To solve the given problem, we need to understand that the problem involves an integral equation and a differential equation. We will proceed by analyzing the conditions and deriving the necessary expressions.
The given equation is:
\[\int_{0}^{x} \sqrt{1 - (y'(t))^2} \, dt = \int_{0}^{x} y(t) \, dt, \quad 0 \leq x \leq 3, \, y \geq 0, \, y(0) = 0.\]
We differentiate both sides with respect to \( x \) to get:
\[\sqrt{1 - (y'(x))^2} = y(x).\]
Squaring both sides, we get:
\[1 - (y'(x))^2 = y(x)^2.\]
This can be rearranged to:
\[(y'(x))^2 = 1 - y(x)^2.\]
Taking the second derivative with respect to \( x \), we differentiate both sides:
\[2y'(x)y''(x) = -2y(x)y'(x).\]
Assuming \( y'(x) \neq 0 \), we can divide by \( 2y'(x) \):
\[y''(x) = -y(x).\]
Substituting into the expression \( y'' + y + 1 \) gives us:
\[y''(2) + y(2) + 1 = -y(2) + y(2) + 1 = 1.\]
Thus, at \( x = 2 \), the value of \( y'' + y + 1 \) is 1.
Correct choice: 1
The given equation is:
\[\int_{0}^{x} \sqrt{1 - (y'(t))^2} \, dt = \int_{0}^{x} y(t) \, dt.\]
Differentiating both sides with respect to \(x\):
\[\sqrt{1 - (y'(x))^2} = y(x).\]
Squaring both sides:
\[1 - (y'(x))^2 = y(x)^2.\]
Rearranging terms:
\[(y'(x))^2 + y(x)^2 = 1.\]
Differentiating this equation with respect to \(x\):
\[2y'(x)y''(x) + 2y(x)y'(x) = 0.\]
Simplify:
\[y'(x)(y''(x) + y(x)) = 0.\]
Since \(y'(x) \neq 0\) in general, it must be that:
\[y''(x) + y(x) = 0.\]
Now consider the term \(y'' + y + 1\):
\[y''(x) + y(x) + 1 = 0 + 1 = 1.\]
Thus, at \(x = 2\):
\[1.\]
Answer: (1) 1
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,