We are solving the differential equation:
\( \cos x (\ln(\cos x))^2 \, dy + (\sin x - 3y \sin x \ln(\cos x)) \, dx = 0 \)
Rearranging terms and dividing through by \( \cos x (\ln(\cos x))^2 \), we get:
\( \frac{dy}{dx} - \frac{3 \tan x}{\ln(\cos x)} y = -\frac{\tan x}{(\ln(\cos x))^2} \)
Since \( \ln(\cos x) = -\ln(\sec x) \), the equation becomes:
\( \frac{dy}{dx} + \frac{3 \tan x}{\ln(\sec x)} y = -\frac{\tan x}{(\ln(\sec x))^2} \)
1. Finding the Integrating Factor (I.F.):
The integrating factor is given by:
\( I.F. = e^{\int \frac{3 \tan x}{\ln(\sec x)} \, dx} \)
To compute this, note that:
\( \int \frac{\tan x}{\ln(\sec x)} \, dx = \ln(\ln(\sec x)) \)
Thus:
\( I.F. = e^{3 \ln(\ln(\sec x))} = (\ln(\sec x))^3 \)
2. Solving the Differential Equation:
Multiply through by the integrating factor \( (\ln(\sec x))^3 \):
\( y \cdot (\ln(\sec x))^3 = -\int \frac{\tan x}{(\ln(\sec x))^2} \cdot (\ln(\sec x))^3 \, dx \)
Simplify the integral:
\( y \cdot (\ln(\sec x))^3 = -\int \tan x \cdot \ln(\sec x) \, dx \)
Using substitution \( u = \ln(\sec x) \), \( du = \tan x \, dx \):
\( y \cdot (\ln(\sec x))^3 = -\int u \, du = -\frac{u^2}{2} + C = -\frac{(\ln(\sec x))^2}{2} + C \)
3. Applying the Initial Condition:
We are given \( x = \frac{\pi}{4} \) and \( y = -\frac{1}{\ln 2} \). Substituting these values:
\( -\frac{1}{\ln 2} \cdot (\ln(\sqrt{2}))^3 = -\frac{1}{2} \cdot (\ln(\sqrt{2}))^2 + C \)
Note that \( \ln(\sqrt{2}) = \frac{1}{2} \ln 2 \):
\( -\frac{1}{\ln 2} \cdot \left(\frac{1}{2} \ln 2\right)^3 = -\frac{1}{2} \cdot \left(\frac{1}{2} \ln 2\right)^2 + C \)
Simplify:
\( -\frac{1}{8 (\ln 2)^2} \cdot (\ln 2)^3 = -\frac{1}{8 (\ln 2)^2} \cdot (\ln 2)^2 + C \)
\( -\frac{1}{8} (\ln 2)^2 = -\frac{1}{8} (\ln 2)^2 + C \)
\( C = 0 \)
4. Final Solution:
The solution becomes:
\( y \cdot (\ln(\sec x))^3 = -\frac{1}{2} (\ln(\sec x))^2 \)
Divide through by \( (\ln(\sec x))^3 \):
\( y = -\frac{1}{2 \ln(\sec x)} \)
Since \( \ln(\sec x) = -\ln(\cos x) \):
\( y = \frac{1}{2 \ln(\cos x)} \)
5. Evaluating \( y \) at \( x = \frac{\pi}{6} \):
Substitute \( x = \frac{\pi}{6} \):
\( y = \frac{1}{2 \ln(\cos \frac{\pi}{6})} \)
\( \cos \frac{\pi}{6} = \frac{\sqrt{3}}{2} \):
\( y = \frac{1}{2 \ln\left(\frac{\sqrt{3}}{2}\right)} \)
Using \( \ln\left(\frac{\sqrt{3}}{2}\right) = \frac{1}{2} \ln 3 - \ln 2 \):
\( y = \frac{1}{2 \left(\frac{1}{2} \ln 3 - \ln 2\right)} = \frac{1}{\ln 3 - \ln 4} \)
Final Answer:
The value of \( y \) at \( x = \frac{\pi}{6} \) is \( \frac{1}{\ln 3 - \ln 4} \).
Let $y=y(x)$ be the solution of the differential equation $\left(x^2-3 y^2\right) d x+3 x y d y=0, y(1)=1$.Then $6 y^2( e )$ is equal to
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,