To find the required value, we first determine the points of intersection of the curves C 1 : y = e − x C_1: y = e^{-x} C 1 : y = e − x and C 2 : y = e − x ( sin x + cos x ) C_2: y = e^{-x}(\sin x + \cos x) C 2 : y = e − x ( sin x + cos x ) in the domain x ∈ [ 0 , 10 π ] x \in [0, 10\pi] x ∈ [ 0 , 10 π ] .
Step 1: Points of Intersection
Equating the two curves:
e − x = e − x ( sin x + cos x ) e^{-x} = e^{-x}(\sin x + \cos x) e − x = e − x ( sin x + cos x )
Since e − x ≠ 0 e^{-x} \neq 0 e − x = 0 for all real x x x , we can divide by e − x e^{-x} e − x :
sin x + cos x = 1 \sin x + \cos x = 1 sin x + cos x = 1
Dividing by 2 \sqrt{2} 2 :
1 2 sin x + 1 2 cos x = 1 2 \frac{1}{\sqrt{2}}\sin x + \frac{1}{\sqrt{2}}\cos x = \frac{1}{\sqrt{2}} 2 1 sin x + 2 1 cos x = 2 1
sin ( x + π 4 ) = sin ( π 4 ) \sin\left(x + \frac{\pi}{4}\right) = \sin\left(\frac{\pi}{4}\right) sin ( x + 4 π ) = sin ( 4 π )
This gives the general solution:
x + π 4 = 2 k π + π 4 or x + π 4 = 2 k π + 3 π 4 for k ∈ Z x + \frac{\pi}{4} = 2k\pi + \frac{\pi}{4} \quad \text{or} \quad x + \frac{\pi}{4} = 2k\pi + \frac{3\pi}{4} \quad \text{for } k \in \mathbb{Z} x + 4 π = 2 k π + 4 π or x + 4 π = 2 k π + 4 3 π for k ∈ Z
x = 2 k π or x = 2 k π + π 2 x = 2k\pi \quad \text{or} \quad x = 2k\pi + \frac{\pi}{2} x = 2 k π or x = 2 k π + 2 π
Arranging the x x x -coordinates of the intersection points in [ 0 , 10 π ] [0, 10\pi] [ 0 , 10 π ] in ascending order:
α 1 = 0 , α 2 = π 2 , α 3 = 2 π , α 4 = 5 π 2 , … \alpha_1 = 0, \quad \alpha_2 = \frac{\pi}{2}, \quad \alpha_3 = 2\pi, \quad \alpha_4 = \frac{5\pi}{2}, \dots α 1 = 0 , α 2 = 2 π , α 3 = 2 π , α 4 = 2 5 π , …
Step 2: Set Up the Area Integral
The area β \beta β enclosed between C 1 C_1 C 1 , C 2 C_2 C 2 , and the lines x = α 1 = 0 x = \alpha_1 = 0 x = α 1 = 0 and x = α 4 = 5 π 2 x = \alpha_4 = \frac{5\pi}{2} x = α 4 = 2 5 π is given by:
β = ∫ 0 5 π 2 ∣ C 1 ( x ) − C 2 ( x ) ∣ d x = ∫ 0 5 π 2 e − x ∣ 1 − sin x − cos x ∣ d x \beta = \int_{0}^{\frac{5\pi}{2}} |C_1(x) - C_2(x)| \, dx = \int_{0}^{\frac{5\pi}{2}} e^{-x} |1 - \sin x - \cos x| \, dx β = ∫ 0 2 5 π ∣ C 1 ( x ) − C 2 ( x ) ∣ d x = ∫ 0 2 5 π e − x ∣1 − sin x − cos x ∣ d x
We split the domain of integration according to the sign of ( 1 − sin x − cos x ) (1 - \sin x - \cos x) ( 1 − sin x − cos x ) :
For x ∈ [ 0 , π 2 ] x \in \left[0, \frac{\pi}{2}\right] x ∈ [ 0 , 2 π ] : sin x + cos x ≥ 1 ⟹ ∣ 1 − sin x − cos x ∣ = sin x + cos x − 1 \sin x + \cos x \ge 1 \implies |1 - \sin x - \cos x| = \sin x + \cos x - 1 sin x + cos x ≥ 1 ⟹ ∣1 − sin x − cos x ∣ = sin x + cos x − 1
For x ∈ [ π 2 , 2 π ] x \in \left[\frac{\pi}{2}, 2\pi\right] x ∈ [ 2 π , 2 π ] : sin x + cos x ≤ 1 ⟹ ∣ 1 − sin x − cos x ∣ = 1 − sin x − cos x \sin x + \cos x \le 1 \implies |1 - \sin x - \cos x| = 1 - \sin x - \cos x sin x + cos x ≤ 1 ⟹ ∣1 − sin x − cos x ∣ = 1 − sin x − cos x
For x ∈ [ 2 π , 5 π 2 ] x \in \left[2\pi, \frac{5\pi}{2}\right] x ∈ [ 2 π , 2 5 π ] : sin x + cos x ≥ 1 ⟹ ∣ 1 − sin x − cos x ∣ = sin x + cos x − 1 \sin x + \cos x \ge 1 \implies |1 - \sin x - \cos x| = \sin x + \cos x - 1 sin x + cos x ≥ 1 ⟹ ∣1 − sin x − cos x ∣ = sin x + cos x − 1
Step 3: Evaluate the Indefinite Integral
Let J ( x ) = ∫ e − x ( sin x + cos x − 1 ) d x J(x) = \int e^{-x} (\sin x + \cos x - 1) \, dx J ( x ) = ∫ e − x ( sin x + cos x − 1 ) d x .
Using standard exponential-trigonometric integrals:
∫ e − x sin x d x = e − x 2 ( − sin x − cos x ) \int e^{-x} \sin x \, dx = \frac{e^{-x}}{2}(-\sin x - \cos x) ∫ e − x sin x d x = 2 e − x ( − sin x − cos x )
∫ e − x cos x d x = e − x 2 ( sin x − cos x ) \int e^{-x} \cos x \, dx = \frac{e^{-x}}{2}(\sin x - \cos x) ∫ e − x cos x d x = 2 e − x ( sin x − cos x )
Adding these two:
∫ e − x ( sin x + cos x ) d x = − e − x cos x \int e^{-x} (\sin x + \cos x) \, dx = -e^{-x} \cos x ∫ e − x ( sin x + cos x ) d x = − e − x cos x
Thus:
J ( x ) = − e − x cos x − ( − e − x ) = e − x ( 1 − cos x ) J(x) = -e^{-x} \cos x - (-e^{-x}) = e^{-x}(1 - \cos x) J ( x ) = − e − x cos x − ( − e − x ) = e − x ( 1 − cos x )
Step 4: Calculate Area β \beta β
β = I 1 + I 2 + I 3 \beta = I_1 + I_2 + I_3 β = I 1 + I 2 + I 3
First region:
I 1 = ∫ 0 π 2 e − x ( sin x + cos x − 1 ) d x = [ J ( x ) ] 0 π 2 = e − π 2 ( 1 − 0 ) − e 0 ( 1 − 1 ) = e − π 2 I_1 = \int_0^{\frac{\pi}{2}} e^{-x}(\sin x + \cos x - 1) \, dx = [J(x)]_0^{\frac{\pi}{2}} = e^{-\frac{\pi}{2}}(1 - 0) - e^0(1 - 1) = e^{-\frac{\pi}{2}} I 1 = ∫ 0 2 π e − x ( sin x + cos x − 1 ) d x = [ J ( x ) ] 0 2 π = e − 2 π ( 1 − 0 ) − e 0 ( 1 − 1 ) = e − 2 π
Second region:
I 2 = ∫ π 2 2 π e − x ( 1 − sin x − cos x ) d x = − [ J ( x ) ] π 2 2 π = − ( e − 2 π ( 1 − 1 ) − e − π 2 ( 1 − 0 ) ) = e − π 2 I_2 = \int_{\frac{\pi}{2}}^{2\pi} e^{-x}(1 - \sin x - \cos x) \, dx = -[J(x)]_{\frac{\pi}{2}}^{2\pi} = - \left( e^{-2\pi}(1 - 1) - e^{-\frac{\pi}{2}}(1 - 0) \right) = e^{-\frac{\pi}{2}} I 2 = ∫ 2 π 2 π e − x ( 1 − sin x − cos x ) d x = − [ J ( x ) ] 2 π 2 π = − ( e − 2 π ( 1 − 1 ) − e − 2 π ( 1 − 0 ) ) = e − 2 π
Third region:
I 3 = ∫ 2 π 5 π 2 e − x ( sin x + cos x − 1 ) d x = [ J ( x ) ] 2 π 5 π 2 = e − 5 π 2 ( 1 − 0 ) − e − 2 π ( 1 − 1 ) = e − 5 π 2 I_3 = \int_{2\pi}^{\frac{5\pi}{2}} e^{-x}(\sin x + \cos x - 1) \, dx = [J(x)]_{2\pi}^{\frac{5\pi}{2}} = e^{-\frac{5\pi}{2}}(1 - 0) - e^{-2\pi}(1 - 1) = e^{-\frac{5\pi}{2}} I 3 = ∫ 2 π 2 5 π e − x ( sin x + cos x − 1 ) d x = [ J ( x ) ] 2 π 2 5 π = e − 2 5 π ( 1 − 0 ) − e − 2 π ( 1 − 1 ) = e − 2 5 π
Summing these up:
β = e − π 2 + e − π 2 + e − 5 π 2 = 2 e − π 2 + e − 5 π 2 \beta = e^{-\frac{\pi}{2}} + e^{-\frac{\pi}{2}} + e^{-\frac{5\pi}{2}} = 2e^{-\frac{\pi}{2}} + e^{-\frac{5\pi}{2}} β = e − 2 π + e − 2 π + e − 2 5 π = 2 e − 2 π + e − 2 5 π
Step 5: Evaluate the Final Expression
Substituting β \beta β into the given expression:
− 1 π log e ( β − 2 e − π 2 ) = − 1 π log e ( 2 e − π 2 + e − 5 π 2 − 2 e − π 2 ) -\frac{1}{\pi} \log_e \left( \beta - 2 e^{-\frac{\pi}{2}} \right) = -\frac{1}{\pi} \log_e \left( 2e^{-\frac{\pi}{2}} + e^{-\frac{5\pi}{2}} - 2 e^{-\frac{\pi}{2}} \right) − π 1 log e ( β − 2 e − 2 π ) = − π 1 log e ( 2 e − 2 π + e − 2 5 π − 2 e − 2 π )
= − 1 π log e ( e − 5 π 2 ) = − 1 π ( − 5 π 2 ) = 5 2 = 2.5 = -\frac{1}{\pi} \log_e \left( e^{-\frac{5\pi}{2}} \right) = -\frac{1}{\pi} \left( -\frac{5\pi}{2} \right) = \frac{5}{2} = 2.5 = − π 1 log e ( e − 2 5 π ) = − π 1 ( − 2 5 π ) = 2 5 = 2.5