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Integration techniques and applications - TCE Mathematics Specialised (Tasmania)

Syllabus dot point

“Integrate using substitution, integration by parts and partial fractions, and find volumes of revolution.”

TCESpecialist MathematicsUnit 49 min read

Quick answer

Choose the right tool for the integral: substitution reverses the chain rule, integration by parts reverses the product rule, and partial fractions break a rational function into simple pieces. Volumes of revolution use V=π∫y2 dxV = \pi\int y^2 \, dx.

What this dot point is asking

Basic antiderivatives only cover a handful of forms. Specialised integration is about recognising structure and applying the matching technique.

Substitution

Substitution reverses the chain rule. If part of the integrand is the derivative of another part, let uu be the inner function. With u=g(x)u = g(x) and du=g′(x) dxdu = g'(x)\,dx,

∫f(g(x)) g′(x) dx=∫f(u) du. \int f(g(x))\, g'(x)\, dx = \int f(u)\, du.

For a definite integral, change the limits to values of uu rather than substituting back.

Integration by parts

Integration by parts reverses the product rule:

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

Choose uu to be the factor that becomes simpler when differentiated. A useful priority for picking uu is logarithms, then inverse trigonometric functions, then algebraic, then trigonometric, then exponential.

Integration by parts

Evaluate ∫xex dx\displaystyle \int x e^{x}\, dx.

Step 1: Choose uu and dvdx\dfrac{dv}{dx}

Integration by parts requires choosing which factor to call uu and which to call dvdx\dfrac{dv}{dx}. We want uu to become simpler when differentiated. Here u=xu = x is algebraic and differentiates to 11, while exe^x is easy to integrate. This is the natural split:

u=x,dudx=1,dvdx=ex,v=ex. u = x, \quad \frac{du}{dx} = 1, \qquad \frac{dv}{dx} = e^{x}, \quad v = e^{x}.

Step 2: Apply the integration by parts formula

The formula ∫u dvdx dx=uv−∫v dudx dx\displaystyle\int u\,\frac{dv}{dx}\,dx = uv - \int v\,\frac{du}{dx}\,dx gives:

∫xex dx=xex−∫ex⋅1 dx=xex−ex+C=ex(x−1)+C. \int x e^{x}\, dx = x e^{x} - \int e^{x}\cdot 1\, dx = x e^{x} - e^{x} + C = e^{x}(x - 1) + C.

Step 3: Verify by differentiating

Differentiating the result using the product rule confirms correctness: ddx(ex(x−1))=ex(x−1)+ex=xex\tfrac{d}{dx}\big(e^{x}(x-1)\big) = e^{x}(x-1) + e^{x} = x e^{x}.

Final answer: ∫xex dx=ex(x−1)+C\displaystyle\int x e^{x}\, dx = e^{x}(x - 1) + C.

Partial fractions

A proper rational function with a factorised denominator can be split into simpler fractions. For distinct linear factors,

P(x)(x−a)(x−b)=Ax−a+Bx−b, \frac{P(x)}{(x - a)(x - b)} = \frac{A}{x - a} + \frac{B}{x - b},

and each piece integrates to a logarithm.

Partial fractions

Evaluate ∫5x−1(x−1)(x+2) dx\displaystyle \int \frac{5x - 1}{(x - 1)(x + 2)}\, dx.

Step 1: Set up the partial fraction decomposition

Because the denominator has two distinct linear factors, we can write the integrand as a sum of two simpler fractions. We assume:

5x−1(x−1)(x+2)=Ax−1+Bx+2. \frac{5x - 1}{(x-1)(x+2)} = \frac{A}{x-1} + \frac{B}{x+2}.

Multiplying both sides by (x−1)(x+2)(x-1)(x+2) clears the denominators:

5x−1=A(x+2)+B(x−1). 5x - 1 = A(x + 2) + B(x - 1).

Step 2: Find AA and BB by substituting convenient values

Choosing values of xx that zero out one factor at a time is the quickest method. Set x=1x = 1: 5(1)−1=A(3)5(1) - 1 = A(3), so A=43A = \tfrac{4}{3}. Set x=−2x = -2: 5(−2)−1=B(−3)5(-2) - 1 = B(-3), so B=113B = \tfrac{11}{3}.

Step 3: Integrate each partial fraction

Each piece integrates to a logarithm:

∫5x−1(x−1)(x+2) dx=43ln⁡∣x−1∣+113ln⁡∣x+2∣+C. \int \frac{5x - 1}{(x-1)(x+2)}\, dx = \frac{4}{3}\ln|x - 1| + \frac{11}{3}\ln|x + 2| + C.

Final answer: 43ln⁡∣x−1∣+113ln⁡∣x+2∣+C\dfrac{4}{3}\ln|x - 1| + \dfrac{11}{3}\ln|x + 2| + C.

Volumes of revolution

When the region under y=f(x)y = f(x) between x=ax = a and x=bx = b is rotated about the xx axis, the solid formed has volume

V=π∫aby2 dx=π∫ab(f(x))2 dx. V = \pi \int_a^b y^2 \, dx = \pi \int_a^b \big(f(x)\big)^2 \, dx.

Rotation about the yy axis gives V=π∫cdx2 dyV = \pi\int_c^d x^2 \, dy.

Volume of revolution

The region under y=xy = \sqrt{x} from x=0x = 0 to x=4x = 4 is rotated about the xx-axis. Find the volume.

Step 1: Write down the volume formula

When a region is rotated about the xx-axis, each thin vertical strip sweeps out a disc of radius y=f(x)y = f(x) and thickness dxdx. Summing these discs gives:

V=π∫ab(f(x))2 dx. V = \pi \int_a^b \big(f(x)\big)^2 \, dx.

Step 2: Substitute and simplify the integrand

With f(x)=xf(x) = \sqrt{x}, squaring removes the square root:

V=π∫04(x)2 dx=π∫04x dx. V = \pi \int_0^4 \big(\sqrt{x}\big)^2 \, dx = \pi \int_0^4 x \, dx.

Step 3: Evaluate the definite integral

π∫04x dx=π[x22]04=π⋅162=8π. \pi \int_0^4 x \, dx = \pi \left[\frac{x^2}{2}\right]_0^4 = \pi\cdot\frac{16}{2} = 8\pi.

Final answer: V=8πV = 8\pi cubic units.

Partial fractions with repeated and quadratic factors

The split depends on the denominator's factor types. A repeated linear factor needs one term per power, and an irreducible quadratic factor needs a linear numerator:

P(x)(x−a)2=Ax−a+B(x−a)2,P(x)(x−a)(x2+c)=Ax−a+Bx+Cx2+c. \frac{P(x)}{(x - a)^2} = \frac{A}{x - a} + \frac{B}{(x - a)^2}, \qquad \frac{P(x)}{(x - a)(x^2 + c)} = \frac{A}{x - a} + \frac{Bx + C}{x^2 + c}.

Always reduce an improper fraction (numerator degree at least the denominator degree) by polynomial division first; partial fractions only apply to a proper fraction.

Integration using trigonometric identities

Powers of sin⁡\sin and cos⁡\cos are integrated by first reducing the power with an identity. For even powers use the double-angle forms sin⁡2θ=1−cos⁡2θ2\sin^2\theta = \dfrac{1 - \cos 2\theta}{2} and cos⁡2θ=1+cos⁡2θ2\cos^2\theta = \dfrac{1 + \cos 2\theta}{2}; for odd powers peel off one factor and convert the rest with sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1, then substitute.

Integrating an even power of cosine

Evaluate ∫0π/2cos⁡2x dx\displaystyle\int_0^{\pi/2} \cos^2 x\,dx.

Step 1: Use the double-angle identity to reduce the power

cos⁡2x\cos^2 x cannot be integrated directly in its current form. The double-angle identity cos⁡2x=1+cos⁡2x2\cos^2 x = \dfrac{1 + \cos 2x}{2} rewrites the integrand as a sum of an easy constant and a cosine with a doubled argument:

∫0π/2cos⁡2x dx=12∫0π/2(1+cos⁡2x) dx. \int_0^{\pi/2}\cos^2 x\,dx = \frac{1}{2}\int_0^{\pi/2}(1 + \cos 2x)\,dx.

Step 2: Integrate term by term

Both terms are straightforward: 11 integrates to xx, and cos⁡2x\cos 2x integrates to sin⁡2x2\dfrac{\sin 2x}{2}:

=12[x+sin⁡2x2]0π/2. = \frac{1}{2}\left[x + \frac{\sin 2x}{2}\right]_0^{\pi/2}.

Step 3: Evaluate at the limits

At x=π2x = \dfrac{\pi}{2}: the bracket gives π2+sin⁡π2=π2+0=π2\dfrac{\pi}{2} + \dfrac{\sin\pi}{2} = \dfrac{\pi}{2} + 0 = \dfrac{\pi}{2}. At x=0x = 0: the bracket gives 0+0=00 + 0 = 0. So the integral is 12⋅π2=π4\dfrac{1}{2}\cdot\dfrac{\pi}{2} = \dfrac{\pi}{4}.

Final answer: ∫0π/2cos⁡2x dx=π4\displaystyle\int_0^{\pi/2} \cos^2 x\,dx = \dfrac{\pi}{4}.

Inverse-trigonometric standard forms

Two integrals appear constantly and should be recognised on sight:

∫dxa2−x2=arcsin⁡xa+C,∫dxa2+x2=1aarctan⁡xa+C. \int \frac{dx}{\sqrt{a^2 - x^2}} = \arcsin\frac{x}{a} + C, \qquad \int \frac{dx}{a^2 + x^2} = \frac{1}{a}\arctan\frac{x}{a} + C.

Spotting an a2−x2a^2 - x^2 under a square root, or an a2+x2a^2 + x^2 in a denominator, signals one of these forms (or a trigonometric substitution x=asin⁡θx = a\sin\theta or x=atan⁡θx = a\tan\theta).

Forgetting to change the limits after substitution

With a definite integral and substitution u=g(x)u = g(x), the limits are values of xx, not uu. Either change them to u=g(a)u = g(a) and u=g(b)u = g(b), or substitute back to xx before applying the original limits. Plugging xx limits into a uu expression gives a wrong answer. The same care applies to the squared integrand in volumes: it is π∫y2 dx\pi\int y^2\,dx, not π∫y dx\pi\int y\,dx or (π∫y dx)2(\pi\int y\,dx)^2.

Why this matters

The integration toolkit (substitution, parts, partial fractions and the trigonometric and inverse-trigonometric standard forms) is the engine behind volumes of revolution and the solution of differential equations. Recognising which technique a given integrand calls for is the skill TASC tests most often, so practise classifying an integral before you start computing.

Exam-style questions

Questions in the style of TASC exam questions on this dot point, each with a worked answer. They are written by ExamExplained unless tagged "Past paper"; the year shows the paper a question is modelled on.

Practice5 marks
Use the substitution u=xu = \sqrt{x} to evaluate ∫49dx1+x\displaystyle\int_4^9 \dfrac{dx}{1 + \sqrt{x}}.
Show worked answer →

Let u=xu = \sqrt{x}, so x=u2x = u^2 and dx=2u dudx = 2u\,du. Change the limits: when x=4x = 4, u=2u = 2; when x=9x = 9, u=3u = 3.

The integral becomes ∫232u1+u du\displaystyle\int_2^3 \dfrac{2u}{1 + u}\,du.

Rewrite the integrand by division: u1+u=1−11+u\dfrac{u}{1 + u} = 1 - \dfrac{1}{1 + u}. So the integral is 2∫23[1−11+u]du=2[u−ln⁡(1+u)]232\displaystyle\int_2^3\left[1 - \dfrac{1}{1 + u}\right]du = 2\Big[u - \ln(1 + u)\Big]_2^3.

Evaluate: 2[(3−ln⁡4)−(2−ln⁡3)]=2[1−ln⁡4+ln⁡3]=2−2ln⁡432\big[(3 - \ln 4) - (2 - \ln 3)\big] = 2\big[1 - \ln 4 + \ln 3\big] = 2 - 2\ln\dfrac{4}{3}. Markers reward changing the limits with the substitution and the algebraic division before integrating.

Practice6 marks
Determine ∫e−xsin⁡(2x) dx\displaystyle\int e^{-x}\sin(2x)\,dx.
Show worked answer →

Use integration by parts twice. Let I=∫e−xsin⁡(2x) dxI = \displaystyle\int e^{-x}\sin(2x)\,dx.

First parts: take u=sin⁡(2x)u = \sin(2x), dv=e−x dxdv = e^{-x}\,dx, so I=−e−xsin⁡(2x)+2∫e−xcos⁡(2x) dxI = -e^{-x}\sin(2x) + 2\displaystyle\int e^{-x}\cos(2x)\,dx.

Second parts on the remaining integral: take u=cos⁡(2x)u = \cos(2x), dv=e−x dxdv = e^{-x}\,dx, giving ∫e−xcos⁡(2x) dx=−e−xcos⁡(2x)−2I\displaystyle\int e^{-x}\cos(2x)\,dx = -e^{-x}\cos(2x) - 2I.

Substitute back: I=−e−xsin⁡(2x)+2[−e−xcos⁡(2x)−2I]=−e−xsin⁡(2x)−2e−xcos⁡(2x)−4II = -e^{-x}\sin(2x) + 2\big[-e^{-x}\cos(2x) - 2I\big] = -e^{-x}\sin(2x) - 2e^{-x}\cos(2x) - 4I.

So 5I=−e−x(sin⁡(2x)+2cos⁡(2x))5I = -e^{-x}\big(\sin(2x) + 2\cos(2x)\big), giving I=−15e−x(sin⁡(2x)+2cos⁡(2x))+CI = -\dfrac{1}{5}e^{-x}\big(\sin(2x) + 2\cos(2x)\big) + C. Markers reward applying parts twice and solving the resulting equation for II.

Practice5 marks
The area bounded by the curves y=x(4−x)y = x(4 - x) and y=2x(4−x)y = 2x(4 - x) is rotated completely about the xx-axis. Find the volume of the solid of revolution formed.
Show worked answer →

Both curves pass through x=0x = 0 and x=4x = 4, and for 0<x<40 < x < 4 the outer curve is y=2x(4−x)y = 2x(4 - x) and the inner is y=x(4−x)y = x(4 - x).

The volume by the washer method is V=π∫04[(2x(4−x))2−(x(4−x))2]dx=π∫043[x(4−x)]2 dxV = \pi\displaystyle\int_0^4\Big[\big(2x(4 - x)\big)^2 - \big(x(4 - x)\big)^2\Big]dx = \pi\displaystyle\int_0^4 3\big[x(4 - x)\big]^2\,dx.

Expand: [x(4−x)]2=x2(16−8x+x2)=16x2−8x3+x4\big[x(4 - x)\big]^2 = x^2(16 - 8x + x^2) = 16x^2 - 8x^3 + x^4. Integrate from 00 to 44: 16⋅643−8⋅64+10245=10243−512+10245=5121516\cdot\dfrac{64}{3} - 8\cdot 64 + \dfrac{1024}{5} = \dfrac{1024}{3} - 512 + \dfrac{1024}{5} = \dfrac{512}{15}.

So V=3π⋅51215=512π5V = 3\pi\cdot\dfrac{512}{15} = \dfrac{512\pi}{5}. Markers reward the difference of squares of the outer and inner radii, correct expansion, and the final volume.

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