis.
Hint 5Express $x$ in terms of $y$ ($x = \sqrt{y}$) and integrate with respect to $y$ from $0$ to $4$ Or use the Shell method: $V = 2\pi\int_0^2 x\cdot x^2\,dx$.
Answer 5Using the disc method about the $y$-axis: $V = \pi\int_0^4 x^2\,dy = \pi\int_0^4 y\,dy = \pi\left[\frac{y^2}{2}\right]_0^4 = 8\pi$.
Problem 6Find $\dfrac{d}{dx}\left[x\arcsin x + \sqrt{1-x^2}\right]$ and hence evaluate $\displaystyle\int_0^{1/2} \arcsin x\,dx$.
Hint 6Differentiate using the product rule and the chain rule with $\dfrac{d}{dx}\arcsin x$.
Answer 6$\dfrac{d}{dx}\bigl[x\arcsin x + \sqrt{1-x^2}\bigr] = \arcsin x + \dfrac{x}{\sqrt{1-x^2}} + \dfrac{-x}{\sqrt{1-x^2}} = \arcsin x$.

Therefore ∫arcsin⁡x dx=xarcsin⁡x+1−x2+C\displaystyle\int \arcsin x\,dx = x\arcsin x + \sqrt{1-x^2} + C.

∫01/2arcsin⁡x dx=[xarcsin⁡x+1−x2]01/2=12⋅π6+32−1=π12+32−1\displaystyle\int_0^{1/2}\arcsin x\,dx = \left[x\arcsin x + \sqrt{1-x^2}\right]_0^{1/2} = \frac{1}{2}\cdot\frac{\pi}{6} + \frac{\sqrt{3}}{2} - 1 = \frac{\pi}{12} + \frac{\sqrt{3}}{2} - 1.

Problem 7Find the arc length of the curve $y = \dfrac{x^3}{6} + \dfrac{1}{2x}$ from $x = 1$ to $x = 3$.
Hint 7Compute $\dfrac{dy}{dx} = \dfrac{x^2}{2} - \dfrac{1}{2x^2}$. Show that $1+\left(\dfrac{dy}{dx}\right)^2$ is a perfect square.
Answer 7$\dfrac{dy}{dx} = \dfrac{x^2}{2} - \dfrac{1}{2x^2}$.

1+(dydx)2=1+x44−12+14x4=x44+12+14x4=(x22+12x2)21+\left(\dfrac{dy}{dx}\right)^2 = 1 + \dfrac{x^4}{4} - \dfrac{1}{2} + \dfrac{1}{4x^4} = \dfrac{x^4}{4} + \dfrac{1}{2} + \dfrac{1}{4x^4} = \left(\dfrac{x^2}{2} + \dfrac{1}{2x^2}\right)^2

s=∫13(x22+12x2)dx=[x36−12x]13=(92−16)−(16−12)=143s = \displaystyle\int_1^3\left(\dfrac{x^2}{2} + \dfrac{1}{2x^2}\right)dx = \left[\dfrac{x^3}{6} - \dfrac{1}{2x}\right]_1^3 = \left(\dfrac{9}{2}-\dfrac{1}{6}\right)-\left(\dfrac{1}{6}-\dfrac{1}{2}\right) = \dfrac{14}{3}.

Problem 8Evaluate $\displaystyle\int_0^{\infty}\frac{1}{4+x^2}\,dx$.
Hint 8Use $\displaystyle\int\frac{1}{a^2+x^2}\,dx = \frac{1}{a}\arctan\frac{x}{a}$. Here $a = 2$.
Answer 8$\displaystyle\int_0^{\infty}\frac{1}{4+x^2}\,dx = \left[\frac{1}{2}\arctan\frac{x}{2}\right]_0^{\infty} = \frac{1}{2}\cdot\frac{\pi}{2} - 0 = \frac{\pi}{4}$.
Problem 9The curve $x = t^2$$y = t^3$ for $0 \leq t \leq 2$ is rotated about the $x$-axis. Find the volume of Revolution.
Hint 9Use $V = \pi\displaystyle\int_{t_1}^{t_2}y^2\,\frac{dx}{dt}\,dt$. Here $\dfrac{dx}{dt} = 2t$.
Answer 9$V = \pi\displaystyle\int_0^2 t^6 \cdot 2t\,dt = 2\pi\int_0^2 t^7\,dt = 2\pi\left[\frac{t^8}{8}\right]_0^2 = 2\pi\cdot\frac{256}{8} = 64\pi$.
Problem 10Find $\displaystyle\int e^x\sin 2x\,dx$.
Hint 10Apply integration by parts twice. Keep $u = e^x$ on both applications. The original integral will reappear.
Answer 10Let $I = \displaystyle\int e^x\sin 2x\,dx$. First: $u = e^x$$dv = \sin 2x\,dx$. $du = e^x\,dx$$v = -\frac{1}{2}\cos 2x$.

I=−12excos⁡2x+12∫excos⁡2x dxI = -\frac{1}{2}e^x\cos 2x + \frac{1}{2}\int e^x\cos 2x\,dx.

Second on ∫excos⁡2x dx\int e^x\cos 2x\,dx: u = e^x$$dv = \cos 2x\,dx. du=ex dxdu = e^x\,dx v=12sin⁡2xv = \frac{1}{2}\sin 2x.

∫excos⁡2x dx=12exsin⁡2x−12∫exsin⁡2x dx=12exsin⁡2x−12I\int e^x\cos 2x\,dx = \frac{1}{2}e^x\sin 2x - \frac{1}{2}\int e^x\sin 2x\,dx = \frac{1}{2}e^x\sin 2x - \frac{1}{2}I.

I=−12excos⁡2x+14exsin⁡2x−14II = -\frac{1}{2}e^x\cos 2x + \frac{1}{4}e^x\sin 2x - \frac{1}{4}I.

54I=ex(sin⁡2x4−cos⁡2x2)\frac{5}{4}I = e^x\left(\frac{\sin 2x}{4} - \frac{\cos 2x}{2}\right).

I=ex(sin⁡2x−2cos⁡2x)5+C\boxed{I = \frac{e^x(\sin 2x - 2\cos 2x)}{5} + C}


Example 8.1: Leibniz’s rule for higher derivatives of a product

Section titled “Example 8.1: Leibniz’s rule for higher derivatives of a product”

Problem. If y=x2e3xy = x^2 e^{3x} Find d4ydx4\dfrac{d^4 y}{dx^4}.

Solution. We use Leibniz’s rule: (uv)(n)=∑k=0n(nk)u(k)v(n−k)(uv)^{(n)} = \displaystyle\sum_{k=0}^{n} \binom{n}{k} u^{(k)} v^{(n-k)}.

Let u=x2u = x^2 and v=e3xv = e^{3x}.

  • u' = 2x$$u'' = 2$$u''' = 0$$u^{(4)} = 0.
  • v(k)=3ke3xv^{(k)} = 3^k e^{3x} for all kk.
d4ydx4=(40)x2⋅34e3x+(41)2x⋅33e3x+(42)2⋅32e3x+0+0\frac{d^4 y}{dx^4} = \binom{4}{0} x^2 \cdot 3^4 e^{3x} + \binom{4}{1} 2x \cdot 3^3 e^{3x} + \binom{4}{2} 2 \cdot 3^2 e^{3x} + 0 + 0 =81x2e3x+4⋅54xe3x+6⋅18e3x= 81x^2 e^{3x} + 4 \cdot 54x e^{3x} + 6 \cdot 18 e^{3x} =(81x2+216x+108)e3x\boxed{= (81x^2 + 216x + 108)e^{3x}}

Example 8.2: Reduction formula for ∫xnex dx\int x^n e^x\,dx

Section titled “Example 8.2: Reduction formula for ∫xnex dx\int x^n e^x\,dx∫xnexdx”

Problem. Establish and use a reduction formula for In=∫xnex dxI_n = \int x^n e^x\,dx.

Solution. Using integration by parts with u = x^n$$dv = e^x\,dx:

In=xnex−∫nxn−1ex dx=xnex−nIn−1I_n = x^n e^x - \int nx^{n-1} e^x\,dx = x^n e^x - nI_{n-1}

Therefore In=xnex−nIn−1\boxed{I_n = x^n e^x - nI_{n-1}} with I0=ex+CI_0 = e^x + C.

To find I3I_3:

I_1 = x e^x - e^x$$I_2 = x^2 e^x - 2x e^x + 2e^x$$I_3 = x^3 e^x - 3x^2 e^x + 6x e^x - 6e^x.

I3=(x3−3x2+6x−6)ex+C\boxed{I_3 = (x^3 - 3x^2 + 6x - 6)e^x + C}

Example 8.3: Improper integral convergence test

Section titled “Example 8.3: Improper integral convergence test”

Problem. Determine whether ∫011x dx\displaystyle\int_0^1 \frac{1}{\sqrt{x}}\,dx converges, And evaluate if it does.

Solution. The integrand is undefined at x=0x = 0. Write:

∫01x−1/2 dx=lim⁡a→0+∫a1x−1/2 dx=lim⁡a→0+[2x1/2]a1=lim⁡a→0+(2−2a)=2\int_0^1 x^{-1/2}\,dx = \lim_{a \to 0^+} \int_a^1 x^{-1/2}\,dx = \lim_{a \to 0^+} \left[2x^{1/2}\right]_a^1 = \lim_{a \to 0^+} (2 - 2\sqrt{a}) = 2

Since the limit exists and is finite, the integral converges. ∫011x dx=2\boxed{\displaystyle\int_0^1 \frac{1}{\sqrt{x}}\,dx = 2}

Example 8.4: Integration using the t=tan⁡(x/2)t = \tan(x/2) substitution

Section titled “Example 8.4: Integration using the t=tan⁡(x/2)t = \tan(x/2)t=tan(x/2) substitution”

Problem. Evaluate ∫0π/211+sin⁡x dx\displaystyle\int_0^{\pi/2} \frac{1}{1 + \sin x}\,dx using the Weierstrass substitution.

Solution. Let t=tan⁡(x/2)t = \tan(x/2) So sin⁡x=2t1+t2\sin x = \dfrac{2t}{1+t^2} and dx=2 dt1+t2dx = \dfrac{2\,dt}{1+t^2}.

When x=0x = 0: t=0t = 0. When x=π/2x = \pi/2: t=1t = 1.

∫0111+2t1+t2⋅2 dt1+t2=∫012 dt(1+t2)+2t=∫012 dtt2+2t+1=∫012 dt(t+1)2\int_0^1 \frac{1}{1 + \frac{2t}{1+t^2}} \cdot \frac{2\,dt}{1+t^2} = \int_0^1 \frac{2\,dt}{(1+t^2) + 2t} = \int_0^1 \frac{2\,dt}{t^2 + 2t + 1} = \int_0^1 \frac{2\,dt}{(t+1)^2} =[−2t+1]01=−1+2=1= \left[-\frac{2}{t+1}\right]_0^1 = -1 + 2 = \boxed{1}

Example 8.5: Differentiation of parametric arc length

Section titled “Example 8.5: Differentiation of parametric arc length”

Problem. A curve is given by x=t−sin⁡tx = t - \sin t, y=1−cos⁡ty = 1 - \cos t for 0≤t≤2π0 \leq t \leq 2\pi. Find The total arc length.

Solution. dxdt=1−cos⁡t\dfrac{dx}{dt} = 1 - \cos t, dydt=sin⁡t\dfrac{dy}{dt} = \sin t.

s=∫02π(1−cos⁡t)2+sin⁡2t dt=∫02π1−2cos⁡t+cos⁡2t+sin⁡2t dts = \int_0^{2\pi} \sqrt{(1-\cos t)^2 + \sin^2 t}\,dt = \int_0^{2\pi} \sqrt{1 - 2\cos t + \cos^2 t + \sin^2 t}\,dt =∫02π2−2cos⁡t dt=∫02π4sin⁡2(t/2) dt=∫02π2∣sin⁡(t/2)∣ dt= \int_0^{2\pi} \sqrt{2 - 2\cos t}\,dt = \int_0^{2\pi} \sqrt{4\sin^2(t/2)}\,dt = \int_0^{2\pi} 2|\sin(t/2)|\,dt

For 0≤t≤2π0 \leq t \leq 2\pi, sin⁡(t/2)≥0\sin(t/2) \geq 0 So:

s=2∫02πsin⁡(t/2) dt=2[−2cos⁡(t/2)]02π=2(2+2)=8s = 2\int_0^{2\pi} \sin(t/2)\,dt = 2\left[-2\cos(t/2)\right]_0^{2\pi} = 2(2 + 2) = \boxed{8}

Example 8.6: Taylor series approach to a difficult limit

Section titled “Example 8.6: Taylor series approach to a difficult limit”

Problem. Evaluate lim⁡x→0x−sin⁡xx3\displaystyle\lim_{x \to 0} \frac{x - \sin x}{x^3}.

Solution. Expand sin⁡x\sin x as a Maclaurin series:

sin⁡x=x−x36+x5120−⋯\sin x = x - \frac{x^3}{6} + \frac{x^5}{120} - \cdots x−sin⁡xx3=x−(x−x36+x5120−⋯ )x3=x36−x5120+⋯x3=16−x2120+⋯\frac{x - \sin x}{x^3} = \frac{x - \left(x - \frac{x^3}{6} + \frac{x^5}{120} - \cdots\right)}{x^3} = \frac{\frac{x^3}{6} - \frac{x^5}{120} + \cdots}{x^3} = \frac{1}{6} - \frac{x^2}{120} + \cdots

Taking x→0x \to 0: lim⁡x→0x−sin⁡xx3=16\boxed{\displaystyle\lim_{x \to 0} \frac{x - \sin x}{x^3} = \frac{1}{6}}

Example 8.7: Integration involving inverse trigonometric functions

Section titled “Example 8.7: Integration involving inverse trigonometric functions”

Problem. Evaluate ∫arcsin⁡x dx\displaystyle\int \arcsin x\,dx.

Solution. Use integration by parts with u=arcsin⁡xu = \arcsin x, dv=dxdv = dx:

du=11−x2 dx,v=xdu = \frac{1}{\sqrt{1-x^2}}\,dx, \quad v = x ∫arcsin⁡x dx=xarcsin⁡x−∫x1−x2 dx\int \arcsin x\,dx = x\arcsin x - \int \frac{x}{\sqrt{1-x^2}}\,dx

For the second integral, let w=1−x2w = 1 - x^2, dw=−2x dxdw = -2x\,dx:

∫x1−x2 dx=−1−x2\int \frac{x}{\sqrt{1-x^2}}\,dx = -\sqrt{1-x^2} ∫arcsin⁡x dx=xarcsin⁡x+1−x2+C\boxed{\int \arcsin x\,dx = x\arcsin x + \sqrt{1-x^2} + C}
flowchart TD
A[04 Further Calculus] --> B[Key Concepts]
A --> C[Core Principles]
A --> D[Practical Applications]
B --> E[Fundamental definitions]
C --> F[Design patterns]
D --> G[Real-world usage]

Integration by parts is the reverse of the product rule, allowing you to transfer derivatives between functions. Think of it as a negotiation: you give away one function’s derivative in exchange for integrating the other. Reduction formulae create a staircase where each integral is expressed in terms of a simpler one, allowing you to climb down to a base case you can evaluate directly. Inverse trigonometric functions arise because their derivatives produce rational functions, creating a bridge between algebraic and trigonometric integration. Volumes of revolution are computed by summing infinitesimally thin discs stacked along an axis, like building a solid from a stack of coins. Arc length measures the actual distance along a curve rather than straight-line approximation.


PitfallCorrect Approach
Forgetting the chain rule when differentiating composite inverse trig functionsAlways write ddx ⁣[arcsin⁡(u)]=u′1−u2\dfrac{d}{dx}\!\left[\arcsin(u)\right] = \dfrac{u'}{\sqrt{1-u^2}}
Using ln⁡∥x∥\ln \| x \| before checking if the integral is improperCheck for discontinuities in the interval first
Forgetting +C+C on every antiderivativeEvery indefinite integral needs an arbitrary constant
Applying reduction formulae without checking the base caseAlways state I0I_0 or I1I_1 explicitly
Confusing dnydxn\dfrac{d^n y}{dx^n} notation with (dydx)n\left(\dfrac{dy}{dx}\right)^ndnydxn\dfrac{d^n y}{dx^n} is the nn-th derivative, not the nn-th power

Using the substitution u=exu = e^x Find ∫exe2x+1 dx\displaystyle\int \frac{e^x}{e^{2x} + 1}\,dx.

Solution

u=exu = e^x, du=ex dxdu = e^x\,dx.

∫duu2+1=arctan⁡u+C=arctan⁡(ex)+C\int \frac{du}{u^2 + 1} = \arctan u + C = \boxed{\arctan(e^x) + C}

The reduction formula In=∫0π/4tan⁡nx dxI_n = \displaystyle\int_0^{\pi/4} \tan^n x\,dx satisfies In=1n−1−In−2I_n = \dfrac{1}{n-1} - I_{n-2} for n≥2n \geq 2. Given I0=π4I_0 = \dfrac{\pi}{4} and I1=12ln⁡2I_1 = \dfrac{1}{2}\ln 2 Find I3I_3.

Solution

I3=12−I1=12−12ln⁡2=12(1−ln⁡2)I_3 = \dfrac{1}{2} - I_1 = \dfrac{1}{2} - \dfrac{1}{2}\ln 2 = \dfrac{1}{2}(1 - \ln 2).

To verify: I2=11−I0=1−π4I_2 = \dfrac{1}{1} - I_0 = 1 - \dfrac{\pi}{4}. Then I3=12−I1=12−12ln⁡2I_3 = \dfrac{1}{2} - I_1 = \dfrac{1}{2} - \dfrac{1}{2}\ln 2. Consistent. I3=12(1−ln⁡2)\boxed{I_3 = \dfrac{1}{2}(1 - \ln 2)}

Find the area enclosed by the curve x=t2x = t^2, y=t3−ty = t^3 - t for −1≤t≤1-1 \leq t \leq 1.

Solution

Using the parametric area formula A=∫y dxdt dtA = \displaystyle\int y\,\frac{dx}{dt}\,dt:

A=∫−11(t3−t)(2t) dt=2∫−11(t4−t2) dt=2[t55−t33]−11A = \int_{-1}^{1} (t^3 - t)(2t)\,dt = 2\int_{-1}^{1} (t^4 - t^2)\,dt = 2\left[\frac{t^5}{5} - \frac{t^3}{3}\right]_{-1}^{1}

Since t5−53t3t^5 - \frac{5}{3}t^3 is odd (each term is odd), the integral from −1-1 to 11 is zero.

A=0\boxed{A = 0} (the curve traces back over itself symmetrically).

Prove that ddx ⁣[arctan⁡x]=11+x2\dfrac{d}{dx}\!\left[\arctan x\right] = \dfrac{1}{1+x^2} from first principles Using implicit differentiation.

Solution

Let y=arctan⁡xy = \arctan x So x=tan⁡yx = \tan y. Differentiating implicitly with respect to xx:

1=sec⁡2y⋅dydx1 = \sec^2 y \cdot \frac{dy}{dx} dydx=cos⁡2y=1sec⁡2y=11+tan⁡2y=11+x2\frac{dy}{dx} = \cos^2 y = \frac{1}{\sec^2 y} = \frac{1}{1 + \tan^2 y} = \frac{1}{1 + x^2}

■\blacksquare

Evaluate ∫01ln⁡x1+x dx\displaystyle\int_0^1 \frac{\ln x}{1+x}\,dx Expressing your answer in terms Of ∑n=1∞(−1)n+1n2\displaystyle\sum_{n=1}^{\infty} \frac{(-1)^{n+1}}{n^2}.

Solution

Expand 11+x=∑n=0∞(−1)nxn\dfrac{1}{1+x} = \displaystyle\sum_{n=0}^{\infty} (-1)^n x^n for ∣x∣<1|x| < 1:

∫01ln⁡x∑n=0∞(−1)nxn dx=∑n=0∞(−1)n∫01xnln⁡x dx\int_0^1 \ln x \sum_{n=0}^{\infty} (-1)^n x^n\,dx = \sum_{n=0}^{\infty} (-1)^n \int_0^1 x^n \ln x\,dx

Using integration by parts or the standard result ∫01xnln⁡x dx=−1(n+1)2\displaystyle\int_0^1 x^n \ln x\,dx = -\frac{1}{(n+1)^2}:

=−∑n=0∞(−1)n(n+1)2=−∑n=1∞(−1)n−1n2=∑n=1∞(−1)nn2= -\sum_{n=0}^{\infty} \frac{(-1)^n}{(n+1)^2} = -\sum_{n=1}^{\infty} \frac{(-1)^{n-1}}{n^2} = \sum_{n=1}^{\infty} \frac{(-1)^n}{n^2}

This equals −π212-\dfrac{\pi^2}{12}.


11.1 Further calculus and differential equations

Section titled “11.1 Further calculus and differential equations”

Integration techniques (substitution, parts, partial fractions) are essential tools for solving Differential equations. See Differential Equations.

Taylor and Maclaurin expansions provide powerful tools for evaluating integrals that cannot be found in closed form. See Maclaurin and Taylor Series.

Arc length and area calculations are used extensively in mechanics for work-energy problems. See Circular Motion.

The inverse hyperbolic functions arise from integration: ∫dxx2+a2=arsinh⁡(x/a)+C\displaystyle\int \frac{dx}{\sqrt{x^2+a^2}} = \operatorname{arsinh}(x/a) + C. See Hyperbolic Functions.


When choosing uu and dvdv for integration by parts, use the LIATE priority:

  • Logarithmic functions
  • Inverse trigonometric functions
  • Algebraic functions (polynomials)
  • Trigonometric functions
  • Exponential functions

The function higher on the list should be chosen as uu.

For integrals involving rational functions of sin⁡x\sin x and cos⁡x\cos x The substitution t=tan⁡(x/2)t = \tan(x/2) converts them to rational functions of tt:

\sin x = \dfrac{2t}{1+t^2}$$\cos x = \dfrac{1-t^2}{1+t^2}$$dx = \dfrac{2\,dt}{1+t^2}.

FormResult
∫f′(x)f(x) dx\displaystyle\int \frac{f'(x)}{f(x)}\,dxln⁡∥f(x)∥+C\ln \| f(x) \| + C
∫f′(x)f(x) dx\displaystyle\int \frac{f'(x)}{\sqrt{f(x)}}\,dx2f(x)+C2\sqrt{f(x)} + C
∫f(x)⋅f′(x) dx\displaystyle\int f(x) \cdot f'(x)\,dx[f(x)]22+C\dfrac{[f(x)]^2}{2} + C

ResultFormula
Integration by parts∫u dv=uv−∫v du\displaystyle\int u\,dv = uv - \int v\,du
Reduction formula (by parts)Express InI_n in terms of In−1I_{n-1} or In−2I_{n-2}
Arc length (Cartesian)s=∫ab1+(dydx)2 dxs = \displaystyle\int_a^b \sqrt{1+\left(\frac{dy}{dx}\right)^2}\,dx
Arc length (parametric)s=∫αβx˙2+y˙2 dts = \displaystyle\int_\alpha^\beta \sqrt{\dot{x}^2+\dot{y}^2}\,dt
Area under parametric curveA=∫ydxdt dtA = \displaystyle\int y\frac{dx}{dt}\,dt
Surface of revolutionS=2π∫aby1+(y′)2 dxS = 2\pi\displaystyle\int_a^b y\sqrt{1+(y')^2}\,dx
Derivative of arcsin⁡x\arcsin x11−x2\dfrac{1}{\sqrt{1-x^2}}
Derivative of arctan⁡x\arctan x11+x2\dfrac{1}{1+x^2}
Improper integral test∫a∞f(x) dx=lim⁡b→∞∫abf(x) dx\displaystyle\int_a^\infty f(x)\,dx = \lim_{b\to\infty}\int_a^b f(x)\,dx

Using integration by parts, evaluate ∫x3e−x dx\displaystyle\int x^3 e^{-x}\,dx.

Solution

Let u = x^3$$dv = e^{-x}\,dx. du = 3x^2\,dx$$v = -e^{-x}.

∫x3e−x dx=−x3e−x+3∫x2e−x dx\int x^3 e^{-x}\,dx = -x^3 e^{-x} + 3\int x^2 e^{-x}\,dx.

Repeating: ∫x2e−x dx=−x2e−x+2∫xe−x dx=−x2e−x−2xe−x+2∫e−x dx\int x^2 e^{-x}\,dx = -x^2 e^{-x} + 2\int xe^{-x}\,dx = -x^2 e^{-x} - 2xe^{-x} + 2\int e^{-x}\,dx.

=−x2e−x−2xe−x−2e−x= -x^2 e^{-x} - 2xe^{-x} - 2e^{-x}.

Therefore: ∫x3e−x dx=−x3e−x−3x2e−x−6xe−x−6e−x+C\int x^3 e^{-x}\,dx = -x^3 e^{-x} - 3x^2 e^{-x} - 6xe^{-x} - 6e^{-x} + C.

=−e−x(x3+3x2+6x+6)+C\boxed{= -e^{-x}(x^3 + 3x^2 + 6x + 6) + C}

Find the arc length of the curve y=ln⁡(cos⁡x)y = \ln(\cos x) from x=0x = 0 to x=π/4x = \pi/4.

Solution

y′=−tan⁡xy' = -\tan x. 1+(y′)2=1+tan⁡2x=sec⁡2x1 + (y')^2 = 1 + \tan^2 x = \sec^2 x.

s=∫0π/4sec⁡x dx=[ln⁡∣sec⁡x+tan⁡x∣]0π/4=ln⁡(2+1)−ln⁡(1)=ln⁡(2+1)s = \displaystyle\int_0^{\pi/4} \sec x\,dx = [\ln|\sec x + \tan x|]_0^{\pi/4} = \ln(\sqrt{2}+1) - \ln(1) = \boxed{\ln(\sqrt{2}+1)}.

Prove that ∫0π/2sin⁡nx dx=n−1n⋅n−3n−2⋯×{1n oddπ2n even\displaystyle\int_0^{\pi/2} \sin^n x\,dx = \dfrac{n-1}{n} \cdot \dfrac{n-3}{n-2} \cdots \times \begin{cases} 1 & n \text{ odd} \\ \dfrac{\pi}{2} & n \text{ even}\end{cases} (Wallis’ formula).

Solution

Let In=∫0π/2sin⁡nx dxI_n = \displaystyle\int_0^{\pi/2} \sin^n x\,dx.

Integration by parts with u = \sin^{n-1}x$$dv = \sin x\,dx:

In=[−cos⁡xsin⁡n−1x]0π/2+(n−1)∫0π/2cos⁡2xsin⁡n−2x dxI_n = [-\cos x \sin^{n-1}x]_0^{\pi/2} + (n-1)\displaystyle\int_0^{\pi/2} \cos^2 x \sin^{n-2}x\,dx

=0+(n−1)∫0π/2(1−sin⁡2x)sin⁡n−2x dx=(n−1)(In−2−In)= 0 + (n-1)\displaystyle\int_0^{\pi/2} (1-\sin^2 x)\sin^{n-2}x\,dx = (n-1)(I_{n-2} - I_n).

nIn=(n−1)In−2nI_n = (n-1)I_{n-2} So In=n−1nIn−2\boxed{I_n = \dfrac{n-1}{n}I_{n-2}}.

Base cases: I_0 = \pi/2$$I_1 = 1.

For even nn: In=n−1n⋅n−3n−2⋯12⋅π2I_n = \dfrac{n-1}{n} \cdot \dfrac{n-3}{n-2} \cdots \dfrac{1}{2} \cdot \dfrac{\pi}{2}.

For odd nn: In=n−1n⋅n−3n−2⋯23⋅1I_n = \dfrac{n-1}{n} \cdot \dfrac{n-3}{n-2} \cdots \dfrac{2}{3} \cdot 1. ■\blacksquare


The gamma function extends the factorial: Γ(n)=(n−1)!\Gamma(n) = (n-1)! for positive integers, and Γ(x)=∫0∞tx−1e−t dt\Gamma(x) = \displaystyle\int_0^{\infty} t^{x-1}e^{-t}\,dt for x>0x > 0.

Wallis’ formula leads to the important result: Γ(1/2)=π\Gamma(1/2) = \sqrt{\pi}.

For suitable functions ff: ∫0∞f(ax)−f(bx)x dx=(f(0)−f(∞))ln⁡ba\displaystyle\int_0^{\infty} \frac{f(ax)-f(bx)}{x}\,dx = (f(0)-f(\infty))\ln\frac{b}{a}.

Example: ∫0∞e−ax−e−bxx dx=ln⁡ba\displaystyle\int_0^{\infty} \frac{e^{-ax}-e^{-bx}}{x}\,dx = \ln\frac{b}{a}.

15.3 Differentiation under the integral sign

Section titled “15.3 Differentiation under the integral sign”

Leibniz’s rule: ddα∫abf(x,α) dx=∫ab∂f∂α dx\dfrac{d}{d\alpha}\displaystyle\int_a^b f(x,\alpha)\,dx = \int_a^b \frac{\partial f}{\partial\alpha}\,dx.

This is a powerful technique for evaluating integrals that depend on a parameter.

If 0≤f(x)≤g(x)0 \leq f(x) \leq g(x) for x≥ax \geq a and ∫a∞g(x) dx\displaystyle\int_a^{\infty} g(x)\,dx converges, Then ∫a∞f(x) dx\displaystyle\int_a^{\infty} f(x)\,dx also converges.


Evaluate ∫0∞xe−x dx\displaystyle\int_0^{\infty} xe^{-x}\,dx and relate it to the mean of the exponential Distribution.

Solution

Integration by parts with u = x$$dv = e^{-x}\,dx:

=[−xe−x]0∞+∫0∞e−x dx=0+1=1= [-xe^{-x}]_0^{\infty} + \displaystyle\int_0^{\infty} e^{-x}\,dx = 0 + 1 = \boxed{1}.

This equals E(X)E(X) for X∼Exp(1)X \sim \mathrm{Exp}(1) Confirming the result E(X)=1/λE(X) = 1/\lambda with λ=1\lambda = 1.

Prove that ∫0π/2sin⁡2xcos⁡2x dx=π16\displaystyle\int_0^{\pi/2} \sin^2 x\cos^2 x\,dx = \frac{\pi}{16}.

Solution

sin⁡2xcos⁡2x=sin⁡22x4=1−cos⁡4x8\sin^2 x\cos^2 x = \dfrac{\sin^2 2x}{4} = \dfrac{1-\cos 4x}{8}.

∫0π/21−cos⁡4x8 dx=18 ⁣[x−sin⁡4x4]0π/2=18⋅π2=π16\displaystyle\int_0^{\pi/2} \frac{1-\cos 4x}{8}\,dx = \frac{1}{8}\!\left[x-\frac{\sin 4x}{4}\right]_0^{\pi/2} = \frac{1}{8}\cdot\frac{\pi}{2} = \boxed{\dfrac{\pi}{16}}. ■\blacksquare

Use integration by parts twice to evaluate ∫excos⁡x dx\displaystyle\int e^x\cos x\,dx.

Solution

I=∫excos⁡x dx=exsin⁡x−∫exsin⁡x dx=exsin⁡x−(−excos⁡x+∫excos⁡x dx)I = \displaystyle\int e^x\cos x\,dx = e^x\sin x - \int e^x\sin x\,dx = e^x\sin x - (-e^x\cos x + \int e^x\cos x\,dx).

I=exsin⁡x+excos⁡x−II = e^x\sin x + e^x\cos x - I.

2I=ex(sin⁡x+cos⁡x)2I = e^x(\sin x+\cos x).

I=ex(sin⁡x+cos⁡x)2+C\boxed{I = \dfrac{e^x(\sin x+\cos x)}{2} + C}


Evaluate ∫01x31+x2 dx\displaystyle\int_0^1 \frac{x^3}{1+x^2}\,dx.

Solution

Let u = 1+x^2$$du = 2x\,dx. Note x2=u−1x^2 = u-1 So x3 dx=x2⋅x dx=(u−1)⋅du2x^3\,dx = x^2 \cdot x\,dx = (u-1)\cdot\dfrac{du}{2}.

∫01x31+x2 dx=12∫12u−1u du=12∫12 ⁣(1−1u)du\displaystyle\int_0^1 \frac{x^3}{1+x^2}\,dx = \frac{1}{2}\int_1^2 \frac{u-1}{u}\,du = \frac{1}{2}\int_1^2 \!\left(1-\frac{1}{u}\right)du

=12[u−ln⁡u]12=12(2−ln⁡2−1)=12(1−ln⁡2)= \frac{1}{2}\Big[u-\ln u\Big]_1^2 = \frac{1}{2}(2-\ln 2 - 1) = \boxed{\frac{1}{2}(1-\ln 2)}.

Prove that the function F(x)=∫0xdt1+t4F(x) = \displaystyle\int_0^x \frac{dt}{1+t^4} is increasing and Bounded above.

Solution

F′(x)=11+x4>0F'(x) = \dfrac{1}{1+x^4} > 0 for all x≥0x \geq 0 So FF is strictly increasing. ✓

F(x)<F(∞)=∫0∞dt1+t4<∫0∞dt1+t2=π2F(x) < F(\infty) = \displaystyle\int_0^{\infty} \frac{dt}{1+t^4} < \int_0^{\infty} \frac{dt}{1+t^2} = \frac{\pi}{2}. ✓

Therefore FF is increasing and bounded above by π/2\pi/2. ■\blacksquare