This topic extends the calculus of A Level Mathematics to more powerful integration techniques, Inverse trigonometric functions, volumes of revolution, arc length, and surface area. These tools are essential for university-level mathematics, physics, and engineering.
Board Paper Notes AQA Paper 1 Integration by parts, inverse trig integrals, volumes, arc length Edexcel FP1, FP2 Parts in FP1; inverse trig, volumes, arc length in FP2 OCR (A) Paper 1 Parts, inverse trig integrals, volumes CIE (9231) P1, P2 Parts and volumes in P1; arc length and surface area in P2
Theorem. For differentiable functions u ( x ) u(x) u ( x ) and v ( x ) v(x) v ( x ) :
∫ u d v d x d x = u v − ∫ v d u d x d x \boxed{\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 From the product rule:
d d x ( u v ) = u d v d x + v d u d x \frac{d}{dx}(uv) = u\frac{dv}{dx} + v\frac{du}{dx} d x d ( uv ) = u d x d v + v d x d u Integrating both sides with respect to x x x :
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 Rearranging:
∫ 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 \quad \blacksquare ∫ u d x d v d x = uv − ∫ v d x d u d x ■ When the integral does not simplify in one step, apply integration by parts repeatedly until it does.
Example. Find ∫ x 2 e x d x \displaystyle\int x^2 e^x\,dx ∫ x 2 e x d x .
First application: u = x^2$$dv = e^x\,dx . du = 2x\,dx$$v = e^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 - 2\int x e^x\,dx ∫ x 2 e x d x = x 2 e x − 2 ∫ x e x d x Second application on ∫ x e x d x \int x e^x\,dx ∫ x e x d x : u = x$$dv = e^x\,dx . du = dx$$v = e^x .
∫ x e x d x = x e x − ∫ e x d x = x e x − e x + C \int x e^x\,dx = xe^x - \int e^x\,dx = xe^x - e^x + C ∫ x e x d x = x e x − ∫ e x d x = x e x − e x + C Therefore:
∫ x 2 e x d x = x 2 e x − 2 ( x e x − e x ) + C = e x ( x 2 − 2 x + 2 ) + C \int x^2 e^x\,dx = x^2 e^x - 2(xe^x - e^x) + C = e^x(x^2 - 2x + 2) + C ∫ x 2 e x d x = x 2 e x − 2 ( x e x − e x ) + C = e x ( x 2 − 2 x + 2 ) + C Example. Find ∫ e a x cos b x d x \displaystyle\int e^{ax}\cos bx\,dx ∫ e a x cos b x d x .
Let I = ∫ e a x cos b x d x I = \int e^{ax}\cos bx\,dx I = ∫ e a x cos b x d x . First application: u = e a x u = e^{ax} u = e a x , d v = cos b x d x dv = \cos bx\,dx d v = cos b x d x .
d u = a e a x d x , v = 1 b sin b x du = ae^{ax}\,dx, \quad v = \frac{1}{b}\sin bx d u = a e a x d x , v = b 1 sin b x I = e a x sin b x b − a b ∫ e a x sin b x d x I = \frac{e^{ax}\sin bx}{b} - \frac{a}{b}\int e^{ax}\sin bx\,dx I = b e a x sin b x − b a ∫ e a x sin b x d x Second application on ∫ e a x sin b x d x \int e^{ax}\sin bx\,dx ∫ e a x sin b x d x : u = e a x u = e^{ax} u = e a x , d v = sin b x d x dv = \sin bx\,dx d v = sin b x d x .
d u = a e a x d x , v = − 1 b cos b x du = ae^{ax}\,dx, \quad v = -\frac{1}{b}\cos bx d u = a e a x d x , v = − b 1 cos b x ∫ e a x sin b x d x = − e a x cos b x b + a b ∫ e a x cos b x d x = − e a x cos b x b + a b I \int e^{ax}\sin bx\,dx = -\frac{e^{ax}\cos bx}{b} + \frac{a}{b}\int e^{ax}\cos bx\,dx = -\frac{e^{ax}\cos bx}{b} + \frac{a}{b}I ∫ e a x sin b x d x = − b e a x cos b x + b a ∫ e a x cos b x d x = − b e a x cos b x + b a I Substituting back:
I = e a x sin b x b − a b ( − e a x cos b x b + a b I ) I = \frac{e^{ax}\sin bx}{b} - \frac{a}{b}\left(-\frac{e^{ax}\cos bx}{b} + \frac{a}{b}I\right) I = b e a x sin b x − b a ( − b e a x cos b x + b a I ) I = e a x sin b x b + a e a x cos b x b 2 − a 2 b 2 I I = \frac{e^{ax}\sin bx}{b} + \frac{ae^{ax}\cos bx}{b^2} - \frac{a^2}{b^2}I I = b e a x sin b x + b 2 a e a x cos b x − b 2 a 2 I I ( 1 + a 2 b 2 ) = e a x ( sin b x b + a cos b x b 2 ) I\left(1 + \frac{a^2}{b^2}\right) = e^{ax}\left(\frac{\sin bx}{b} + \frac{a\cos bx}{b^2}\right) I ( 1 + b 2 a 2 ) = e a x ( b sin b x + b 2 a cos b x ) I = e a x ( a cos b x + b sin b x ) a 2 + b 2 + C \boxed{I = \frac{e^{ax}(a\cos bx + b\sin bx)}{a^2 + b^2} + C} I = a 2 + b 2 e a x ( a cos b x + b sin b x ) + C A reduction formula expresses an integral I n I_n I n (depending on a parameter n n n ) in terms of I n − 1 I_{n-1} I n − 1 or I n − 2 I_{n-2} I n − 2 .
Write 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 . Then:
d u = ( n − 1 ) sin n − 2 x cos x d x , v = − cos x du = (n-1)\sin^{n-2}x\cos x\,dx, \quad v = -\cos x d u = ( n − 1 ) sin n − 2 x cos x d 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 = \bigl[-\sin^{n-1}x\cos x\bigr]_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: at x = 0$$\sin 0 = 0 ; at x = \pi/2$$\cos(\pi/2) = 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 d x − ( n − 1 ) ∫ 0 π / 2 sin n x d x I_n = (n-1)\int_0^{\pi/2}\sin^{n-2}x\,dx - (n-1)\int_0^{\pi/2}\sin^n x\,dx I n = ( n − 1 ) ∫ 0 π /2 sin n − 2 x d x − ( n − 1 ) ∫ 0 π /2 sin n x d x 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 , n ≥ 2 \boxed{I_n = \frac{n-1}{n}\,I_{n-2}, \quad n \geq 2} I n = n n − 1 I n − 2 , n ≥ 2 The base cases are I 0 = ∫ 0 π / 2 1 d x = π 2 I_0 = \displaystyle\int_0^{\pi/2}1\,dx = \dfrac{\pi}{2} I 0 = ∫ 0 π /2 1 d x = 2 π and I 1 = ∫ 0 π / 2 sin x d x = 1 I_1 = \displaystyle\int_0^{\pi/2}\sin x\,dx = 1 I 1 = ∫ 0 π /2 sin x d x = 1 .
Example. Using the reduction formula, I 4 = 3 4 I 2 = 3 4 ⋅ 1 2 I 0 = 3 4 ⋅ 1 2 ⋅ π 2 = 3 π 16 I_4 = \dfrac{3}{4}I_2 = \dfrac{3}{4}\cdot\dfrac{1}{2}I_0 = \dfrac{3}{4}\cdot\dfrac{1}{2}\cdot\dfrac{\pi}{2} = \dfrac{3\pi}{16} I 4 = 4 3 I 2 = 4 3 ⋅ 2 1 I 0 = 4 3 ⋅ 2 1 ⋅ 2 π = 16 3 π .
Caution: warning 0 0 0 and π / 2 \pi/2 π /2 . For general limits, the boundary term must be evaluated. 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$$dv = e^x\,dx . Then du = nx^{n-1}\,dx$$v = e^x .
I n = x n e x − n I n − 1 \boxed{I_n = x^n e^x - nI_{n-1}} I n = x n e x − n I n − 1 With I 0 = e x + C I_0 = e^x + C I 0 = e x + C .
When the denominator factorises into distinct linear factors, decompose and integrate each term.
Example. ∫ 2 x + 3 ( x + 1 ) ( x + 2 ) d x \displaystyle\int \frac{2x+3}{(x+1)(x+2)}\,dx ∫ ( x + 1 ) ( x + 2 ) 2 x + 3 d x .
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 ) . Setting x = − 1 x = -1 x = − 1 : 1 = A 1 = A 1 = A . Setting x = − 2 x = -2 x = − 2 : − 1 = − B ⟹ B = 1 -1 = -B \implies B = 1 − 1 = − B ⟹ B = 1 .
∫ 1 x + 1 + 1 x + 2 d x = ln ∣ x + 1 ∣ + ln ∣ x + 2 ∣ + C = ln ∣ ( x + 1 ) ( x + 2 ) ∣ + C \int \frac{1}{x+1} + \frac{1}{x+2}\,dx = \ln|x+1| + \ln|x+2| + C = \ln|(x+1)(x+2)| + C ∫ x + 1 1 + x + 2 1 d x = ln ∣ x + 1∣ + ln ∣ x + 2∣ + C = ln ∣ ( x + 1 ) ( x + 2 ) ∣ + C When the denominator contains an irreducible quadratic a x 2 + b x + c ax^2 + bx + c a x 2 + b x + c (discriminant b 2 − 4 a c < 0 b^2 - 4ac < 0 b 2 − 4 a c < 0 ), the partial fraction has a linear numerator over the quadratic, leading to ln \ln ln and arctan \arctan arctan terms.
Example. ∫ 3 x + 1 x 2 + 2 x + 5 d x \displaystyle\int \frac{3x + 1}{x^2 + 2x + 5}\,dx ∫ x 2 + 2 x + 5 3 x + 1 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 .
Split the numerator to match the derivative of the denominator:
3 x + 1 x 2 + 2 x + 5 = 3 2 ( 2 x + 2 ) + 1 − 3 x 2 + 2 x + 5 = 3 2 ⋅ 2 x + 2 x 2 + 2 x + 5 − 2 ( x + 1 ) 2 + 4 \frac{3x+1}{x^2+2x+5} = \frac{\frac{3}{2}(2x+2) + 1 - 3}{x^2+2x+5} = \frac{3}{2}\cdot\frac{2x+2}{x^2+2x+5} - \frac{2}{(x+1)^2+4} x 2 + 2 x + 5 3 x + 1 = x 2 + 2 x + 5 2 3 ( 2 x + 2 ) + 1 − 3 = 2 3 ⋅ x 2 + 2 x + 5 2 x + 2 − ( x + 1 ) 2 + 4 2 ∫ 3 x + 1 x 2 + 2 x + 5 d x = 3 2 ln ( x 2 + 2 x + 5 ) − 2 ⋅ 1 2 arctan ( x + 1 2 ) + C \int \frac{3x+1}{x^2+2x+5}\,dx = \frac{3}{2}\ln(x^2+2x+5) - 2\cdot\frac{1}{2}\arctan\!\left(\frac{x+1}{2}\right) + C ∫ x 2 + 2 x + 5 3 x + 1 d x = 2 3 ln ( x 2 + 2 x + 5 ) − 2 ⋅ 2 1 arctan ( 2 x + 1 ) + C = 3 2 ln ( x 2 + 2 x + 5 ) − arctan ( x + 1 2 ) + C = \frac{3}{2}\ln(x^2+2x+5) - \arctan\!\left(\frac{x+1}{2}\right) + C = 2 3 ln ( x 2 + 2 x + 5 ) − arctan ( 2 x + 1 ) + C Example. ∫ 1 x ( x − 1 ) 2 d x \displaystyle\int \frac{1}{x(x-1)^2}\,dx ∫ x ( x − 1 ) 2 1 d x .
1 x ( x − 1 ) 2 = A x + B x − 1 + C ( x − 1 ) 2 \frac{1}{x(x-1)^2} = \frac{A}{x} + \frac{B}{x-1} + \frac{C}{(x-1)^2} x ( x − 1 ) 2 1 = x A + x − 1 B + ( x − 1 ) 2 C 1 = A ( x − 1 ) 2 + B x ( x − 1 ) + C x 1 = A(x-1)^2 + Bx(x-1) + Cx 1 = A ( x − 1 ) 2 + B x ( x − 1 ) + C x .
x = 0 x = 0 x = 0 : 1 = A 1 = A 1 = A . x = 1 x = 1 x = 1 : 1 = C 1 = C 1 = C . x = 2 x = 2 x = 2 : 1 = A + 2 B + 2 C = 1 + 2 B + 2 ⟹ B = − 1 1 = A + 2B + 2C = 1 + 2B + 2 \implies B = -1 1 = A + 2 B + 2 C = 1 + 2 B + 2 ⟹ B = − 1 .
∫ ( 1 x − 1 x − 1 + 1 ( x − 1 ) 2 ) d x = ln ∣ x ∣ − ln ∣ x − 1 ∣ − 1 x − 1 + C \int\left(\frac{1}{x} - \frac{1}{x-1} + \frac{1}{(x-1)^2}\right)dx = \ln|x| - \ln|x-1| - \frac{1}{x-1} + C ∫ ( x 1 − x − 1 1 + ( x − 1 ) 2 1 ) d x = ln ∣ x ∣ − ln ∣ x − 1∣ − x − 1 1 + C Theorem. The following integrals hold for a > 0 a > 0 a > 0 :
∫ 1 a 2 + x 2 d x = 1 a arctan x a + C \boxed{\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 \boxed{\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 a 2 − x 2 d x = 1 2 a ln ∣ a + x a − x ∣ + C \boxed{\int \frac{1}{a^2-x^2}\,dx = \frac{1}{2a}\ln\left|\frac{a+x}{a-x}\right| + C} ∫ a 2 − x 2 1 d x = 2 a 1 ln a − x a + x + C Let x = a tan θ x = a\tan\theta x = a tan θ So d x = a sec 2 θ d θ dx = a\sec^2\theta\,d\theta d x = a sec 2 θ d θ .
∫ 1 a 2 + a 2 tan 2 θ ⋅ a sec 2 θ d θ = ∫ a sec 2 θ a 2 sec 2 θ d θ = 1 a ∫ 1 d θ = θ a + C \int \frac{1}{a^2 + a^2\tan^2\theta}\cdot a\sec^2\theta\,d\theta = \int \frac{a\sec^2\theta}{a^2\sec^2\theta}\,d\theta = \frac{1}{a}\int 1\,d\theta = \frac{\theta}{a} + C ∫ a 2 + a 2 tan 2 θ 1 ⋅ a sec 2 θ d θ = ∫ a 2 sec 2 θ a sec 2 θ d θ = a 1 ∫ 1 d θ = a θ + C Since θ = arctan ( x / a ) \theta = \arctan(x/a) θ = arctan ( x / a ) :
∫ 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 \quad \blacksquare ∫ a 2 + x 2 1 d x = a 1 arctan a x + C ■ Let x = a sin θ x = a\sin\theta x = a sin θ So d x = a cos θ d θ dx = a\cos\theta\,d\theta d x = a cos θ d θ and a 2 − x 2 = a cos θ \sqrt{a^2 - x^2} = a\cos\theta a 2 − x 2 = a cos θ (for ∣ θ ∣ ≤ π / 2 |\theta| \leq \pi/2 ∣ θ ∣ ≤ π /2 ).
∫ a cos θ a cos θ d θ = ∫ 1 d θ = θ + C = arcsin x a + C ■ \int \frac{a\cos\theta}{a\cos\theta}\,d\theta = \int 1\,d\theta = \theta + C = \arcsin\frac{x}{a} + C \quad \blacksquare ∫ a cos θ a cos θ d θ = ∫ 1 d θ = θ + C = arcsin a x + C ■ By partial fractions:
1 a 2 − x 2 = 1 ( a − x ) ( a + x ) = 1 2 a ( 1 a − x + 1 a + x ) \frac{1}{a^2-x^2} = \frac{1}{(a-x)(a+x)} = \frac{1}{2a}\left(\frac{1}{a-x} + \frac{1}{a+x}\right) a 2 − x 2 1 = ( a − x ) ( a + x ) 1 = 2 a 1 ( a − x 1 + a + x 1 ) ∫ 1 a 2 − x 2 d x = 1 2 a [ − ln ∣ a − x ∣ + ln ∣ a + x ∣ ] + C = 1 2 a ln ∣ a + x a − x ∣ + C ■ \int \frac{1}{a^2-x^2}\,dx = \frac{1}{2a}\bigl[-\ln|a-x| + \ln|a+x|\bigr] + C = \frac{1}{2a}\ln\left|\frac{a+x}{a-x}\right| + C \quad \blacksquare ∫ a 2 − x 2 1 d x = 2 a 1 [ − ln ∣ a − x ∣ + ln ∣ a + x ∣ ] + C = 2 a 1 ln a − x a + x + C ■ ∫ 1 a 2 + ( x + b ) 2 d x = 1 a arctan x + b a + C \int \frac{1}{a^2 + (x+b)^2}\,dx = \frac{1}{a}\arctan\frac{x+b}{a} + C ∫ a 2 + ( x + b ) 2 1 d x = a 1 arctan a x + b + C ∫ 1 a 2 − ( x + b ) 2 d x = arcsin x + b a + C \int \frac{1}{\sqrt{a^2 - (x+b)^2}}\,dx = \arcsin\frac{x+b}{a} + C ∫ a 2 − ( x + b ) 2 1 d x = arcsin a x + b + C These follow directly from the standard forms via the substitution u = x + b u = x + b u = x + b .
d d x arcsin x = 1 1 − x 2 , ∣ x ∣ < 1 \boxed{\frac{d}{dx}\arcsin x = \frac{1}{\sqrt{1-x^2}}, \quad |x| < 1} d x d arcsin x = 1 − x 2 1 , ∣ x ∣ < 1 d d x arccos x = − 1 1 − x 2 , ∣ x ∣ < 1 \boxed{\frac{d}{dx}\arccos x = -\frac{1}{\sqrt{1-x^2}}, \quad |x| < 1} d x d arccos x = − 1 − x 2 1 , ∣ x ∣ < 1 d d x arctan x = 1 1 + x 2 \boxed{\frac{d}{dx}\arctan x = \frac{1}{1+x^2}} d x d arctan x = 1 + x 2 1 Let y = arctan x y = \arctan x y = arctan x . Then x = tan y x = \tan y x = tan y .
Differentiating implicitly with respect to x x x :
1 = sec 2 y ⋅ d y d x 1 = \sec^2 y \cdot \frac{dy}{dx} 1 = sec 2 y ⋅ d x d y d y d x = 1 sec 2 y = 1 1 + tan 2 y = 1 1 + x 2 ■ \frac{dy}{dx} = \frac{1}{\sec^2 y} = \frac{1}{1 + \tan^2 y} = \frac{1}{1+x^2} \quad \blacksquare d x d y = sec 2 y 1 = 1 + tan 2 y 1 = 1 + x 2 1 ■ Let y = arcsin x y = \arcsin x y = arcsin x . Then x = sin y x = \sin y x = sin y .
Differentiating implicitly:
1 = cos y ⋅ d y d x 1 = \cos y \cdot \frac{dy}{dx} 1 = cos y ⋅ d x d y Since arcsin x \arcsin x arcsin x has range [ − π / 2 , π / 2 ] [-\pi/2, \pi/2] [ − π /2 , π /2 ] We have cos y ≥ 0 \cos y \geq 0 cos y ≥ 0 So cos y = 1 − sin 2 y = 1 − x 2 \cos y = \sqrt{1-\sin^2 y} = \sqrt{1-x^2} cos y = 1 − sin 2 y = 1 − x 2 .
d y d x = 1 cos y = 1 1 − x 2 ■ \frac{dy}{dx} = \frac{1}{\cos y} = \frac{1}{\sqrt{1-x^2}} \quad \blacksquare d x d y = cos y 1 = 1 − x 2 1 ■ Example. d d x arcsin ( 3 x ) = 3 1 − 9 x 2 \dfrac{d}{dx}\arcsin(3x) = \dfrac{3}{\sqrt{1-9x^2}} d x d arcsin ( 3 x ) = 1 − 9 x 2 3 .
Example. d d x arctan ( x 2 ) = 1 / 2 1 + x 2 / 4 = 2 4 + x 2 \dfrac{d}{dx}\arctan\!\left(\dfrac{x}{2}\right) = \dfrac{1/2}{1 + x^2/4} = \dfrac{2}{4+x^2} d x d arctan ( 2 x ) = 1 + x 2 /4 1/2 = 4 + x 2 2 .
Definition. The volume generated by rotating the region bounded by 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 about the x x x -axis is:
V = π ∫ a b y 2 d x = π ∫ a b [ f ( x ) ] 2 d x \boxed{V = \pi\int_a^b y^2\,dx = \pi\int_a^b [f(x)]^2\,dx} V = π ∫ a b y 2 d x = π ∫ a b [ f ( x ) ] 2 d x Definition. The volume generated by rotating the region bounded by x = g ( y ) x = g(y) x = g ( y ) The y y y -axis, y = c y = c y = c And y = d y = d y = d about the y y y -axis is:
V = π ∫ c d x 2 d y = π ∫ c d [ g ( y ) ] 2 d y \boxed{V = \pi\int_c^d x^2\,dy = \pi\int_c^d [g(y)]^2\,dy} V = π ∫ c d x 2 d y = π ∫ c d [ g ( y ) ] 2 d y When a curve is given parametrically by x = x ( t ) x = x(t) x = x ( t ) , y = y ( t ) y = y(t) y = y ( t ) :
Rotation about the x x x -axis: V = π ∫ t 1 t 2 y 2 d x d t d t V = \pi\displaystyle\int_{t_1}^{t_2} y^2\,\frac{dx}{dt}\,dt V = π ∫ t 1 t 2 y 2 d t d x d t Rotation about the y y y -axis: V = π ∫ t 1 t 2 x 2 d y d t d t V = \pi\displaystyle\int_{t_1}^{t_2} x^2\,\frac{dy}{dt}\,dt V = π ∫ t 1 t 2 x 2 d t d y d t Example. Find the volume generated by rotating the curve y = x y = \sqrt{x} y = x from x = 0 x = 0 x = 0 to x = 4 x = 4 x = 4 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 Example. The curve x = 2 cos t x = 2\cos t x = 2 cos t , y = 2 sin t y = 2\sin t y = 2 sin t for 0 ≤ t ≤ π 0 \leq t \leq \pi 0 ≤ t ≤ π is rotated about the x x x -axis. Find the volume.
V = π ∫ 0 π ( 2 sin t ) 2 ⋅ d x d t d t = π ∫ 0 π 4 sin 2 t ⋅ ( − 2 sin t ) d t V = \pi\int_0^{\pi} (2\sin t)^2 \cdot \frac{dx}{dt}\,dt = \pi\int_0^{\pi} 4\sin^2 t \cdot (-2\sin t)\,dt V = π ∫ 0 π ( 2 sin t ) 2 ⋅ d t d x d t = π ∫ 0 π 4 sin 2 t ⋅ ( − 2 sin t ) d t = − 8 π ∫ 0 π sin 3 t d t = 8 π ∫ 0 π sin 3 t d t = -8\pi\int_0^{\pi}\sin^3 t\,dt = 8\pi\int_0^{\pi}\sin^3 t\,dt = − 8 π ∫ 0 π sin 3 t d t = 8 π ∫ 0 π sin 3 t d t Using sin 3 t = sin t ( 1 − cos 2 t ) \sin^3 t = \sin t(1-\cos^2 t) sin 3 t = sin t ( 1 − cos 2 t ) and the substitution u = cos t u = \cos t u = cos t :
= 8 π ∫ − 1 1 ( 1 − u 2 ) d u = 8 π [ u − u 3 3 ] − 1 1 = 8 π ( 2 3 − ( − 2 3 ) ) = 32 π 3 = 8\pi\int_{-1}^{1}(1-u^2)\,du = 8\pi\left[u - \frac{u^3}{3}\right]_{-1}^1 = 8\pi\left(\frac{2}{3} - \left(-\frac{2}{3}\right)\right) = \frac{32\pi}{3} = 8 π ∫ − 1 1 ( 1 − u 2 ) d u = 8 π [ u − 3 u 3 ] − 1 1 = 8 π ( 3 2 − ( − 3 2 ) ) = 3 32 π Theorem. For 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 :
s = ∫ a b 1 + ( d y d x ) 2 d x \boxed{s = \int_a^b \sqrt{1 + \left(\frac{dy}{dx}\right)^2}\,dx} s = ∫ a b 1 + ( d x d y ) 2 d x For a curve given parametrically by x = x ( t ) x = x(t) x = x ( t ) , y = y ( t ) y = y(t) y = y ( t ) from t = t 1 t = t_1 t = t 1 to t = t 2 t = t_2 t = t 2 :
s = ∫ t 1 t 2 ( d x d t ) 2 + ( d y d t ) 2 d t \boxed{s = \int_{t_1}^{t_2} \sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2}\,dt} s = ∫ t 1 t 2 ( d t d x ) 2 + ( d t d y ) 2 d t Derivation (Cartesian). The arc length element d s ds d s satisfies d s 2 = d x 2 + d y 2 ds^2 = dx^2 + dy^2 d s 2 = d x 2 + d y 2 by the Pythagorean theorem applied to an infinitesimal segment. Therefore:
d s = 1 + ( d y d x ) 2 d x ds = \sqrt{1 + \left(\frac{dy}{dx}\right)^2}\,dx d s = 1 + ( d x d y ) 2 d x Integrating from a a a to b b b gives the total arc length.
Example. Find the arc length of y = ln ( cos x ) y = \ln(\cos x) y = ln ( cos x ) from x = 0 x = 0 x = 0 to x = π / 3 x = \pi/3 x = π /3 .
d y d x = − sin x cos x = − tan x \frac{dy}{dx} = \frac{-\sin x}{\cos x} = -\tan x d x d y = cos x − sin x = − tan x s = ∫ 0 π / 3 1 + tan 2 x d x = ∫ 0 π / 3 sec x d x = [ ln ∣ sec x + tan x ∣ ] 0 π / 3 s = \int_0^{\pi/3}\sqrt{1+\tan^2 x}\,dx = \int_0^{\pi/3}\sec x\,dx = \Bigl[\ln|\sec x + \tan x|\Bigr]_0^{\pi/3} s = ∫ 0 π /3 1 + tan 2 x d x = ∫ 0 π /3 sec x d x = [ ln ∣ sec x + tan x ∣ ] 0 π /3 = ln ( 2 + 3 ) − ln ( 1 ) = ln ( 2 + 3 ) = \ln(2 + \sqrt{3}) - \ln(1) = \ln(2+\sqrt{3}) = ln ( 2 + 3 ) − ln ( 1 ) = ln ( 2 + 3 ) Theorem. The surface area 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:
S = 2 π ∫ a b y 1 + ( d y d x ) 2 d x \boxed{S = 2\pi\int_a^b y\,\sqrt{1 + \left(\frac{dy}{dx}\right)^2}\,dx} S = 2 π ∫ a b y 1 + ( d x d y ) 2 d x For a parametric curve rotated about the x x x -axis:
S = 2 π ∫ t 1 t 2 y ( d x d t ) 2 + ( d y d t ) 2 d t \boxed{S = 2\pi\int_{t_1}^{t_2} y\,\sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2}\,dt} S = 2 π ∫ t 1 t 2 y ( d t d x ) 2 + ( d t d y ) 2 d t Example. Find the surface area generated by rotating y = x 2 y = x^2 y = x 2 from x = 0 x = 0 x = 0 to x = 1 x = 1 x = 1 about the x x x -axis.
S = 2 π ∫ 0 1 x 2 1 + 4 x 2 d x S = 2\pi\int_0^1 x^2\sqrt{1+4x^2}\,dx S = 2 π ∫ 0 1 x 2 1 + 4 x 2 d x Let x = 1 2 tan θ x = \frac{1}{2}\tan\theta x = 2 1 tan θ , d x = 1 2 sec 2 θ d θ dx = \frac{1}{2}\sec^2\theta\,d\theta d x = 2 1 sec 2 θ d θ . When x = 0 x = 0 x = 0 θ = 0 \theta = 0 θ = 0 ; when x = 1 x = 1 x = 1 , θ = arctan 2 \theta = \arctan 2 θ = arctan 2 .
S = 2 π ∫ 0 arctan 2 tan 2 θ 4 ⋅ sec θ ⋅ 1 2 sec 2 θ d θ = π 4 ∫ 0 arctan 2 tan 2 θ sec 3 θ d θ S = 2\pi\int_0^{\arctan 2}\frac{\tan^2\theta}{4}\cdot\sec\theta\cdot\frac{1}{2}\sec^2\theta\,d\theta = \frac{\pi}{4}\int_0^{\arctan 2}\tan^2\theta\sec^3\theta\,d\theta S = 2 π ∫ 0 a r c t a n 2 4 tan 2 θ ⋅ sec θ ⋅ 2 1 sec 2 θ d θ = 4 π ∫ 0 a r c t a n 2 tan 2 θ sec 3 θ d θ Using tan 2 θ = sec 2 θ − 1 \tan^2\theta = \sec^2\theta - 1 tan 2 θ = sec 2 θ − 1 and integrating by parts with u = sec θ u = \sec\theta u = sec θ d v = sec 2 θ d θ dv = \sec^2\theta\,d\theta d v = sec 2 θ d θ :
This integral evaluates to π 4 [ 1 4 sec θ tan θ + 1 4 ln ∣ sec θ + tan θ ∣ − 1 4 sec θ tan θ + 1 8 ln ∣ sec θ + tan θ ∣ ] 0 arctan 2 \dfrac{\pi}{4}\left[\dfrac{1}{4}\sec\theta\tan\theta + \dfrac{1}{4}\ln|\sec\theta+\tan\theta| - \dfrac{1}{4}\sec\theta\tan\theta + \dfrac{1}{8}\ln|\sec\theta+\tan\theta|\right]_0^{\arctan 2} 4 π [ 4 1 sec θ tan θ + 4 1 ln ∣ sec θ + tan θ ∣ − 4 1 sec θ tan θ + 8 1 ln ∣ sec θ + tan θ ∣ ] 0 a r c t a n 2 .
Simplifying with sec ( arctan 2 ) = 5 \sec(\arctan 2) = \sqrt{5} sec ( arctan 2 ) = 5 and tan ( arctan 2 ) = 2 \tan(\arctan 2) = 2 tan ( arctan 2 ) = 2 :
S = 9 π 5 16 − π 32 ln ( 2 + 5 ) S = \frac{9\pi\sqrt{5}}{16} - \frac{\pi}{32}\ln(2+\sqrt{5}) S = 16 9 π 5 − 32 π ln ( 2 + 5 ) Integral Result ∫ 1 a 2 + x 2 d x \displaystyle\int\frac{1}{a^2+x^2}\,dx ∫ a 2 + x 2 1 d x 1 a arctan x a + C \dfrac{1}{a}\arctan\dfrac{x}{a}+C a 1 arctan a x + C ∫ 1 a 2 − x 2 d x \displaystyle\int\frac{1}{\sqrt{a^2-x^2}}\,dx ∫ a 2 − x 2 1 d x arcsin x a + C \arcsin\dfrac{x}{a}+C arcsin a x + C ∫ 1 a 2 − x 2 d x \displaystyle\int\frac{1}{a^2-x^2}\,dx ∫ a 2 − x 2 1 d x 1 2 a ln ∥ a + x a − x ∥ + C \dfrac{1}{2a}\ln\left\|\dfrac{a+x}{a-x}\right\|+C 2 a 1 ln a − x a + x + C d d x arcsin x \dfrac{d}{dx}\arcsin x d x d arcsin x 1 1 − x 2 \dfrac{1}{\sqrt{1-x^2}} 1 − x 2 1 d d x arctan x \dfrac{d}{dx}\arctan x d x d arctan x 1 1 + x 2 \dfrac{1}{1+x^2} 1 + x 2 1 Vol. About x x x -axis π ∫ a b y 2 d x \pi\displaystyle\int_a^b y^2\,dx π ∫ a b y 2 d x Arc length ∫ 1 + ( d y d x ) 2 d x \displaystyle\int\sqrt{1+\left(\frac{dy}{dx}\right)^2}\,dx ∫ 1 + ( d x d y ) 2 d x
Problem 1 Find $\displaystyle\int x^3 e^{-x}\,dx$.Hint 1 Apply integration by parts three times, reducing the power of $x$ each time.Answer 1 First: $u = x^3$$dv = e^{-x}\,dx$. $du = 3x^2\,dx$$v = -e^{-x}$.∫ x 3 e − x d x = − x 3 e − x + 3 ∫ x 2 e − x d x \displaystyle\int x^3 e^{-x}\,dx = -x^3 e^{-x} + 3\int x^2 e^{-x}\,dx ∫ x 3 e − x d x = − x 3 e − x + 3 ∫ x 2 e − x d x
Second: u = x^2$$dv = e^{-x}\,dx . ∫ x 2 e − x d x = − x 2 e − x + 2 ∫ x e − x d x \int x^2 e^{-x}\,dx = -x^2 e^{-x} + 2\int x e^{-x}\,dx ∫ x 2 e − x d x = − x 2 e − x + 2 ∫ x e − x d x .
Third: u = x$$dv = e^{-x}\,dx . ∫ x e − x d x = − x e − x + ∫ e − x d x = − x e − x − e − x \int x e^{-x}\,dx = -xe^{-x} + \int e^{-x}\,dx = -xe^{-x} - e^{-x} ∫ x e − x d x = − x e − x + ∫ e − x d x = − x e − x − e − x .
Combining: ∫ x 3 e − x d x = − x 3 e − x − 3 x 2 e − x − 6 x e − x − 6 e − x + C = − e − x ( x 3 + 3 x 2 + 6 x + 6 ) + C \int x^3 e^{-x}\,dx = -x^3 e^{-x} - 3x^2 e^{-x} - 6x e^{-x} - 6e^{-x} + C = -e^{-x}(x^3 + 3x^2 + 6x + 6) + C ∫ x 3 e − x d x = − x 3 e − x − 3 x 2 e − x − 6 x e − x − 6 e − x + C = − e − x ( x 3 + 3 x 2 + 6 x + 6 ) + C .
Problem 2 Find a reduction formula for $I_n = \displaystyle\int \cos^n x\,dx$ for $n \geq 2$.Hint 2 Write $\cos^n x = \cos^{n-1}x \cdot \cos x$ and apply integration by parts with $u = \cos^{n-1}x$$dv = \cos x\,dx$. Use $\sin^2 x = 1 - \cos^2 x$.Answer 2 $I_n = \int\cos^{n-1}x\cos x\,dx$. Let $u = \cos^{n-1}x$$dv = \cos x\,dx$.du = -(n-1)\cos^{n-2}x\sin x\,dx$$v = \sin x .
I n = cos n − 1 x sin x + ( n − 1 ) ∫ cos n − 2 x sin 2 x d x I_n = \cos^{n-1}x\sin x + (n-1)\int\cos^{n-2}x\sin^2 x\,dx I n = cos n − 1 x sin x + ( n − 1 ) ∫ cos n − 2 x sin 2 x d x
= cos n − 1 x sin x + ( n − 1 ) ∫ cos n − 2 x ( 1 − cos 2 x ) d x = \cos^{n-1}x\sin x + (n-1)\int\cos^{n-2}x(1-\cos^2 x)\,dx = cos n − 1 x sin x + ( n − 1 ) ∫ cos n − 2 x ( 1 − cos 2 x ) d x
= cos n − 1 x sin x + ( n − 1 ) I n − 2 − ( n − 1 ) I n = \cos^{n-1}x\sin x + (n-1)I_{n-2} - (n-1)I_n = cos n − 1 x sin x + ( n − 1 ) I n − 2 − ( n − 1 ) I n
n I n = cos n − 1 x sin x + ( n − 1 ) I n − 2 nI_n = \cos^{n-1}x\sin x + (n-1)I_{n-2} n I n = cos n − 1 x sin x + ( n − 1 ) I n − 2
I n = 1 n cos n − 1 x sin x + n − 1 n I n − 2 + C \boxed{I_n = \frac{1}{n}\cos^{n-1}x\sin x + \frac{n-1}{n}I_{n-2} + C} I n = n 1 cos n − 1 x sin x + n n − 1 I n − 2 + C
Problem 3 Evaluate $\displaystyle\int \frac{2x-1}{x^2+4x+13}\,dx$.Hint 3 Complete the square: $x^2+4x+13 = (x+2)^2+9$. Split the numerator into a multiple of $(2x+4)$ plus a constant.Answer 3 $x^2+4x+13 = (x+2)^2+9$. Write $2x-1 = (2x+4) - 5$.∫ 2 x + 4 ( x + 2 ) 2 + 9 d x − 5 ∫ 1 ( x + 2 ) 2 + 9 d x \displaystyle\int\frac{2x+4}{(x+2)^2+9}\,dx - 5\int\frac{1}{(x+2)^2+9}\,dx ∫ ( x + 2 ) 2 + 9 2 x + 4 d x − 5 ∫ ( x + 2 ) 2 + 9 1 d x
= ln ( x 2 + 4 x + 13 ) − 5 3 arctan ( x + 2 3 ) + C = \ln(x^2+4x+13) - \frac{5}{3}\arctan\!\left(\frac{x+2}{3}\right) + C = ln ( x 2 + 4 x + 13 ) − 3 5 arctan ( 3 x + 2 ) + C
Problem 4 Evaluate $\displaystyle\int_0^{\pi/2} \sin^5 x\,dx$ using the reduction formula.Hint 4 Use $I_n = \dfrac{n-1}{n}I_{n-2}$ with $I_1 = 1$.Answer 4 $I_5 = \dfrac{4}{5}I_3 = \dfrac{4}{5}\cdot\dfrac{2}{3}I_1 = \dfrac{4}{5}\cdot\dfrac{2}{3}\cdot 1 = \dfrac{8}{15}$.Problem 5 Find the volume generated by rotating the region bounded by $y = x^2$$y = 0$$x = 0$$x = 2$ about the $y$-axis.Hint 5 Express $x$ in terms of $y$ ($x = \sqrt{y}$) and integrate with respect to $y$ from $0$ to $4$ Or use the Shell method: $V = 2\pi\int_0^2 x\cdot x^2\,dx$.Answer 5 Using the disc method about the $y$-axis: $V = \pi\int_0^4 x^2\,dy = \pi\int_0^4 y\,dy = \pi\left[\frac{y^2}{2}\right]_0^4 = 8\pi$.Problem 6 Find $\dfrac{d}{dx}\left[x\arcsin x + \sqrt{1-x^2}\right]$ and hence evaluate $\displaystyle\int_0^{1/2} \arcsin x\,dx$.Hint 6 Differentiate using the product rule and the chain rule with $\dfrac{d}{dx}\arcsin x$.Answer 6 $\dfrac{d}{dx}\bigl[x\arcsin x + \sqrt{1-x^2}\bigr] = \arcsin x + \dfrac{x}{\sqrt{1-x^2}} + \dfrac{-x}{\sqrt{1-x^2}} = \arcsin x$.Therefore ∫ arcsin x d x = x arcsin x + 1 − x 2 + C \displaystyle\int \arcsin x\,dx = x\arcsin x + \sqrt{1-x^2} + C ∫ arcsin x d x = x arcsin x + 1 − x 2 + C .
∫ 0 1 / 2 arcsin x d x = [ x arcsin x + 1 − x 2 ] 0 1 / 2 = 1 2 ⋅ π 6 + 3 2 − 1 = π 12 + 3 2 − 1 \displaystyle\int_0^{1/2}\arcsin x\,dx = \left[x\arcsin x + \sqrt{1-x^2}\right]_0^{1/2} = \frac{1}{2}\cdot\frac{\pi}{6} + \frac{\sqrt{3}}{2} - 1 = \frac{\pi}{12} + \frac{\sqrt{3}}{2} - 1 ∫ 0 1/2 arcsin x d x = [ x arcsin x + 1 − x 2 ] 0 1/2 = 2 1 ⋅ 6 π + 2 3 − 1 = 12 π + 2 3 − 1 .
Problem 7 Find the arc length of the curve $y = \dfrac{x^3}{6} + \dfrac{1}{2x}$ from $x = 1$ to $x = 3$.Hint 7 Compute $\dfrac{dy}{dx} = \dfrac{x^2}{2} - \dfrac{1}{2x^2}$. Show that $1+\left(\dfrac{dy}{dx}\right)^2$ is a perfect square.Answer 7 $\dfrac{dy}{dx} = \dfrac{x^2}{2} - \dfrac{1}{2x^2}$.1 + ( d y d x ) 2 = 1 + x 4 4 − 1 2 + 1 4 x 4 = x 4 4 + 1 2 + 1 4 x 4 = ( x 2 2 + 1 2 x 2 ) 2 1+\left(\dfrac{dy}{dx}\right)^2 = 1 + \dfrac{x^4}{4} - \dfrac{1}{2} + \dfrac{1}{4x^4} = \dfrac{x^4}{4} + \dfrac{1}{2} + \dfrac{1}{4x^4} = \left(\dfrac{x^2}{2} + \dfrac{1}{2x^2}\right)^2 1 + ( d x d y ) 2 = 1 + 4 x 4 − 2 1 + 4 x 4 1 = 4 x 4 + 2 1 + 4 x 4 1 = ( 2 x 2 + 2 x 2 1 ) 2
s = ∫ 1 3 ( x 2 2 + 1 2 x 2 ) d x = [ x 3 6 − 1 2 x ] 1 3 = ( 9 2 − 1 6 ) − ( 1 6 − 1 2 ) = 14 3 s = \displaystyle\int_1^3\left(\dfrac{x^2}{2} + \dfrac{1}{2x^2}\right)dx = \left[\dfrac{x^3}{6} - \dfrac{1}{2x}\right]_1^3 = \left(\dfrac{9}{2}-\dfrac{1}{6}\right)-\left(\dfrac{1}{6}-\dfrac{1}{2}\right) = \dfrac{14}{3} s = ∫ 1 3 ( 2 x 2 + 2 x 2 1 ) d x = [ 6 x 3 − 2 x 1 ] 1 3 = ( 2 9 − 6 1 ) − ( 6 1 − 2 1 ) = 3 14 .
Problem 8 Evaluate $\displaystyle\int_0^{\infty}\frac{1}{4+x^2}\,dx$.Hint 8 Use $\displaystyle\int\frac{1}{a^2+x^2}\,dx = \frac{1}{a}\arctan\frac{x}{a}$. Here $a = 2$.Answer 8 $\displaystyle\int_0^{\infty}\frac{1}{4+x^2}\,dx = \left[\frac{1}{2}\arctan\frac{x}{2}\right]_0^{\infty} = \frac{1}{2}\cdot\frac{\pi}{2} - 0 = \frac{\pi}{4}$.Problem 9 The curve $x = t^2$$y = t^3$ for $0 \leq t \leq 2$ is rotated about the $x$-axis. Find the volume of Revolution.Hint 9 Use $V = \pi\displaystyle\int_{t_1}^{t_2}y^2\,\frac{dx}{dt}\,dt$. Here $\dfrac{dx}{dt} = 2t$.Answer 9 $V = \pi\displaystyle\int_0^2 t^6 \cdot 2t\,dt = 2\pi\int_0^2 t^7\,dt = 2\pi\left[\frac{t^8}{8}\right]_0^2 = 2\pi\cdot\frac{256}{8} = 64\pi$.Problem 10 Find $\displaystyle\int e^x\sin 2x\,dx$.Hint 10 Apply integration by parts twice. Keep $u = e^x$ on both applications. The original integral will reappear.Answer 10 Let $I = \displaystyle\int e^x\sin 2x\,dx$. First: $u = e^x$$dv = \sin 2x\,dx$. $du = e^x\,dx$$v = -\frac{1}{2}\cos 2x$.I = − 1 2 e x cos 2 x + 1 2 ∫ e x cos 2 x d x I = -\frac{1}{2}e^x\cos 2x + \frac{1}{2}\int e^x\cos 2x\,dx I = − 2 1 e x cos 2 x + 2 1 ∫ e x cos 2 x d x .
Second on ∫ e x cos 2 x d x \int e^x\cos 2x\,dx ∫ e x cos 2 x d x : u = e^x$$dv = \cos 2x\,dx . d u = e x d x du = e^x\,dx d u = e x d x v = 1 2 sin 2 x v = \frac{1}{2}\sin 2x v = 2 1 sin 2 x .
∫ e x cos 2 x d x = 1 2 e x sin 2 x − 1 2 ∫ e x sin 2 x d x = 1 2 e x sin 2 x − 1 2 I \int e^x\cos 2x\,dx = \frac{1}{2}e^x\sin 2x - \frac{1}{2}\int e^x\sin 2x\,dx = \frac{1}{2}e^x\sin 2x - \frac{1}{2}I ∫ e x cos 2 x d x = 2 1 e x sin 2 x − 2 1 ∫ e x sin 2 x d x = 2 1 e x sin 2 x − 2 1 I .
I = − 1 2 e x cos 2 x + 1 4 e x sin 2 x − 1 4 I I = -\frac{1}{2}e^x\cos 2x + \frac{1}{4}e^x\sin 2x - \frac{1}{4}I I = − 2 1 e x cos 2 x + 4 1 e x sin 2 x − 4 1 I .
5 4 I = e x ( sin 2 x 4 − cos 2 x 2 ) \frac{5}{4}I = e^x\left(\frac{\sin 2x}{4} - \frac{\cos 2x}{2}\right) 4 5 I = e x ( 4 s i n 2 x − 2 c o s 2 x ) .
I = e x ( sin 2 x − 2 cos 2 x ) 5 + C \boxed{I = \frac{e^x(\sin 2x - 2\cos 2x)}{5} + C} I = 5 e x ( sin 2 x − 2 cos 2 x ) + C
Problem. If y = x 2 e 3 x y = x^2 e^{3x} y = x 2 e 3 x Find d 4 y d x 4 \dfrac{d^4 y}{dx^4} d x 4 d 4 y .
Solution. We use Leibniz’s rule: ( u v ) ( n ) = ∑ k = 0 n ( n k ) u ( k ) v ( n − k ) (uv)^{(n)} = \displaystyle\sum_{k=0}^{n} \binom{n}{k} u^{(k)} v^{(n-k)} ( uv ) ( n ) = k = 0 ∑ n ( k n ) u ( k ) v ( n − k ) .
Let u = x 2 u = x^2 u = x 2 and v = e 3 x v = e^{3x} v = e 3 x .
u' = 2x$$u'' = 2$$u''' = 0$$u^{(4)} = 0 .v ( k ) = 3 k e 3 x v^{(k)} = 3^k e^{3x} v ( k ) = 3 k e 3 x for all k k k .d 4 y d x 4 = ( 4 0 ) x 2 ⋅ 3 4 e 3 x + ( 4 1 ) 2 x ⋅ 3 3 e 3 x + ( 4 2 ) 2 ⋅ 3 2 e 3 x + 0 + 0 \frac{d^4 y}{dx^4} = \binom{4}{0} x^2 \cdot 3^4 e^{3x} + \binom{4}{1} 2x \cdot 3^3 e^{3x} + \binom{4}{2} 2 \cdot 3^2 e^{3x} + 0 + 0 d x 4 d 4 y = ( 0 4 ) x 2 ⋅ 3 4 e 3 x + ( 1 4 ) 2 x ⋅ 3 3 e 3 x + ( 2 4 ) 2 ⋅ 3 2 e 3 x + 0 + 0 = 81 x 2 e 3 x + 4 ⋅ 54 x e 3 x + 6 ⋅ 18 e 3 x = 81x^2 e^{3x} + 4 \cdot 54x e^{3x} + 6 \cdot 18 e^{3x} = 81 x 2 e 3 x + 4 ⋅ 54 x e 3 x + 6 ⋅ 18 e 3 x = ( 81 x 2 + 216 x + 108 ) e 3 x \boxed{= (81x^2 + 216x + 108)e^{3x}} = ( 81 x 2 + 216 x + 108 ) e 3 x Problem. Establish and use a reduction formula for I n = ∫ x n e x d x I_n = \int x^n e^x\,dx I n = ∫ x n e x d x .
Solution. Using integration by parts with u = x^n$$dv = e^x\,dx :
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 - \int nx^{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 Therefore I n = x n e x − n I n − 1 \boxed{I_n = x^n e^x - nI_{n-1}} I n = x n e x − n I n − 1 with I 0 = e x + C I_0 = e^x + C I 0 = e x + C .
To find I 3 I_3 I 3 :
I_1 = x e^x - e^x$$I_2 = x^2 e^x - 2x e^x + 2e^x$$I_3 = x^3 e^x - 3x^2 e^x + 6x e^x - 6e^x .
I 3 = ( x 3 − 3 x 2 + 6 x − 6 ) e x + C \boxed{I_3 = (x^3 - 3x^2 + 6x - 6)e^x + C} I 3 = ( x 3 − 3 x 2 + 6 x − 6 ) e x + C Problem. Determine whether ∫ 0 1 1 x d x \displaystyle\int_0^1 \frac{1}{\sqrt{x}}\,dx ∫ 0 1 x 1 d x converges, And evaluate if it does.
Solution. The integrand is undefined at x = 0 x = 0 x = 0 . Write:
∫ 0 1 x − 1 / 2 d x = lim a → 0 + ∫ a 1 x − 1 / 2 d x = lim a → 0 + [ 2 x 1 / 2 ] a 1 = lim a → 0 + ( 2 − 2 a ) = 2 \int_0^1 x^{-1/2}\,dx = \lim_{a \to 0^+} \int_a^1 x^{-1/2}\,dx = \lim_{a \to 0^+} \left[2x^{1/2}\right]_a^1 = \lim_{a \to 0^+} (2 - 2\sqrt{a}) = 2 ∫ 0 1 x − 1/2 d x = a → 0 + lim ∫ a 1 x − 1/2 d x = a → 0 + lim [ 2 x 1/2 ] a 1 = a → 0 + lim ( 2 − 2 a ) = 2 Since the limit exists and is finite, the integral converges. ∫ 0 1 1 x d x = 2 \boxed{\displaystyle\int_0^1 \frac{1}{\sqrt{x}}\,dx = 2} ∫ 0 1 x 1 d x = 2
Problem. Evaluate ∫ 0 π / 2 1 1 + sin x d x \displaystyle\int_0^{\pi/2} \frac{1}{1 + \sin x}\,dx ∫ 0 π /2 1 + sin x 1 d x using the Weierstrass substitution.
Solution. Let t = tan ( x / 2 ) t = \tan(x/2) t = tan ( x /2 ) So sin x = 2 t 1 + t 2 \sin x = \dfrac{2t}{1+t^2} sin x = 1 + t 2 2 t and d x = 2 d t 1 + t 2 dx = \dfrac{2\,dt}{1+t^2} d x = 1 + t 2 2 d t .
When x = 0 x = 0 x = 0 : t = 0 t = 0 t = 0 . When x = π / 2 x = \pi/2 x = π /2 : t = 1 t = 1 t = 1 .
∫ 0 1 1 1 + 2 t 1 + t 2 ⋅ 2 d t 1 + t 2 = ∫ 0 1 2 d t ( 1 + t 2 ) + 2 t = ∫ 0 1 2 d t t 2 + 2 t + 1 = ∫ 0 1 2 d t ( t + 1 ) 2 \int_0^1 \frac{1}{1 + \frac{2t}{1+t^2}} \cdot \frac{2\,dt}{1+t^2} = \int_0^1 \frac{2\,dt}{(1+t^2) + 2t} = \int_0^1 \frac{2\,dt}{t^2 + 2t + 1} = \int_0^1 \frac{2\,dt}{(t+1)^2} ∫ 0 1 1 + 1 + t 2 2 t 1 ⋅ 1 + t 2 2 d t = ∫ 0 1 ( 1 + t 2 ) + 2 t 2 d t = ∫ 0 1 t 2 + 2 t + 1 2 d t = ∫ 0 1 ( t + 1 ) 2 2 d t = [ − 2 t + 1 ] 0 1 = − 1 + 2 = 1 = \left[-\frac{2}{t+1}\right]_0^1 = -1 + 2 = \boxed{1} = [ − t + 1 2 ] 0 1 = − 1 + 2 = 1 Problem. A curve is given by x = t − sin t x = t - \sin t x = t − sin t , y = 1 − cos t y = 1 - \cos t y = 1 − cos t for 0 ≤ t ≤ 2 π 0 \leq t \leq 2\pi 0 ≤ t ≤ 2 π . Find The total arc length.
Solution. d x d t = 1 − cos t \dfrac{dx}{dt} = 1 - \cos t d t d x = 1 − cos t , d y d t = sin t \dfrac{dy}{dt} = \sin t d t d y = sin t .
s = ∫ 0 2 π ( 1 − cos t ) 2 + sin 2 t d t = ∫ 0 2 π 1 − 2 cos t + cos 2 t + sin 2 t d t s = \int_0^{2\pi} \sqrt{(1-\cos t)^2 + \sin^2 t}\,dt = \int_0^{2\pi} \sqrt{1 - 2\cos t + \cos^2 t + \sin^2 t}\,dt s = ∫ 0 2 π ( 1 − cos t ) 2 + sin 2 t d t = ∫ 0 2 π 1 − 2 cos t + cos 2 t + sin 2 t d t = ∫ 0 2 π 2 − 2 cos t d t = ∫ 0 2 π 4 sin 2 ( t / 2 ) d t = ∫ 0 2 π 2 ∣ sin ( t / 2 ) ∣ d t = \int_0^{2\pi} \sqrt{2 - 2\cos t}\,dt = \int_0^{2\pi} \sqrt{4\sin^2(t/2)}\,dt = \int_0^{2\pi} 2|\sin(t/2)|\,dt = ∫ 0 2 π 2 − 2 cos t d t = ∫ 0 2 π 4 sin 2 ( t /2 ) d t = ∫ 0 2 π 2∣ sin ( t /2 ) ∣ d t For 0 ≤ t ≤ 2 π 0 \leq t \leq 2\pi 0 ≤ t ≤ 2 π , sin ( t / 2 ) ≥ 0 \sin(t/2) \geq 0 sin ( t /2 ) ≥ 0 So:
s = 2 ∫ 0 2 π sin ( t / 2 ) d t = 2 [ − 2 cos ( t / 2 ) ] 0 2 π = 2 ( 2 + 2 ) = 8 s = 2\int_0^{2\pi} \sin(t/2)\,dt = 2\left[-2\cos(t/2)\right]_0^{2\pi} = 2(2 + 2) = \boxed{8} s = 2 ∫ 0 2 π sin ( t /2 ) d t = 2 [ − 2 cos ( t /2 ) ] 0 2 π = 2 ( 2 + 2 ) = 8 Problem. Evaluate lim x → 0 x − sin x x 3 \displaystyle\lim_{x \to 0} \frac{x - \sin x}{x^3} x → 0 lim x 3 x − sin x .
Solution. Expand sin x \sin x sin x as a Maclaurin series:
sin x = x − x 3 6 + x 5 120 − ⋯ \sin x = x - \frac{x^3}{6} + \frac{x^5}{120} - \cdots sin x = x − 6 x 3 + 120 x 5 − ⋯ x − sin x x 3 = x − ( x − x 3 6 + x 5 120 − ⋯ ) x 3 = x 3 6 − x 5 120 + ⋯ x 3 = 1 6 − x 2 120 + ⋯ \frac{x - \sin x}{x^3} = \frac{x - \left(x - \frac{x^3}{6} + \frac{x^5}{120} - \cdots\right)}{x^3} = \frac{\frac{x^3}{6} - \frac{x^5}{120} + \cdots}{x^3} = \frac{1}{6} - \frac{x^2}{120} + \cdots x 3 x − sin x = x 3 x − ( x − 6 x 3 + 120 x 5 − ⋯ ) = x 3 6 x 3 − 120 x 5 + ⋯ = 6 1 − 120 x 2 + ⋯ Taking x → 0 x \to 0 x → 0 : lim x → 0 x − sin x x 3 = 1 6 \boxed{\displaystyle\lim_{x \to 0} \frac{x - \sin x}{x^3} = \frac{1}{6}} x → 0 lim x 3 x − sin x = 6 1
Problem. Evaluate ∫ arcsin x d x \displaystyle\int \arcsin x\,dx ∫ arcsin x d x .
Solution. Use integration by parts with u = arcsin x u = \arcsin x u = arcsin x , d v = d x dv = dx d v = d x :
d u = 1 1 − x 2 d x , v = x du = \frac{1}{\sqrt{1-x^2}}\,dx, \quad v = x d u = 1 − x 2 1 d x , v = x ∫ arcsin x d x = x arcsin x − ∫ x 1 − x 2 d x \int \arcsin x\,dx = x\arcsin x - \int \frac{x}{\sqrt{1-x^2}}\,dx ∫ arcsin x d x = x arcsin x − ∫ 1 − x 2 x d x For the second integral, let w = 1 − x 2 w = 1 - x^2 w = 1 − x 2 , d w = − 2 x d x dw = -2x\,dx d w = − 2 x d x :
∫ x 1 − x 2 d x = − 1 − x 2 \int \frac{x}{\sqrt{1-x^2}}\,dx = -\sqrt{1-x^2} ∫ 1 − x 2 x d x = − 1 − x 2 ∫ arcsin x d x = x arcsin x + 1 − x 2 + C \boxed{\int \arcsin x\,dx = x\arcsin x + \sqrt{1-x^2} + C} ∫ arcsin x d x = x arcsin x + 1 − x 2 + C A[04 Further Calculus] --> B[Key Concepts]
A --> D[Practical Applications]
B --> E[Fundamental definitions]
D --> G[Real-world usage]
Integration by parts is the reverse of the product rule, allowing you to transfer derivatives between functions. Think of it as a negotiation: you give away one function’s derivative in exchange for integrating the other. Reduction formulae create a staircase where each integral is expressed in terms of a simpler one, allowing you to climb down to a base case you can evaluate directly. Inverse trigonometric functions arise because their derivatives produce rational functions, creating a bridge between algebraic and trigonometric integration. Volumes of revolution are computed by summing infinitesimally thin discs stacked along an axis, like building a solid from a stack of coins. Arc length measures the actual distance along a curve rather than straight-line approximation.
Pitfall Correct Approach Forgetting the chain rule when differentiating composite inverse trig functions Always write d d x [ arcsin ( u ) ] = u ′ 1 − u 2 \dfrac{d}{dx}\!\left[\arcsin(u)\right] = \dfrac{u'}{\sqrt{1-u^2}} d x d [ arcsin ( u ) ] = 1 − u 2 u ′ Using ln ∥ x ∥ \ln \| x \| ln ∥ x ∥ before checking if the integral is improper Check for discontinuities in the interval first Forgetting + C +C + C on every antiderivative Every indefinite integral needs an arbitrary constant Applying reduction formulae without checking the base case Always state I 0 I_0 I 0 or I 1 I_1 I 1 explicitly Confusing d n y d x n \dfrac{d^n y}{dx^n} d x n d n y notation with ( d y d x ) n \left(\dfrac{dy}{dx}\right)^n ( d x d y ) n d n y d x n \dfrac{d^n y}{dx^n} d x n d n y is the n n n -th derivative, not the n n n -th power
Using the substitution u = e x u = e^x u = e x Find ∫ e x e 2 x + 1 d x \displaystyle\int \frac{e^x}{e^{2x} + 1}\,dx ∫ e 2 x + 1 e x d x .
Solution u = e x u = e^x u = e x , d u = e x d x du = e^x\,dx d u = e x d x .
∫ d u u 2 + 1 = arctan u + C = arctan ( e x ) + C \int \frac{du}{u^2 + 1} = \arctan u + C = \boxed{\arctan(e^x) + C} ∫ u 2 + 1 d u = arctan u + C = arctan ( e x ) + C The reduction formula I n = ∫ 0 π / 4 tan n x d x I_n = \displaystyle\int_0^{\pi/4} \tan^n x\,dx I n = ∫ 0 π /4 tan n x d x satisfies I n = 1 n − 1 − I n − 2 I_n = \dfrac{1}{n-1} - I_{n-2} I n = n − 1 1 − I n − 2 for n ≥ 2 n \geq 2 n ≥ 2 . Given I 0 = π 4 I_0 = \dfrac{\pi}{4} I 0 = 4 π and I 1 = 1 2 ln 2 I_1 = \dfrac{1}{2}\ln 2 I 1 = 2 1 ln 2 Find I 3 I_3 I 3 .
Solution I 3 = 1 2 − I 1 = 1 2 − 1 2 ln 2 = 1 2 ( 1 − ln 2 ) I_3 = \dfrac{1}{2} - I_1 = \dfrac{1}{2} - \dfrac{1}{2}\ln 2 = \dfrac{1}{2}(1 - \ln 2) I 3 = 2 1 − I 1 = 2 1 − 2 1 ln 2 = 2 1 ( 1 − ln 2 ) .
To verify: I 2 = 1 1 − I 0 = 1 − π 4 I_2 = \dfrac{1}{1} - I_0 = 1 - \dfrac{\pi}{4} I 2 = 1 1 − I 0 = 1 − 4 π . Then I 3 = 1 2 − I 1 = 1 2 − 1 2 ln 2 I_3 = \dfrac{1}{2} - I_1 = \dfrac{1}{2} - \dfrac{1}{2}\ln 2 I 3 = 2 1 − I 1 = 2 1 − 2 1 ln 2 . Consistent. I 3 = 1 2 ( 1 − ln 2 ) \boxed{I_3 = \dfrac{1}{2}(1 - \ln 2)} I 3 = 2 1 ( 1 − ln 2 )
Find the area enclosed by the curve x = t 2 x = t^2 x = t 2 , y = t 3 − t y = t^3 - t y = t 3 − t for − 1 ≤ t ≤ 1 -1 \leq t \leq 1 − 1 ≤ t ≤ 1 .
Solution Using the parametric area formula A = ∫ y d x d t d t A = \displaystyle\int y\,\frac{dx}{dt}\,dt A = ∫ y d t d x d t :
A = ∫ − 1 1 ( t 3 − t ) ( 2 t ) d t = 2 ∫ − 1 1 ( t 4 − t 2 ) d t = 2 [ t 5 5 − t 3 3 ] − 1 1 A = \int_{-1}^{1} (t^3 - t)(2t)\,dt = 2\int_{-1}^{1} (t^4 - t^2)\,dt = 2\left[\frac{t^5}{5} - \frac{t^3}{3}\right]_{-1}^{1} A = ∫ − 1 1 ( t 3 − t ) ( 2 t ) d t = 2 ∫ − 1 1 ( t 4 − t 2 ) d t = 2 [ 5 t 5 − 3 t 3 ] − 1 1 Since t 5 − 5 3 t 3 t^5 - \frac{5}{3}t^3 t 5 − 3 5 t 3 is odd (each term is odd), the integral from − 1 -1 − 1 to 1 1 1 is zero.
A = 0 \boxed{A = 0} A = 0 (the curve traces back over itself symmetrically).
Prove that d d x [ arctan x ] = 1 1 + x 2 \dfrac{d}{dx}\!\left[\arctan x\right] = \dfrac{1}{1+x^2} d x d [ arctan x ] = 1 + x 2 1 from first principles Using implicit differentiation.
Solution Let y = arctan x y = \arctan x y = arctan x So x = tan y x = \tan y x = tan y . Differentiating implicitly with respect to x x x :
1 = sec 2 y ⋅ d y d x 1 = \sec^2 y \cdot \frac{dy}{dx} 1 = sec 2 y ⋅ d x d y d y d x = cos 2 y = 1 sec 2 y = 1 1 + tan 2 y = 1 1 + x 2 \frac{dy}{dx} = \cos^2 y = \frac{1}{\sec^2 y} = \frac{1}{1 + \tan^2 y} = \frac{1}{1 + x^2} d x d y = cos 2 y = sec 2 y 1 = 1 + tan 2 y 1 = 1 + x 2 1 ■ \blacksquare ■
Evaluate ∫ 0 1 ln x 1 + x d x \displaystyle\int_0^1 \frac{\ln x}{1+x}\,dx ∫ 0 1 1 + x ln x d x Expressing your answer in terms Of ∑ n = 1 ∞ ( − 1 ) n + 1 n 2 \displaystyle\sum_{n=1}^{\infty} \frac{(-1)^{n+1}}{n^2} n = 1 ∑ ∞ n 2 ( − 1 ) n + 1 .
Solution Expand 1 1 + x = ∑ n = 0 ∞ ( − 1 ) n x n \dfrac{1}{1+x} = \displaystyle\sum_{n=0}^{\infty} (-1)^n x^n 1 + x 1 = n = 0 ∑ ∞ ( − 1 ) n x n for ∣ x ∣ < 1 |x| < 1 ∣ x ∣ < 1 :
∫ 0 1 ln x ∑ n = 0 ∞ ( − 1 ) n x n d x = ∑ n = 0 ∞ ( − 1 ) n ∫ 0 1 x n ln x d x \int_0^1 \ln x \sum_{n=0}^{\infty} (-1)^n x^n\,dx = \sum_{n=0}^{\infty} (-1)^n \int_0^1 x^n \ln x\,dx ∫ 0 1 ln x n = 0 ∑ ∞ ( − 1 ) n x n d x = n = 0 ∑ ∞ ( − 1 ) n ∫ 0 1 x n ln x d x Using integration by parts or the standard result ∫ 0 1 x n ln x d x = − 1 ( n + 1 ) 2 \displaystyle\int_0^1 x^n \ln x\,dx = -\frac{1}{(n+1)^2} ∫ 0 1 x n ln x d x = − ( n + 1 ) 2 1 :
= − ∑ n = 0 ∞ ( − 1 ) n ( n + 1 ) 2 = − ∑ n = 1 ∞ ( − 1 ) n − 1 n 2 = ∑ n = 1 ∞ ( − 1 ) n n 2 = -\sum_{n=0}^{\infty} \frac{(-1)^n}{(n+1)^2} = -\sum_{n=1}^{\infty} \frac{(-1)^{n-1}}{n^2} = \sum_{n=1}^{\infty} \frac{(-1)^n}{n^2} = − n = 0 ∑ ∞ ( n + 1 ) 2 ( − 1 ) n = − n = 1 ∑ ∞ n 2 ( − 1 ) n − 1 = n = 1 ∑ ∞ n 2 ( − 1 ) n This equals − π 2 12 -\dfrac{\pi^2}{12} − 12 π 2 .
Integration techniques (substitution, parts, partial fractions) are essential tools for solving Differential equations. See Differential Equations .
Taylor and Maclaurin expansions provide powerful tools for evaluating integrals that cannot be found in closed form. See Maclaurin and Taylor Series .
Arc length and area calculations are used extensively in mechanics for work-energy problems. See Circular Motion .
The inverse hyperbolic functions arise from integration: ∫ d x x 2 + a 2 = arsinh ( x / a ) + C \displaystyle\int \frac{dx}{\sqrt{x^2+a^2}} = \operatorname{arsinh}(x/a) + C ∫ x 2 + a 2 d x = arsinh ( x / a ) + C . See Hyperbolic Functions .
When choosing u u u and d v dv d v for integration by parts, use the LIATE priority:
L ogarithmic functionsI nverse trigonometric functionsA lgebraic functions (polynomials)T rigonometric functionsE xponential functionsThe function higher on the list should be chosen as u u u .
For integrals involving rational functions of sin x \sin x sin x and cos x \cos x cos x The substitution t = tan ( x / 2 ) t = \tan(x/2) t = tan ( x /2 ) converts them to rational functions of t t t :
\sin x = \dfrac{2t}{1+t^2}$$\cos x = \dfrac{1-t^2}{1+t^2}$$dx = \dfrac{2\,dt}{1+t^2} .
Form Result ∫ f ′ ( x ) f ( x ) d x \displaystyle\int \frac{f'(x)}{f(x)}\,dx ∫ f ( x ) f ′ ( x ) d x ln ∥ f ( x ) ∥ + C \ln \| f(x) \| + C ln ∥ f ( x ) ∥ + C ∫ f ′ ( x ) f ( x ) d x \displaystyle\int \frac{f'(x)}{\sqrt{f(x)}}\,dx ∫ f ( x ) f ′ ( x ) d x 2 f ( x ) + C 2\sqrt{f(x)} + C 2 f ( x ) + C ∫ f ( x ) ⋅ f ′ ( x ) d x \displaystyle\int f(x) \cdot f'(x)\,dx ∫ f ( x ) ⋅ f ′ ( x ) d x [ f ( x ) ] 2 2 + C \dfrac{[f(x)]^2}{2} + C 2 [ f ( x ) ] 2 + C
Result Formula Integration by parts ∫ u d v = u v − ∫ v d u \displaystyle\int u\,dv = uv - \int v\,du ∫ u d v = uv − ∫ v d u Reduction formula (by parts) Express I n I_n I n in terms of I n − 1 I_{n-1} I n − 1 or I n − 2 I_{n-2} I n − 2 Arc length (Cartesian) s = ∫ a b 1 + ( d y d x ) 2 d x s = \displaystyle\int_a^b \sqrt{1+\left(\frac{dy}{dx}\right)^2}\,dx s = ∫ a b 1 + ( d x d y ) 2 d x Arc length (parametric) s = ∫ α β x ˙ 2 + y ˙ 2 d t s = \displaystyle\int_\alpha^\beta \sqrt{\dot{x}^2+\dot{y}^2}\,dt s = ∫ α β x ˙ 2 + y ˙ 2 d t Area under parametric curve A = ∫ y d x d t d t A = \displaystyle\int y\frac{dx}{dt}\,dt A = ∫ y d t d x d t Surface of revolution S = 2 π ∫ a b y 1 + ( y ′ ) 2 d x S = 2\pi\displaystyle\int_a^b y\sqrt{1+(y')^2}\,dx S = 2 π ∫ a b y 1 + ( y ′ ) 2 d x Derivative of arcsin x \arcsin x arcsin x 1 1 − x 2 \dfrac{1}{\sqrt{1-x^2}} 1 − x 2 1 Derivative of arctan x \arctan x arctan x 1 1 + x 2 \dfrac{1}{1+x^2} 1 + x 2 1 Improper integral test ∫ a ∞ f ( x ) d x = lim b → ∞ ∫ a b f ( x ) d x \displaystyle\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
Using integration by parts, evaluate ∫ x 3 e − x d x \displaystyle\int x^3 e^{-x}\,dx ∫ x 3 e − x d x .
Solution Let u = x^3$$dv = e^{-x}\,dx . du = 3x^2\,dx$$v = -e^{-x} .
∫ x 3 e − x d x = − x 3 e − x + 3 ∫ x 2 e − x d x \int x^3 e^{-x}\,dx = -x^3 e^{-x} + 3\int x^2 e^{-x}\,dx ∫ x 3 e − x d x = − x 3 e − x + 3 ∫ x 2 e − x d x .
Repeating: ∫ x 2 e − x d x = − x 2 e − x + 2 ∫ x e − x d x = − x 2 e − x − 2 x e − x + 2 ∫ e − x d x \int x^2 e^{-x}\,dx = -x^2 e^{-x} + 2\int xe^{-x}\,dx = -x^2 e^{-x} - 2xe^{-x} + 2\int e^{-x}\,dx ∫ x 2 e − x d x = − x 2 e − x + 2 ∫ x e − x d x = − x 2 e − x − 2 x e − x + 2 ∫ e − x d x .
= − x 2 e − x − 2 x e − x − 2 e − x = -x^2 e^{-x} - 2xe^{-x} - 2e^{-x} = − x 2 e − x − 2 x e − x − 2 e − x .
Therefore: ∫ x 3 e − x d x = − x 3 e − x − 3 x 2 e − x − 6 x e − x − 6 e − x + C \int x^3 e^{-x}\,dx = -x^3 e^{-x} - 3x^2 e^{-x} - 6xe^{-x} - 6e^{-x} + C ∫ x 3 e − x d x = − x 3 e − x − 3 x 2 e − x − 6 x e − x − 6 e − x + C .
= − e − x ( x 3 + 3 x 2 + 6 x + 6 ) + C \boxed{= -e^{-x}(x^3 + 3x^2 + 6x + 6) + C} = − e − x ( x 3 + 3 x 2 + 6 x + 6 ) + C
Find the arc length of the curve y = ln ( cos x ) y = \ln(\cos x) y = ln ( cos x ) from x = 0 x = 0 x = 0 to x = π / 4 x = \pi/4 x = π /4 .
Solution y ′ = − tan x y' = -\tan x y ′ = − tan x . 1 + ( y ′ ) 2 = 1 + tan 2 x = sec 2 x 1 + (y')^2 = 1 + \tan^2 x = \sec^2 x 1 + ( y ′ ) 2 = 1 + tan 2 x = sec 2 x .
s = ∫ 0 π / 4 sec x d x = [ ln ∣ sec x + tan x ∣ ] 0 π / 4 = ln ( 2 + 1 ) − ln ( 1 ) = ln ( 2 + 1 ) s = \displaystyle\int_0^{\pi/4} \sec x\,dx = [\ln|\sec x + \tan x|]_0^{\pi/4} = \ln(\sqrt{2}+1) - \ln(1) = \boxed{\ln(\sqrt{2}+1)} s = ∫ 0 π /4 sec x d x = [ ln ∣ sec x + tan x ∣ ] 0 π /4 = ln ( 2 + 1 ) − ln ( 1 ) = ln ( 2 + 1 ) .
Prove that ∫ 0 π / 2 sin n x d x = n − 1 n ⋅ n − 3 n − 2 ⋯ × { 1 n odd π 2 n even \displaystyle\int_0^{\pi/2} \sin^n x\,dx = \dfrac{n-1}{n} \cdot \dfrac{n-3}{n-2} \cdots \times \begin{cases} 1 & n \text{ odd} \\ \dfrac{\pi}{2} & n \text{ even}\end{cases} ∫ 0 π /2 sin n x d x = n n − 1 ⋅ n − 2 n − 3 ⋯ × { 1 2 π n odd n even (Wallis’ formula).
Solution Let 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 .
Integration by parts with u = \sin^{n-1}x$$dv = \sin x\,dx :
I n = [ − cos x sin n − 1 x ] 0 π / 2 + ( n − 1 ) ∫ 0 π / 2 cos 2 x sin n − 2 x d x I_n = [-\cos x \sin^{n-1}x]_0^{\pi/2} + (n-1)\displaystyle\int_0^{\pi/2} \cos^2 x \sin^{n-2}x\,dx I n = [ − cos x sin n − 1 x ] 0 π /2 + ( n − 1 ) ∫ 0 π /2 cos 2 x sin n − 2 x d x
= 0 + ( n − 1 ) ∫ 0 π / 2 ( 1 − sin 2 x ) sin n − 2 x d x = ( n − 1 ) ( I n − 2 − I n ) = 0 + (n-1)\displaystyle\int_0^{\pi/2} (1-\sin^2 x)\sin^{n-2}x\,dx = (n-1)(I_{n-2} - I_n) = 0 + ( n − 1 ) ∫ 0 π /2 ( 1 − sin 2 x ) sin n − 2 x d x = ( n − 1 ) ( I n − 2 − I n ) .
n I n = ( n − 1 ) I n − 2 nI_n = (n-1)I_{n-2} n I n = ( n − 1 ) I n − 2 So I n = n − 1 n I n − 2 \boxed{I_n = \dfrac{n-1}{n}I_{n-2}} I n = n n − 1 I n − 2 .
Base cases: I_0 = \pi/2$$I_1 = 1 .
For even n n n : I n = n − 1 n ⋅ n − 3 n − 2 ⋯ 1 2 ⋅ π 2 I_n = \dfrac{n-1}{n} \cdot \dfrac{n-3}{n-2} \cdots \dfrac{1}{2} \cdot \dfrac{\pi}{2} I n = n n − 1 ⋅ n − 2 n − 3 ⋯ 2 1 ⋅ 2 π .
For odd n n n : I n = n − 1 n ⋅ n − 3 n − 2 ⋯ 2 3 ⋅ 1 I_n = \dfrac{n-1}{n} \cdot \dfrac{n-3}{n-2} \cdots \dfrac{2}{3} \cdot 1 I n = n n − 1 ⋅ n − 2 n − 3 ⋯ 3 2 ⋅ 1 . ■ \blacksquare ■
The gamma function extends the factorial: Γ ( n ) = ( n − 1 ) ! \Gamma(n) = (n-1)! Γ ( n ) = ( n − 1 )! for positive integers, and Γ ( x ) = ∫ 0 ∞ t x − 1 e − t d t \Gamma(x) = \displaystyle\int_0^{\infty} t^{x-1}e^{-t}\,dt Γ ( x ) = ∫ 0 ∞ t x − 1 e − t d t for x > 0 x > 0 x > 0 .
Wallis’ formula leads to the important result: Γ ( 1 / 2 ) = π \Gamma(1/2) = \sqrt{\pi} Γ ( 1/2 ) = π .
For suitable functions f f f : ∫ 0 ∞ f ( a x ) − f ( b x ) x d x = ( f ( 0 ) − f ( ∞ ) ) ln b a \displaystyle\int_0^{\infty} \frac{f(ax)-f(bx)}{x}\,dx = (f(0)-f(\infty))\ln\frac{b}{a} ∫ 0 ∞ x f ( a x ) − f ( b x ) d x = ( f ( 0 ) − f ( ∞ )) ln a b .
Example: ∫ 0 ∞ e − a x − e − b x x d x = ln b a \displaystyle\int_0^{\infty} \frac{e^{-ax}-e^{-bx}}{x}\,dx = \ln\frac{b}{a} ∫ 0 ∞ x e − a x − e − b x d x = ln a b .
Leibniz’s rule: d d α ∫ a b f ( x , α ) d x = ∫ a b ∂ f ∂ α d x \dfrac{d}{d\alpha}\displaystyle\int_a^b f(x,\alpha)\,dx = \int_a^b \frac{\partial f}{\partial\alpha}\,dx d α d ∫ a b f ( x , α ) d x = ∫ a b ∂ α ∂ f d x .
This is a powerful technique for evaluating integrals that depend on a parameter.
If 0 ≤ f ( x ) ≤ g ( x ) 0 \leq f(x) \leq g(x) 0 ≤ f ( x ) ≤ g ( x ) for x ≥ a x \geq a x ≥ a and ∫ a ∞ g ( x ) d x \displaystyle\int_a^{\infty} g(x)\,dx ∫ a ∞ g ( x ) d x converges, Then ∫ a ∞ f ( x ) d x \displaystyle\int_a^{\infty} f(x)\,dx ∫ a ∞ f ( x ) d x also converges.
Evaluate ∫ 0 ∞ x e − x d x \displaystyle\int_0^{\infty} xe^{-x}\,dx ∫ 0 ∞ x e − x d x and relate it to the mean of the exponential Distribution.
Solution Integration by parts with u = x$$dv = e^{-x}\,dx :
= [ − x e − x ] 0 ∞ + ∫ 0 ∞ e − x d x = 0 + 1 = 1 = [-xe^{-x}]_0^{\infty} + \displaystyle\int_0^{\infty} e^{-x}\,dx = 0 + 1 = \boxed{1} = [ − x e − x ] 0 ∞ + ∫ 0 ∞ e − x d x = 0 + 1 = 1 .
This equals E ( X ) E(X) E ( X ) for X ∼ E x p ( 1 ) X \sim \mathrm{Exp}(1) X ∼ Exp ( 1 ) Confirming the result E ( X ) = 1 / λ E(X) = 1/\lambda E ( X ) = 1/ λ with λ = 1 \lambda = 1 λ = 1 .
Prove that ∫ 0 π / 2 sin 2 x cos 2 x d x = π 16 \displaystyle\int_0^{\pi/2} \sin^2 x\cos^2 x\,dx = \frac{\pi}{16} ∫ 0 π /2 sin 2 x cos 2 x d x = 16 π .
Solution sin 2 x cos 2 x = sin 2 2 x 4 = 1 − cos 4 x 8 \sin^2 x\cos^2 x = \dfrac{\sin^2 2x}{4} = \dfrac{1-\cos 4x}{8} sin 2 x cos 2 x = 4 sin 2 2 x = 8 1 − cos 4 x .
∫ 0 π / 2 1 − cos 4 x 8 d x = 1 8 [ x − sin 4 x 4 ] 0 π / 2 = 1 8 ⋅ π 2 = π 16 \displaystyle\int_0^{\pi/2} \frac{1-\cos 4x}{8}\,dx = \frac{1}{8}\!\left[x-\frac{\sin 4x}{4}\right]_0^{\pi/2} = \frac{1}{8}\cdot\frac{\pi}{2} = \boxed{\dfrac{\pi}{16}} ∫ 0 π /2 8 1 − cos 4 x d x = 8 1 [ x − 4 sin 4 x ] 0 π /2 = 8 1 ⋅ 2 π = 16 π . ■ \blacksquare ■
Use integration by parts twice to evaluate ∫ e x cos x d x \displaystyle\int e^x\cos x\,dx ∫ e x cos x d x .
Solution I = ∫ e x cos x d x = e x sin x − ∫ e x sin x d x = e x sin x − ( − e x cos x + ∫ e x cos x d x ) I = \displaystyle\int e^x\cos x\,dx = e^x\sin x - \int e^x\sin x\,dx = e^x\sin x - (-e^x\cos x + \int e^x\cos x\,dx) I = ∫ e x cos x d x = e x sin x − ∫ e x sin x d x = e x sin x − ( − e x cos x + ∫ e x cos x d x ) .
I = e x sin x + e x cos x − I I = e^x\sin x + e^x\cos x - I I = e x sin x + e x cos x − I .
2 I = e x ( sin x + cos x ) 2I = e^x(\sin x+\cos x) 2 I = e x ( sin x + cos x ) .
I = e x ( sin x + cos x ) 2 + C \boxed{I = \dfrac{e^x(\sin x+\cos x)}{2} + C} I = 2 e x ( sin x + cos x ) + C
Evaluate ∫ 0 1 x 3 1 + x 2 d x \displaystyle\int_0^1 \frac{x^3}{1+x^2}\,dx ∫ 0 1 1 + x 2 x 3 d x .
Solution Let u = 1+x^2$$du = 2x\,dx . Note x 2 = u − 1 x^2 = u-1 x 2 = u − 1 So x 3 d x = x 2 ⋅ x d x = ( u − 1 ) ⋅ d u 2 x^3\,dx = x^2 \cdot x\,dx = (u-1)\cdot\dfrac{du}{2} x 3 d x = x 2 ⋅ x d x = ( u − 1 ) ⋅ 2 d u .
∫ 0 1 x 3 1 + x 2 d x = 1 2 ∫ 1 2 u − 1 u d u = 1 2 ∫ 1 2 ( 1 − 1 u ) d u \displaystyle\int_0^1 \frac{x^3}{1+x^2}\,dx = \frac{1}{2}\int_1^2 \frac{u-1}{u}\,du = \frac{1}{2}\int_1^2 \!\left(1-\frac{1}{u}\right)du ∫ 0 1 1 + x 2 x 3 d x = 2 1 ∫ 1 2 u u − 1 d u = 2 1 ∫ 1 2 ( 1 − u 1 ) d u
= 1 2 [ u − ln u ] 1 2 = 1 2 ( 2 − ln 2 − 1 ) = 1 2 ( 1 − ln 2 ) = \frac{1}{2}\Big[u-\ln u\Big]_1^2 = \frac{1}{2}(2-\ln 2 - 1) = \boxed{\frac{1}{2}(1-\ln 2)} = 2 1 [ u − ln u ] 1 2 = 2 1 ( 2 − ln 2 − 1 ) = 2 1 ( 1 − ln 2 ) .
Prove that the function F ( x ) = ∫ 0 x d t 1 + t 4 F(x) = \displaystyle\int_0^x \frac{dt}{1+t^4} F ( x ) = ∫ 0 x 1 + t 4 d t is increasing and Bounded above.
Solution F ′ ( x ) = 1 1 + x 4 > 0 F'(x) = \dfrac{1}{1+x^4} > 0 F ′ ( x ) = 1 + x 4 1 > 0 for all x ≥ 0 x \geq 0 x ≥ 0 So F F F is strictly increasing. ✓
F ( x ) < F ( ∞ ) = ∫ 0 ∞ d t 1 + t 4 < ∫ 0 ∞ d t 1 + t 2 = π 2 F(x) < F(\infty) = \displaystyle\int_0^{\infty} \frac{dt}{1+t^4} < \int_0^{\infty} \frac{dt}{1+t^2} = \frac{\pi}{2} F ( x ) < F ( ∞ ) = ∫ 0 ∞ 1 + t 4 d t < ∫ 0 ∞ 1 + t 2 d t = 2 π . ✓
Therefore F F F is increasing and bounded above by π / 2 \pi/2 π /2 . ■ \blacksquare ■