[THOUGHT]
To solve the given problem, we will address each part step-by-step and use Python to verify critical calculations.
Part I: Solving the Differential Equation
The differential equation d y d x = y ( 1 − y ) \frac{dy}{dx} = y(1 - y) d x d y = y ( 1 − y ) is separable. Separating variables and integrating gives:
∫ 1 y ( 1 − y ) d y = ∫ 1 d x \int \frac{1}{y(1 - y)} \, dy = \int 1 \, dx ∫ y ( 1 − y ) 1 d y = ∫ 1 d x
Using partial fractions, we decompose the left-hand side:
1 y ( 1 − y ) = 1 y + 1 1 − y \frac{1}{y(1 - y)} = \frac{1}{y} + \frac{1}{1 - y} y ( 1 − y ) 1 = y 1 + 1 − y 1
Integrating both sides:
ln ∣ y ∣ − ln ∣ 1 − y ∣ = x + C ⟹ ln ∣ y 1 − y ∣ = x + C \ln|y| - \ln|1 - y| = x + C \implies \ln\left|\frac{y}{1 - y}\right| = x + C ln ∣ y ∣ − ln ∣1 − y ∣ = x + C ⟹ ln 1 − y y = x + C
Exponentiating both sides:
y 1 − y = C e x ⟹ y = C e x 1 + C e x \frac{y}{1 - y} = Ce^x \implies y = \frac{Ce^x}{1 + Ce^x} 1 − y y = C e x ⟹ y = 1 + C e x C e x
Applying the initial condition y ( 0 ) = 1 2 y(0) = \frac{1}{2} y ( 0 ) = 2 1 :
1 2 = C 1 + C ⟹ C = 1 \frac{1}{2} = \frac{C}{1 + C} \implies C = 1 2 1 = 1 + C C ⟹ C = 1
Thus, the solution is:
y ∗ ( x ) = e x 1 + e x y_*(x) = \frac{e^x}{1 + e^x} y ∗ ( x ) = 1 + e x e x
For a = y ∗ ( ln 3 ) a = y_*(\ln 3) a = y ∗ ( ln 3 ) :
a = e ln 3 1 + e ln 3 = 3 1 + 3 = 3 4 a = \frac{e^{\ln 3}}{1 + e^{\ln 3}} = \frac{3}{1 + 3} = \frac{3}{4} a = 1 + e l n 3 e l n 3 = 1 + 3 3 = 4 3
Part II: Evaluating the Definite Integral
The integral is:
I = ∫ − 1 1 arccos ( x 2 ) cos 2 ( π 3 x ) d x I = \int_{-1}^{1} \frac{\arccos\left(\frac{x}{2}\right)}{\cos^2\left(\frac{\pi}{3}x\right)} \, dx I = ∫ − 1 1 cos 2 ( 3 π x ) arccos ( 2 x ) d x
Using the symmetry of the integrand and the identity arccos ( − z ) = π − arccos ( z ) \arccos(-z) = \pi - \arccos(z) arccos ( − z ) = π − arccos ( z ) , we split the integral:
I = ∫ − 1 0 arccos ( x 2 ) cos 2 ( π 3 x ) d x + ∫ 0 1 arccos ( x 2 ) cos 2 ( π 3 x ) d x I = \int_{-1}^{0} \frac{\arccos\left(\frac{x}{2}\right)}{\cos^2\left(\frac{\pi}{3}x\right)} \, dx + \int_{0}^{1} \frac{\arccos\left(\frac{x}{2}\right)}{\cos^2\left(\frac{\pi}{3}x\right)} \, dx I = ∫ − 1 0 cos 2 ( 3 π x ) arccos ( 2 x ) d x + ∫ 0 1 cos 2 ( 3 π x ) arccos ( 2 x ) d x
Substituting x = − t x = -t x = − t in the first integral:
∫ − 1 0 arccos ( x 2 ) cos 2 ( π 3 x ) d x = ∫ 1 0 π − arccos ( t 2 ) cos 2 ( π 3 t ) ( − d t ) = ∫ 0 1 π − arccos ( t 2 ) cos 2 ( π 3 t ) d t \int_{-1}^{0} \frac{\arccos\left(\frac{x}{2}\right)}{\cos^2\left(\frac{\pi}{3}x\right)} \, dx = \int_{1}^{0} \frac{\pi - \arccos\left(\frac{t}{2}\right)}{\cos^2\left(\frac{\pi}{3}t\right)} (-dt) = \int_{0}^{1} \frac{\pi - \arccos\left(\frac{t}{2}\right)}{\cos^2\left(\frac{\pi}{3}t\right)} \, dt ∫ − 1 0 cos 2 ( 3 π x ) arccos ( 2 x ) d x = ∫ 1 0 cos 2 ( 3 π t ) π − arccos ( 2 t ) ( − d t ) = ∫ 0 1 cos 2 ( 3 π t ) π − arccos ( 2 t ) d t
Combining the integrals:
I = ∫ 0 1 π − arccos ( t 2 ) cos 2 ( π 3 t ) d t + ∫ 0 1 arccos ( t 2 ) cos 2 ( π 3 t ) d t = π ∫ 0 1 1 cos 2 ( π 3 t ) d t I = \int_{0}^{1} \frac{\pi - \arccos\left(\frac{t}{2}\right)}{\cos^2\left(\frac{\pi}{3}t\right)} \, dt + \int_{0}^{1} \frac{\arccos\left(\frac{t}{2}\right)}{\cos^2\left(\frac{\pi}{3}t\right)} \, dt = \pi \int_{0}^{1} \frac{1}{\cos^2\left(\frac{\pi}{3}t\right)} \, dt I = ∫ 0 1 cos 2 ( 3 π t ) π − arccos ( 2 t ) d t + ∫ 0 1 cos 2 ( 3 π t ) arccos ( 2 t ) d t = π ∫ 0 1 cos 2 ( 3 π t ) 1 d t
The integral of sec 2 ( u ) \sec^2(u) sec 2 ( u ) is tan ( u ) \tan(u) tan ( u ) :
I = π [ 3 π tan ( π 3 t ) ] 0 1 = 3 ( tan ( π 3 ) − tan ( 0 ) ) = 3 3 I = \pi \left[ \frac{3}{\pi} \tan\left(\frac{\pi}{3}t\right) \right]_{0}^{1} = 3 \left( \tan\left(\frac{\pi}{3}\right) - \tan(0) \right) = 3 \sqrt{3} I = π [ π 3 tan ( 3 π t ) ] 0 1 = 3 ( tan ( 3 π ) − tan ( 0 ) ) = 3 3
Part III: Hyperbolic Functions and Integrals
Given:
f ( x ) = ∑ m = 0 ∞ x 2 m ( 2 m ) ! = cosh ( x ) , g ( x ) = d d x f ( x ) = sinh ( x ) f(x) = \sum_{m=0}^{\infty} \frac{x^{2m}}{(2m)!} = \cosh(x), \quad g(x) = \frac{d}{dx} f(x) = \sinh(x) f ( x ) = m = 0 ∑ ∞ ( 2 m )! x 2 m = cosh ( x ) , g ( x ) = d x d f ( x ) = sinh ( x )
Calculate f ( x ) 2 − g ( x ) 2 f(x)^2 - g(x)^2 f ( x ) 2 − g ( x ) 2 :
f ( x ) 2 − g ( x ) 2 = cosh 2 ( x ) − sinh 2 ( x ) = 1 f(x)^2 - g(x)^2 = \cosh^2(x) - \sinh^2(x) = 1 f ( x ) 2 − g ( x ) 2 = cosh 2 ( x ) − sinh 2 ( x ) = 1
Express I n + 2 ( x ) I_{n+2}(x) I n + 2 ( x ) using I n ( x ) I_n(x) I n ( x ) :
I n ( x ) = ∫ 0 x ( g ( X ) f ( X ) ) n d X = ∫ 0 x tanh n ( X ) d X I_n(x) = \int_0^x \left(\frac{g(X)}{f(X)}\right)^n \, dX = \int_0^x \tanh^n(X) \, dX I n ( x ) = ∫ 0 x ( f ( X ) g ( X ) ) n d X = ∫ 0 x tanh n ( X ) d X
Using the identity tanh 2 ( X ) = 1 − sech 2 ( X ) \tanh^2(X) = 1 - \text{sech}^2(X) tanh 2 ( X ) = 1 − sech 2 ( X ) :
I n + 2 ( x ) = ∫ 0 x tanh n ( X ) ( 1 − sech 2 ( X ) ) d X = I n ( x ) − ∫ 0 x tanh n ( X ) sech 2 ( X ) d X I_{n+2}(x) = \int_0^x \tanh^n(X) (1 - \text{sech}^2(X)) \, dX = I_n(x) - \int_0^x \tanh^n(X) \text{sech}^2(X) \, dX I n + 2 ( x ) = ∫ 0 x tanh n ( X ) ( 1 − sech 2 ( X )) d X = I n ( x ) − ∫ 0 x tanh n ( X ) sech 2 ( X ) d X
Let u = tanh ( X ) u = \tanh(X) u = tanh ( X ) , then d u = sech 2 ( X ) d X du = \text{sech}^2(X) \, dX d u = sech 2 ( X ) d X :
∫ 0 x tanh n ( X ) sech 2 ( X ) d X = ∫ 0 tanh ( x ) u n d u = tanh n + 1 ( x ) n + 1 \int_0^x \tanh^n(X) \text{sech}^2(X) \, dX = \int_0^{\tanh(x)} u^n \, du = \frac{\tanh^{n+1}(x)}{n+1} ∫ 0 x tanh n ( X ) sech 2 ( X ) d X = ∫ 0 t a n h ( x ) u n d u = n + 1 tanh n + 1 ( x )
Thus:
I n + 2 ( x ) = I n ( x ) − tanh n + 1 ( x ) n + 1 I_{n+2}(x) = I_n(x) - \frac{\tanh^{n+1}(x)}{n+1} I n + 2 ( x ) = I n ( x ) − n + 1 tanh n + 1 ( x )
Part IV: Final Calculation
Given:
x 0 = ln ( 2 + 3 ) , F 0 = f ( x 0 ) = cosh ( x 0 ) , G 0 = g ( x 0 ) = sinh ( x 0 ) x_0 = \ln(2 + \sqrt{3}), \quad F_0 = f(x_0) = \cosh(x_0), \quad G_0 = g(x_0) = \sinh(x_0) x 0 = ln ( 2 + 3 ) , F 0 = f ( x 0 ) = cosh ( x 0 ) , G 0 = g ( x 0 ) = sinh ( x 0 )
Using the properties of hyperbolic functions:
cosh ( ln ( 2 + 3 ) ) = 2 , sinh ( ln ( 2 + 3 ) ) = 3 \cosh(\ln(2 + \sqrt{3})) = 2, \quad \sinh(\ln(2 + \sqrt{3})) = \sqrt{3} cosh ( ln ( 2 + 3 )) = 2 , sinh ( ln ( 2 + 3 )) = 3
Thus:
F 0 = 2 , G 0 = 3 F_0 = 2, \quad G_0 = \sqrt{3} F 0 = 2 , G 0 = 3
Now, compute S S S :
S = 4 a + I G 0 + F 0 = 4 ( 3 4 ) + 3 3 3 + 2 = 3 + 3 + 2 = 8 S = 4a + \frac{I}{G_0} + F_0 = 4 \left(\frac{3}{4}\right) + \frac{3\sqrt{3}}{\sqrt{3}} + 2 = 3 + 3 + 2 = 8 S = 4 a + G 0 I + F 0 = 4 ( 4 3 ) + 3 3 3 + 2 = 3 + 3 + 2 = 8
Finally, compute K \mathcal{K} K :
K = 999 S 2 + 7 = 999 × 64 + 7 = 63936 + 7 = 63943 \mathcal{K} = 999S^2 + 7 = 999 \times 64 + 7 = 63936 + 7 = 63943 K = 999 S 2 + 7 = 999 × 64 + 7 = 63936 + 7 = 63943
[PYTHON]
Verification of key values
import math
Part I: a = y*(ln 3)
a = math.exp(math.log(3)) / (1 + math.exp(math.log(3)))
a = 3 / 4 # Simplified
Part II: I = 3 * sqrt(3)
I = 3 * math.sqrt(3)
Part III: F0 and G0
x0 = math.log(2 + math.sqrt(3))
F0 = math.cosh(x0)
G0 = math.sinh(x0)
Part IV: Compute S and K
S = 4 * a + I / G0 + F0
K = 999 * S**2 + 7
print(f"a = {a}")
print(f"I = {I}")
print(f"F0 = {F0}, G0 = {G0}")
print(f"S = {S}")
print(f"K = {K}")
[/PYTHON]