Problem Analysis #6

A.X-4.0 (72B) · Run 1

45.41s
7,410 toks
Problem Statement

\subsection*{I.}Find the general solution y(x)y(x) of the following differential equation:

dydx=y(1y),\frac{dy}{dx} = y(1-y),

where 0<y<10 < y < 1.\subsection*{II.}Find the value of the definite integral

I=11arccos(x2)cos2(π3x)dx,I = \int_{-1}^{1} \frac{\arccos\left(\dfrac{x}{2}\right)}{\cos^2\left(\dfrac{\pi}{3}x\right)} \, dx,

where 0arccos(x2)π0 \leq \arccos\left(\dfrac{x}{2}\right) \leq \pi.\subsection*{III.}For any positive variable xx, define

f(x)=m=01(2m)!x2m,\qquadg(x)=ddxf(x).f(x) = \sum_{m=0}^{\infty} \frac{1}{(2m)!} x^{2m},\qquadg(x) = \frac{d}{dx} f(x).

For any non-negative integer nn, define

In(x)=0x(g(X)f(X))ndX.I_n(x) = \int_0^x \left(\frac{g(X)}{f(X)}\right)^n \, dX.

You may use

exp(x)=m=0xmm!.\exp(x) = \sum_{m=0}^{\infty} \frac{x^m}{m!}.
  • [(1)] Calculate f(x)2g(x)2f(x)^2 - g(x)^2.
  • [(2)] Express In+2(x)I_{n+2}(x) using In(x)I_n(x). \subsection*{IV. Final quantity}Let y(x)y_*(x) be the solution of the differential equation in {\rm I} that satisfies
y(0)=12,y_*(0) = \frac{1}{2},

and define

a:=y(ln3).a := y_*(\ln 3).

In {\rm II}, let II be the value of the definite integral. In {\rm III}, let

x0=ln(2+3),\qquadF0:=f(x0),G0:=g(x0).x_0 = \ln(2+\sqrt{3}),\qquadF_0 := f(x_0),\quad G_0 := g(x_0).

Define

S:=4a+IG0+F0,K:=999S2+7.S := 4a + \frac{I}{G_0} + F_0,\qquad\mathcal{K} := 999\,S^2 + 7.

Compute the integer K\mathcal{K}.\

Ground Truth
63943
Execution Trace
Reasoning Process

[THOUGHT] Let's solve each part of the problem step-by-step using Python code verification.

Part I: Differential Equation

The given differential equation is:

dydx=y(1y)\frac{dy}{dx} = y(1-y)

This is a separable differential equation. We can rewrite it as:

1y(1y)dy=dx\frac{1}{y(1-y)} \, dy = dx

Using partial fractions, we get:

1y(1y)=1y+11y\frac{1}{y(1-y)} = \frac{1}{y} + \frac{1}{1-y}

So the equation becomes:

(1y+11y)dy=dx\left( \frac{1}{y} + \frac{1}{1-y} \right) dy = dx

Integrating both sides:

(1y+11y)dy=dx\int \left( \frac{1}{y} + \frac{1}{1-y} \right) dy = \int dx lnyln1y=x+C\ln |y| - \ln |1-y| = x + C lny1y=x+C\ln \left| \frac{y}{1-y} \right| = x + C

Exponentiating both sides:

y1y=ex+C\left| \frac{y}{1-y} \right| = e^{x+C}

Let eC=Ke^C = K, then:

y1y=Kex\frac{y}{1-y} = K e^x

Solving for yy:

y=Kex1+Kexy = \frac{K e^x}{1 + K e^x}

Given 0<y<10 < y < 1, we can drop the absolute value.

Part II: Definite Integral

The given integral is:

I=11arccos(x2)cos2(π3x)dxI = \int_{-1}^{1} \frac{\arccos\left(\frac{x}{2}\right)}{\cos^2\left(\frac{\pi}{3}x\right)} \, dx

To evaluate this integral, we will use numerical integration in Python.

Part III: Series Functions

(1) Calculate f(x)2g(x)2f(x)^2 - g(x)^2

Given:

f(x)=m=01(2m)!x2m,g(x)=ddxf(x)f(x) = \sum_{m=0}^{\infty} \frac{1}{(2m)!} x^{2m},\qquad g(x) = \frac{d}{dx} f(x)

First, let's find g(x)g(x):

g(x)=m=12m(2m)!x2m1=m=11(2m1)!x2m1g(x) = \sum_{m=1}^{\infty} \frac{2m}{(2m)!} x^{2m-1} = \sum_{m=1}^{\infty} \frac{1}{(2m-1)!} x^{2m-1}

We recognize that:

f(x)=cosh(x),g(x)=sinh(x)f(x) = \cosh(x),\qquad g(x) = \sinh(x)

Using the hyperbolic identity:

cosh2(x)sinh2(x)=1\cosh^2(x) - \sinh^2(x) = 1

So:

f(x)2g(x)2=1f(x)^2 - g(x)^2 = 1

(2) Express In+2(x)I_{n+2}(x) using In(x)I_n(x)

Given:

In(x)=0x(g(X)f(X))ndXI_n(x) = \int_0^x \left(\frac{g(X)}{f(X)}\right)^n \, dX

We know:

g(x)f(x)=sinh(x)cosh(x)=tanh(x)\frac{g(x)}{f(x)} = \frac{\sinh(x)}{\cosh(x)} = \tanh(x)

So:

In(x)=0xtanhn(X)dXI_n(x) = \int_0^x \tanh^n(X) \, dX

Using integration by parts for In+2(x)I_{n+2}(x): Let u=tanhn+1(X)u = \tanh^{n+1}(X) and dv=tanh(X)dXdv = \tanh(X) \, dX. Then du=(n+1)tanhn(X)sech2(X)dXdu = (n+1) \tanh^n(X) \text{sech}^2(X) \, dX and v=ln(cosh(X))v = \ln(\cosh(X)).

Applying integration by parts:

In+2(x)=0xtanhn+2(X)dX=[tanhn+1(X)ln(cosh(X))]0x0x(n+1)tanhn(X)sech2(X)ln(cosh(X))dXI_{n+2}(x) = \int_0^x \tanh^{n+2}(X) \, dX = \left[ \tanh^{n+1}(X) \ln(\cosh(X)) \right]_0^x - \int_0^x (n+1) \tanh^n(X) \text{sech}^2(X) \ln(\cosh(X)) \, dX

Since tanh(0)=0\tanh(0) = 0 and ln(cosh(0))=ln(1)=0\ln(\cosh(0)) = \ln(1) = 0:

In+2(x)=tanhn+1(x)ln(cosh(x))(n+1)0xtanhn(X)sech2(X)ln(cosh(X))dXI_{n+2}(x) = \tanh^{n+1}(x) \ln(\cosh(x)) - (n+1) \int_0^x \tanh^n(X) \text{sech}^2(X) \ln(\cosh(X)) \, dX

Notice that:

sech2(X)=1tanh2(X)\text{sech}^2(X) = 1 - \tanh^2(X)

Thus:

In+2(x)=tanhn+1(x)ln(cosh(x))(n+1)(0xtanhn(X)ln(cosh(X))dX0xtanhn+2(X)ln(cosh(X))dX)I_{n+2}(x) = \tanh^{n+1}(x) \ln(\cosh(x)) - (n+1) \left( \int_0^x \tanh^n(X) \ln(\cosh(X)) \, dX - \int_0^x \tanh^{n+2}(X) \ln(\cosh(X)) \, dX \right)

Let Jn(x)=0xtanhn(X)ln(cosh(X))dXJ_n(x) = \int_0^x \tanh^n(X) \ln(\cosh(X)) \, dX:

In+2(x)=tanhn+1(x)ln(cosh(x))(n+1)Jn(x)+(n+1)Jn+2(x)I_{n+2}(x) = \tanh^{n+1}(x) \ln(\cosh(x)) - (n+1) J_n(x) + (n+1) J_{n+2}(x)

Since Jn+2(x)J_{n+2}(x) contains In+2(x)I_{n+2}(x) and Jn(x)J_n(x) contains In(x)I_n(x), we focus on simplifying:

In+2(x)=tanhn+1(x)ln(cosh(x))(n+1)Jn(x)+(n+1)(0xtanhn+2(X)ln(cosh(X))dX)I_{n+2}(x) = \tanh^{n+1}(x) \ln(\cosh(x)) - (n+1) J_n(x) + (n+1) \left( \int_0^x \tanh^{n+2}(X) \ln(\cosh(X)) \, dX \right) In+2(x)=tanhn+1(x)ln(cosh(x))(n+1)(0xtanhn(X)ln(cosh(X))dX0xtanhn+2(X)ln(cosh(X))dX)I_{n+2}(x) = \tanh^{n+1}(x) \ln(\cosh(x)) - (n+1) \left( \int_0^x \tanh^n(X) \ln(\cosh(X)) \, dX - \int_0^x \tanh^{n+2}(X) \ln(\cosh(X)) \, dX \right) In+2(x)=tanhn+1(x)ln(cosh(x))(n+1)In(x)+nIn+2(x)I_{n+2}(x) = \tanh^{n+1}(x) \ln(\cosh(x)) - (n+1) I_n(x) + n I_{n+2}(x) In+2(x)=1n+1tanhn+1(x)ln(cosh(x))In(x)I_{n+2}(x) = \frac{1}{n+1} \tanh^{n+1}(x) \ln(\cosh(x)) - I_n(x)

Part IV: Final Quantity

First, find y(x)y_*(x) that satisfies y(0)=12y_*(0) = \frac{1}{2}:

y(x)=Kex1+Kexy_*(x) = \frac{K e^x}{1 + K e^x}

Using the initial condition:

12=K1+K\frac{1}{2} = \frac{K}{1 + K} 1+K=2K1 + K = 2K K=1K = 1

Thus:

y(x)=ex1+exy_*(x) = \frac{e^x}{1 + e^x}

Now find a=y(ln3)a = y_*(\ln 3):

a=y(ln3)=eln31+eln3=31+3=34a = y_*(\ln 3) = \frac{e^{\ln 3}}{1 + e^{\ln 3}} = \frac{3}{1 + 3} = \frac{3}{4}

Next, evaluate the integral II using Python:

I=11arccos(x2)cos2(π3x)dxI = \int_{-1}^{1} \frac{\arccos\left(\frac{x}{2}\right)}{\cos^2\left(\frac{\pi}{3}x\right)} \, dx

Then, compute F0F_0 and G0G_0 where x0=ln(2+3)x_0 = \ln(2+\sqrt{3}):

F0=f(x0)=cosh(x0),G0=g(x0)=sinh(x0)F_0 = f(x_0) = \cosh(x_0),\quad G_0 = g(x_0) = \sinh(x_0)

Finally, compute SS and K\mathcal{K}.

Let's execute the Python code for these calculations. [/THOUGHT] [PYTHON] import numpy as np from scipy.integrate import quad

Part I: Differential Equation

We already have the solution y_*(x) = e^x / (1 + e^x)

a = y_*(ln 3)

a = 3 / 4

Part II: Definite Integral

def integrand(x): return np.arccos(x / 2) / np.cos(np.pi / 3 * x)**2

I, _ = quad(integrand, -1, 1)

Part III: Series Functions

x_0 = ln(2 + sqrt(3))

x_0 = np.log(2 + np.sqrt(3))

F_0 = f(x_0) = cosh(x_0)

F_0 = np.cosh(x_0)

G_0 = g(x_0) = sinh(x_0)

G_0 = np.sinh(x_0)

Part IV: Final Quantity

S = 4 * a + I / G_0 + F_0 K = 999 * S**2 + 7

print(K)

Tool Output
[PYTHON OUTPUT] 63943.0 [/PYTHON OUTPUT]
Reasoning Process

[THOUGHT] The Python output confirms the final value of K\mathcal{K} to be 63943. Therefore, the integer K\mathcal{K} is 63943\boxed{63943}.

Final Model Output
63943

Comparative Analysis (P6) (Average across runs)

Avg Time Taken

K-EXAONE-236B-A23B
330.0
GPT-5.2 (high)
111.5
Kanana-2-30B-Thinking-2601
76.9
Solar-Open-100B
67.2
GPT-5.1 (high)
57.7
HCX-007(high)
55.6
Llama-VARCO-8B-Instruct
54.7
Deepseek-V3.2
48.3
Gemini-3-Pro-Preview
47.6
A.X-4.0 (72B)
45.4
Kanana-2-30B-Thinking
42.7
Solar-Pro-2 (31B)(high)
40.2
Grok-4.1-fast
29.0
K-EXAONE-236B-A23B
22.8
Claude-Opus-4.5
20.6
EXAONE-4.0.1-32B (high)
11.1

Avg Token Usage

K-EXAONE-236B-A23B
39,933
GPT-5.2 (high)
26,193
Kanana-2-30B-Thinking-2601
19,787
Solar-Open-100B
12,619
HCX-007(high)
10,581
EXAONE-4.0.1-32B (high)
9,149
Solar-Pro-2 (31B)(high)
9,027
GPT-5.1 (high)
8,547
Grok-4.1-fast
8,351
Kanana-2-30B-Thinking
8,050
Gemini-3-Pro-Preview
7,889
A.X-4.0 (72B)
7,410
K-EXAONE-236B-A23B
6,804
Claude-Opus-4.5
5,887
Deepseek-V3.2
5,395
Llama-VARCO-8B-Instruct
1,716