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
A conducting bar moves on two conducting rails as shown in the figure. A constant magnetic field \( B \) exists into the page. The bar starts to move from the vertex at time \( t = 0 \) with a constant velocity. If the induced EMF is \( E \propto t^n \), then the value of \( n \) is _____. 