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Integration

Board Coverage

BoardPaperNotes
AQAPaper 1, 2Basic integration in P1; by parts, substitution in P2
EdexcelP1, P2Similar split
OCR (A)Paper 1, 2Includes trapezium rule
CIE (9709)P1, P2, P3Basic in P1; by parts/substitution in P2/P3; further in P3
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The formula booklet provides standard integrals. You must know how to apply integration techniques and when to use each method.


1. Integration as Area: Riemann Sums

1.1 Definition

Definition. The definite integral of ff from aa to bb is defined as the limit of Riemann sums:

abf(x)dx=limni=1nf(xi)Δx\int_a^b f(x)\,dx = \lim_{n\to\infty}\sum_{i=1}^{n}f(x_i^*)\,\Delta x

where [a,b][a,b] is divided into nn subintervals of width Δx=ban\Delta x = \dfrac{b-a}{n}, and xix_i^* is a sample point in the ii-th subinterval.

Geometric picture. We divide the area under y=f(x)y = f(x) between x=ax = a and x=bx = b into nn thin rectangles. The sum of their areas approximates the total area. As nn \to \infty (rectangles become infinitely thin), the approximation becomes exact.

  • If we take the upper rectangle height (right endpoint), we get an upper sum.
  • If we take the lower rectangle height (left endpoint), we get a lower sum.
  • The integral exists when the upper and lower sums converge to the same limit.

Intuition. Integration is "accumulation" — adding up infinitely many infinitesimal contributions. If f(x)f(x) is a rate (like velocity), then abf(x)dx\int_a^b f(x)\,dx is the total change (displacement).

Integration as Area Under a Curve

Increase the number of rectangles to see how Riemann sums converge to the exact area under the curve. Compare the upper and lower sums as the partition gets finer.


2. The Fundamental Theorem of Calculus

Theorem (FTC). If ff is continuous on [a,b][a,b], then

(Part1)ddxaxf(t)dt=f(x)(\mathrm{Part 1})\quad \frac{d}{dx}\int_a^x f(t)\,dt = f(x)

(Part2)abf(x)dx=F(b)F(a)(\mathrm{Part 2})\quad \int_a^b f(x)\,dx = F(b) - F(a)

where FF is any antiderivative of ff (i.e., F(x)=f(x)F'(x) = f(x)).

2.1 Sketch proof of Part 2

Let G(x)=axf(t)dtG(x) = \int_a^x f(t)\,dt. By Part 1, G(x)=f(x)G'(x) = f(x).

If FF is any other antiderivative of ff, then F(x)=G(x)=f(x)F'(x) = G'(x) = f(x), so F(x)G(x)=CF(x) - G(x) = C (a constant).

F(x)=G(x)+C    F(b)F(a)=G(b)G(a)=abf(t)dt0F(x) = G(x) + C \implies F(b) - F(a) = G(b) - G(a) = \int_a^b f(t)\,dt - 0

Hence abf(x)dx=F(b)F(a)\displaystyle\int_a^b f(x)\,dx = F(b) - F(a). \blacksquare

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The Fundamental Theorem of Calculus is one of the most important results in all of mathematics. It connects the two seemingly unrelated operations of differentiation (finding rates of change) and integration (finding areas).


3. Standard Integrals

Each standard integral can be derived by reversing the corresponding differentiation.

3.1 Derivation of key standard integrals

Power rule. Since ddx(xn+1n+1)=xn\dfrac{d}{dx}\left(\dfrac{x^{n+1}}{n+1}\right) = x^n for n1n \neq -1:

xndx=xn+1n+1+C,n1\int x^n\,dx = \frac{x^{n+1}}{n+1} + C, \quad n \neq -1

Reciprocal. Since ddxlnx=1x\dfrac{d}{dx}\ln|x| = \dfrac{1}{x}:

1xdx=lnx+C\int \frac{1}{x}\,dx = \ln|x| + C

Exponential. Since ddxekx=kekx\dfrac{d}{dx}e^{kx} = ke^{kx}:

ekxdx=1kekx+C\int e^{kx}\,dx = \frac{1}{k}e^{kx} + C

Trigonometric. Since ddxsinx=cosx\dfrac{d}{dx}\sin x = \cos x:

cosxdx=sinx+C\int \cos x\,dx = \sin x + C

sinxdx=cosx+C\int \sin x\,dx = -\cos x + C

sec2xdx=tanx+C\int \sec^2 x\,dx = \tan x + C

3.2 Summary table

| f(x)f(x) | f(x)dx\int f(x)\,dx | | ------------------- | -------------------------- | --- | ---- | | xnx^n (n1n \neq -1) | xn+1n+1+C\dfrac{x^{n+1}}{n+1} + C | | 1/x1/x | lnx+C\ln | x | + C | | ekxe^{kx} | 1kekx+C\dfrac{1}{k}e^{kx} + C | | cosx\cos x | sinx+C\sin x + C | | sinx\sin x | cosx+C-\cos x + C | | sec2x\sec^2 x | tanx+C\tan x + C |


4. Definite Integration and Areas

4.1 Area under a curve

The area between y=f(x)y = f(x), the xx-axis, x=ax = a, and x=bx = b is

A=abf(x)dxA = \int_a^b f(x)\,dx

provided f(x)0f(x) \geq 0 on [a,b][a,b].

4.2 Area between a curve and the xx-axis

If f(x)f(x) changes sign on [a,b][a,b], we must split the integral at each root:

A=abf(x)dxA = \int_a^b |f(x)|\,dx

warning

abf(x)dx\int_a^b f(x)\,dx gives the signed area (negative below the xx-axis). To find the actual geometric area, take the absolute value and integrate separately over regions where ff is positive and negative.

4.3 Area between two curves

The area between y=f(x)y = f(x) and y=g(x)y = g(x) from x=ax = a to x=bx = b (where f(x)g(x)f(x) \geq g(x)) is

A=ab[f(x)g(x)]dxA = \int_a^b [f(x) - g(x)]\,dx

4.4 Area under a parametric curve

A=t1t2ydxdtdtA = \int_{t_1}^{t_2} y\,\frac{dx}{dt}\,dt


5. Integration by Substitution

5.1 The method

Theorem. f(g(x))g(x)dx=F(g(x))+C\displaystyle\int f(g(x))g'(x)\,dx = F(g(x)) + C where F=fF' = f.

5.2 Proof via the chain rule

Let u=g(x)u = g(x). By the chain rule, ddxF(u)=F(u)dudx=f(u)dudx=f(g(x))g(x)\dfrac{d}{dx}F(u) = F'(u)\dfrac{du}{dx} = f(u)\dfrac{du}{dx} = f(g(x))g'(x).

Therefore f(g(x))g(x)dx=F(g(x))+C\int f(g(x))g'(x)\,dx = F(g(x)) + C. \blacksquare

In practice:

  1. Choose a substitution u=g(x)u = g(x).
  2. Compute du=g(x)dxdu = g'(x)\,dx.
  3. Rewrite the integral entirely in terms of uu.
  4. Integrate, then substitute back.

Example. Find 2xx2+1dx\displaystyle\int 2x\sqrt{x^2+1}\,dx.

Let u=x2+1u = x^2 + 1, du=2xdxdu = 2x\,dx.

2xx2+1dx=udu=23u3/2+C=23(x2+1)3/2+C\int 2x\sqrt{x^2+1}\,dx = \int \sqrt{u}\,du = \frac{2}{3}u^{3/2} + C = \frac{2}{3}(x^2+1)^{3/2} + C

tip

tip g(x)\sqrt{g(x)} and g(x)g'(x) in the integrand, try u=g(x)u = g(x).

5.3 Definite integrals with substitution

For a definite integral, you can either:

  • Substitute back to xx before evaluating, or
  • Change the limits: when x=ax = a, u=g(a)u = g(a); when x=bx = b, u=g(b)u = g(b).

6. Integration by Parts

6.1 The formula

Theorem. udv=uvvdu\displaystyle\int u\,dv = uv - \int v\,du

6.2 Proof via the product rule

From the product rule: ddx(uv)=udvdx+vdudx\dfrac{d}{dx}(uv) = u\dfrac{dv}{dx} + v\dfrac{du}{dx}.

Integrating both sides:

uv=udvdxdx+vdudxdxuv = \int u\frac{dv}{dx}\,dx + \int v\frac{du}{dx}\,dx

udvdxdx=uvvdudxdx\int u\frac{dv}{dx}\,dx = uv - \int v\frac{du}{dx}\,dx

i.e., udv=uvvdu\displaystyle\int u\,dv = uv - \int v\,du. \blacksquare

6.3 Choosing uu and dvdv

Use the mnemonic LIATE (Logarithmic, Inverse trig, Algebraic, Trig, Exponential). Choose uu from the leftmost category that appears.

warning

warning after applying the formula, swap uu and dvdv.

Example. Find xexdx\displaystyle\int x e^x\,dx.

Let u=xu = x, dv=exdxdv = e^x\,dx. Then du=dxdu = dx, v=exv = e^x.

xexdx=xexexdx=xexex+C=ex(x1)+C\int x e^x\,dx = x e^x - \int e^x\,dx = x e^x - e^x + C = e^x(x-1) + C

6.4 Reduction formulas

Integration by parts can produce reduction formulas relating InI_n to In1I_{n-1}.

Example. Find a reduction formula for In=xnexdxI_n = \displaystyle\int x^n e^x\,dx.

Let u=xnu = x^n, dv=exdxdv = e^x\,dx. Then du=nxn1dxdu = nx^{n-1}\,dx, v=exv = e^x.

In=xnexnxn1exdx=xnexnIn1I_n = x^n e^x - n\int x^{n-1} e^x\,dx = x^n e^x - nI_{n-1}

This gives In=xnexnIn1I_n = x^n e^x - nI_{n-1}, allowing us to reduce any InI_n to I0=ex+CI_0 = e^x + C.


7. The Trapezium Rule

7.1 Formula

To approximate abf(x)dx\displaystyle\int_a^b f(x)\,dx, divide [a,b][a,b] into nn equal strips of width h=banh = \dfrac{b-a}{n}:

abf(x)dxh2[y0+2y1+2y2++2yn1+yn]\int_a^b f(x)\,dx \approx \frac{h}{2}\left[y_0 + 2y_1 + 2y_2 + \cdots + 2y_{n-1} + y_n\right]

where yi=f(a+ih)y_i = f(a + ih).

7.2 Derivation

Each strip is approximated by a trapezium. The area of the ii-th trapezium is:

Ai=h2(yi1+yi)A_i = \frac{h}{2}(y_{i-1} + y_i)

Summing all trapezia:

Total=h2(y0+y1)+h2(y1+y2)++h2(yn1+yn)=h2[y0+2y1+2y2++2yn1+yn]\begin{aligned} \mathrm{Total} &= \frac{h}{2}(y_0+y_1) + \frac{h}{2}(y_1+y_2) + \cdots + \frac{h}{2}(y_{n-1}+y_n) \\ &= \frac{h}{2}\left[y_0 + 2y_1 + 2y_2 + \cdots + 2y_{n-1} + y_n\right] \end{aligned}

7.3 Error bound

If ff'' is continuous on [a,b][a,b] and f(x)M|f''(x)| \leq M for all x[a,b]x \in [a,b], then the error EE satisfies

E(ba)312n2M|E| \leq \frac{(b-a)^3}{12n^2}M

Proof (sketch). For a single strip of width hh, the trapezium rule gives area h2[f(a)+f(a+h)]\dfrac{h}{2}[f(a) + f(a+h)], while the true area is aa+hf(x)dx\int_a^{a+h}f(x)\,dx. By Taylor's theorem, the error per strip is h312f(ξ)-\dfrac{h^3}{12}f''(\xi) for some ξ(a,a+h)\xi \in (a, a+h). Summing nn strips and using the bound fM|f''| \leq M:

Enh312M=n(ba)312n3M=(ba)312n2M|E| \leq n \cdot \frac{h^3}{12} M = n \cdot \frac{(b-a)^3}{12n^3}M = \frac{(b-a)^3}{12n^2}M \quad \blacksquare

Intuition. The error decreases as 1/n21/n^2 — doubling the number of strips quarters the error. The error also depends on how curved the function is (via ff''). For a straight line (f=0f'' = 0), the trapezium rule is exact.

tip

tip concave-down functions and overestimates for concave-up functions.


8. Further Techniques

8.1 Integrating f(x)f(x)\dfrac{f'(x)}{f(x)}

f(x)f(x)dx=lnf(x)+C\int \frac{f'(x)}{f(x)}\,dx = \ln|f(x)| + C

This follows from the substitution u=f(x)u = f(x).

8.2 Partial fractions

Rational functions can be integrated by first decomposing into partial fractions.

Example. 1x21dx=12(1x11x+1)dx=12lnx1x+1+C\displaystyle\int \frac{1}{x^2-1}\,dx = \int \frac{1}{2}\left(\frac{1}{x-1} - \frac{1}{x+1}\right)dx = \frac{1}{2}\ln\left|\frac{x-1}{x+1}\right| + C.

tanxdx=LBsinxRB◆◆LBcosxRBdx=lncosx+C=lnsecx+C\int \tan x\,dx = \int \frac◆LB◆\sin x◆RB◆◆LB◆\cos x◆RB◆\,dx = -\ln|\cos x| + C = \ln|\sec x| + C


Problem Set

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Problem 1 Evaluate 02(3x24x+1)dx\displaystyle\int_0^2 (3x^2 - 4x + 1)\,dx.

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Solution 1 02(3x24x+1)dx=[x32x2+x]02=(88+2)0=2\int_0^2 (3x^2 - 4x + 1)\,dx = \left[x^3 - 2x^2 + x\right]_0^2 = (8 - 8 + 2) - 0 = 2

If you get this wrong, revise: Standard Integrals — Section 3.

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Problem 2 Find the area enclosed between y=x2y = x^2 and y=2xy = 2x.

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Solution 2 Intersection: x2=2x    x(x2)=0    x=0,2x^2 = 2x \implies x(x-2) = 0 \implies x = 0, 2.

On [0,2][0,2]: 2xx22x \geq x^2 (since 2xx2=x(2x)02x - x^2 = x(2-x) \geq 0).

A=02(2xx2)dx=[x2x33]02=483=43A = \int_0^2 (2x - x^2)\,dx = \left[x^2 - \frac{x^3}{3}\right]_0^2 = 4 - \frac{8}{3} = \frac{4}{3}

If you get this wrong, revise: Definite Integration and Areas — Section 4.3.

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Problem 3 Find 2xx2+3dx\displaystyle\int \frac{2x}{x^2+3}\,dx.

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Solution 3 Let u=x2+3u = x^2 + 3, du=2xdxdu = 2x\,dx.

2xx2+3dx=1udu=lnu+C=ln(x2+3)+C\int \frac{2x}{x^2+3}\,dx = \int \frac{1}{u}\,du = \ln|u| + C = \ln(x^2+3) + C

(Since x2+3>0x^2+3 \gt{} 0, no absolute value needed.)

If you get this wrong, revise: Integration by Substitution — Section 5.

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Problem 4 Evaluate 0π/2xsinxdx\displaystyle\int_0^{\pi/2} x\sin x\,dx.

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Solution 4 Integration by parts: u=xu = x, dv=sinxdxdv = \sin x\,dx. Then du=dxdu = dx, v=cosxv = -\cos x.

xsinxdx=xcosx+cosxdx=xcosx+sinx+C\int x\sin x\,dx = -x\cos x + \int \cos x\,dx = -x\cos x + \sin x + C

[xcosx+sinx]0π/2=(0+1)(0+0)=1\left[-x\cos x + \sin x\right]_0^{\pi/2} = \left(0 + 1\right) - \left(0 + 0\right) = 1

If you get this wrong, revise: Integration by Parts — Section 6.

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Problem 5 Use the trapezium rule with 4 strips to approximate 0211+x2dx\displaystyle\int_0^2 \frac{1}{1+x^2}\,dx, and give an error bound given f(x)2|f''(x)| \leq 2 on [0,2][0,2].

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Solution 5 h=204=0.5h = \dfrac{2-0}{4} = 0.5. Values: y0=1y_0 = 1, y1=1/(1+0.25)=0.8y_1 = 1/(1+0.25) = 0.8, y2=1/(1+1)=0.5y_2 = 1/(1+1) = 0.5, y3=1/(1+2.25)0.3077y_3 = 1/(1+2.25) \approx 0.3077, y4=1/5=0.2y_4 = 1/5 = 0.2.

Approx=0.52[1+2(0.8)+2(0.5)+2(0.3077)+0.2]=0.25[1+1.6+1.0+0.6154+0.2]=0.25×4.41541.104\mathrm{Approx} = \frac{0.5}{2}\left[1 + 2(0.8) + 2(0.5) + 2(0.3077) + 0.2\right] = 0.25[1 + 1.6 + 1.0 + 0.6154 + 0.2] = 0.25 \times 4.4154 \approx 1.104

Error bound: ELB23RB◆◆LB12×16RB×2=8192×2=1120.0833|E| \leq \dfrac◆LB◆2^3◆RB◆◆LB◆12 \times 16◆RB◆ \times 2 = \dfrac{8}{192} \times 2 = \dfrac{1}{12} \approx 0.0833.

If you get this wrong, revise: The Trapezium Rule — Section 7.

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Problem 6 Find LBxRB◆◆LBx+1RBdx\displaystyle\int \frac◆LB◆x◆RB◆◆LB◆\sqrt{x+1}◆RB◆\,dx.

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Solution 6 Let u=x+1u = x+1, so x=u1x = u-1 and dx=dudx = du.

LBu1RB◆◆LBuRBdu=(u1/2u1/2)du=23u3/22u1/2+C=23(x+1)3/22(x+1)1/2+C\int \frac◆LB◆u-1◆RB◆◆LB◆\sqrt{u}◆RB◆\,du = \int(u^{1/2} - u^{-1/2})\,du = \frac{2}{3}u^{3/2} - 2u^{1/2} + C = \frac{2}{3}(x+1)^{3/2} - 2(x+1)^{1/2} + C

If you get this wrong, revise: Integration by Substitution — Section 5.

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Problem 7 Find a reduction formula for In=0π/2sinnxdxI_n = \displaystyle\int_0^{\pi/2} \sin^n x\,dx for n2n \geq 2.

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Solution 7 In=0π/2sinn1xsinxdxI_n = \int_0^{\pi/2}\sin^{n-1}x \cdot \sin x\,dx.

Let u=sinn1xu = \sin^{n-1}x, dv=sinxdxdv = \sin x\,dx. du=(n1)sinn2xcosxdxdu = (n-1)\sin^{n-2}x\cos x\,dx, v=cosxv = -\cos x.

In=[sinn1xcosx]0π/2+(n1)0π/2sinn2xcos2xdxI_n = \left[-\sin^{n-1}x\cos x\right]_0^{\pi/2} + (n-1)\int_0^{\pi/2}\sin^{n-2}x\cos^2 x\,dx

The boundary term vanishes (since cos(π/2)=0\cos(\pi/2) = 0 and sin0=0\sin 0 = 0). Using cos2x=1sin2x\cos^2 x = 1 - \sin^2 x:

In=(n1)0π/2sinn2x(1sin2x)dx=(n1)(In2In)I_n = (n-1)\int_0^{\pi/2}\sin^{n-2}x(1-\sin^2 x)\,dx = (n-1)(I_{n-2} - I_n)

In=(n1)In2(n1)InI_n = (n-1)I_{n-2} - (n-1)I_n nIn=(n1)In2nI_n = (n-1)I_{n-2} In=n1nIn2I_n = \frac{n-1}{n}I_{n-2}

If you get this wrong, revise: Reduction Formulas — Section 6.4.

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Problem 8 Find the total area between y=x(x2)(x+1)y = x(x-2)(x+1) and the xx-axis.

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Solution 8 y=x(x2)(x+1)=x3x22xy = x(x-2)(x+1) = x^3 - x^2 - 2x. Roots at x=1,0,2x = -1, 0, 2.

10(x3x22x)dx=[x44x33x2]10=0(14+131)=(3+41212)=512\int_{-1}^0 (x^3-x^2-2x)\,dx = \left[\frac{x^4}{4}-\frac{x^3}{3}-x^2\right]_{-1}^0 = 0 - \left(\frac{1}{4}+\frac{1}{3}-1\right) = -\left(\frac{3+4-12}{12}\right) = \frac{5}{12}

02(x3x22x)dx=[x44x33x2]02=(4834)0=83\int_0^2 (x^3-x^2-2x)\,dx = \left[\frac{x^4}{4}-\frac{x^3}{3}-x^2\right]_0^2 = \left(4-\frac{8}{3}-4\right) - 0 = -\frac{8}{3}

Total area = 512+83=5+3212=3712\dfrac{5}{12} + \dfrac{8}{3} = \dfrac{5+32}{12} = \dfrac{37}{12}.

If you get this wrong, revise: Definite Integration and Areas — Section 4.2.

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Problem 9 Find e2xcosxdx\displaystyle\int e^{2x}\cos x\,dx.

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Solution 9 Apply integration by parts twice. Let I=e2xcosxdxI = \int e^{2x}\cos x\,dx.

First: u=e2xu = e^{2x}, dv=cosxdxdv = \cos x\,dx. du=2e2xdxdu = 2e^{2x}\,dx, v=sinxv = \sin x.

I=e2xsinx2e2xsinxdxI = e^{2x}\sin x - 2\int e^{2x}\sin x\,dx.

Second: u=e2xu = e^{2x}, dv=sinxdxdv = \sin x\,dx. du=2e2xdxdu = 2e^{2x}\,dx, v=cosxv = -\cos x.

e2xsinxdx=e2xcosx+2e2xcosxdx=e2xcosx+2I\int e^{2x}\sin x\,dx = -e^{2x}\cos x + 2\int e^{2x}\cos x\,dx = -e^{2x}\cos x + 2I.

I=e2xsinx2(e2xcosx+2I)=e2xsinx+2e2xcosx4II = e^{2x}\sin x - 2(-e^{2x}\cos x + 2I) = e^{2x}\sin x + 2e^{2x}\cos x - 4I.

5I=e2x(sinx+2cosx)5I = e^{2x}(\sin x + 2\cos x).

I=LBe2x(sinx+2cosx)RB◆◆LB5RB+CI = \frac◆LB◆e^{2x}(\sin x + 2\cos x)◆RB◆◆LB◆5◆RB◆ + C

If you get this wrong, revise: Integration by Parts — Section 6.

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Problem 10 Evaluate 1eLBlnxRB◆◆LBxRBdx\displaystyle\int_1^e \frac◆LB◆\ln x◆RB◆◆LB◆x◆RB◆\,dx.

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Solution 10 Let u=lnxu = \ln x, du=1xdxdu = \dfrac{1}{x}\,dx.

LBlnxRB◆◆LBxRBdx=udu=u22+C=LB(lnx)2RB◆◆LB2RB+C\int \frac◆LB◆\ln x◆RB◆◆LB◆x◆RB◆\,dx = \int u\,du = \frac{u^2}{2} + C = \frac◆LB◆(\ln x)^2◆RB◆◆LB◆2◆RB◆ + C

[LB(lnx)2RB◆◆LB2RB]1e=120=12\left[\frac◆LB◆(\ln x)^2◆RB◆◆LB◆2◆RB◆\right]_1^e = \frac{1}{2} - 0 = \frac{1}{2}

If you get this wrong, revise: Integration by Substitution — Section 5.

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Problem 11 The curve CC has parametric equations x=t2x = t^2, y=2ty = 2t for 0t30 \leq t \leq 3. Find the area under CC.

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Solution 11 A=t=0t=3ydxdtdt=032t2tdt=034t2dt=[4t33]03=LB4×27RB◆◆LB3RB=36A = \int_{t=0}^{t=3} y\,\frac{dx}{dt}\,dt = \int_0^3 2t \cdot 2t\,dt = \int_0^3 4t^2\,dt = \left[\frac{4t^3}{3}\right]_0^3 = \frac◆LB◆4 \times 27◆RB◆◆LB◆3◆RB◆ = 36

If you get this wrong, revise: Definite Integration and Areas — Section 4.4.

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Problem 12 Find 3x+5x2+4x+3dx\displaystyle\int \frac{3x+5}{x^2+4x+3}\,dx.

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Solution 12 x2+4x+3=(x+1)(x+3)x^2 + 4x + 3 = (x+1)(x+3).

3x+5(x+1)(x+3)=Ax+1+Bx+3\frac{3x+5}{(x+1)(x+3)} = \frac{A}{x+1} + \frac{B}{x+3}

3x+5=A(x+3)+B(x+1)3x + 5 = A(x+3) + B(x+1).

x=1x = -1: 2=2A    A=12 = 2A \implies A = 1. x=3x = -3: 4=2B    B=2-4 = -2B \implies B = 2.

1x+1+2x+3dx=lnx+1+2lnx+3+C\int \frac{1}{x+1} + \frac{2}{x+3}\,dx = \ln|x+1| + 2\ln|x+3| + C

If you get this wrong, revise: Partial Fractions — Section 8.2.

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Problem 13 Sketch proof: explain why aaf(x)dx=0\displaystyle\int_{-a}^a f(x)\,dx = 0 when ff is an odd function.

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Solution 13 If ff is odd, then f(x)=f(x)f(-x) = -f(x).

aaf(x)dx=a0f(x)dx+0af(x)dx\int_{-a}^a f(x)\,dx = \int_{-a}^0 f(x)\,dx + \int_0^a f(x)\,dx

Let u=xu = -x in the first integral:

a0f(x)dx=a0f(u)(du)=0af(u)du=0af(u)du\int_{-a}^0 f(x)\,dx = \int_a^0 f(-u)(-du) = \int_0^a -f(u)\,du = -\int_0^a f(u)\,du

Therefore aaf(x)dx=0af(x)dx+0af(x)dx=0\displaystyle\int_{-a}^a f(x)\,dx = -\int_0^a f(x)\,dx + \int_0^a f(x)\,dx = 0. \blacksquare

If you get this wrong, revise: Definite Integration and Areas — Section 4.

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tip

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