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(a) Let I = ∫ e x sin x d x I = \displaystyle\int e^x\sin x\,dx I = ∫ e x sin x d x . Integrating by parts, with sin x \sin x sin x as the first function,
Why?
The integrand is a product of a trig function and an exponential, so use integration by parts:
∫ u v d x = u ∫ v d x − ∫ ( d u d x ∫ v d x ) d x \begin{aligned} \int u\,v\,dx &= u\int v\,dx \\ &\quad - \int\left(\frac{du}{dx}\int v\,dx\right)dx \end{aligned} ∫ u v d x = u ∫ v d x − ∫ ( d x d u ∫ v d x ) d x
Take u = sin x u = \sin x u = sin x and v = e x v = e^x v = e x , so ∫ v d x = e x \int v\,dx = e^x ∫ v d x = e x and d u d x = cos x \frac{du}{dx} = \cos x d x d u = cos x .
Either choice of first function works, as long as the second step keeps the trig function first again.
I = ( sin x ) ( e x ) − ∫ ( cos x ) ( e x ) d x \begin{aligned} I &= (\sin x)(e^x) - \int(\cos x)(e^x)\,dx \end{aligned} I = ( sin x ) ( e x ) − ∫ ( cos x ) ( e x ) d x
I = e x sin x − ∫ cos x e x d x = e x sin x − [ cos x e x − ∫ ( − sin x ) e x d x ] = e x sin x − cos x e x − I \begin{aligned} I &= e^x\sin x - \int\cos x\,e^x\,dx \\ &= e^x\sin x - \Big[\cos x\,e^x \\ &\qquad - \int(-\sin x)\,e^x\,dx\Big] \\ &= e^x\sin x - \cos x\,e^x - I \end{aligned} I = e x sin x − ∫ cos x e x d x = e x sin x − [ cos x e x − ∫ ( − sin x ) e x d x ] = e x sin x − cos x e x − I
Why?
The first step leaves ∫ cos x e x d x \int\cos x\,e^x\,dx ∫ cos x e x d x . Integrate it by parts again with cos x \cos x cos x first. Its derivative is − sin x -\sin x − sin x .
∫ cos x e x d x = ( cos x ) ( e x ) − ∫ ( − sin x ) ( e x ) d x = e x cos x + ∫ e x sin x d x = e x cos x + I \begin{aligned} &\int\cos x\,e^x\,dx \\ &= (\cos x)(e^x) - \int(-\sin x)(e^x)\,dx \\ &= e^x\cos x + \int e^x\sin x\,dx \\ &= e^x\cos x + I \end{aligned} ∫ cos x e x d x = ( cos x ) ( e x ) − ∫ ( − sin x ) ( e x ) d x = e x cos x + ∫ e x sin x d x = e x cos x + I
Put this back into the first line:
I = e x sin x − ( e x cos x + I ) = e x sin x − e x cos x − I \begin{aligned} I &= e^x\sin x - (e^x\cos x + I) \\ &= e^x\sin x - e^x\cos x - I \end{aligned} I = e x sin x − ( e x cos x + I ) = e x sin x − e x cos x − I
That brings back ∫ e x sin x d x \int e^x\sin x\,dx ∫ e x sin x d x , which is I I I itself. Watch the signs: opening the bracket turns − ∫ ( − sin x ) e x d x -\int(-\sin x)e^x\,dx − ∫ ( − sin x ) e x d x into + ∫ ( − sin x ) e x d x +\int(-\sin x)e^x\,dx + ∫ ( − sin x ) e x d x , and that is − I -I − I .
∴ I = 1 2 e x ( sin x − cos x ) \therefore\ I = \frac12e^x(\sin x - \cos x) ∴ I = 2 1 e x ( sin x − cos x )
Why?
I I I appears on both sides, so move it across: 2 I = e x sin x − e x cos x 2I = e^x\sin x - e^x\cos x 2 I = e x sin x − e x cos x . Then divide by 2.
I + I = e x sin x − e x cos x 2 I = e x ( sin x − cos x ) I = 1 2 e x ( sin x − cos x ) \begin{aligned} I + I &= e^x\sin x - e^x\cos x \\ 2I &= e^x(\sin x - \cos x) \\ I &= \frac12e^x(\sin x - \cos x) \end{aligned} I + I 2 I I = e x sin x − e x cos x = e x ( sin x − cos x ) = 2 1 e x ( sin x − cos x )
No + C + C + C is written here, because this result is only used for the definite integral.
∫ 0 π / 2 e x sin x d x = 1 2 [ e x ( sin x − cos x ) ] 0 π / 2 = 1 2 e π / 2 ( 1 − 0 ) − 1 2 e 0 ( 0 − 1 ) \begin{aligned} &\int_0^{\pi/2}e^x\sin x\,dx \\ &= \frac12\Big[e^x(\sin x - \cos x)\Big]_0^{\pi/2} \\ &= \frac12e^{\pi/2}(1 - 0) - \frac12e^0(0 - 1) \end{aligned} ∫ 0 π /2 e x sin x d x = 2 1 [ e x ( sin x − cos x ) ] 0 π /2 = 2 1 e π /2 ( 1 − 0 ) − 2 1 e 0 ( 0 − 1 )
Why?
Put in the limits, upper minus lower, with
sin π 2 = 1 , cos π 2 = 0 sin 0 = 0 , cos 0 = 1 \begin{aligned} \sin\frac{\pi}{2} &= 1,\ \cos\frac{\pi}{2} = 0 \\ \sin 0 &= 0,\ \cos 0 = 1 \end{aligned} sin 2 π sin 0 = 1 , cos 2 π = 0 = 0 , cos 0 = 1
and e 0 = 1 e^0 = 1 e 0 = 1 . Watch the sign: − 1 2 ( 0 − 1 ) = + 1 2 -\frac12(0 - 1) = +\frac12 − 2 1 ( 0 − 1 ) = + 2 1 .
At x = π 2 : 1 2 e π / 2 ( 1 − 0 ) = 1 2 e π / 2 At x = 0 : 1 2 e 0 ( 0 − 1 ) = 1 2 ( 1 ) ( − 1 ) = − 1 2 1 2 e π / 2 − ( − 1 2 ) = 1 2 e π / 2 + 1 2 \begin{aligned} &\text{At } x = \tfrac{\pi}{2}\text{: } \frac12e^{\pi/2}(1 - 0) \\ &= \frac12e^{\pi/2} \\[4pt] &\text{At } x = 0\text{: } \frac12e^0(0 - 1) \\ &= \frac12(1)(-1) = -\frac12 \\[4pt] &\frac12e^{\pi/2} - \left(-\frac12\right) \\ &= \frac12e^{\pi/2} + \frac12 \end{aligned} At x = 2 π : 2 1 e π /2 ( 1 − 0 ) = 2 1 e π /2 At x = 0 : 2 1 e 0 ( 0 − 1 ) = 2 1 ( 1 ) ( − 1 ) = − 2 1 2 1 e π /2 − ( − 2 1 ) = 2 1 e π /2 + 2 1
Take out 1 2 \frac12 2 1 for the second form: 1 2 ( e π / 2 + 1 ) \frac12\left(e^{\pi/2} + 1\right) 2 1 ( e π /2 + 1 ) .
∴ ∫ 0 π / 2 e x sin x d x = 1 2 e π / 2 + 1 2 \therefore\ \displaystyle\int_0^{\pi/2}e^x\sin x\,dx = \frac12e^{\pi/2} + \frac12 ∴ ∫ 0 π /2 e x sin x d x = 2 1 e π /2 + 2 1 or 1 2 ( e π / 2 + 1 ) \frac12\left(e^{\pi/2} + 1\right) 2 1 ( e π /2 + 1 ) .
(b) Let I = ∫ d x cos ( x − a ) cos ( x − b ) I = \displaystyle\int\frac{dx}{\cos(x - a)\cos(x - b)} I = ∫ cos ( x − a ) cos ( x − b ) d x . As ( x − b ) − ( x − a ) = a − b (x - b) - (x - a) = a - b ( x − b ) − ( x − a ) = a − b ,
I = 1 sin ( a − b ) × ∫ sin [ ( x − b ) − ( x − a ) ] cos ( x − a ) cos ( x − b ) d x \begin{aligned} I &= \frac{1}{\sin(a - b)} \\ &\quad\times\int\frac{\sin[(x - b) - (x - a)]}{\cos(x - a)\cos(x - b)}\,dx \end{aligned} I = sin ( a − b ) 1 × ∫ cos ( x − a ) cos ( x − b ) sin [( x − b ) − ( x − a )] d x
Why?
The trick is to multiply and divide by the constant sin ( a − b ) \sin(a - b) sin ( a − b ) . Written as sin [ ( x − b ) − ( x − a ) ] \sin[(x - b) - (x - a)] sin [( x − b ) − ( x − a )] , the top can be expanded into the same angles as the bottom.
This needs sin ( a − b ) ≠ 0 \sin(a - b) \ne 0 sin ( a − b ) = 0 , which the question assumes.
( x − b ) − ( x − a ) = x − b − x + a = a − b \begin{aligned} &(x - b) - (x - a) \\ &= x - b - x + a \\ &= a - b \end{aligned} ( x − b ) − ( x − a ) = x − b − x + a = a − b
Multiplying and dividing by the same number changes nothing: sin ( a − b ) sin ( a − b ) = 1 \frac{\sin(a - b)}{\sin(a - b)} = 1 s i n ( a − b ) s i n ( a − b ) = 1 .
Using sin ( A − B ) \sin(A - B) sin ( A − B ) = sin A cos B − cos A sin B = \sin A\cos B - \cos A\sin B = sin A cos B − cos A sin B , the integrand becomes
sin ( x − b ) cos ( x − a ) cos ( x − a ) cos ( x − b ) − cos ( x − b ) sin ( x − a ) cos ( x − a ) cos ( x − b ) = tan ( x − b ) − tan ( x − a ) \begin{aligned} &\frac{\sin(x - b)\cos(x - a)}{\cos(x - a)\cos(x - b)} \\ &\quad - \frac{\cos(x - b)\sin(x - a)}{\cos(x - a)\cos(x - b)} \\ &= \tan(x - b) - \tan(x - a) \end{aligned} cos ( x − a ) cos ( x − b ) sin ( x − b ) cos ( x − a ) − cos ( x − a ) cos ( x − b ) cos ( x − b ) sin ( x − a ) = tan ( x − b ) − tan ( x − a )
Why?
Take A = x − b A = x - b A = x − b and B = x − a B = x - a B = x − a . Each part then cancels one cosine:
sin [ ( x − b ) − ( x − a ) ] = sin ( x − b ) cos ( x − a ) − cos ( x − b ) sin ( x − a ) \begin{aligned} &\sin[(x - b) - (x - a)] \\ &= \sin(x - b)\cos(x - a) \\ &\quad - \cos(x - b)\sin(x - a) \end{aligned} sin [( x − b ) − ( x − a )] = sin ( x − b ) cos ( x − a ) − cos ( x − b ) sin ( x − a )
Split the fraction into two. In the first part cos ( x − a ) \cos(x - a) cos ( x − a ) cancels; in the second part cos ( x − b ) \cos(x - b) cos ( x − b ) cancels:
sin ( x − b ) cos ( x − b ) = tan ( x − b ) \frac{\sin(x - b)}{\cos(x - b)} = \tan(x - b) cos ( x − b ) sin ( x − b ) = tan ( x − b )
In the same way the second part gives tan ( x − a ) \tan(x - a) tan ( x − a ) .
sin ( x − a ) cos ( x − a ) = tan ( x − a ) \frac{\sin(x - a)}{\cos(x - a)} = \tan(x - a) cos ( x − a ) sin ( x − a ) = tan ( x − a )
I = 1 sin ( a − b ) ∫ tan ( x − b ) d x − 1 sin ( a − b ) ∫ tan ( x − a ) d x \begin{aligned} I &= \frac{1}{\sin(a - b)}\int\tan(x - b)\,dx \\ &\quad - \frac{1}{\sin(a - b)}\int\tan(x - a)\,dx \end{aligned} I = sin ( a − b ) 1 ∫ tan ( x − b ) d x − sin ( a − b ) 1 ∫ tan ( x − a ) d x
Why?
Standard integral:
∫ tan u d u = log ∣ sec u ∣ + C \int\tan u\,du = \log|\sec u| + C ∫ tan u d u = log ∣ sec u ∣ + C
With u = x − b u = x - b u = x − b we have d u = d x du = dx d u = d x , so
∫ tan ( x − b ) d x = log ∣ sec ( x − b ) ∣ + C \begin{aligned} &\int\tan(x - b)\,dx \\ &= \log|\sec(x - b)| + C \end{aligned} ∫ tan ( x − b ) d x = log ∣ sec ( x − b ) ∣ + C
The same holds with a a a in place of b b b .
∴ I = 1 sin ( a − b ) \therefore\ I = \dfrac{1}{\sin(a - b)} ∴ I = sin ( a − b ) 1 × [ log ∣ sec ( x − b ) ∣ \times\big[\log|\sec(x - b)| × [ log ∣ sec ( x − b ) ∣ − log ∣ sec ( x − a ) ∣ ] + C - \log|\sec(x - a)|\big] + C − log ∣ sec ( x − a ) ∣ ] + C .
Where this comes from Chapter 7, Integrals : Integration by parts; trig identity integral.
Question type: (a) Integration by parts
How to spot it: click to see (a) Type 8. Integration by parts: a product of two different kinds
Spot it: a product such as x sin x x\sin x x sin x , x e x xe^x x e x or x log x x\log x x log x . A lone log x \log x log x or tan − 1 x \tan^{-1}x tan − 1 x works too: take the other function as 1.
Here: In e x sin x e^x\sin x e x sin x , take u = sin x u = \sin x u = sin x and integrate by parts twice. I I I comes back on the right, so solve 2 I = e x ( sin x − cos x ) 2I = e^x(\sin x - \cos x) 2 I = e x ( sin x − cos x ) before putting in the limits.
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