Part (a) 2 marks
We use the identity tan 2 θ = sec 2 θ − 1 \tan^{2}\theta = \sec^{2}\theta - 1 to rewrite the integrand.
∫ tan 2 5 x d x \int\tan^{2}5x\ dx
= ∫ ( sec 2 5 x − 1 ) d x = \int\left( \sec^{2}5x - 1 \right)\ dx
= 1 5 tan 5 x − x + C = \frac{1}{5}\tan 5x - x + C
To check your answer: differentiating 1 5 tan 5 x − x + C \frac{1}{5}\tan 5x - x + C gives sec 2 5 x − 1 = tan 2 5 x \sec^{2}5x - 1 = \tan^{2}5x , the original integrand. ✓
∴ \therefore ∫ tan 2 5 x d x = 1 5 tan 5 x − x + C \int\tan^{2}5x\ dx = \frac{1}{5}\tan 5x - x + C .
Part (b) 3 marks
Approach
the product sin 2 x sin 3 x \sin 2x\sin 3x has no elementary antiderivative as it stands, so we first turn it into a sum of cosines using the product-to-sum identity, which we can integrate term by term.
We use sin A sin B = 1 2 [ cos ( A − B ) − cos ( A + B ) ] \sin A\sin B = \frac{1}{2}\left\lbrack \cos(A - B) - \cos(A + B) \right\rbrack with A = 2 x A = 2x , B = 3 x B = 3x .
sin 2 x sin 3 x = 1 2 [ cos ( 2 x − 3 x ) − cos ( 2 x + 3 x ) ] \sin 2x\sin 3x = \frac{1}{2}\left\lbrack \cos(2x - 3x) - \cos(2x + 3x) \right\rbrack
= 1 2 [ cos ( − x ) − cos 5 x ] = \frac{1}{2}\left\lbrack \cos( - x) - \cos 5x \right\rbrack
= 1 2 ( cos x − cos 5 x ) = \frac{1}{2}\left( \cos x - \cos 5x \right)
since cos \cos is even. Integrating term by term,
∫ 0 b sin 2 x sin 3 x d x \int_{0}^{b}\sin 2x\sin 3x\ dx
= 1 2 ∫ 0 b ( cos x − cos 5 x ) d x = \frac{1}{2}\int_{0}^{b}\left( \cos x - \cos 5x \right)\ dx
= 1 2 [ sin x − 1 5 sin 5 x ] 0 b = \frac{1}{2}\left\lbrack \sin x - \frac{1}{5}\sin 5x \right\rbrack_{0}^{b}
= 1 2 sin b − 1 10 sin 5 b = \frac{1}{2}\sin b - \frac{1}{10}\sin 5b
(the lower limit contributes 0 0 , since sin 0 = 0 \sin 0 = 0 ).
To check your answer: at b = π 2 b = \frac{\pi}{2} : 1 2 sin π 2 − 1 10 sin 5 π 2 = 1 2 ( 1 ) − 1 10 ( 1 ) = 0.4 \frac{1}{2}\sin\frac{\pi}{2} - \frac{1}{10}\sin\frac{5\pi}{2} = \frac{1}{2}(1) - \frac{1}{10}(1) = 0.4 , matching direct numerical integration of sin 2 x sin 3 x \sin 2x\sin 3x from 0 0 to π 2 \frac{\pi}{2} . ✓
∴ \therefore ∫ 0 b sin 2 x sin 3 x d x = 1 2 sin b − 1 10 sin 5 b \int_{0}^{b}\sin 2x\sin 3x\ dx = \frac{1}{2}\sin b - \frac{1}{10}\sin 5b .
Part (c) 3 marks
Since the derivative of ln x \ln x is 1 x \frac{1}{x} , we let u = ln x u = \ln x , so d u = 1 x d x du = \frac{1}{x}\ dx . When x = a x = a , u = ln a u = \ln a ; when x = b x = b , u = ln b u = \ln b .
∫ a b 1 x ln x d x \int_{a}^{b}\frac{1}{x\ln x}\ dx
= ∫ ln a ln b 1 u d u = \int_{\ln a}^{\ln b}\frac{1}{u}\ du
= [ ln ∣ u ∣ ] ln a ln b = \left\lbrack \ln|u| \right\rbrack_{\ln a}^{\ln b}
= ln ( ln b ) − ln ( ln a ) = \ln\left( \ln b \right) - \ln\left( \ln a \right)
Since 1 < a < b 1 < a < b , both ln a > 0 \ln a > 0 and ln b > 0 \ln b > 0 , so by the quotient rule for logarithms,
ln ( ln b ) − ln ( ln a ) = ln ( ln b ln a ) \ln\left( \ln b \right) - \ln\left( \ln a \right) = \ln\left( \frac{\ln b}{\ln a} \right)
To check your answer: with a = e a = e , b = e 2 b = e^{2} : ln ( ln b ) − ln ( ln a ) = ln 2 − ln 1 = ln 2 ≈ 0.693 \ln\left( \ln b \right) - \ln\left( \ln a \right) = \ln 2 - \ln 1 = \ln 2 \approx 0.693 ; direct numerical integration of 1 x ln x \frac{1}{x\ln x} from e e to e 2 e^{2} also gives ≈ 0.693 \text{≈}0.693 . ✓
∴ \therefore ∫ a b 1 x ln x d x = ln ( ln b ln a ) \int_{a}^{b}\frac{1}{x\ln x}\ dx = \ln\left( \frac{\ln b}{\ln a} \right) .
Part (d) 3 marks
We are given u = 1 + e 2 x u = 1 + e^{2x} , so d u d x = 2 e 2 x \frac{du}{dx} = 2e^{2x} , i.e. e 2 x d x = 1 2 d u e^{2x}\ dx = \frac{1}{2}\ du .
∫ e 2 x ( 1 + e 2 x ) 3 d x \int\frac{e^{2x}}{\left( 1 + e^{2x} \right)^{3}}\ dx
= ∫ 1 u 3 ⋅ 1 2 d u = \int\frac{1}{u^{3}} \cdot \frac{1}{2}\ du
= 1 2 ∫ u − 3 d u = \frac{1}{2}\int u^{- 3}\ du
= 1 2 ( u − 2 − 2 ) + C = \frac{1}{2}\left( \frac{u^{- 2}}{- 2} \right) + C
= − 1 4 u 2 + C = - \frac{1}{4u^{2}} + C
Substituting back u = 1 + e 2 x u = 1 + e^{2x} ,
− 1 4 u 2 + C = − 1 4 ( 1 + e 2 x ) 2 + C - \frac{1}{4u^{2}} + C = - \frac{1}{4\left( 1 + e^{2x} \right)^{2}} + C
To check your answer: differentiating − 1 4 ( 1 + e 2 x ) 2 + C - \frac{1}{4\left( 1 + e^{2x} \right)^{2}} + C by the chain rule gives − 1 4 × ( − 2 ) ( 1 + e 2 x ) − 3 × 2 e 2 x = e 2 x ( 1 + e 2 x ) 3 - \frac{1}{4} \times ( - 2)\left( 1 + e^{2x} \right)^{- 3} \times 2e^{2x} = \frac{e^{2x}}{\left( 1 + e^{2x} \right)^{3}} , the original integrand. ✓
∴ \therefore ∫ e 2 x ( 1 + e 2 x ) 3 d x = − 1 4 ( 1 + e 2 x ) 2 + C \int\frac{e^{2x}}{\left( 1 + e^{2x} \right)^{3}}\ dx = - \frac{1}{4\left( 1 + e^{2x} \right)^{2}} + C .
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Question 6 → Discrete random variables