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
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 _____. 