To solve the differential equation given by:
\(\frac{dy}{dx} = \frac{(\tan x) + y}{\sin x (\sec x - \sin x \tan x)}\)
with the initial condition \( y \left( \frac{\pi}{4} \right) = 2 \), we need to determine \( y \left( \frac{\pi}{3} \right) \).
Step 1: Simplify the Differential Equation
The differential equation is
\(\frac{dy}{dx} = \frac{\tan x + y}{\sin x (\sec x - \sin x \tan x)}\)
First, simplify the denominator:
\(\sec x - \sin x \tan x = \frac{1}{\cos x} - \sin x \cdot \frac{\sin x}{\cos x} = \frac{1 - \sin^2 x}{\cos x} = \frac{\cos^2 x}{\cos x} = \cos x\)
Thus, the differential equation simplifies to:
\(\frac{dy}{dx} = \frac{\tan x + y}{\sin x \cos x}\)
Step 2: Separate Variables
Rewrite this as:
\((\tan x + y) dx = \sin x \cos x \, dy\)
Separate variables:
\((\tan x + y) dx = \sin x \cos x \, dy\)
Step 3: Integrate Both Sides
Integrate both sides:
\(\int \frac{1}{\sin x \cos x} \, dx = \int \frac{1}{\tan x + y} \, dy\)
The integration yields:
\(\log |\sin x| = \log |\tan x + y| + C\)
where \( C \) is the constant of integration.
Step 4: Apply Initial Condition
Using the initial condition \( y \left( \frac{\pi}{4} \right) = 2 \):
\(\log |\sin(\frac{\pi}{4})| = \log |1 + 2| + C\)
\(\log \left(\frac{\sqrt{2}}{2}\right) = \log 3 + C\)
Thus,
\(C = \log \left(\frac{\sqrt{2}}{6}\right)\)
Step 5: Solve for \( y \left( \frac{\pi}{3} \right) \)
Substituting back, resolve for \( y \left( \frac{\pi}{3} \right) \):
\(\log |\sin(\frac{\pi}{3})| = \log |1 + y(\frac{\pi}{3})| + \log \left(\frac{\sqrt{2}}{6}\right)\)
Since \( \sin(\frac{\pi}{3}) = \frac{\sqrt{3}}{2} \), simplify to find
\(y(\frac{\pi}{3}) = \sqrt{3} \left(2 + \log_e \sqrt{3} \right)\)
By comparing with the options provided, the correct solution is:
\(\sqrt{3} \left( 2 + \log_e \sqrt{3} \right)\)
\[ \frac{dy}{dx} - 2 \cos(2x) \cdot y = \sec^2 x \] \[ \frac{dy}{dx} + p \cdot y = Q \]
Integrating Factor (IF):
\[ IF = e^{\int p \, dx} = e^{-2 \int \csc(2x) \, dx} \]
Let \( 2x = t \):
\[ 2dx = dt \implies dx = \frac{dt}{2} \]
Calculating the Integrating Factor:
\[ e^{\int \csc(2x) dx} = e^{-\int \tan t \, dt} = e^{-\ln |\tan x|} = \frac{1}{|\tan x|} \]
So, the solution becomes:
\[ y(IF) = \int Q \cdot (IF) \, dx + c \] \[ y = \frac{1}{|\tan x|} \int \sec^2 x \cdot \frac{1}{|\tan x|} \, dx + c \] \[ y = \frac{1}{|\tan x|} \int \frac{dt}{|t|} + c \quad \text{(for \( \tan x = t \))} \] \[ y = \frac{1}{|\tan x|} \ln |t| + c \] \[ y = |\tan x| \left( \ln |\tan x| + c \right) \]
Setting specific values:
Put \( x = \frac{\pi}{4} \), \( y = 2 \):
\[ 2 = \ln 1 + c \implies c = 2 \] \[ y = |\tan x| \left( \ln |\tan x| + 2 \right) \] \[ y\left(\frac{\pi}{3}\right) = \sqrt{3} \left( \ln \sqrt{3} + 2 \right) \]
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,