Given differential equation:
\[ \frac{dy}{dx} - y = 1 + 4 \sin x. \]
This is a first-order linear differential equation. To solve, we use an integrating factor (IF):
\[ \text{IF} = e^{-x}. \]
Multiplying the entire equation by the integrating factor: \[ e^{-x} \frac{dy}{dx} - e^{-x} y = e^{-x} + 4e^{-x} \sin x. \]
The left-hand side becomes the derivative of \(y e^{-x}\): \[ \frac{d}{dx}(y e^{-x}) = e^{-x} + 4e^{-x} \sin x. \]
Integrating both sides:
\[ y e^{-x} = \int \left(e^{-x} + 4e^{-x} \sin x\right) dx. \]
Evaluating the integral:
\[ y e^{-x} = \int e^{-x} dx + 4 \int e^{-x} \sin x \, dx. \]
The first integral is straightforward:
\[ \int e^{-x} dx = -e^{-x}. \]
For the second integral, we use integration by parts or known results:
\[ 4 \int e^{-x} \sin x \, dx = -2e^{-x} (\sin x + \cos x). \]
Thus: \[ y e^{-x} = -e^{-x} - 2e^{-x} (\sin x + \cos x) + C. \]
Multiplying through by \(e^x\): \[ y = -1 - 2(\sin x + \cos x) + C e^x. \]
Using the initial condition \(y(\pi) = 1\):
\[ 1 = -1 - 2(\sin \pi + \cos \pi) + C e^\pi. \]
Since \(\sin \pi = 0\) and \(\cos \pi = -1\):
\[ 1 = -1 - 2(-1) + C e^\pi \implies 1 = 1 + C e^\pi \implies C = 0. \]
Thus, the solution simplifies to: \[ y = -1 - 2(\sin x + \cos x). \]
Evaluating at \(x = \frac{\pi}{2}\):
\[ y\left(\frac{\pi}{2}\right) = -1 - 2\left(\sin \frac{\pi}{2} + \cos \frac{\pi}{2}\right) = -1 - 2(1 + 0) = -3. \]
Calculating \(y\left(\frac{\pi}{2}\right) + 10\):
\[ y\left(\frac{\pi}{2}\right) + 10 = -3 + 10 = 7. \]
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,