Antidifferentiation Review
Integration (antidifferentiation) is the reverse process of differentiation. If F ′ ( x ) = f ( x ) F'(x) = f(x) F ′ ( x ) = f ( x ) ,
then:
∫ f ( x ) d x = F ( x ) + C \int f(x)\,dx = F(x) + C ∫ f ( x ) d x = F ( x ) + C
where C C C is the constant of integration.
Basic Integration Rules
Rule Formula Power rule ∫ x n d x = x n + 1 n + 1 + C ( n ≠ − 1 ) \displaystyle\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 ∫ 1 x d x = ln ∥ x ∥ + C \displaystyle\int \frac{1}{x}\,dx = \ln\|x\| + C ∫ x 1 d x = ln ∥ x ∥ + C Constant multiple ∫ k f ( x ) d x = k ∫ f ( x ) d x \displaystyle\int kf(x)\,dx = k\int f(x)\,dx ∫ k f ( x ) d x = k ∫ f ( x ) d x Sum/difference ∫ [ f ( x ) ± g ( x ) ] d x = ∫ f ( x ) d x ± ∫ g ( x ) d x \displaystyle\int [f(x) \pm g(x)]\,dx = \int f(x)\,dx \pm \int g(x)\,dx ∫ [ f ( x ) ± g ( x )] d x = ∫ f ( x ) d x ± ∫ g ( x ) d x
Standard Integrals
f ( x ) f(x) f ( x ) ∫ f ( x ) d x \int f(x)\,dx ∫ f ( x ) d x e x e^x e x e x + C e^x + C e x + C a x a^x a x a x ln a + C \dfrac{a^x}{\ln a} + C ln a a x + C sin x \sin x sin x − cos x + C -\cos x + C − cos x + C cos x \cos x cos x sin x + C \sin x + C sin x + C sec 2 x \sec^2 x sec 2 x tan x + C \tan x + C tan x + C csc 2 x \csc^2 x csc 2 x − cot x + C -\cot x + C − cot x + C sec x tan x \sec x \tan x sec x tan x sec x + C \sec x + C sec x + C 1 1 − x 2 \dfrac{1}{\sqrt{1-x^2}} 1 − x 2 1 arcsin x + C \arcsin x + C arcsin x + C 1 1 + x 2 \dfrac{1}{1+x^2} 1 + x 2 1 arctan x + C \arctan x + C arctan x + C
The Fundamental Theorem of Calculus
First Fundamental Theorem
If f f f is continuous on [ a , b ] [a, b] [ a , b ] and F ′ ( x ) = f ( x ) F'(x) = f(x) F ′ ( x ) = f ( x ) , then:
∫ a b f ( x ) d x = F ( b ) − F ( a ) \int_a^b f(x)\,dx = F(b) - F(a) ∫ a b f ( x ) d x = F ( b ) − F ( a )
Second Fundamental Theorem
If f f f is continuous on an interval containing a a a , then:
\frac{d}`\{dx}`\left[\int_a^x f(t)\,dt\right] = f(x)
Definite Integrals
Properties
For continuous functions f f f and g g g on [ a , b ] [a, b] [ a , b ] :
∫ a b k f ( x ) d x = k ∫ a b f ( x ) d x \displaystyle\int_a^b kf(x)\,dx = k\int_a^b f(x)\,dx ∫ a b k f ( x ) d x = k ∫ a b f ( x ) d x
∫ a b [ f ( x ) ± g ( x ) ] d x = ∫ a b f ( x ) d x ± ∫ a b g ( x ) d x \displaystyle\int_a^b [f(x) \pm g(x)]\,dx = \int_a^b f(x)\,dx \pm \int_a^b g(x)\,dx ∫ a b [ f ( x ) ± g ( x )] d x = ∫ a b f ( x ) d x ± ∫ a b g ( x ) d x
∫ a a f ( x ) d x = 0 \displaystyle\int_a^a f(x)\,dx = 0 ∫ a a f ( x ) d x = 0
∫ a b f ( x ) d x = − ∫ b a f ( x ) d x \displaystyle\int_a^b f(x)\,dx = -\int_b^a f(x)\,dx ∫ a b f ( x ) d x = − ∫ b a f ( x ) d x
∫ a b f ( x ) d x = ∫ a c f ( x ) d x + ∫ c b f ( x ) d x \displaystyle\int_a^b f(x)\,dx = \int_a^c f(x)\,dx + \int_c^b f(x)\,dx ∫ a b f ( x ) d x = ∫ a c f ( x ) d x + ∫ c b f ( x ) d x for any c c c
Even and Odd Functions
If f f f is even (f ( − x ) = f ( x ) f(-x) = f(x) f ( − x ) = f ( x ) ):
∫ − a a f ( x ) d x = 2 ∫ 0 a f ( x ) d x \int_{-a}^{a} f(x)\,dx = 2\int_0^a f(x)\,dx ∫ − a a f ( x ) d x = 2 ∫ 0 a f ( x ) d x
If f f f is odd (f ( − x ) = − f ( x ) f(-x) = -f(x) f ( − x ) = − f ( x ) ):
∫ − a a f ( x ) d x = 0 \int_{-a}^{a} f(x)\,dx = 0 ∫ − a a f ( x ) d x = 0
Always check if a function is odd or even before integrating over a symmetric interval. This can
save significant computation time.
Evaluate ∫ − 2 2 x 3 cos ( x 2 ) d x \displaystyle\int_{-2}^{2} x^3\cos(x^2)\,dx ∫ − 2 2 x 3 cos ( x 2 ) d x .
Since x 3 cos ( x 2 ) x^3\cos(x^2) x 3 cos ( x 2 ) is odd (odd × \times × even = = = odd):
∫ − 2 2 x 3 cos ( x 2 ) d x = 0 \int_{-2}^{2} x^3\cos(x^2)\,dx = 0 ∫ − 2 2 x 3 cos ( x 2 ) d x = 0
Integration by Substitution
Method
When the integrand contains a function and its derivative (or a composite function), substitute
u = g ( x ) u = g(x) u = g ( x ) where g ( x ) g(x) g ( x ) is the "inner" function:
∫ f ( g ( x ) ) g ′ ( x ) d x = ∫ f ( u ) d u \int f(g(x))g'(x)\,dx = \int f(u)\,du ∫ f ( g ( x )) g ′ ( x ) d x = ∫ f ( u ) d u
Steps
Choose u = g ( x ) u = g(x) u = g ( x ) (the inner function).
Compute d u d x = g ′ ( x ) \dfrac{du}{dx} = g'(x) d x d u = g ′ ( x ) , so d u = g ′ ( x ) d x du = g'(x)\,dx d u = g ′ ( x ) d x .
Rewrite the integral in terms of u u u .
Integrate with respect to u u u .
Substitute back u = g ( x ) u = g(x) u = g ( x ) .
Evaluate ∫ 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 , so d u d x = 2 x \dfrac{du}{dx} = 2x d x d u = 2 x , giving d u = 2 x d x du = 2x\,dx d u = 2 x d x .
∫ u d u = ∫ u 1 / 2 d u = 2 3 u 3 / 2 + C = 2 3 ( x 2 + 1 ) 3 / 2 + C \int \sqrt{u}\,du = \int u^{1/2}\,du = \frac{2}{3}u^{3/2} + C = \frac{2}{3}(x^2+1)^{3/2} + C ∫ u d u = ∫ u 1/2 d u = 3 2 u 3/2 + C = 3 2 ( x 2 + 1 ) 3/2 + C
Evaluate ∫ 0 1 x e x 2 d x \displaystyle\int_0^1 xe^{x^2}\,dx ∫ 0 1 x e x 2 d x .
Let u = x 2 u = x^2 u = x 2 , so d u = 2 x d x du = 2x\,dx d u = 2 x d x .
When x = 0 x = 0 x = 0 : u = 0 u = 0 u = 0 . When x = 1 x = 1 x = 1 : u = 1 u = 1 u = 1 .
∫ 0 1 x e x 2 d x = 1 2 ∫ 0 1 e u d u = 1 2 [ e u ] 0 1 = 1 2 ( e − 1 ) \int_0^1 xe^{x^2}\,dx = \frac{1}{2}\int_0^1 e^u\,du = \frac{1}{2}\big[e^u\big]_0^1 = \frac{1}{2}(e - 1) ∫ 0 1 x e x 2 d x = 2 1 ∫ 0 1 e u d u = 2 1 [ e u ] 0 1 = 2 1 ( e − 1 )
Trigonometric Substitutions
Certain integrals can be simplified using trigonometric substitutions:
Expression Substitution Identity a 2 − x 2 \sqrt{a^2 - x^2} a 2 − x 2 x = a sin θ x = a\sin\theta x = a sin θ 1 − sin 2 θ = cos 2 θ 1 - \sin^2\theta = \cos^2\theta 1 − sin 2 θ = cos 2 θ a 2 + x 2 \sqrt{a^2 + x^2} a 2 + x 2 x = a tan θ x = a\tan\theta x = a tan θ 1 + tan 2 θ = sec 2 θ 1 + \tan^2\theta = \sec^2\theta 1 + tan 2 θ = sec 2 θ x 2 − a 2 \sqrt{x^2 - a^2} x 2 − a 2 x = a sec θ x = a\sec\theta x = a sec θ sec 2 θ − 1 = tan 2 θ \sec^2\theta - 1 = \tan^2\theta sec 2 θ − 1 = tan 2 θ
Evaluate ∫ 1 4 − x 2 d x \displaystyle\int \frac{1}{\sqrt{4-x^2}}\,dx ∫ 4 − x 2 1 d x .
This is a standard integral: arcsin ( x 2 ) + C \arcsin\!\left(\dfrac{x}{2}\right) + C arcsin ( 2 x ) + C .
Alternatively, let x = 2 sin θ x = 2\sin\theta x = 2 sin θ , so d x = 2 cos θ d θ dx = 2\cos\theta\,d\theta d x = 2 cos θ d θ :
∫ 2 cos θ 2 cos θ d θ = ∫ 1 d θ = θ + C = arcsin ( x 2 ) + C \int \frac{2\cos\theta}{2\cos\theta}\,d\theta = \int 1\,d\theta = \theta + C = \arcsin\!\left(\frac{x}{2}\right) + C ∫ 2 cos θ 2 cos θ d θ = ∫ 1 d θ = θ + C = arcsin ( 2 x ) + C
Integration by Parts
For the product of two functions:
∫ u d v = u v − ∫ v d u \int u\,dv = uv - \int v\,du ∫ u d v = uv − ∫ v d u
Choosing u u u and d v dv d v
Use the LIATE rule (prioritise choosing u u u from):
L ogarithmic functions
I nverse trig functions
A lgebraic functions (polynomials)
T rigonometric functions
E xponential functions
Evaluate ∫ x e x d x \displaystyle\int x e^x\,dx ∫ x e x d x .
Let u = x u = x u = x (algebraic) and 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 and 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 = xe^x - \int e^x\,dx = xe^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
Evaluate ∫ x sin x d x \displaystyle\int x\sin x\,dx ∫ x sin x d x .
Let u = x u = x u = x and 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 and 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
Repeated Integration by Parts
For integrals like ∫ x 2 e x d x \displaystyle\int x^2 e^x\,dx ∫ x 2 e x d x or ∫ x 2 sin x d x \displaystyle\int x^2 \sin x\,dx ∫ x 2 sin x d x , apply
integration by parts repeatedly.
Evaluate ∫ x 2 e x d x \displaystyle\int x^2 e^x\,dx ∫ x 2 e x d x .
First application: u = x 2 u = x^2 u = x 2 , d v = e x d x dv = e^x\,dx d v = e x d x :
∫ x 2 e x d x = x 2 e x − ∫ 2 x e x d x \int x^2 e^x\,dx = x^2 e^x - \int 2x e^x\,dx ∫ x 2 e x d x = x 2 e x − ∫ 2 x e x d x Second application on ∫ 2 x e x d x \int 2x e^x\,dx ∫ 2 x e x d x : u = 2 x u = 2x u = 2 x , d v = e x d x dv = e^x\,dx d v = e x d x :
∫ 2 x e x d x = 2 x e x − ∫ 2 e x d x = 2 x e x − 2 e x \int 2x e^x\,dx = 2xe^x - \int 2e^x\,dx = 2xe^x - 2e^x ∫ 2 x e x d x = 2 x e x − ∫ 2 e x d x = 2 x e x − 2 e x Combining:
∫ x 2 e x d x = x 2 e x − 2 x e x + 2 e x + C = e x ( x 2 − 2 x + 2 ) + C \int x^2 e^x\,dx = x^2 e^x - 2xe^x + 2e^x + C = e^x(x^2 - 2x + 2) + C ∫ x 2 e x d x = x 2 e x − 2 x e x + 2 e x + C = e x ( x 2 − 2 x + 2 ) + C
Cyclic Integration by Parts
Integrals like ∫ e x sin x d x \displaystyle\int e^x \sin x\,dx ∫ e x sin x d x require applying integration by parts twice and
solving algebraically.
Evaluate ∫ e x sin x d x \displaystyle\int e^x \sin x\,dx ∫ e x sin x d x .
Let u = e x u = e^x u = e x , d v = sin x d x dv = \sin x\,dx d v = sin x d x . Then d u = e x d x du = e^x\,dx d u = e x d x , v = − cos x v = -\cos x v = − cos x .
I = − e x cos x + ∫ e x cos x d x I = -e^x\cos x + \int e^x\cos x\,dx I = − e x cos x + ∫ e x cos x d x Now let u = e x u = e^x u = e x , d v = cos x d x dv = \cos x\,dx d v = cos x d x . Then d u = e x d x du = e^x\,dx d u = e x d x , v = sin x v = \sin x v = sin x .
∫ e x cos x d x = e x sin x − ∫ e x sin x d x = e x sin x − I \int e^x\cos x\,dx = e^x\sin x - \int e^x\sin x\,dx = e^x\sin x - I ∫ e x cos x d x = e x sin x − ∫ e x sin x d x = e x sin x − I Substituting back:
I = − e x cos x + e x sin x − I I = -e^x\cos x + e^x\sin x - I I = − e x cos x + e x sin x − I 2 I = e x ( sin x − cos x ) 2I = e^x(\sin x - \cos x) 2 I = e x ( sin x − cos x ) I = e x ( sin x − cos x ) 2 + C I = \frac{e^x(\sin x - \cos x)}{2} + C I = 2 e x ( sin x − cos x ) + C
Partial Fractions
When the integrand is a rational function with a denominator that can be factorised, decompose into
partial fractions.
Types of Decomposition
Denominator Partial Fractions ( a x + b ) ( c x + d ) (ax+b)(cx+d) ( a x + b ) ( c x + d ) A a x + b + B c x + d \dfrac{A}{ax+b} + \dfrac{B}{cx+d} a x + b A + c x + d B ( a x + b ) 2 (ax+b)^2 ( a x + b ) 2 A a x + b + B ( a x + b ) 2 \dfrac{A}{ax+b} + \dfrac{B}{(ax+b)^2} a x + b A + ( a x + b ) 2 B ( a x + b ) ( x 2 + c ) (ax+b)(x^2+c) ( a x + b ) ( x 2 + c ) A a x + b + B x + C x 2 + c \dfrac{A}{ax+b} + \dfrac{Bx+C}{x^2+c} a x + b A + x 2 + c B x + C
Evaluate ∫ 5 x + 1 ( x + 1 ) ( x − 2 ) d x \displaystyle\int \frac{5x+1}{(x+1)(x-2)}\,dx ∫ ( x + 1 ) ( x − 2 ) 5 x + 1 d x .
5 x + 1 ( x + 1 ) ( x − 2 ) = A x + 1 + B x − 2 \frac{5x+1}{(x+1)(x-2)} = \frac{A}{x+1} + \frac{B}{x-2} ( x + 1 ) ( x − 2 ) 5 x + 1 = x + 1 A + x − 2 B 5 x + 1 = A ( x − 2 ) + B ( x + 1 ) 5x + 1 = A(x-2) + B(x+1) 5 x + 1 = A ( x − 2 ) + B ( x + 1 ) x = − 1 x = -1 x = − 1 : − 5 + 1 = A ( − 3 ) ⟹ A = 4 3 -5 + 1 = A(-3) \implies A = \dfrac{4}{3} − 5 + 1 = A ( − 3 ) ⟹ A = 3 4 .
x = 2 x = 2 x = 2 : 10 + 1 = B ( 3 ) ⟹ B = 11 3 10 + 1 = B(3) \implies B = \dfrac{11}{3} 10 + 1 = B ( 3 ) ⟹ B = 3 11 .
∫ 5 x + 1 ( x + 1 ) ( x − 2 ) d x = 4 3 ln ∥ x + 1 ∥ + 11 3 ln ∥ 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 ∫ ( x + 1 ) ( x − 2 ) 5 x + 1 d x = 3 4 ln ∥ x + 1∥ + 3 11 ln ∥ x − 2∥ + C
Area Under Curves
Area Between a Curve and the x x x -axis
The signed area between y = f ( x ) y = f(x) y = f ( x ) and the x x x -axis from x = a x = a x = a to x = b x = b x = b is:
A r e a = ∫ a b f ( x ) d x \mathrm{Area} = \int_a^b f(x)\,dx Area = ∫ a b f ( x ) d x
If the curve crosses the x x x -axis, split the integral at the zeros and take the absolute value of
each part.
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) \ge g(x) f ( x ) ≥ g ( x ) ):
A r e a = ∫ a b [ f ( x ) − g ( x ) ] d x \mathrm{Area} = \int_a^b [f(x) - g(x)]\,dx Area = ∫ a b [ f ( x ) − g ( x )] d x
Find the area enclosed by y = x 2 y = x^2 y = x 2 and y = 2 x y = 2x y = 2 x .
Intersection points: x 2 = 2 x ⟹ x ( x − 2 ) = 0 ⟹ x = 0 x^2 = 2x \implies x(x-2) = 0 \implies x = 0 x 2 = 2 x ⟹ x ( x − 2 ) = 0 ⟹ x = 0 or x = 2 x = 2 x = 2 .
For 0 ≤ x ≤ 2 0 \le x \le 2 0 ≤ x ≤ 2 : 2 x ≥ x 2 2x \ge x^2 2 x ≥ x 2 .
A r e a = ∫ 0 2 ( 2 x − x 2 ) d x = [ x 2 − x 3 3 ] 0 2 = 4 − 8 3 = 4 3 \mathrm{Area} = \int_0^2 (2x - x^2)\,dx = \left[x^2 - \frac{x^3}{3}\right]_0^2 = 4 - \frac{8}{3} = \frac{4}{3} Area = ∫ 0 2 ( 2 x − x 2 ) d x = [ x 2 − 3 x 3 ] 0 2 = 4 − 3 8 = 3 4
Find the area enclosed by y = x 2 − 4 y = x^2 - 4 y = x 2 − 4 and the x x x -axis.
Zeros: x 2 − 4 = 0 ⟹ x = ± 2 x^2 - 4 = 0 \implies x = \pm 2 x 2 − 4 = 0 ⟹ x = ± 2 .
A r e a = ∫ − 2 2 ∣ x 2 − 4 ∣ d x = 2 ∫ 0 2 ( 4 − x 2 ) d x = 2 [ 4 x − x 3 3 ] 0 2 = 2 ( 8 − 8 3 ) = 32 3 \mathrm{Area} = \int_{-2}^{2} |x^2 - 4|\,dx = 2\int_0^2 (4 - x^2)\,dx = 2\left[4x - \frac{x^3}{3}\right]_0^2 = 2\left(8 - \frac{8}{3}\right) = \frac{32}{3} Area = ∫ − 2 2 ∣ x 2 − 4∣ d x = 2 ∫ 0 2 ( 4 − x 2 ) d x = 2 [ 4 x − 3 x 3 ] 0 2 = 2 ( 8 − 3 8 ) = 3 32
Volume of Revolution
Rotation about the x x x -axis
The volume generated by rotating y = f ( x ) y = f(x) y = f ( x ) from x = a x = a x = a to x = b x = b x = b about the x x x -axis:
V = π ∫ a b [ f ( x ) ] 2 d x V = \pi \int_a^b [f(x)]^2\,dx V = π ∫ a b [ f ( x ) ] 2 d x
Rotation about the y y y -axis
The volume generated by rotating x = g ( y ) x = g(y) x = g ( y ) from y = c y = c y = c to y = d y = d y = d about the y y y -axis:
V = π ∫ c d [ g ( y ) ] 2 d y V = \pi \int_c^d [g(y)]^2\,dy V = π ∫ c d [ g ( y ) ] 2 d y
Alternatively, using the shell method about the y y y -axis:
V = 2 π ∫ a b x ∣ f ( x ) ∣ d x V = 2\pi \int_a^b x |f(x)|\,dx V = 2 π ∫ a b x ∣ f ( x ) ∣ d x
Find the volume generated by rotating the region bounded by y = x y = \sqrt{x} y = x , x = 4 x = 4 x = 4 , and the
x x x -axis about the x x x -axis.
V = π ∫ 0 4 ( x ) 2 d x = π ∫ 0 4 x d x = π [ x 2 2 ] 0 4 = 8 π V = \pi\int_0^4 (\sqrt{x})^2\,dx = \pi\int_0^4 x\,dx = \pi\left[\frac{x^2}{2}\right]_0^4 = 8\pi V = π ∫ 0 4 ( x ) 2 d x = π ∫ 0 4 x d x = π [ 2 x 2 ] 0 4 = 8 π
Find the volume generated by rotating the region bounded by y = x 2 y = x^2 y = x 2 , y = 0 y = 0 y = 0 , and x = 1 x = 1 x = 1 about
the y y y -axis.
Using the disc method (in terms of y y y ):
x = y x = \sqrt{y} x = y , from y = 0 y = 0 y = 0 to y = 1 y = 1 y = 1 .
V = π ∫ 0 1 ( y ) 2 d y = π ∫ 0 1 y d y = π [ y 2 2 ] 0 1 = π 2 V = \pi\int_0^1 (\sqrt{y})^2\,dy = \pi\int_0^1 y\,dy = \pi\left[\frac{y^2}{2}\right]_0^1 = \frac{\pi}{2} V = π ∫ 0 1 ( y ) 2 d y = π ∫ 0 1 y d y = π [ 2 y 2 ] 0 1 = 2 π
Volume between two curves
When rotating the region between y = f ( x ) y = f(x) y = f ( x ) and y = g ( x ) y = g(x) y = g ( x ) about the x x x -axis:
V = π ∫ a b ( [ f ( x ) ] 2 − [ g ( x ) ] 2 ) d x V = \pi\int_a^b \left([f(x)]^2 - [g(x)]^2\right)\,dx V = π ∫ a b ( [ f ( x ) ] 2 − [ g ( x ) ] 2 ) d x
Find the volume generated by rotating the region between y = x y = x y = x and y = x 2 y = x^2 y = x 2 about the x x x -axis.
Intersection: x = x 2 ⟹ x = 0 x = x^2 \implies x = 0 x = x 2 ⟹ x = 0 or x = 1 x = 1 x = 1 .
V = π ∫ 0 1 ( x 2 − x 4 ) d x = π [ x 3 3 − x 5 5 ] 0 1 = π ( 1 3 − 1 5 ) = 2 π 15 V = \pi\int_0^1 \left(x^2 - x^4\right)\,dx = \pi\left[\frac{x^3}{3} - \frac{x^5}{5}\right]_0^1 = \pi\left(\frac{1}{3} - \frac{1}{5}\right) = \frac{2\pi}{15} V = π ∫ 0 1 ( x 2 − x 4 ) d x = π [ 3 x 3 − 5 x 5 ] 0 1 = π ( 3 1 − 5 1 ) = 15 2 π
Kinematics Applications
Displacement, Velocity, and Acceleration
Velocity is the derivative of displacement: v = d s d t v = \dfrac{ds}{dt} v = d t d s
Acceleration is the derivative of velocity: a = d v d t = d 2 s d t 2 a = \dfrac{dv}{dt} = \dfrac{d^2s}{dt^2} a = d t d v = d t 2 d 2 s
Displacement from velocity: s = ∫ v d t s = \displaystyle\int v\,dt s = ∫ v d t
Velocity from acceleration: v = ∫ a d t v = \displaystyle\int a\,dt v = ∫ a d t
Total Distance vs Displacement
D i s p l a c e m e n t = ∫ t 1 t 2 v ( t ) d t \mathrm{Displacement} = \int_{t_1}^{t_2} v(t)\,dt Displacement = ∫ t 1 t 2 v ( t ) d t
T o t a l d i s t a n c e = ∫ t 1 t 2 ∣ v ( t ) ∣ d t \mathrm{Total distance} = \int_{t_1}^{t_2} |v(t)|\,dt Totaldistance = ∫ t 1 t 2 ∣ v ( t ) ∣ d t
A particle moves with velocity v ( t ) = t 2 − 4 t + 3 m / s v(t) = t^2 - 4t + 3\mathrm{ m/s} v ( t ) = t 2 − 4 t + 3 m/s for 0 ≤ t ≤ 5 0 \le t \le 5 0 ≤ t ≤ 5 .
(a) Find the displacement.
s = ∫ 0 5 ( t 2 − 4 t + 3 ) d t = [ t 3 3 − 2 t 2 + 3 t ] 0 5 = 125 3 − 50 + 15 = 40 3 m s = \int_0^5 (t^2 - 4t + 3)\,dt = \left[\frac{t^3}{3} - 2t^2 + 3t\right]_0^5 = \frac{125}{3} - 50 + 15 = \frac{40}{3}\mathrm{ m} s = ∫ 0 5 ( t 2 − 4 t + 3 ) d t = [ 3 t 3 − 2 t 2 + 3 t ] 0 5 = 3 125 − 50 + 15 = 3 40 m (b) Find the total distance travelled.
Find when v = 0 v = 0 v = 0 : t 2 − 4 t + 3 = 0 ⟹ ( t − 1 ) ( t − 3 ) = 0 ⟹ t = 1 , 3 t^2 - 4t + 3 = 0 \implies (t-1)(t-3) = 0 \implies t = 1, 3 t 2 − 4 t + 3 = 0 ⟹ ( t − 1 ) ( t − 3 ) = 0 ⟹ t = 1 , 3 .
Interval Sign of v v v Motion 0 < t < 1 0 \lt t \lt 1 0 < t < 1 + + + Forward 1 < t < 3 1 \lt t \lt 3 1 < t < 3 − - − Backward 3 < t < 5 3 \lt t \lt 5 3 < t < 5 + + + Forward
D i s t a n c e = ∫ 0 1 v d t + ∣ ∫ 1 3 v d t ∣ + ∫ 3 5 v d t \mathrm{Distance} = \int_0^1 v\,dt + \left|\int_1^3 v\,dt\right| + \int_3^5 v\,dt Distance = ∫ 0 1 v d t + ∫ 1 3 v d t + ∫ 3 5 v d t = 4 3 + ∣ − 4 3 ∣ + 20 3 = 4 3 + 4 3 + 20 3 = 28 3 m = \frac{4}{3} + \left|-\frac{4}{3}\right| + \frac{20}{3} = \frac{4}{3} + \frac{4}{3} + \frac{20}{3} = \frac{28}{3}\mathrm{ m} = 3 4 + − 3 4 + 3 20 = 3 4 + 3 4 + 3 20 = 3 28 m
Improper Integrals
Type 1: Infinite Limits
∫ a ∞ f ( x ) d x = lim b → ∞ ∫ a b f ( x ) d x \int_a^{\infty} f(x)\,dx = \lim_{b \to \infty} \int_a^b f(x)\,dx ∫ a ∞ f ( x ) d x = b → ∞ lim ∫ a b f ( x ) d x
Type 2: Discontinuous Integrand
∫ a b f ( x ) d x = lim t → a + ∫ t b f ( x ) d x \int_a^b f(x)\,dx = \lim_{t \to a^+} \int_t^b f(x)\,dx ∫ a b f ( x ) d x = t → a + lim ∫ t b f ( x ) d x
An improper integral converges if the limit exists (is finite) and diverges otherwise.
Determine whether ∫ 1 ∞ 1 x 2 d x \displaystyle\int_1^{\infty} \frac{1}{x^2}\,dx ∫ 1 ∞ x 2 1 d x converges.
∫ 1 ∞ 1 x 2 d x = lim b → ∞ ∫ 1 b x − 2 d x = lim b → ∞ [ − 1 x ] 1 b = lim b → ∞ ( − 1 b + 1 ) = 1 \int_1^{\infty} \frac{1}{x^2}\,dx = \lim_{b \to \infty}\int_1^b x^{-2}\,dx = \lim_{b \to \infty}\left[-\frac{1}{x}\right]_1^b = \lim_{b \to \infty}\left(-\frac{1}{b} + 1\right) = 1 ∫ 1 ∞ x 2 1 d x = b → ∞ lim ∫ 1 b x − 2 d x = b → ∞ lim [ − x 1 ] 1 b = b → ∞ lim ( − b 1 + 1 ) = 1 The integral converges to 1 1 1 .
Determine whether ∫ 1 ∞ 1 x d x \displaystyle\int_1^{\infty} \frac{1}{x}\,dx ∫ 1 ∞ x 1 d x converges.
∫ 1 ∞ 1 x d x = lim b → ∞ [ ln x ] 1 b = lim b → ∞ ln b = ∞ \int_1^{\infty} \frac{1}{x}\,dx = \lim_{b \to \infty}[\ln x]_1^b = \lim_{b \to \infty}\ln b = \infty ∫ 1 ∞ x 1 d x = b → ∞ lim [ ln x ] 1 b = b → ∞ lim ln b = ∞ The integral diverges.
IB Exam-Style Questions
Question 1 (Paper 1 style)
Evaluate ∫ 0 π / 2 sin 2 x d x \displaystyle\int_0^{\pi/2} \sin^2 x\,dx ∫ 0 π /2 sin 2 x d x .
Using the identity sin 2 x = 1 − cos 2 x 2 \sin^2 x = \dfrac{1 - \cos 2x}{2} sin 2 x = 2 1 − cos 2 x :
∫ 0 π / 2 1 − cos 2 x 2 d x = 1 2 [ x − sin 2 x 2 ] 0 π / 2 = 1 2 ( π 2 − 0 ) = π 4 \int_0^{\pi/2} \frac{1 - \cos 2x}{2}\,dx = \frac{1}{2}\left[x - \frac{\sin 2x}{2}\right]_0^{\pi/2} = \frac{1}{2}\left(\frac{\pi}{2} - 0\right) = \frac{\pi}{4} ∫ 0 π /2 2 1 − cos 2 x d x = 2 1 [ x − 2 sin 2 x ] 0 π /2 = 2 1 ( 2 π − 0 ) = 4 π
Question 2 (Paper 2 style)
Let R R R be the region bounded by the curve y = x ( x − 2 ) y = x(x-2) y = x ( x − 2 ) and the x x x -axis.
(a) Find the area of R R R .
Zeros: x = 0 x = 0 x = 0 and x = 2 x = 2 x = 2 . The curve is below the axis (opens upward).
A r e a = ∫ 0 2 ∣ x ( x − 2 ) ∣ d x = ∫ 0 2 ( 2 x − x 2 ) d x = [ x 2 − x 3 3 ] 0 2 = 4 − 8 3 = 4 3 \mathrm{Area} = \int_0^2 |x(x-2)|\,dx = \int_0^2 (2x - x^2)\,dx = \left[x^2 - \frac{x^3}{3}\right]_0^2 = 4 - \frac{8}{3} = \frac{4}{3} Area = ∫ 0 2 ∣ x ( x − 2 ) ∣ d x = ∫ 0 2 ( 2 x − x 2 ) d x = [ x 2 − 3 x 3 ] 0 2 = 4 − 3 8 = 3 4
(b) Find the volume when R R R is rotated 360 ° 360\degree 360° about the x x x -axis.
V = π ∫ 0 2 [ x ( x − 2 ) ] 2 d x = π ∫ 0 2 x 2 ( x − 2 ) 2 d x V = \pi\int_0^2 [x(x-2)]^2\,dx = \pi\int_0^2 x^2(x-2)^2\,dx V = π ∫ 0 2 [ x ( x − 2 ) ] 2 d x = π ∫ 0 2 x 2 ( x − 2 ) 2 d x
= π ∫ 0 2 ( x 4 − 4 x 3 + 4 x 2 ) d x = π [ x 5 5 − x 4 + 4 x 3 3 ] 0 2 = \pi\int_0^2 (x^4 - 4x^3 + 4x^2)\,dx = \pi\left[\frac{x^5}{5} - x^4 + \frac{4x^3}{3}\right]_0^2 = π ∫ 0 2 ( x 4 − 4 x 3 + 4 x 2 ) d x = π [ 5 x 5 − x 4 + 3 4 x 3 ] 0 2
= π ( 32 5 − 16 + 32 3 ) = π ⋅ 16 15 = 16 π 15 = \pi\left(\frac{32}{5} - 16 + \frac{32}{3}\right) = \pi \cdot \frac{16}{15} = \frac{16\pi}{15} = π ( 5 32 − 16 + 3 32 ) = π ⋅ 15 16 = 15 16 π
Question 3 (Paper 2 style)
Evaluate ∫ 2 x + 3 x 2 + 3 x + 2 d x \displaystyle\int \frac{2x + 3}{x^2 + 3x + 2}\,dx ∫ x 2 + 3 x + 2 2 x + 3 d x .
Factorise the denominator: x 2 + 3 x + 2 = ( x + 1 ) ( x + 2 ) x^2 + 3x + 2 = (x+1)(x+2) x 2 + 3 x + 2 = ( x + 1 ) ( x + 2 ) .
2 x + 3 ( x + 1 ) ( x + 2 ) = A x + 1 + B x + 2 \frac{2x+3}{(x+1)(x+2)} = \frac{A}{x+1} + \frac{B}{x+2} ( x + 1 ) ( x + 2 ) 2 x + 3 = x + 1 A + x + 2 B
2 x + 3 = A ( x + 2 ) + B ( x + 1 ) 2x + 3 = A(x+2) + B(x+1) 2 x + 3 = A ( x + 2 ) + B ( x + 1 )
x = − 1 x = -1 x = − 1 : 1 = A ⟹ A = 1 1 = A \implies A = 1 1 = A ⟹ A = 1 .
x = − 2 x = -2 x = − 2 : − 1 = − B ⟹ B = 1 -1 = -B \implies B = 1 − 1 = − B ⟹ B = 1 .
∫ 2 x + 3 x 2 + 3 x + 2 d x = ln ∥ x + 1 ∥ + ln ∥ x + 2 ∥ + C = ln ∥ ( x + 1 ) ( x + 2 ) ∥ + C \int \frac{2x+3}{x^2+3x+2}\,dx = \ln\|x+1\| + \ln\|x+2\| + C = \ln\|(x+1)(x+2)\| + C ∫ x 2 + 3 x + 2 2 x + 3 d x = ln ∥ x + 1∥ + ln ∥ x + 2∥ + C = ln ∥ ( x + 1 ) ( x + 2 ) ∥ + C
Question 4 (Paper 1 style)
Use integration by parts to evaluate ∫ 0 1 x e 2 x d x \displaystyle\int_0^1 xe^{2x}\,dx ∫ 0 1 x e 2 x d x .
Let u = x u = x u = x , d v = e 2 x d x dv = e^{2x}\,dx d v = e 2 x d x . Then d u = d x du = dx d u = d x , v = 1 2 e 2 x v = \dfrac{1}{2}e^{2x} v = 2 1 e 2 x .
∫ 0 1 x e 2 x d x = [ 1 2 x e 2 x ] 0 1 − 1 2 ∫ 0 1 e 2 x d x = e 2 2 − 1 2 [ e 2 x 2 ] 0 1 \int_0^1 xe^{2x}\,dx = \left[\frac{1}{2}xe^{2x}\right]_0^1 - \frac{1}{2}\int_0^1 e^{2x}\,dx = \frac{e^2}{2} - \frac{1}{2}\left[\frac{e^{2x}}{2}\right]_0^1 ∫ 0 1 x e 2 x d x = [ 2 1 x e 2 x ] 0 1 − 2 1 ∫ 0 1 e 2 x d x = 2 e 2 − 2 1 [ 2 e 2 x ] 0 1
= e 2 2 − e 2 4 + 1 4 = e 2 4 + 1 4 = e 2 + 1 4 = \frac{e^2}{2} - \frac{e^2}{4} + \frac{1}{4} = \frac{e^2}{4} + \frac{1}{4} = \frac{e^2 + 1}{4} = 2 e 2 − 4 e 2 + 4 1 = 4 e 2 + 4 1 = 4 e 2 + 1
Question 5 (Paper 2 style)
A particle moves in a straight line with acceleration a ( t ) = 6 t − 2 m / s 2 a(t) = 6t - 2\mathrm{ m/s}^2 a ( t ) = 6 t − 2 m/s 2 . At t = 0 t = 0 t = 0 ,
the velocity is 4 m / s 4\mathrm{ m/s} 4 m/s and the displacement is 0 m 0\mathrm{ m} 0 m .
(a) Find the velocity function.
v ( t ) = ∫ ( 6 t − 2 ) d t = 3 t 2 − 2 t + C v(t) = \int (6t-2)\,dt = 3t^2 - 2t + C v ( t ) = ∫ ( 6 t − 2 ) d t = 3 t 2 − 2 t + C
v ( 0 ) = 4 ⟹ C = 4 v(0) = 4 \implies C = 4 v ( 0 ) = 4 ⟹ C = 4 .
v ( t ) = 3 t 2 − 2 t + 4 v(t) = 3t^2 - 2t + 4 v ( t ) = 3 t 2 − 2 t + 4
(b) Find the displacement function.
s ( t ) = ∫ ( 3 t 2 − 2 t + 4 ) d t = t 3 − t 2 + 4 t + D s(t) = \int (3t^2 - 2t + 4)\,dt = t^3 - t^2 + 4t + D s ( t ) = ∫ ( 3 t 2 − 2 t + 4 ) d t = t 3 − t 2 + 4 t + D
s ( 0 ) = 0 ⟹ D = 0 s(0) = 0 \implies D = 0 s ( 0 ) = 0 ⟹ D = 0 .
s ( t ) = t 3 − t 2 + 4 t s(t) = t^3 - t^2 + 4t s ( t ) = t 3 − t 2 + 4 t
(c) Find the total distance travelled in the first 3 seconds.
Check if v = 0 v = 0 v = 0 : 3 t 2 − 2 t + 4 = 0 3t^2 - 2t + 4 = 0 3 t 2 − 2 t + 4 = 0 . Discriminant = 4 − 48 < 0 = 4 - 48 \lt 0 = 4 − 48 < 0 , so v > 0 v \gt 0 v > 0 always.
D i s t a n c e = ∫ 0 3 v d t = ∫ 0 3 ( 3 t 2 − 2 t + 4 ) d t = [ t 3 − t 2 + 4 t ] 0 3 = 27 − 9 + 12 = 30 m \mathrm{Distance} = \int_0^3 v\,dt = \int_0^3 (3t^2 - 2t + 4)\,dt = \left[t^3 - t^2 + 4t\right]_0^3 = 27 - 9 + 12 = 30\mathrm{ m} Distance = ∫ 0 3 v d t = ∫ 0 3 ( 3 t 2 − 2 t + 4 ) d t = [ t 3 − t 2 + 4 t ] 0 3 = 27 − 9 + 12 = 30 m
Question 6 (Paper 2 style)
The region bounded by y = e x y = e^x y = e x , y = 1 y = 1 y = 1 , x = 0 x = 0 x = 0 , and x = 2 x = 2 x = 2 is rotated about the x x x -axis. Find
the volume.
V = π ∫ 0 2 [ ( e x ) 2 − 1 2 ] d x = π ∫ 0 2 ( e 2 x − 1 ) d x = π [ e 2 x 2 − x ] 0 2 V = \pi\int_0^2 [(e^x)^2 - 1^2]\,dx = \pi\int_0^2 (e^{2x} - 1)\,dx = \pi\left[\frac{e^{2x}}{2} - x\right]_0^2 V = π ∫ 0 2 [( e x ) 2 − 1 2 ] d x = π ∫ 0 2 ( e 2 x − 1 ) d x = π [ 2 e 2 x − x ] 0 2
= π ( e 4 2 − 2 − 1 2 + 0 ) = π ( e 4 2 − 5 2 ) = π ( e 4 − 5 ) 2 = \pi\left(\frac{e^4}{2} - 2 - \frac{1}{2} + 0\right) = \pi\left(\frac{e^4}{2} - \frac{5}{2}\right) = \frac{\pi(e^4 - 5)}{2} = π ( 2 e 4 − 2 − 2 1 + 0 ) = π ( 2 e 4 − 2 5 ) = 2 π ( e 4 − 5 )
Summary Table of Techniques
Technique When to Use Key Idea Direct Simple power functions, standard forms Apply basic rules directly Substitution Composite functions, f ( g ( x ) ) g ′ ( x ) f(g(x))g'(x) f ( g ( x )) g ′ ( x ) Let u = g ( x ) u = g(x) u = g ( x ) By parts Product of different function types ∫ u d v = u v − ∫ v d u \int u\,dv = uv - \int v\,du ∫ u d v = uv − ∫ v d u Partial fractions Rational functions, factorisable denominator Decompose then integrate each term Trig substitution a 2 ± x 2 \sqrt{a^2 \pm x^2} a 2 ± x 2 or x 2 − a 2 \sqrt{x^2 - a^2} x 2 − a 2 Replace with trig function
When facing an integral, first check if it is a standard form. If not, consider substitution
(especially if you see a function and its derivative). If it is a product of different function
types, use integration by parts. If it is a rational function, consider partial fractions.
Additional Integration Techniques
Integrals Involving Trigonometric Identities
Many trigonometric integrals require using identities to simplify before integrating.
Powers of Sine and Cosine
Odd power of sine : Factor out one sin x \sin x sin x , convert the rest to cosines using
sin 2 x = 1 − cos 2 x \sin^2 x = 1 - \cos^2 x sin 2 x = 1 − cos 2 x , then substitute u = cos x u = \cos x u = cos x .
Evaluate ∫ sin 3 x d x \displaystyle\int \sin^3 x\,dx ∫ sin 3 x d x .
∫ sin 2 x sin x d x = ∫ ( 1 − cos 2 x ) sin x d x \int \sin^2 x \sin x\,dx = \int (1 - \cos^2 x)\sin x\,dx ∫ sin 2 x sin x d x = ∫ ( 1 − cos 2 x ) sin x d x Let u = cos x u = \cos x u = cos x , d u = − sin x d x du = -\sin x\,dx d u = − sin x d x :
= − ∫ ( 1 − u 2 ) d u = − u + u 3 3 + C = − cos x + cos 3 x 3 + C = -\int (1 - u^2)\,du = -u + \frac{u^3}{3} + C = -\cos x + \frac{\cos^3 x}{3} + C = − ∫ ( 1 − u 2 ) d u = − u + 3 u 3 + C = − cos x + 3 cos 3 x + C
Even powers of sine or cosine : Use the half-angle formulas.
sin 2 x = 1 − cos 2 x 2 , cos 2 x = 1 + cos 2 x 2 \sin^2 x = \frac{1 - \cos 2x}{2}, \quad \cos^2 x = \frac{1 + \cos 2x}{2} sin 2 x = 2 1 − cos 2 x , cos 2 x = 2 1 + cos 2 x
Evaluate ∫ cos 4 x d x \displaystyle\int \cos^4 x\,dx ∫ cos 4 x d x .
cos 4 x = ( cos 2 x ) 2 = ( 1 + cos 2 x 2 ) 2 = 1 + 2 cos 2 x + cos 2 2 x 4 \cos^4 x = (\cos^2 x)^2 = \left(\frac{1 + \cos 2x}{2}\right)^2 = \frac{1 + 2\cos 2x + \cos^2 2x}{4} cos 4 x = ( cos 2 x ) 2 = ( 2 1 + cos 2 x ) 2 = 4 1 + 2 cos 2 x + cos 2 2 x = 1 + 2 cos 2 x + 1 + cos 4 x 2 4 = 3 + 4 cos 2 x + cos 4 x 8 = \frac{1 + 2\cos 2x + \frac{1 + \cos 4x}{2}}{4} = \frac{3 + 4\cos 2x + \cos 4x}{8} = 4 1 + 2 cos 2 x + 2 1 + c o s 4 x = 8 3 + 4 cos 2 x + cos 4 x ∫ cos 4 x d x = 3 x 8 + sin 2 x 4 + sin 4 x 32 + C \int \cos^4 x\,dx = \frac{3x}{8} + \frac{\sin 2x}{4} + \frac{\sin 4x}{32} + C ∫ cos 4 x d x = 8 3 x + 4 sin 2 x + 32 sin 4 x + C
Products of Sine and Cosine
For ∫ sin m x cos n x d x \displaystyle\int \sin mx \cos nx\,dx ∫ sin m x cos n x d x , use the product-to-sum identities:
sin A cos B = 1 2 [ sin ( A + B ) + sin ( A − B ) ] \sin A \cos B = \frac{1}{2}[\sin(A+B) + \sin(A-B)] sin A cos B = 2 1 [ sin ( A + B ) + sin ( A − B )]
sin A sin B = 1 2 [ cos ( A − B ) − cos ( A + B ) ] \sin A \sin B = \frac{1}{2}[\cos(A-B) - \cos(A+B)] sin A sin B = 2 1 [ cos ( A − B ) − cos ( A + B )]
cos A cos B = 1 2 [ cos ( A − B ) + cos ( A + B ) ] \cos A \cos B = \frac{1}{2}[\cos(A-B) + \cos(A+B)] cos A cos B = 2 1 [ cos ( A − B ) + cos ( A + B )]
Evaluate ∫ sin 3 x cos 5 x d x \displaystyle\int \sin 3x \cos 5x\,dx ∫ sin 3 x cos 5 x d x .
sin 3 x cos 5 x = 1 2 [ sin 8 x + sin ( − 2 x ) ] = 1 2 ( sin 8 x − sin 2 x ) \sin 3x \cos 5x = \frac{1}{2}[\sin 8x + \sin(-2x)] = \frac{1}{2}(\sin 8x - \sin 2x) sin 3 x cos 5 x = 2 1 [ sin 8 x + sin ( − 2 x )] = 2 1 ( sin 8 x − sin 2 x ) ∫ sin 3 x cos 5 x d x = 1 2 ( − cos 8 x 8 + cos 2 x 2 ) + C \int \sin 3x \cos 5x\,dx = \frac{1}{2}\left(-\frac{\cos 8x}{8} + \frac{\cos 2x}{2}\right) + C ∫ sin 3 x cos 5 x d x = 2 1 ( − 8 cos 8 x + 2 cos 2 x ) + C
∫ 1 a 2 + x 2 d x = 1 a arctan x a + C \int \frac{1}{a^2 + x^2}\,dx = \frac{1}{a}\arctan\frac{x}{a} + C ∫ a 2 + x 2 1 d x = a 1 arctan a x + C
∫ 1 a 2 − x 2 d x = arcsin x a + C \int \frac{1}{\sqrt{a^2 - x^2}}\,dx = \arcsin\frac{x}{a} + C ∫ a 2 − x 2 1 d x = arcsin a x + C
∫ 1 x 2 − a 2 d x = 1 2 a ln ∣ x − a x + a ∣ + C \int \frac{1}{x^2 - a^2}\,dx = \frac{1}{2a}\ln\left|\frac{x-a}{x+a}\right| + C ∫ x 2 − a 2 1 d x = 2 a 1 ln x + a x − a + C
Evaluate ∫ 1 4 + 9 x 2 d x \displaystyle\int \frac{1}{4 + 9x^2}\,dx ∫ 4 + 9 x 2 1 d x .
Rewrite as: ∫ 1 4 + ( 3 x ) 2 d x \displaystyle\int \frac{1}{4 + (3x)^2}\,dx ∫ 4 + ( 3 x ) 2 1 d x .
Let u = 3 x u = 3x u = 3 x , d u = 3 d x du = 3\,dx d u = 3 d x :
= 1 3 ∫ 1 4 + u 2 d u = 1 3 ⋅ 1 2 arctan u 2 + C = 1 6 arctan 3 x 2 + C = \frac{1}{3}\int \frac{1}{4 + u^2}\,du = \frac{1}{3} \cdot \frac{1}{2}\arctan\frac{u}{2} + C = \frac{1}{6}\arctan\frac{3x}{2} + C = 3 1 ∫ 4 + u 2 1 d u = 3 1 ⋅ 2 1 arctan 2 u + C = 6 1 arctan 2 3 x + C
Integrals Involving e x e^x e x and ln x \ln x ln x
Integrals with e x e^x e x and Polynomials
Use integration by parts when e x e^x e x is multiplied by a polynomial.
Integrals with ln x \ln x ln x
Use integration by parts with u = ln x u = \ln x u = ln x and d v = d x dv = dx d v = d x :
∫ ln x d x = x ln x − x + C \int \ln x\,dx = x\ln x - x + C ∫ ln x d x = x ln x − x + C
Evaluate ∫ x 2 ln x d x \displaystyle\int x^2 \ln x\,dx ∫ x 2 ln x d x .
Let u = ln x u = \ln x u = ln x , d v = x 2 d x dv = x^2\,dx d v = x 2 d x . Then d u = 1 x d x du = \dfrac{1}{x}\,dx d u = x 1 d x , v = x 3 3 v = \dfrac{x^3}{3} v = 3 x 3 .
∫ x 2 ln x d x = x 3 3 ln x − ∫ x 3 3 ⋅ 1 x d x = x 3 3 ln x − 1 3 ∫ x 2 d x \int x^2 \ln x\,dx = \frac{x^3}{3}\ln x - \int \frac{x^3}{3} \cdot \frac{1}{x}\,dx = \frac{x^3}{3}\ln x - \frac{1}{3}\int x^2\,dx ∫ x 2 ln x d x = 3 x 3 ln x − ∫ 3 x 3 ⋅ x 1 d x = 3 x 3 ln x − 3 1 ∫ x 2 d x = x 3 3 ln x − x 3 9 + C = \frac{x^3}{3}\ln x - \frac{x^3}{9} + C = 3 x 3 ln x − 9 x 3 + C
Arc Length
The arc length of a curve y = f ( x ) y = f(x) y = f ( x ) from x = a x = a x = a to x = b x = b x = b :
L = \int_a^b \sqrt{1 + \left(\frac`\{dy}``\{dx}`\right)^2}\,dx
For a parametric curve ( x ( t ) , y ( t ) ) (x(t), y(t)) ( x ( t ) , y ( t )) from t = t 1 t = t_1 t = t 1 to t = t 2 t = t_2 t = t 2 :
L = \int_{t_1}^{t_2} \sqrt{\left(\frac`\{dx}``\{dt}`\right)^2 + \left(\frac`\{dy}``\{dt}`\right)^2}\,dt
Find the arc length of y = x 3 6 + 1 2 x y = \dfrac{x^3}{6} + \dfrac{1}{2x} y = 6 x 3 + 2 x 1 from x = 1 x = 1 x = 1 to x = 3 x = 3 x = 3 .
\frac`\{dy}``\{dx}` = \frac{x^2}{2} - \frac{1}{2x^2} \left(\frac`\{dy}``\{dx}`\right)^2 = \frac{x^4}{4} - \frac{1}{2} + \frac{1}{4x^4} 1 + \left(\frac`\{dy}``\{dx}`\right)^2 = \frac{x^4}{4} + \frac{1}{2} + \frac{1}{4x^4} = \left(\frac{x^2}{2} + \frac{1}{2x^2}\right)^2 L = ∫ 1 3 ( x 2 2 + 1 2 x 2 ) d x = [ x 3 6 − 1 2 x ] 1 3 L = \int_1^3 \left(\frac{x^2}{2} + \frac{1}{2x^2}\right)\,dx = \left[\frac{x^3}{6} - \frac{1}{2x}\right]_1^3 L = ∫ 1 3 ( 2 x 2 + 2 x 2 1 ) d x = [ 6 x 3 − 2 x 1 ] 1 3 = ( 27 6 − 1 6 ) − ( 1 6 − 1 2 ) = 26 6 + 1 3 = 14 3 = \left(\frac{27}{6} - \frac{1}{6}\right) - \left(\frac{1}{6} - \frac{1}{2}\right) = \frac{26}{6} + \frac{1}{3} = \frac{14}{3} = ( 6 27 − 6 1 ) − ( 6 1 − 2 1 ) = 6 26 + 3 1 = 3 14
Mean Value of a Function
The mean value of a function f ( x ) f(x) f ( x ) over [ a , b ] [a, b] [ a , b ] :
f ˉ = 1 b − a ∫ a b f ( x ) d x \bar{f} = \frac{1}{b - a}\int_a^b f(x)\,dx f ˉ = b − a 1 ∫ a b f ( x ) d x
Find the mean value of f ( x ) = x 2 f(x) = x^2 f ( x ) = x 2 over [ 0 , 3 ] [0, 3] [ 0 , 3 ] .
f ˉ = 1 3 ∫ 0 3 x 2 d x = 1 3 [ x 3 3 ] 0 3 = 1 3 × 9 = 3 \bar{f} = \frac{1}{3}\int_0^3 x^2\,dx = \frac{1}{3}\left[\frac{x^3}{3}\right]_0^3 = \frac{1}{3} \times 9 = 3 f ˉ = 3 1 ∫ 0 3 x 2 d x = 3 1 [ 3 x 3 ] 0 3 = 3 1 × 9 = 3
Additional Exam-Style Questions
Question 7 (Paper 2 style)
Evaluate ∫ 0 π / 4 x cos 2 x d x \displaystyle\int_0^{\pi/4} x\cos 2x\,dx ∫ 0 π /4 x cos 2 x d x .
Let u = x u = x u = x , d v = cos 2 x d x dv = \cos 2x\,dx d v = cos 2 x d x . Then d u = d x du = dx d u = d x , v = sin 2 x 2 v = \dfrac{\sin 2x}{2} v = 2 sin 2 x .
∫ 0 π / 4 x cos 2 x d x = [ x sin 2 x 2 ] 0 π / 4 − 1 2 ∫ 0 π / 4 sin 2 x d x \int_0^{\pi/4} x\cos 2x\,dx = \left[\frac{x\sin 2x}{2}\right]_0^{\pi/4} - \frac{1}{2}\int_0^{\pi/4}\sin 2x\,dx ∫ 0 π /4 x cos 2 x d x = [ 2 x sin 2 x ] 0 π /4 − 2 1 ∫ 0 π /4 sin 2 x d x
= ( π / 4 × 1 2 − 0 ) − 1 2 [ − cos 2 x 2 ] 0 π / 4 = \left(\frac{\pi/4 \times 1}{2} - 0\right) - \frac{1}{2}\left[-\frac{\cos 2x}{2}\right]_0^{\pi/4} = ( 2 π /4 × 1 − 0 ) − 2 1 [ − 2 cos 2 x ] 0 π /4
= π 8 − 1 2 ( − 0 2 + 1 2 ) = π 8 − 1 4 = \frac{\pi}{8} - \frac{1}{2}\left(-\frac{0}{2} + \frac{1}{2}\right) = \frac{\pi}{8} - \frac{1}{4} = 8 π − 2 1 ( − 2 0 + 2 1 ) = 8 π − 4 1
Question 8 (Paper 2 style)
Find the area enclosed by the curves y = x 3 y = x^3 y = x 3 and y = x y = \sqrt{x} y = x .
Intersection: x 3 = x ⟹ x 6 = x ⟹ x ( x 5 − 1 ) = 0 ⟹ x = 0 x^3 = \sqrt{x} \implies x^6 = x \implies x(x^5 - 1) = 0 \implies x = 0 x 3 = x ⟹ x 6 = x ⟹ x ( x 5 − 1 ) = 0 ⟹ x = 0 or x = 1 x = 1 x = 1 .
For 0 ≤ x ≤ 1 0 \le x \le 1 0 ≤ x ≤ 1 : x ≥ x 3 \sqrt{x} \ge x^3 x ≥ x 3 .
A r e a = ∫ 0 1 ( x − x 3 ) d x = [ 2 x 3 / 2 3 − x 4 4 ] 0 1 = 2 3 − 1 4 = 5 12 \mathrm{Area} = \int_0^1 (\sqrt{x} - x^3)\,dx = \left[\frac{2x^{3/2}}{3} - \frac{x^4}{4}\right]_0^1 = \frac{2}{3} - \frac{1}{4} = \frac{5}{12} Area = ∫ 0 1 ( x − x 3 ) d x = [ 3 2 x 3/2 − 4 x 4 ] 0 1 = 3 2 − 4 1 = 12 5
Question 9 (Paper 1 style)
Evaluate ∫ x x 2 + 2 x + 5 d x \displaystyle\int \frac{x}{x^2 + 2x + 5}\,dx ∫ x 2 + 2 x + 5 x d x .
Complete the square: x 2 + 2 x + 5 = ( x + 1 ) 2 + 4 x^2 + 2x + 5 = (x+1)^2 + 4 x 2 + 2 x + 5 = ( x + 1 ) 2 + 4 .
Let u = x 2 + 2 x + 5 u = x^2 + 2x + 5 u = x 2 + 2 x + 5 , d u = ( 2 x + 2 ) d x du = (2x + 2)\,dx d u = ( 2 x + 2 ) d x .
We need to split:
x x 2 + 2 x + 5 = ( 2 x + 2 ) / 2 − 1 x 2 + 2 x + 5 = 1 2 ⋅ 2 x + 2 x 2 + 2 x + 5 − 1 x 2 + 2 x + 5 \dfrac{x}{x^2+2x+5} = \dfrac{(2x+2)/2 - 1}{x^2+2x+5} = \dfrac{1}{2} \cdot \dfrac{2x+2}{x^2+2x+5} - \dfrac{1}{x^2+2x+5} x 2 + 2 x + 5 x = x 2 + 2 x + 5 ( 2 x + 2 ) /2 − 1 = 2 1 ⋅ x 2 + 2 x + 5 2 x + 2 − x 2 + 2 x + 5 1 .
∫ x x 2 + 2 x + 5 d x = 1 2 ln ( x 2 + 2 x + 5 ) − ∫ 1 ( x + 1 ) 2 + 4 d x \int \frac{x}{x^2+2x+5}\,dx = \frac{1}{2}\ln(x^2+2x+5) - \int \frac{1}{(x+1)^2 + 4}\,dx ∫ x 2 + 2 x + 5 x d x = 2 1 ln ( x 2 + 2 x + 5 ) − ∫ ( x + 1 ) 2 + 4 1 d x
= 1 2 ln ( x 2 + 2 x + 5 ) − 1 2 arctan ( x + 1 2 ) + C = \frac{1}{2}\ln(x^2+2x+5) - \frac{1}{2}\arctan\!\left(\frac{x+1}{2}\right) + C = 2 1 ln ( x 2 + 2 x + 5 ) − 2 1 arctan ( 2 x + 1 ) + C
Question 10 (Paper 2 style)
The region bounded by y = ln x y = \ln x y = ln x , y = 0 y = 0 y = 0 , and x = e x = e x = e is rotated 360 ° 360\degree 360° about the x x x -axis.
Find the volume.
V = π ∫ 1 e ( ln x ) 2 d x V = \pi\int_1^e (\ln x)^2\,dx V = π ∫ 1 e ( ln x ) 2 d x
Using integration by parts with u = ( ln x ) 2 u = (\ln x)^2 u = ( ln x ) 2 , d v = d x dv = dx d v = d x :
= π [ x ( ln x ) 2 ] 1 e − 2 π ∫ 1 e ln x d x = \pi\left[x(\ln x)^2\right]_1^e - 2\pi\int_1^e \ln x\,dx = π [ x ( ln x ) 2 ] 1 e − 2 π ∫ 1 e ln x d x
= π ( e − 0 ) − 2 π [ x ln x − x ] 1 e = π e − 2 π ( e − e + 1 ) = π e − 2 π = π ( e − 2 ) = \pi(e - 0) - 2\pi[x\ln x - x]_1^e = \pi e - 2\pi(e - e + 1) = \pi e - 2\pi = \pi(e - 2) = π ( e − 0 ) − 2 π [ x ln x − x ] 1 e = π e − 2 π ( e − e + 1 ) = π e − 2 π = π ( e − 2 )
For the A-Level treatment of this topic, see Integration .
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