2\(1 - sin2\)
2\(\sin(2) + 1\)
We start with the differential equation:
\(\sec x \, dy + \{ 2(1 - x) \tan x + x(2 - x) \} \, dx = 0\)
Divide by \(\sec x\) to simplify:
\(\dfrac{dy}{dx} = -\{ 2(1 - x) \sin x + x(2 - x) \cos x \}\)
Integrate both sides:
\(y(x) = - \int \{ 2(1 - x) \sin x + x(2 - x) \cos x \} \, dx + C\)
Separate the integrals:
\(y(x) = - \int 2(1 - x) \sin x \, dx - \int x(2 - x) \cos x \, dx + C\)
Calculate each integral:
\(y(x) = (x^2 - 2x) \sin x + C\)
Using the initial condition \(y(0) = 2\):
\(y(0) = 0 + C \Rightarrow C = 2\)
Thus,
\(y(x) = (x^2 - 2x) \sin x + 2\)
Finally, substituting \(x = 2\):
\(y(2) = (2^2 - 2 \times 2) \sin 2 + 2 = 2\)
To solve the given differential equation, we first rewrite it in a more standard form:
\(\sec(x) \frac{dy}{dx} + [2(1 - x) \tan(x) + x(2 - x)] = 0\)
Reorganizing the terms, we find:
\(\frac{dy}{dx} = -\sec(x) \left[ 2(1 - x) \tan(x) + x(2 - x)\right]\)
Let's solve this differential equation using the method of separation of variables.
We separate the variables and integrate:
\(\int \sec(x) \, dx = - \int \left[ 2(1 - x) \tan(x) + x(2 - x)\right] \, dx\)
Integrating separately on each side:
The solution \(y(x)\) comes in the form:
\(y(x) = C - \ln|\sec(x) + \tan(x)| + \left[x^2 - x^2(2) + 2x \ln|x|\right]\)
We apply the initial condition \(y(0) = 2\):
Calculate:
Therefore, the constant \(C = 2\).
Now substitute back to find \(y(2)\):
Calculate:
Thus, given the simplification, \(y(2) = 2\).
Thus, the correct answer to the question is: 2
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,