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Integration techniques: antiderivatives, substitution, definite integrals and the FTC

Syllabus dot point

“Find antiderivatives of standard functions, apply integration by substitution and evaluate definite integrals using the Fundamental Theorem of Calculus”

HSCMaths AdvancedYear 12: Calculus16 min read

Quick answer

Integration finds antiderivatives, the substitution rule reverses the chain rule, and the Fundamental Theorem of Calculus evaluates a definite integral as the change of any antiderivative across the interval.

Jump to a section
  1. What this dot point is asking
  2. The answer
  3. Exam-style questions
  4. Practice questions

What this dot point is asking

NESA wants you to find antiderivatives of standard functions, apply the reverse chain rule via substitution, and evaluate definite integrals using the Fundamental Theorem of Calculus (FTC). Integration underlies areas, volumes, motion problems and growth models.

Note

Differentiating tells you how fast something is changing; integrating runs the film backwards, adding up all those tiny changes to recover the total. Picture a car's speedometer: if you know how fast the car is going at every instant, integrating that speed over a trip gives the total distance travelled, because you are summing up all the little bits of distance covered second by second. Antiderivatives are just "what function had this rate of change?", so integrating is undoing a derivative. The Fundamental Theorem of Calculus is the shortcut that saves you from adding up millions of thin slices by hand: find the total-so-far function, read it at the start and the end, and subtract. A definite integral is really the area trapped between a curve and the horizontal axis, where anything below the axis counts as a negative amount.

The answer

Standard antiderivatives

Memorise these. The constant CC is omitted in definite integrals.

∫xn dx=xn+1n+1+C(n≠−1)\int x^n \, dx = \frac{x^{n + 1}}{n + 1} + C \quad (n \neq -1)

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

∫ex dx=ex+C,∫ekx dx=ekxk+C\int e^x \, dx = e^x + C, \qquad \int e^{kx} \, dx = \frac{e^{kx}}{k} + C

∫sin⁡x dx=−cos⁡x+C,∫cos⁡x dx=sin⁡x+C\int \sin x \, dx = -\cos x + C, \qquad \int \cos x \, dx = \sin x + C

∫sec⁡2x dx=tan⁡x+C\int \sec^2 x \, dx = \tan x + C

Linear inside argument

If the argument is linear, divide by the coefficient.

∫sin⁡(kx) dx=−1kcos⁡(kx)+C\int \sin(k x) \, dx = -\frac{1}{k} \cos(k x) + C

∫(ax+b)n dx=(ax+b)n+1a(n+1)+C(n≠−1)\int (a x + b)^n \, dx = \frac{(a x + b)^{n + 1}}{a (n + 1)} + C \quad (n \neq -1)

Integration by substitution

The substitution rule reverses the chain rule. To evaluate ∫f(g(x))g′(x) dx\int f(g(x)) g'(x) \, dx, set u=g(x)u = g(x), so du=g′(x) dxdu = g'(x) \, dx. The integral becomes ∫f(u) du\int f(u) \, du, which you evaluate, then substitute back.

For a definite integral, you can either substitute back to xx and use the original limits, or change the limits to values of uu and skip the back-substitution.

The Fundamental Theorem of Calculus

If FF is any antiderivative of ff (so F′(x)=f(x)F'(x) = f(x)), then

∫abf(x) dx=F(b)−F(a).\int_a^b f(x) \, dx = F(b) - F(a).

The word any is the part textbooks rush past, and it is what makes the theorem usable. Two antiderivatives of the same function differ only by a constant, and that constant cancels in F(b)−F(a)F(b) - F(a), so you never need the "right" antiderivative, just a convenient one, and you never need the +C+ C for a definite integral. Notice too what the theorem buys you: an integral is defined as a limit of sums of thin strips, an object that looks impossible to compute, yet the FTC says you can get it exactly by evaluating a single function at two points. That shortcut is the whole reason calculus is practical.

A second statement: the function G(x)=∫axf(t) dtG(x) = \int_a^x f(t) \, dt, the "area so far" as the upper limit slides, satisfies G′(x)=f(x)G'(x) = f(x). In short, differentiation and integration are inverse operations: integrating then differentiating gets you back where you started.

Key fact

The Fundamental Theorem of Calculus says ∫abf(x) dx=F(b)−F(a)\int_a^b f(x)\,dx = F(b) - F(a) for any antiderivative FF of ff. Evaluate the antiderivative at the top limit, subtract its value at the bottom limit. The lay-out markers want is [F(x)]ab=F(b)−F(a)[F(x)]_a^b = F(b) - F(a), with the antiderivative shown explicitly inside the square brackets before you substitute.

Choosing a substitution

The whole skill of substitution is recognising that the integrand contains a function and (a multiple of) its derivative. Scan the integrand for an inner function u=g(x)u = g(x) whose derivative g′(x)g'(x) also appears, possibly up to a constant factor. Good signals include a power of a bracket multiplied by the bracket's derivative, a function inside a root, or a fraction whose numerator is the derivative of the denominator. If no such pair appears, substitution will not help and you should look for a standard form instead.

A clean substitution layout, written out in full, is what markers reward: state u=g(x)u = g(x), compute dudx\frac{du}{dx}, rearrange to replace dxdx, rewrite the entire integral in terms of uu (including the limits for a definite integral), integrate, and either substitute back or evaluate the uu-limits.

The definite integral as signed area

Geometrically, ∫abf(x) dx\int_a^b f(x)\,dx is the signed area between the curve and the xx-axis: regions above the axis count positive, regions below count negative. This is why a definite integral can be zero even when the curve is non-zero, as when an odd function is integrated over a symmetric interval. To find a genuine geometric area where the curve crosses the axis, split the integral at the crossing points and add the magnitudes, exactly as you split a motion problem at the times when velocity is zero.

The definite integral as signed area, stage by stage

The single most useful picture in this whole topic is the definite integral as a signed area. Below it is built up one stage at a time on a curve that is above the axis on the left part of the interval and below it on the right, so you can see exactly where the sign comes from.

Stage 1, mark the curve and the limits. Draw y=f(x)y = f(x) and the interval you are integrating over, from x=ax = a to x=bx = b. Nothing is shaded yet; this is just the geometry the integral measures.

The curve and the interval from a to bThe curve y equals f of x is drawn with the x and y axes. The limits x equals a and x equals b are labelled on the x axis where the curve meets it, but nothing is shaded yet. x y a b y = f(x) 1 Stage 1: mark the curve and the limits x = a and x = b.

Stage 2, shade the part above the axis. Where the curve lies above the xx-axis (here from aa to the crossing point), the region between the curve and the axis contributes a positive amount to the integral, equal to its ordinary geometric area.

Shade the region above the axisThe part of the region between the curve and the x axis from a to the crossing point, where the curve is above the axis, is shaded. This area counts as positive. x y a + y = f(x) 2 Stage 2: the area above the axis counts as positive.

Stage 3, shade the part below the axis. Where the curve dips below the axis (from the crossing point to bb), the region contributes a negative amount: the integral subtracts that area rather than adding it. It is drawn in a second tone to keep the two contributions distinct.

Shade the region below the axisThe part of the region from the crossing point to b, where the curve dips below the x axis, is shaded in a second tone. This area counts as negative in the signed-area integral. x y a b + − y = f(x) 3 Stage 3: the area below the axis counts as negative.

Stage 4, add the signed pieces. The definite integral ∫abf(x) dx\int_a^b f(x)\,dx is the positive area minus the negative area. The crossing point, where f=0f = 0, is marked because it is exactly where the sign of the contribution flips, and it is where you must split the integral if a question asks for the geometric (always-positive) area instead.

The definite integral is the signed areaBoth regions are shown together. The definite integral of f from a to b equals the positive area above the axis minus the negative area below it. The crossing point is marked because it is where the sign of the contribution flips. x y a b + − y = f(x) 4 Stage 4: the integral is the positive area minus the negative area.

Properties worth quoting

Two properties simplify many definite integrals: ∫abf(x) dx=−∫baf(x) dx\int_a^b f(x)\,dx = -\int_b^a f(x)\,dx (reversing the limits flips the sign), and ∫abf+∫bcf=∫acf\int_a^b f + \int_b^c f = \int_a^c f (adjacent intervals combine). For an even function ∫−aaf=2∫0af\int_{-a}^{a} f = 2\int_0^a f, and for an odd function ∫−aaf=0\int_{-a}^{a} f = 0. Quoting the odd-function rule on a symmetric interval can turn a page of working into a one-line "the integral is 00 by symmetry", which markers accept and which removes the chance of an arithmetic slip.

How exam questions ask about integration

The wording tells you which tool to reach for. Learn to translate the phrasing into a method:

  • "Find / evaluate ∫… dx\int \ldots \, dx" (no limits). An indefinite integral: produce the antiderivative and you must write +C+ C. Drop it and you lose the final mark.
  • "Evaluate ∫ab… dx\int_a^b \ldots \, dx" (with limits). A definite integral: find the antiderivative, write it in square brackets [ ]ab[\,]_a^b, substitute the top limit minus the bottom limit. No +C+ C.
  • "Using the substitution u=…u = \ldots". The substitution is handed to you; show dudx\frac{du}{dx}, replace dxdx and (for limits) convert them to uu, integrate, then convert back or evaluate. The marks are for the visible transformation, not just the answer.
  • "Find the area bounded by / enclosed by / between." This is a geometric area, so it must be positive. Sketch first, find where the curve meets the axis or where two curves intersect, split at those points, and integrate "upper minus lower" (or take ∫∣f∣\int |f|), taking the magnitude of any piece below the axis.
  • "Show that ddx(…)=…\frac{d}{dx}(\ldots) = \ldots, hence find ∫… dx\int \ldots \, dx". The "hence" is a gift: the differentiation result you just proved is the antiderivative you need, so quote it and reverse it rather than integrating from scratch.
  • "Find ddx∫axf(t) dt\frac{d}{dx} \int_a^x f(t)\,dt". A direct test of the second form of the FTC: the answer is just f(x)f(x), with no integration required.

The single most common silent error is treating "evaluate the integral" and "find the area" as the same task. They agree only when the curve never dips below the axis on the interval; the moment it does, the integral and the area differ, and the question wording decides which the marker wants.

Worked example

This example moves from the most direct integral to the most subtle: a standard antiderivative, a linear-inside-argument case, substitution, a definite integral with changed limits, and finally a direct use of the Fundamental Theorem.

Integrate a standard antiderivative

The integrand is a sum of powers of xx, so we integrate term by term with the power rule ∫xn dx=xn+1n+1\int x^n \, dx = \frac{x^{n+1}}{n+1}, raising each index by one and dividing, and add a single constant at the end:

∫(5x3+4x−7) dx=5x44+2x2−7x+C.\int (5 x^3 + 4 x - 7) \, dx = \frac{5 x^4}{4} + 2 x^2 - 7 x + C.

Integrate functions with a linear inside argument

When the inside of the function is linear, integrating introduces a factor of the inner coefficient, so we divide by that coefficient to compensate. For e3xe^{3x} we divide by 33, and for (2x+1)4(2x+1)^4 we divide by the coefficient 22 as well as the new power 55:

∫e3x dx=e3x3+C,∫(2x+1)4 dx=(2x+1)510+C.\int e^{3 x} \, dx = \frac{e^{3 x}}{3} + C, \qquad \int (2 x + 1)^{4} \, dx = \frac{(2 x + 1)^{5}}{10} + C.

Evaluate ∫xx2+4 dx\int x \sqrt{x^2 + 4} \, dx by substitution

Evaluate ∫xx2+4 dx\int x \sqrt{x^2 + 4} \, dx.

The integrand contains the inner function x2+4x^2 + 4 together with (a multiple of) its derivative 2x2x, which is the signal to substitute. Setting u=x2+4u = x^2 + 4 turns the messy product into a plain power of uu:

u=x2+4  ⇒  du=2x dx  ⇒  x dx=12 du.u = x^2 + 4 \;\Rightarrow\; du = 2 x \, dx \;\Rightarrow\; x \, dx = \tfrac{1}{2} \, du.

Rewriting in uu, integrating, and substituting back gives the answer in terms of xx:

∫xx2+4 dx=∫u⋅12 du=12⋅23u3/2+C=13(x2+4)3/2+C.\int x \sqrt{x^2 + 4} \, dx = \int \sqrt{u} \cdot \tfrac{1}{2} \, du = \tfrac{1}{2} \cdot \tfrac{2}{3} u^{3/2} + C = \tfrac{1}{3} (x^2 + 4)^{3/2} + C.

Evaluate ∫012xex2 dx\int_0^1 2 x e^{x^2} \, dx with changed limits

Evaluate ∫012xex2 dx\int_0^1 2 x e^{x^2} \, dx.

We substitute u=x2u = x^2, and because this is a definite integral we convert the limits to uu values instead of substituting back, which avoids rewriting the antiderivative in xx. The xx-limits 00 and 11 become the uu-limits 00 and 11:

u=x2  ⇒  du=2x dx,x=0⇒u=0,x=1⇒u=1.u = x^2 \;\Rightarrow\; du = 2x\,dx, \qquad x = 0 \Rightarrow u = 0, \quad x = 1 \Rightarrow u = 1.

The integral collapses to a standard exponential, evaluated with the new limits:

∫012xex2 dx=∫01eu du=[eu]01=e−1.\int_0^1 2 x e^{x^2} \, dx = \int_0^1 e^u \, du = [e^u]_0^1 = e - 1.

Differentiate an integral using the FTC in reverse

The second form of the Fundamental Theorem says differentiating an integral with a variable upper limit just returns the integrand evaluated at that limit. So no antiderivative of cos⁡(t2)\cos(t^2) is needed; we read the answer straight off:

G(x)=∫1xcos⁡(t2) dt  ⇒  G′(x)=cos⁡(x2).G(x) = \int_1^x \cos(t^2) \, dt \;\Rightarrow\; G'(x) = \cos(x^2).

Signed integral versus geometric area

Here is the trap the stage-by-stage diagram warns about. Take ∫02(x2−1) dx\int_0^2 (x^2 - 1)\,dx, where the curve is below the axis on [0,1][0, 1] and above it on [1,2][1, 2]. The plain integral mixes the signs:

∫02(x2−1) dx=[x33−x]02=(83−2)−0=23.\int_0^2 (x^2 - 1)\,dx = \left[\frac{x^3}{3} - x\right]_0^2 = \left(\frac{8}{3} - 2\right) - 0 = \frac{2}{3}.

If the question instead asks for the area enclosed by the curve and the axis on [0,2][0, 2], split at the crossing point x=1x = 1 and take the magnitude of each piece. The piece on [0,1][0, 1] is [x33−x]01=13−1=−23\left[\frac{x^3}{3} - x\right]_0^1 = \frac{1}{3} - 1 = -\frac{2}{3}, so its area is 23\frac{2}{3}; the piece on [1,2][1, 2] is (83−2)−(13−1)=23+23=43\left(\frac{8}{3} - 2\right) - \left(\frac{1}{3} - 1\right) = \frac{2}{3} + \frac{2}{3} = \frac{4}{3}.

Area=∣−23∣+43=23+43=2 square units.\text{Area} = \left|-\tfrac{2}{3}\right| + \tfrac{4}{3} = \tfrac{2}{3} + \tfrac{4}{3} = 2 \text{ square units}.

The integral was 23\frac{2}{3} but the geometric area is 22. They differ precisely because the negative piece partly cancelled the positive piece in the plain integral, which is the whole point of stages 2 to 4 above.

Common traps
Forgetting the +C+ C
An indefinite integral must include the constant of integration.
Dividing by the wrong coefficient
∫e2x dx=12e2x+C\int e^{2 x} \, dx = \frac{1}{2} e^{2 x} + C, not 2e2x+C2 e^{2 x} + C.
Substituting without changing dxdx
When you substitute u=g(x)u = g(x), the dxdx must become dug′(x)\frac{du}{g'(x)} (or the integrand must already contain a multiple of g′(x) dxg'(x) \, dx).
Mixing limits and the variable
After a substitution, either change the limits to uu values or substitute back to xx before evaluating. Do not mix the two.
Using the FTC with ∣x∣|x| inside a logarithm wrongly
∫1x dx=ln⁡∣x∣+C\int \frac{1}{x} \, dx = \ln |x| + C. For a definite integral, the interval must not cross x=0x = 0.
Exam technique

Write the antiderivative explicitly inside square brackets, [F(x)]ab[F(x)]_a^b, before you substitute; markers award a method mark for the correct antiderivative even if the final arithmetic slips. For an indefinite integral, the +C+ C is worth a mark on its own, so never omit it. When a substitution is named in the question, show every transformed piece (the dudx\frac{du}{dx} line, the new dxdx, the converted limits) because that visible working is what is being marked, not the number. For an "area" question, sketch the curve, mark where it crosses the axis, and split there before integrating; the difference between the signed integral and the geometric area is the single most common place marks are dropped. Leave volume and area answers in exact form (keep π\pi, fractions and surds) unless a decimal is requested.

Exam-style questions

Questions in the style of NESA 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.

HSC-style3 marks
Evaluate ∫02(3x2+2x) dx\int_0^2 (3 x^2 + 2 x) \, dx.
Show worked answer →

Find the antiderivative.

∫(3x2+2x) dx=x3+x2+C\int (3 x^2 + 2 x) \, dx = x^3 + x^2 + C.

Apply the Fundamental Theorem of Calculus.

∫02(3x2+2x) dx=[x3+x2]02=(8+4)−(0+0)=12\int_0^2 (3 x^2 + 2 x) \, dx = [x^3 + x^2]_0^2 = (8 + 4) - (0 + 0) = 12.

Markers reward the explicit antiderivative, correct bracket notation, and the evaluated answer.

HSC-style3 marks
Use the substitution u=x2+1u = x^2 + 1 to evaluate ∫2x(x2+1)4 dx\int 2 x (x^2 + 1)^4 \, dx.
Show worked answer →

With u=x2+1u = x^2 + 1, dudx=2x\frac{du}{dx} = 2 x, so du=2x dxdu = 2 x \, dx.

The integral becomes ∫u4 du=u55+C\int u^4 \, du = \frac{u^5}{5} + C.

Substitute back: ∫2x(x2+1)4 dx=(x2+1)55+C\int 2 x (x^2 + 1)^4 \, dx = \frac{(x^2 + 1)^5}{5} + C.

Markers expect a clear statement of the substitution, transformation of both the integrand and the differential, the antiderivative in uu, and the substitution back into xx.

Practice questions

Original practice questions graded from foundation to exam level, each with a full worked solution. Try them before revealing the solution.

foundation2 marks
Find ∫(6x2−4x+3) dx\int (6x^2 - 4x + 3) \, dx.
Show worked solution →

Integrate term by term with the power rule ∫xn dx=xn+1n+1\int x^n \, dx = \dfrac{x^{n+1}}{n+1}:

∫(6x2−4x+3) dx=6x33−4x22+3x+C=2x3−2x2+3x+C.\int (6x^2 - 4x + 3) \, dx = \frac{6x^3}{3} - \frac{4x^2}{2} + 3x + C = 2x^3 - 2x^2 + 3x + C.

Marker's note: one mark for correctly integrating each power, one for the fully simplified expression with the +C+ C. Omitting the constant of integration on an indefinite integral loses the second mark.

foundation3 marks
Evaluate ∫134x dx\int_1^3 \dfrac{4}{x} \, dx, giving your answer in exact form.
Show worked solution →

Use the standard antiderivative ∫1x dx=ln⁡∣x∣+C\int \dfrac{1}{x} \, dx = \ln|x| + C, so the 44 comes out as a factor:

∫134x dx=[ 4ln⁡∣x∣ ]13=4ln⁡3−4ln⁡1.\int_1^3 \frac{4}{x} \, dx = \left[\, 4\ln|x| \,\right]_1^3 = 4\ln 3 - 4\ln 1.

Simplify using ln⁡1=0\ln 1 = 0:

4ln⁡3−4(0)=4ln⁡3.4\ln 3 - 4(0) = 4\ln 3.

Marker's note: one mark for the antiderivative 4ln⁡∣x∣4\ln|x|, one for correct substitution of the limits in [  ]13[\;]_1^3 form, one for the exact answer 4ln⁡34\ln 3 (using ln⁡1=0\ln 1 = 0). A decimal without the exact form is penalised when exact form is asked for.

foundation2 marks
Find ∫(2cos⁡x−e2x) dx\int (2\cos x - e^{2x}) \, dx.
Show worked solution →

Integrate each term. The antiderivative of cos⁡x\cos x is sin⁡x\sin x, and for e2xe^{2x} the linear inner coefficient 22 means we divide by 22:

∫(2cos⁡x−e2x) dx=2sin⁡x−12e2x+C.\int (2\cos x - e^{2x}) \, dx = 2\sin x - \frac{1}{2}e^{2x} + C.

Marker's note: one mark for 2sin⁡x2\sin x, one for −12e2x+C-\tfrac{1}{2}e^{2x} + C (dividing by the coefficient 22). Writing −2e2x-2e^{2x} instead of −12e2x-\tfrac{1}{2}e^{2x} is the standard slip.

core3 marks
Use the substitution u=x3+1u = x^3 + 1 to find ∫3x2(x3+1)5 dx\int 3x^2 (x^3 + 1)^5 \, dx.
Show worked solution →

Set up the substitution. With u=x3+1u = x^3 + 1,

dudx=3x2⇒du=3x2 dx.\frac{du}{dx} = 3x^2 \quad\Rightarrow\quad du = 3x^2 \, dx.

Rewrite the whole integral in uu. The factor 3x2 dx3x^2 \, dx is exactly dudu:

∫3x2(x3+1)5 dx=∫u5 du=u66+C.\int 3x^2 (x^3 + 1)^5 \, dx = \int u^5 \, du = \frac{u^6}{6} + C.

Substitute back to xx:

∫3x2(x3+1)5 dx=(x3+1)66+C.\int 3x^2 (x^3 + 1)^5 \, dx = \frac{(x^3 + 1)^6}{6} + C.

Marker's note: one mark for du=3x2 dxdu = 3x^2 \, dx, one for the integral u66+C\dfrac{u^6}{6} + C in uu, one for the back-substitution to (x3+1)66+C\dfrac{(x^3+1)^6}{6} + C. Leaving the answer in uu, or dropping the +C+ C, forfeits the final mark.

core4 marks
A particle moves in a straight line so that its velocity, in metres per second, is v(t)=3t2−12t+9v(t) = 3t^2 - 12t + 9 for 0≤t≤40 \le t \le 4 seconds. A sketch of vv against tt shows a parabola that opens upwards, cuts the time axis at t=1t = 1 and t=3t = 3, is positive on 0≤t<10 \le t < 1 and 3<t≤43 < t \le 4, and is negative on 1<t<31 < t < 3. (a) Find the displacement of the particle over the interval 0≤t≤40 \le t \le 4. (b) Find the total distance travelled over the same interval.
Show worked solution →

Displacement is the signed integral of velocity; distance is the integral of speed, so the sign changes at t=1t = 1 and t=3t = 3 matter for part (b).

Part (a): displacement is ∫04v dt\int_0^4 v \, dt.

∫04(3t2−12t+9) dt=[ t3−6t2+9t ]04=(64−96+36)−0=4 m.\int_0^4 (3t^2 - 12t + 9) \, dt = \left[\, t^3 - 6t^2 + 9t \,\right]_0^4 = (64 - 96 + 36) - 0 = 4 \text{ m}.

Part (b): split at the sign changes and take magnitudes. Let s(t)=t3−6t2+9ts(t) = t^3 - 6t^2 + 9t.

∫01v dt=s(1)−s(0)=4−0=4,∫13v dt=s(3)−s(1)=0−4=−4,\int_0^1 v \, dt = s(1) - s(0) = 4 - 0 = 4, \qquad \int_1^3 v \, dt = s(3) - s(1) = 0 - 4 = -4,

∫34v dt=s(4)−s(3)=4−0=4.\int_3^4 v \, dt = s(4) - s(3) = 4 - 0 = 4.

Adding the magnitudes:

distance=∣4∣+∣−4∣+∣4∣=12 m.\text{distance} = |4| + |-4| + |4| = 12 \text{ m}.

Marker's note: one mark for the antiderivative t3−6t2+9tt^3 - 6t^2 + 9t, one for the displacement 44 m in (a); one for splitting at t=1t = 1 and t=3t = 3 and one for the total distance 1212 m in (b). Reporting the displacement 44 m as the distance (not splitting at the sign changes) is the trap the graph is drawn to expose.

exam5 marks
Consider the curves y=x2y = x^2 and y=2xy = 2x. (a) Find the xx-coordinates of the points where the curves intersect. (b) Sketch is not required: state which curve is the upper boundary on the interval between the intersection points, justifying your choice with a test value. (c) Hence find the exact area of the region enclosed between the two curves.
Show worked solution →

Part (a): set the curves equal.

x2=2x⇒x2−2x=0⇒x(x−2)=0⇒x=0 or x=2.x^2 = 2x \quad\Rightarrow\quad x^2 - 2x = 0 \quad\Rightarrow\quad x(x - 2) = 0 \quad\Rightarrow\quad x = 0 \text{ or } x = 2.

Part (b): decide the upper curve with a test point. Take x=1x = 1 (between 00 and 22):

y=2x=2(1)=2,y=x2=12=1.y = 2x = 2(1) = 2, \qquad y = x^2 = 1^2 = 1.

Since 2>12 > 1, the line y=2xy = 2x lies above the parabola y=x2y = x^2 on 0<x<20 < x < 2.

Part (c): integrate (upper minus lower) across the interval.

A=∫02(2x−x2) dx=[ x2−x33 ]02.A = \int_0^2 \big(2x - x^2\big) \, dx = \left[\, x^2 - \frac{x^3}{3} \,\right]_0^2.

Substitute the limits:

A=(4−83)−0=123−83=43 square units.A = \left(4 - \frac{8}{3}\right) - 0 = \frac{12}{3} - \frac{8}{3} = \frac{4}{3} \text{ square units}.

Marker's note: one mark for both intersection points in (a), one for identifying y=2xy = 2x as the upper curve with a test value in (b), one for the "upper minus lower" integrand 2x−x22x - x^2, one for the antiderivative with the limits substituted, one for the exact area 43\tfrac{4}{3} square units. Integrating "lower minus upper" gives −43-\tfrac{4}{3}; an area must be positive, so the sign matters.

exam5 marks
Let f(x)=xln⁡xf(x) = x \ln x for x>0x > 0. (a) Show that ddx(xln⁡x)=ln⁡x+1\dfrac{d}{dx}\big(x \ln x\big) = \ln x + 1. (b) Hence find ∫ln⁡x dx\int \ln x \, dx. (c) Hence evaluate ∫1eln⁡x dx\int_1^e \ln x \, dx, giving an exact answer.
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Part (a): differentiate the product xln⁡xx \ln x. Using the product rule with u=xu = x and v=ln⁡xv = \ln x:

ddx(xln⁡x)=(1)(ln⁡x)+(x)(1x)=ln⁡x+1.\frac{d}{dx}\big(x \ln x\big) = (1)(\ln x) + (x)\left(\frac{1}{x}\right) = \ln x + 1.

Part (b): reverse the result to integrate ln⁡x\ln x. Integrating both sides of ddx(xln⁡x)=ln⁡x+1\dfrac{d}{dx}(x\ln x) = \ln x + 1 gives

∫(ln⁡x+1) dx=xln⁡x+C.\int (\ln x + 1) \, dx = x \ln x + C.

Split the left side and move the ∫1 dx=x\int 1 \, dx = x term across:

∫ln⁡x dx+x=xln⁡x+C⇒∫ln⁡x dx=xln⁡x−x+C.\int \ln x \, dx + x = x \ln x + C \quad\Rightarrow\quad \int \ln x \, dx = x \ln x - x + C.

Part (c): apply the Fundamental Theorem of Calculus.

∫1eln⁡x dx=[ xln⁡x−x ]1e=(eln⁡e−e)−(1⋅ln⁡1−1).\int_1^e \ln x \, dx = \left[\, x \ln x - x \,\right]_1^e = \big(e \ln e - e\big) - \big(1 \cdot \ln 1 - 1\big).

Using ln⁡e=1\ln e = 1 and ln⁡1=0\ln 1 = 0:

=(e−e)−(0−1)=0−(−1)=1.= (e - e) - (0 - 1) = 0 - (-1) = 1.

Marker's note: one mark for the product-rule differentiation in (a), one for reversing it and one for the rearranged ∫ln⁡x dx=xln⁡x−x+C\int \ln x \, dx = x\ln x - x + C in (b), one for substituting the limits in [  ]1e[\;]_1^e form and one for the exact value 11 in (c). Forgetting the −x-x term in the antiderivative gives the wrong final value of e−e=0e - e = 0.

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