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Integration

Intuition

Integration is the reverse of differentiation — it accumulates tiny pieces into a whole: If differentiation breaks things down (finds the rate of change), integration builds things up (finds the total). The area under a speed-time graph is distance travelled. The area under a power-time graph is energy used. Integration sums up infinitely many infinitesimal contributions to find a total.

Why it matters: Integration is used to find areas, volumes, work done, probability, and many other quantities that involve accumulation. It’s the second fundamental operation of calculus and the complement to differentiation.

The key insight: The Fundamental Theorem of Calculus connects differentiation and integration — they are inverse operations. If 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). This means you can evaluate definite integrals by finding antiderivatives, without doing Riemann sums. This is the most important theorem in calculus.

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

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).

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 ffThen 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


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 = aAnd 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

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 = a$$u = g(a); when x = b$$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.

Caution: Warning After applying the formula, swap uu and dvdv. Example. Find xexdx\displaystyle\int x e^x\,dx.

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

\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 hhThe 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=sinxcosxdx=lncosx+C=lnsecx+C\int \tan x\,dx = \int \frac{\sin x}{\cos x}\,dx = -\ln|\cos x| + C = \ln|\sec x| + C


Problem Set

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

Solution 102(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.

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

Solution 2Intersection: 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.

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

Solution 3Let 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 0No absolute value needed.)

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

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

Solution 4Integration by parts: u = x$$dv = \sin x\,dx. Then du = dx$$v = -\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.

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

Solution 5h=204=0.5h = \dfrac{2-0}{4} = 0.5. Values: y_0 = 1$$y_1 = 1/(1+0.25) = 0.8$$y_2 = 1/(1+1) = 0.5$$y_3 = 1/(1+2.25) \approx 0.3077$$y_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: E2312×16×2=8192×2=1120.0833|E| \leq \dfrac{2^3}{12 \times 16} \times 2 = \dfrac{8}{192} \times 2 = \dfrac{1}{12} \approx 0.0833.

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

Problem 6Find xx+1dx\displaystyle\int \frac{x}{\sqrt{x+1}}\,dx.

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

u1udu=(u1/2u1/2)du=23u3/22u1/2+C=23(x+1)3/22(x+1)1/2+C\int \frac{u-1}{\sqrt{u}}\,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.

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

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

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

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

Solution 8y=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.

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

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

First: u = e^{2x}$$dv = \cos x\,dx. du = 2e^{2x}\,dx$$v = \sin x.

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

Second: u = e^{2x}$$dv = \sin x\,dx. du = 2e^{2x}\,dx$$v = -\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=e2x(sinx+2cosx)5+CI = \frac{e^{2x}(\sin x + 2\cos x)}{5} + C

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

Problem 10Evaluate 1elnxxdx\displaystyle\int_1^e \frac{\ln x}{x}\,dx.

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

lnxxdx=udu=u22+C=(lnx)22+C\int \frac{\ln x}{x}\,dx = \int u\,du = \frac{u^2}{2} + C = \frac{(\ln x)^2}{2} + C

[(lnx)22]1e=120=12\left[\frac{(\ln x)^2}{2}\right]_1^e = \frac{1}{2} - 0 = \frac{1}{2}

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

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

Solution 11A=t=0t=3ydxdtdt=032t2tdt=034t2dt=[4t33]03=4×273=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{4 \times 27}{3} = 36

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

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

Solution 12x2+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.

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

Solution 13If 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.


Common Pitfalls

  1. Forgetting the chain rule when integrating composite functions. Look for an inner function and its derivative.

  2. Confusing definite and indefinite integrals. Definite integrals give a numerical value; indefinite integrals give a family of functions.

  3. Incorrectly applying limits of integration after a substitution. Remember to change the limits to the new variable.

  4. Losing marks by not showing sufficient working. Always write out each step, especially in proof questions.

  5. Misreading the question, particularly with ‘hence’ vs ‘hence or otherwise’. The former requires using previous work.

  6. Forgetting to check that solutions satisfy the original equation (especially with squaring both sides or dividing by variables).

Summary

The key principles covered in this topic are linked in the sub-pages above. Focus on understanding the definitions, applying the formulas or frameworks, and evaluating strengths and limitations of each approach.

Worked Examples

Worked examples demonstrating the application of key concepts are covered in the detailed sub-pages linked above.

Cross-References

  • Differentiation — Integration reverses differentiation, and the Fundamental Theorem of Calculus connects rates of change to accumulated areas.
  • Trigonometry — Trigonometric identities are essential for integrating functions involving sin\sin, cos\cos, and tan\tan.
  • Numerical Methods — The trapezium rule and Simpson’s rule approximate definite integrals when exact integration is difficult.
  • Exponentials and Logarithms — The integral of 1/x1/x gives lnx\ln|x|, linking integration directly to logarithmic functions.