Board Coverage
Board Paper Notes AQA Paper 1, 2 Basic integration in P1; by parts, substitution in P2 Edexcel P1, P2 Similar split OCR (A) Paper 1, 2 Includes trapezium rule CIE (9709) P1, P2, P3 Basic in P1; by parts/substitution in P2/P3; further in P3
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 f f f from a a a to b b b is defined as the limit of Riemann
sums:
∫ a b f ( x ) d x = lim n → ∞ ∑ i = 1 n f ( x i ∗ ) Δ x \int_a^b f(x)\,dx = \lim_{n\to\infty}\sum_{i=1}^{n}f(x_i^*)\,\Delta x ∫ a b f ( x ) d x = lim n → ∞ ∑ i = 1 n f ( x i ∗ ) Δ x
where [ a , b ] [a,b] [ a , b ] is divided into n n n subintervals of width Δ x = b − a n \Delta x = \dfrac{b-a}{n} Δ x = n b − a , and x i ∗ x_i^* x i ∗ is
a sample point in the i i i -th subinterval.
Geometric picture. We divide the area under y = f ( x ) y = f(x) y = f ( x ) between x = a x = a x = a and x = b x = b x = b into n n n thin
rectangles. The sum of their areas approximates the total area. As n → ∞ n \to \infty n → ∞ (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) f ( x ) is a rate (like velocity), then ∫ a b f ( x ) d x \int_a^b f(x)\,dx ∫ a b f ( x ) d x 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 f f f is continuous on [ a , b ] [a,b] [ a , b ] , then
( P a r t 1 ) d d x ∫ a x f ( t ) d t = f ( x ) (\mathrm{Part 1})\quad \frac{d}{dx}\int_a^x f(t)\,dt = f(x) ( Part1 ) d x d ∫ a x f ( t ) d t = f ( x )
( P a r t 2 ) ∫ a b f ( x ) d x = F ( b ) − F ( a ) (\mathrm{Part 2})\quad \int_a^b f(x)\,dx = F(b) - F(a) ( Part2 ) ∫ a b f ( x ) d x = F ( b ) − F ( a )
where F F F is any antiderivative of f f f (i.e., F ′ ( x ) = f ( x ) F'(x) = f(x) F ′ ( x ) = f ( x ) ).
2.1 Sketch proof of Part 2
Let G ( x ) = ∫ a x f ( t ) d t G(x) = \int_a^x f(t)\,dt G ( x ) = ∫ a x f ( t ) d t . By Part 1, G ′ ( x ) = f ( x ) G'(x) = f(x) G ′ ( x ) = f ( x ) .
If F F F is any other antiderivative of f f f , then F ′ ( x ) = G ′ ( x ) = f ( x ) F'(x) = G'(x) = f(x) F ′ ( x ) = G ′ ( x ) = f ( x ) , so F ( x ) − G ( x ) = C F(x) - G(x) = C F ( x ) − G ( x ) = C (a
constant).
F ( x ) = G ( x ) + C ⟹ F ( b ) − F ( a ) = G ( b ) − G ( a ) = ∫ a b f ( t ) d t − 0 F(x) = G(x) + C \implies F(b) - F(a) = G(b) - G(a) = \int_a^b f(t)\,dt - 0 F ( x ) = G ( x ) + C ⟹ F ( b ) − F ( a ) = G ( b ) − G ( a ) = ∫ a b f ( t ) d t − 0
Hence ∫ a b f ( x ) d x = F ( b ) − F ( a ) \displaystyle\int_a^b f(x)\,dx = F(b) - F(a) ∫ a b f ( x ) d x = F ( b ) − F ( a ) . ■ \blacksquare ■
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 d d x ( x n + 1 n + 1 ) = x n \dfrac{d}{dx}\left(\dfrac{x^{n+1}}{n+1}\right) = x^n d x d ( n + 1 x n + 1 ) = x n for n ≠ − 1 n \neq -1 n = − 1 :
∫ x n d x = x n + 1 n + 1 + C , n ≠ − 1 \int x^n\,dx = \frac{x^{n+1}}{n+1} + C, \quad n \neq -1 ∫ x n d x = n + 1 x n + 1 + C , n = − 1
Reciprocal. Since d d x ln ∣ x ∣ = 1 x \dfrac{d}{dx}\ln|x| = \dfrac{1}{x} d x d ln ∣ x ∣ = x 1 :
∫ 1 x d x = ln ∣ x ∣ + C \int \frac{1}{x}\,dx = \ln|x| + C ∫ x 1 d x = ln ∣ x ∣ + C
Exponential. Since d d x e k x = k e k x \dfrac{d}{dx}e^{kx} = ke^{kx} d x d e k x = k e k x :
∫ e k x d x = 1 k e k x + C \int e^{kx}\,dx = \frac{1}{k}e^{kx} + C ∫ e k x d x = k 1 e k x + C
Trigonometric. Since d d x sin x = cos x \dfrac{d}{dx}\sin x = \cos x d x d sin x = cos x :
∫ cos x d x = sin x + C \int \cos x\,dx = \sin x + C ∫ cos x d x = sin x + C
∫ sin x d x = − cos x + C \int \sin x\,dx = -\cos x + C ∫ sin x d x = − cos x + C
∫ sec 2 x d x = tan x + C \int \sec^2 x\,dx = \tan x + C ∫ sec 2 x d x = tan x + C
3.2 Summary table
| f ( x ) f(x) f ( x ) | ∫ f ( x ) d x \int f(x)\,dx ∫ f ( x ) d x |
| ------------------- | -------------------------- | --- | ---- |
| x n x^n x n (n ≠ − 1 n \neq -1 n = − 1 ) | x n + 1 n + 1 + C \dfrac{x^{n+1}}{n+1} + C n + 1 x n + 1 + C |
| 1 / x 1/x 1/ x | ln ∣ x ∣ + C \ln | x | + C ln ∣ x ∣ + C |
| e k x e^{kx} e k x | 1 k e k x + C \dfrac{1}{k}e^{kx} + C k 1 e k x + C |
| cos x \cos x cos x | sin x + C \sin x + C sin x + C |
| sin x \sin x sin x | − cos x + C -\cos x + C − cos x + C |
| sec 2 x \sec^2 x sec 2 x | tan x + C \tan x + C tan x + C |
4. Definite Integration and Areas
4.1 Area under a curve
The area between y = f ( x ) y = f(x) y = f ( x ) , the x x x -axis, x = a x = a x = a , and x = b x = b x = b is
A = ∫ a b f ( x ) d x A = \int_a^b f(x)\,dx A = ∫ a b f ( x ) d x
provided f ( x ) ≥ 0 f(x) \geq 0 f ( x ) ≥ 0 on [ a , b ] [a,b] [ a , b ] .
4.2 Area between a curve and the x x x -axis
If f ( x ) f(x) f ( x ) changes sign on [ a , b ] [a,b] [ a , b ] , we must split the integral at each root:
A = ∫ a b ∣ f ( x ) ∣ d x A = \int_a^b |f(x)|\,dx A = ∫ a b ∣ f ( x ) ∣ d x
∫ a b f ( x ) d x \int_a^b f(x)\,dx ∫ a b f ( x ) d x gives the signed area (negative below the x x x -axis). To find the
actual geometric area, take the absolute value and integrate separately over regions where f f f is
positive and negative.
4.3 Area between two curves
The area between y = f ( x ) y = f(x) y = f ( x ) and y = g ( x ) y = g(x) y = g ( x ) from x = a x = a x = a to x = b x = b x = b (where f ( x ) ≥ g ( x ) f(x) \geq g(x) f ( x ) ≥ g ( x ) ) is
A = ∫ a b [ f ( x ) − g ( x ) ] d x A = \int_a^b [f(x) - g(x)]\,dx A = ∫ a b [ f ( x ) − g ( x )] d x
4.4 Area under a parametric curve
A = ∫ t 1 t 2 y d x d t d t A = \int_{t_1}^{t_2} y\,\frac{dx}{dt}\,dt A = ∫ t 1 t 2 y d t d x d t
5. Integration by Substitution
5.1 The method
Theorem. ∫ f ( g ( x ) ) g ′ ( x ) d x = F ( g ( x ) ) + C \displaystyle\int f(g(x))g'(x)\,dx = F(g(x)) + C ∫ f ( g ( x )) g ′ ( x ) d x = F ( g ( x )) + C where F ′ = f F' = f F ′ = f .
5.2 Proof via the chain rule
Let u = g ( x ) u = g(x) u = g ( x ) . By the chain rule,
d d x F ( u ) = F ′ ( u ) d u d x = f ( u ) d u d x = 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) d x d F ( u ) = F ′ ( u ) d x d u = f ( u ) d x d u = f ( g ( x )) g ′ ( x ) .
Therefore ∫ f ( g ( x ) ) g ′ ( x ) d x = F ( g ( x ) ) + C \int f(g(x))g'(x)\,dx = F(g(x)) + C ∫ f ( g ( x )) g ′ ( x ) d x = F ( g ( x )) + C . ■ \blacksquare ■
In practice:
Choose a substitution u = g ( x ) u = g(x) u = g ( x ) .
Compute d u = g ′ ( x ) d x du = g'(x)\,dx d u = g ′ ( x ) d x .
Rewrite the integral entirely in terms of u u u .
Integrate, then substitute back.
Example. Find ∫ 2 x x 2 + 1 d x \displaystyle\int 2x\sqrt{x^2+1}\,dx ∫ 2 x x 2 + 1 d x .
Let u = x 2 + 1 u = x^2 + 1 u = x 2 + 1 , d u = 2 x d x du = 2x\,dx d u = 2 x d x .
∫ 2 x x 2 + 1 d x = ∫ u d u = 2 3 u 3 / 2 + C = 2 3 ( x 2 + 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 ∫ 2 x x 2 + 1 d x = ∫ u d u = 3 2 u 3/2 + C = 3 2 ( x 2 + 1 ) 3/2 + C
tip
g ( x ) \sqrt{g(x)} g ( x ) and g ′ ( x ) g'(x) g ′ ( x ) in the integrand, try u = g ( x ) u = g(x) u = g ( x ) .
5.3 Definite integrals with substitution
For a definite integral, you can either:
Substitute back to x x x before evaluating, or
Change the limits: when x = a x = a x = a , u = g ( a ) u = g(a) u = g ( a ) ; when x = b x = b x = b , u = g ( b ) u = g(b) u = g ( b ) .
6. Integration by Parts
Theorem. ∫ u d v = u v − ∫ v d u \displaystyle\int u\,dv = uv - \int v\,du ∫ u d v = uv − ∫ v d u
6.2 Proof via the product rule
From the product rule: d d x ( u v ) = u d v d x + v d u d x \dfrac{d}{dx}(uv) = u\dfrac{dv}{dx} + v\dfrac{du}{dx} d x d ( uv ) = u d x d v + v d x d u .
Integrating both sides:
u v = ∫ u d v d x d x + ∫ v d u d x d x uv = \int u\frac{dv}{dx}\,dx + \int v\frac{du}{dx}\,dx uv = ∫ u d x d v d x + ∫ v d x d u d x
∫ u d v d x d x = u v − ∫ v d u d x d x \int u\frac{dv}{dx}\,dx = uv - \int v\frac{du}{dx}\,dx ∫ u d x d v d x = uv − ∫ v d x d u d x
i.e., ∫ u d v = u v − ∫ v d u \displaystyle\int u\,dv = uv - \int v\,du ∫ u d v = uv − ∫ v d u . ■ \blacksquare ■
6.3 Choosing u u u and d v dv d v
Use the mnemonic LIATE (Logarithmic, Inverse trig, Algebraic, Trig, Exponential). Choose u u u
from the leftmost category that appears.
warning
after applying the formula, swap u u u and d v dv d v .
Example. Find ∫ x e x d x \displaystyle\int x e^x\,dx ∫ x e x d x .
Let u = x u = x u = x , d v = e x d x dv = e^x\,dx d v = e x d x . Then d u = d x du = dx d u = d x , v = e x v = e^x v = e x .
∫ x e x d x = x e x − ∫ e x d x = x e x − e x + C = e x ( x − 1 ) + C \int x e^x\,dx = x e^x - \int e^x\,dx = x e^x - e^x + C = e^x(x-1) + C ∫ x e x d x = x e x − ∫ e x d x = x e x − e x + C = e x ( x − 1 ) + C
Integration by parts can produce reduction formulas relating I n I_n I n to I n − 1 I_{n-1} I n − 1 .
Example. Find a reduction formula for I n = ∫ x n e x d x I_n = \displaystyle\int x^n e^x\,dx I n = ∫ x n e x d x .
Let u = x n u = x^n u = x n , d v = e x d x dv = e^x\,dx d v = e x d x . Then d u = n x n − 1 d x du = nx^{n-1}\,dx d u = n x n − 1 d x , v = e x v = e^x v = e x .
I n = x n e x − n ∫ x n − 1 e x d x = x n e x − n I n − 1 I_n = x^n e^x - n\int x^{n-1} e^x\,dx = x^n e^x - nI_{n-1} I n = x n e x − n ∫ x n − 1 e x d x = x n e x − n I n − 1
This gives I n = x n e x − n I n − 1 I_n = x^n e^x - nI_{n-1} I n = x n e x − n I n − 1 , allowing us to reduce any I n I_n I n to I 0 = e x + C I_0 = e^x + C I 0 = e x + C .
7. The Trapezium Rule
To approximate ∫ a b f ( x ) d x \displaystyle\int_a^b f(x)\,dx ∫ a b f ( x ) d x , divide [ a , b ] [a,b] [ a , b ] into n n n equal strips of width
h = b − a n h = \dfrac{b-a}{n} h = n b − a :
∫ a b f ( x ) d x ≈ h 2 [ y 0 + 2 y 1 + 2 y 2 + ⋯ + 2 y n − 1 + y n ] \int_a^b f(x)\,dx \approx \frac{h}{2}\left[y_0 + 2y_1 + 2y_2 + \cdots + 2y_{n-1} + y_n\right] ∫ a b f ( x ) d x ≈ 2 h [ y 0 + 2 y 1 + 2 y 2 + ⋯ + 2 y n − 1 + y n ]
where y i = f ( a + i h ) y_i = f(a + ih) y i = f ( a + ih ) .
7.2 Derivation
Each strip is approximated by a trapezium. The area of the i i i -th trapezium is:
A i = h 2 ( y i − 1 + y i ) A_i = \frac{h}{2}(y_{i-1} + y_i) A i = 2 h ( y i − 1 + y i )
Summing all trapezia:
T o t a l = h 2 ( y 0 + y 1 ) + h 2 ( y 1 + y 2 ) + ⋯ + h 2 ( y n − 1 + y n ) = h 2 [ y 0 + 2 y 1 + 2 y 2 + ⋯ + 2 y n − 1 + y n ] \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} Total = 2 h ( y 0 + y 1 ) + 2 h ( y 1 + y 2 ) + ⋯ + 2 h ( y n − 1 + y n ) = 2 h [ y 0 + 2 y 1 + 2 y 2 + ⋯ + 2 y n − 1 + y n ]
7.3 Error bound
If f ′ ′ f'' f ′′ is continuous on [ a , b ] [a,b] [ a , b ] and ∣ f ′ ′ ( x ) ∣ ≤ M |f''(x)| \leq M ∣ f ′′ ( x ) ∣ ≤ M for all x ∈ [ a , b ] x \in [a,b] x ∈ [ a , b ] , then the error E E E
satisfies
∣ E ∣ ≤ ( b − a ) 3 12 n 2 M |E| \leq \frac{(b-a)^3}{12n^2}M ∣ E ∣ ≤ 12 n 2 ( b − a ) 3 M
Proof (sketch). For a single strip of width h h h , the trapezium rule gives area
h 2 [ f ( a ) + f ( a + h ) ] \dfrac{h}{2}[f(a) + f(a+h)] 2 h [ f ( a ) + f ( a + h )] , while the true area is ∫ a a + h f ( x ) d x \int_a^{a+h}f(x)\,dx ∫ a a + h f ( x ) d x . By Taylor's theorem,
the error per strip is − h 3 12 f ′ ′ ( ξ ) -\dfrac{h^3}{12}f''(\xi) − 12 h 3 f ′′ ( ξ ) for some ξ ∈ ( a , a + h ) \xi \in (a, a+h) ξ ∈ ( a , a + h ) . Summing n n n strips
and using the bound ∣ f ′ ′ ∣ ≤ M |f''| \leq M ∣ f ′′ ∣ ≤ M :
∣ E ∣ ≤ n ⋅ h 3 12 M = n ⋅ ( b − a ) 3 12 n 3 M = ( b − a ) 3 12 n 2 M ■ |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 ∣ E ∣ ≤ n ⋅ 12 h 3 M = n ⋅ 12 n 3 ( b − a ) 3 M = 12 n 2 ( b − a ) 3 M ■
Intuition. The error decreases as 1 / n 2 1/n^2 1/ n 2 — doubling the number of strips quarters the error.
The error also depends on how curved the function is (via f ′ ′ f'' f ′′ ). For a straight line (f ′ ′ = 0 f'' = 0 f ′′ = 0 ),
the trapezium rule is exact.
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 )
∫ f ′ ( x ) f ( x ) d x = ln ∣ f ( x ) ∣ + C \int \frac{f'(x)}{f(x)}\,dx = \ln|f(x)| + C ∫ f ( x ) f ′ ( x ) d x = ln ∣ f ( x ) ∣ + C
This follows from the substitution u = f ( x ) u = f(x) u = f ( x ) .
8.2 Partial fractions
Rational functions can be integrated by first decomposing into partial fractions.
Example.
∫ 1 x 2 − 1 d x = ∫ 1 2 ( 1 x − 1 − 1 x + 1 ) d x = 1 2 ln ∣ x − 1 x + 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 ∫ x 2 − 1 1 d x = ∫ 2 1 ( x − 1 1 − x + 1 1 ) d x = 2 1 ln x + 1 x − 1 + C .
∫ tan x d x = ∫ ◆ L B ◆ sin x ◆ R B ◆◆ L B ◆ cos x ◆ R B ◆ d x = − ln ∣ cos x ∣ + C = ln ∣ sec x ∣ + C \int \tan x\,dx = \int \frac◆LB◆\sin x◆RB◆◆LB◆\cos x◆RB◆\,dx = -\ln|\cos x| + C = \ln|\sec x| + C ∫ tan x d x = ∫ L ◆ B ◆ sin x ◆ R B ◆◆ L B ◆ cos x ◆ R B ◆ d x = − ln ∣ cos x ∣ + C = ln ∣ sec x ∣ + C
Problem Set
Details
Problem 1
Evaluate
∫ 0 2 ( 3 x 2 − 4 x + 1 ) d x \displaystyle\int_0^2 (3x^2 - 4x + 1)\,dx ∫ 0 2 ( 3 x 2 − 4 x + 1 ) d x .
Details
Solution 1
∫ 0 2 ( 3 x 2 − 4 x + 1 ) d x = [ x 3 − 2 x 2 + x ] 0 2 = ( 8 − 8 + 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 ∫ 0 2 ( 3 x 2 − 4 x + 1 ) d x = [ x 3 − 2 x 2 + x ] 0 2 = ( 8 − 8 + 2 ) − 0 = 2
If you get this wrong, revise: Standard Integrals — Section 3.
Details
Problem 2
Find the area enclosed between
y = x 2 y = x^2 y = x 2 and
y = 2 x y = 2x y = 2 x .
Details
Solution 2
Intersection:
x 2 = 2 x ⟹ x ( x − 2 ) = 0 ⟹ x = 0 , 2 x^2 = 2x \implies x(x-2) = 0 \implies x = 0, 2 x 2 = 2 x ⟹ x ( x − 2 ) = 0 ⟹ x = 0 , 2 .
On [ 0 , 2 ] [0,2] [ 0 , 2 ] : 2 x ≥ x 2 2x \geq x^2 2 x ≥ x 2 (since 2 x − x 2 = x ( 2 − x ) ≥ 0 2x - x^2 = x(2-x) \geq 0 2 x − x 2 = x ( 2 − x ) ≥ 0 ).
A = ∫ 0 2 ( 2 x − x 2 ) d x = [ x 2 − x 3 3 ] 0 2 = 4 − 8 3 = 4 3 A = \int_0^2 (2x - x^2)\,dx = \left[x^2 - \frac{x^3}{3}\right]_0^2 = 4 - \frac{8}{3} = \frac{4}{3} A = ∫ 0 2 ( 2 x − x 2 ) d x = [ x 2 − 3 x 3 ] 0 2 = 4 − 3 8 = 3 4
If you get this wrong, revise:
Definite Integration and Areas — Section 4.3.
Details
Problem 3
Find
∫ 2 x x 2 + 3 d x \displaystyle\int \frac{2x}{x^2+3}\,dx ∫ x 2 + 3 2 x d x .
Details
Solution 3
Let
u = x 2 + 3 u = x^2 + 3 u = x 2 + 3 ,
d u = 2 x d x du = 2x\,dx d u = 2 x d x .
∫ 2 x x 2 + 3 d x = ∫ 1 u d u = ln ∣ u ∣ + C = ln ( x 2 + 3 ) + C \int \frac{2x}{x^2+3}\,dx = \int \frac{1}{u}\,du = \ln|u| + C = \ln(x^2+3) + C ∫ x 2 + 3 2 x d x = ∫ u 1 d u = ln ∣ u ∣ + C = ln ( x 2 + 3 ) + C
(Since x 2 + 3 > 0 x^2+3 \gt{} 0 x 2 + 3 > 0 , no absolute value needed.)
If you get this wrong, revise: Integration by Substitution —
Section 5.
Details
Problem 4
Evaluate
∫ 0 π / 2 x sin x d x \displaystyle\int_0^{\pi/2} x\sin x\,dx ∫ 0 π /2 x sin x d x .
Details
Solution 4
Integration by parts:
u = x u = x u = x ,
d v = sin x d x dv = \sin x\,dx d v = sin x d x . Then
d u = d x du = dx d u = d x ,
v = − cos x v = -\cos x v = − cos x .
∫ x sin x d x = − x cos x + ∫ cos x d x = − x cos x + sin x + C \int x\sin x\,dx = -x\cos x + \int \cos x\,dx = -x\cos x + \sin x + C ∫ x sin x d x = − x cos x + ∫ cos x d x = − x cos x + sin x + C
[ − x cos x + sin x ] 0 π / 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 [ − x cos x + sin x ] 0 π /2 = ( 0 + 1 ) − ( 0 + 0 ) = 1
If you get this wrong, revise: Integration by Parts — Section 6.
Details
Problem 5
Use the trapezium rule with 4 strips to approximate
∫ 0 2 1 1 + x 2 d x \displaystyle\int_0^2 \frac{1}{1+x^2}\,dx ∫ 0 2 1 + x 2 1 d x , and give an error bound given
∣ f ′ ′ ( x ) ∣ ≤ 2 |f''(x)| \leq 2 ∣ f ′′ ( x ) ∣ ≤ 2 on
[ 0 , 2 ] [0,2] [ 0 , 2 ] .
Details
Solution 5
h = 2 − 0 4 = 0.5 h = \dfrac{2-0}{4} = 0.5 h = 4 2 − 0 = 0.5 . Values:
y 0 = 1 y_0 = 1 y 0 = 1 ,
y 1 = 1 / ( 1 + 0.25 ) = 0.8 y_1 = 1/(1+0.25) = 0.8 y 1 = 1/ ( 1 + 0.25 ) = 0.8 ,
y 2 = 1 / ( 1 + 1 ) = 0.5 y_2 = 1/(1+1) = 0.5 y 2 = 1/ ( 1 + 1 ) = 0.5 ,
y 3 = 1 / ( 1 + 2.25 ) ≈ 0.3077 y_3 = 1/(1+2.25) \approx 0.3077 y 3 = 1/ ( 1 + 2.25 ) ≈ 0.3077 ,
y 4 = 1 / 5 = 0.2 y_4 = 1/5 = 0.2 y 4 = 1/5 = 0.2 .
A p p r o x = 0.5 2 [ 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 × 4.4154 ≈ 1.104 \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 Approx = 2 0.5 [ 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 × 4.4154 ≈ 1.104
Error bound:
∣ E ∣ ≤ ◆ L B ◆ 2 3 ◆ R B ◆◆ L B ◆ 12 × 16 ◆ R B ◆ × 2 = 8 192 × 2 = 1 12 ≈ 0.0833 |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 ∣ E ∣ ≤ L ◆ B ◆ 2 3 ◆ R B ◆◆ L B ◆12 × 16◆ R B ◆ × 2 = 192 8 × 2 = 12 1 ≈ 0.0833 .
If you get this wrong, revise: The Trapezium Rule — Section 7.
Details
Problem 6
Find
∫ ◆ L B ◆ x ◆ R B ◆◆ L B ◆ x + 1 ◆ R B ◆ d x \displaystyle\int \frac◆LB◆x◆RB◆◆LB◆\sqrt{x+1}◆RB◆\,dx ∫ L ◆ B ◆ x ◆ R B ◆◆ L B ◆ x + 1 ◆ R B ◆ d x .
Details
Solution 6
Let
u = x + 1 u = x+1 u = x + 1 , so
x = u − 1 x = u-1 x = u − 1 and
d x = d u dx = du d x = d u .
∫ ◆ L B ◆ u − 1 ◆ R B ◆◆ L B ◆ u ◆ R B ◆ d u = ∫ ( u 1 / 2 − u − 1 / 2 ) d u = 2 3 u 3 / 2 − 2 u 1 / 2 + C = 2 3 ( x + 1 ) 3 / 2 − 2 ( 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 ∫ L ◆ B ◆ u − 1◆ R B ◆◆ L B ◆ u ◆ R B ◆ d u = ∫ ( u 1/2 − u − 1/2 ) d u = 3 2 u 3/2 − 2 u 1/2 + C = 3 2 ( x + 1 ) 3/2 − 2 ( x + 1 ) 1/2 + C
If you get this wrong, revise: Integration by Substitution —
Section 5.
Details
Problem 7
Find a reduction formula for
I n = ∫ 0 π / 2 sin n x d x I_n = \displaystyle\int_0^{\pi/2} \sin^n x\,dx I n = ∫ 0 π /2 sin n x d x for
n ≥ 2 n \geq 2 n ≥ 2 .
Details
Solution 7
I n = ∫ 0 π / 2 sin n − 1 x ⋅ sin x d x I_n = \int_0^{\pi/2}\sin^{n-1}x \cdot \sin x\,dx I n = ∫ 0 π /2 sin n − 1 x ⋅ sin x d x .
Let u = sin n − 1 x u = \sin^{n-1}x u = sin n − 1 x , d v = sin x d x dv = \sin x\,dx d v = sin x d x . d u = ( n − 1 ) sin n − 2 x cos x d x du = (n-1)\sin^{n-2}x\cos x\,dx d u = ( n − 1 ) sin n − 2 x cos x d x , v = − cos x v = -\cos x v = − cos x .
I n = [ − sin n − 1 x cos x ] 0 π / 2 + ( n − 1 ) ∫ 0 π / 2 sin n − 2 x cos 2 x d x I_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 I n = [ − sin n − 1 x cos x ] 0 π /2 + ( n − 1 ) ∫ 0 π /2 sin n − 2 x cos 2 x d x
The boundary term vanishes (since cos ( π / 2 ) = 0 \cos(\pi/2) = 0 cos ( π /2 ) = 0 and sin 0 = 0 \sin 0 = 0 sin 0 = 0 ). Using
cos 2 x = 1 − sin 2 x \cos^2 x = 1 - \sin^2 x cos 2 x = 1 − sin 2 x :
I n = ( n − 1 ) ∫ 0 π / 2 sin n − 2 x ( 1 − sin 2 x ) d x = ( n − 1 ) ( I n − 2 − I n ) I_n = (n-1)\int_0^{\pi/2}\sin^{n-2}x(1-\sin^2 x)\,dx = (n-1)(I_{n-2} - I_n) I n = ( n − 1 ) ∫ 0 π /2 sin n − 2 x ( 1 − sin 2 x ) d x = ( n − 1 ) ( I n − 2 − I n )
I n = ( n − 1 ) I n − 2 − ( n − 1 ) I n I_n = (n-1)I_{n-2} - (n-1)I_n I n = ( n − 1 ) I n − 2 − ( n − 1 ) I n n I n = ( n − 1 ) I n − 2 nI_n = (n-1)I_{n-2} n I n = ( n − 1 ) I n − 2 I n = n − 1 n I n − 2 I_n = \frac{n-1}{n}I_{n-2} I n = n n − 1 I n − 2
If you get this wrong, revise: Reduction Formulas — Section 6.4.
Details
Problem 8
Find the total area between
y = x ( x − 2 ) ( x + 1 ) y = x(x-2)(x+1) y = x ( x − 2 ) ( x + 1 ) and the
x x x -axis.
Details
Solution 8
y = x ( x − 2 ) ( x + 1 ) = x 3 − x 2 − 2 x y = x(x-2)(x+1) = x^3 - x^2 - 2x y = x ( x − 2 ) ( x + 1 ) = x 3 − x 2 − 2 x . Roots at
x = − 1 , 0 , 2 x = -1, 0, 2 x = − 1 , 0 , 2 .
∫ − 1 0 ( x 3 − x 2 − 2 x ) d x = [ x 4 4 − x 3 3 − x 2 ] − 1 0 = 0 − ( 1 4 + 1 3 − 1 ) = − ( 3 + 4 − 12 12 ) = 5 12 \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} ∫ − 1 0 ( x 3 − x 2 − 2 x ) d x = [ 4 x 4 − 3 x 3 − x 2 ] − 1 0 = 0 − ( 4 1 + 3 1 − 1 ) = − ( 12 3 + 4 − 12 ) = 12 5
∫ 0 2 ( x 3 − x 2 − 2 x ) d x = [ x 4 4 − x 3 3 − x 2 ] 0 2 = ( 4 − 8 3 − 4 ) − 0 = − 8 3 \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} ∫ 0 2 ( x 3 − x 2 − 2 x ) d x = [ 4 x 4 − 3 x 3 − x 2 ] 0 2 = ( 4 − 3 8 − 4 ) − 0 = − 3 8
Total area = 5 12 + 8 3 = 5 + 32 12 = 37 12 \dfrac{5}{12} + \dfrac{8}{3} = \dfrac{5+32}{12} = \dfrac{37}{12} 12 5 + 3 8 = 12 5 + 32 = 12 37 .
If you get this wrong, revise:
Definite Integration and Areas — Section 4.2.
Details
Problem 9
Find
∫ e 2 x cos x d x \displaystyle\int e^{2x}\cos x\,dx ∫ e 2 x cos x d x .
Details
Solution 9
Apply integration by parts twice. Let
I = ∫ e 2 x cos x d x I = \int e^{2x}\cos x\,dx I = ∫ e 2 x cos x d x .
First: u = e 2 x u = e^{2x} u = e 2 x , d v = cos x d x dv = \cos x\,dx d v = cos x d x . d u = 2 e 2 x d x du = 2e^{2x}\,dx d u = 2 e 2 x d x , v = sin x v = \sin x v = sin x .
I = e 2 x sin x − 2 ∫ e 2 x sin x d x I = e^{2x}\sin x - 2\int e^{2x}\sin x\,dx I = e 2 x sin x − 2 ∫ e 2 x sin x d x .
Second: u = e 2 x u = e^{2x} u = e 2 x , d v = sin x d x dv = \sin x\,dx d v = sin x d x . d u = 2 e 2 x d x du = 2e^{2x}\,dx d u = 2 e 2 x d x , v = − cos x v = -\cos x v = − cos x .
∫ e 2 x sin x d x = − e 2 x cos x + 2 ∫ e 2 x cos x d x = − e 2 x cos x + 2 I \int e^{2x}\sin x\,dx = -e^{2x}\cos x + 2\int e^{2x}\cos x\,dx = -e^{2x}\cos x + 2I ∫ e 2 x sin x d x = − e 2 x cos x + 2 ∫ e 2 x cos x d x = − e 2 x cos x + 2 I .
I = e 2 x sin x − 2 ( − e 2 x cos x + 2 I ) = e 2 x sin x + 2 e 2 x cos x − 4 I I = e^{2x}\sin x - 2(-e^{2x}\cos x + 2I) = e^{2x}\sin x + 2e^{2x}\cos x - 4I I = e 2 x sin x − 2 ( − e 2 x cos x + 2 I ) = e 2 x sin x + 2 e 2 x cos x − 4 I .
5 I = e 2 x ( sin x + 2 cos x ) 5I = e^{2x}(\sin x + 2\cos x) 5 I = e 2 x ( sin x + 2 cos x ) .
I = ◆ L B ◆ e 2 x ( sin x + 2 cos x ) ◆ R B ◆◆ L B ◆ 5 ◆ R B ◆ + C I = \frac◆LB◆e^{2x}(\sin x + 2\cos x)◆RB◆◆LB◆5◆RB◆ + C I = L ◆ B ◆ e 2 x ( sin x + 2 cos x ) ◆ R B ◆◆ L B ◆5◆ R B ◆ + C
If you get this wrong, revise: Integration by Parts — Section 6.
Details
Problem 10
Evaluate
∫ 1 e ◆ L B ◆ ln x ◆ R B ◆◆ L B ◆ x ◆ R B ◆ d x \displaystyle\int_1^e \frac◆LB◆\ln x◆RB◆◆LB◆x◆RB◆\,dx ∫ 1 e L ◆ B ◆ ln x ◆ R B ◆◆ L B ◆ x ◆ R B ◆ d x .
Details
Solution 10
Let
u = ln x u = \ln x u = ln x ,
d u = 1 x d x du = \dfrac{1}{x}\,dx d u = x 1 d x .
∫ ◆ L B ◆ ln x ◆ R B ◆◆ L B ◆ x ◆ R B ◆ d x = ∫ u d u = u 2 2 + C = ◆ L B ◆ ( ln x ) 2 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ + 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 ∫ L ◆ B ◆ ln x ◆ R B ◆◆ L B ◆ x ◆ R B ◆ d x = ∫ u d u = 2 u 2 + C = L ◆ B ◆ ( ln x ) 2 ◆ R B ◆◆ L B ◆2◆ R B ◆ + C
[ ◆ L B ◆ ( ln x ) 2 ◆ R B ◆◆ L B ◆ 2 ◆ R B ◆ ] 1 e = 1 2 − 0 = 1 2 \left[\frac◆LB◆(\ln x)^2◆RB◆◆LB◆2◆RB◆\right]_1^e = \frac{1}{2} - 0 = \frac{1}{2} [ L ◆ B ◆ ( ln x ) 2 ◆ R B ◆◆ L B ◆2◆ R B ◆ ] 1 e = 2 1 − 0 = 2 1
If you get this wrong, revise: Integration by Substitution —
Section 5.
Details
Problem 11
The curve
C C C has parametric equations
x = t 2 x = t^2 x = t 2 ,
y = 2 t y = 2t y = 2 t for
0 ≤ t ≤ 3 0 \leq t \leq 3 0 ≤ t ≤ 3 . Find the area under
C C C .
Details
Solution 11
A = ∫ t = 0 t = 3 y d x d t d t = ∫ 0 3 2 t ⋅ 2 t d t = ∫ 0 3 4 t 2 d t = [ 4 t 3 3 ] 0 3 = ◆ L B ◆ 4 × 27 ◆ R B ◆◆ L B ◆ 3 ◆ R B ◆ = 36 A = \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 A = ∫ t = 0 t = 3 y d t d x d t = ∫ 0 3 2 t ⋅ 2 t d t = ∫ 0 3 4 t 2 d t = [ 3 4 t 3 ] 0 3 = L ◆ B ◆4 × 27◆ R B ◆◆ L B ◆3◆ R B ◆ = 36
If you get this wrong, revise:
Definite Integration and Areas — Section 4.4.
Details
Problem 12
Find
∫ 3 x + 5 x 2 + 4 x + 3 d x \displaystyle\int \frac{3x+5}{x^2+4x+3}\,dx ∫ x 2 + 4 x + 3 3 x + 5 d x .
Details
Solution 12
x 2 + 4 x + 3 = ( x + 1 ) ( x + 3 ) x^2 + 4x + 3 = (x+1)(x+3) x 2 + 4 x + 3 = ( x + 1 ) ( x + 3 ) .
3 x + 5 ( x + 1 ) ( x + 3 ) = A x + 1 + B x + 3 \frac{3x+5}{(x+1)(x+3)} = \frac{A}{x+1} + \frac{B}{x+3} ( x + 1 ) ( x + 3 ) 3 x + 5 = x + 1 A + x + 3 B
3 x + 5 = A ( x + 3 ) + B ( x + 1 ) 3x + 5 = A(x+3) + B(x+1) 3 x + 5 = A ( x + 3 ) + B ( x + 1 ) .
x = − 1 x = -1 x = − 1 : 2 = 2 A ⟹ A = 1 2 = 2A \implies A = 1 2 = 2 A ⟹ A = 1 . x = − 3 x = -3 x = − 3 : − 4 = − 2 B ⟹ B = 2 -4 = -2B \implies B = 2 − 4 = − 2 B ⟹ B = 2 .
∫ 1 x + 1 + 2 x + 3 d x = ln ∣ x + 1 ∣ + 2 ln ∣ x + 3 ∣ + C \int \frac{1}{x+1} + \frac{2}{x+3}\,dx = \ln|x+1| + 2\ln|x+3| + C ∫ x + 1 1 + x + 3 2 d x = ln ∣ x + 1∣ + 2 ln ∣ x + 3∣ + C
If you get this wrong, revise: Partial Fractions — Section 8.2.
Details
Problem 13
Sketch proof: explain why
∫ − a a f ( x ) d x = 0 \displaystyle\int_{-a}^a f(x)\,dx = 0 ∫ − a a f ( x ) d x = 0 when
f f f is an odd function.
Details
Solution 13
If
f f f is odd, then
f ( − x ) = − f ( x ) f(-x) = -f(x) f ( − x ) = − f ( x ) .
∫ − a a f ( x ) d x = ∫ − a 0 f ( x ) d x + ∫ 0 a f ( x ) d x \int_{-a}^a f(x)\,dx = \int_{-a}^0 f(x)\,dx + \int_0^a f(x)\,dx ∫ − a a f ( x ) d x = ∫ − a 0 f ( x ) d x + ∫ 0 a f ( x ) d x
Let u = − x u = -x u = − x in the first integral:
∫ − a 0 f ( x ) d x = ∫ a 0 f ( − u ) ( − d u ) = ∫ 0 a − f ( u ) d u = − ∫ 0 a f ( u ) d u \int_{-a}^0 f(x)\,dx = \int_a^0 f(-u)(-du) = \int_0^a -f(u)\,du = -\int_0^a f(u)\,du ∫ − a 0 f ( x ) d x = ∫ a 0 f ( − u ) ( − d u ) = ∫ 0 a − f ( u ) d u = − ∫ 0 a f ( u ) d u
Therefore ∫ − a a f ( x ) d x = − ∫ 0 a f ( x ) d x + ∫ 0 a f ( x ) d x = 0 \displaystyle\int_{-a}^a f(x)\,dx = -\int_0^a f(x)\,dx + \int_0^a f(x)\,dx = 0 ∫ − a a f ( x ) d x = − ∫ 0 a f ( x ) d x + ∫ 0 a f ( x ) d x = 0 .
■ \blacksquare ■
If you get this wrong, revise:
Definite Integration and Areas — Section 4.
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