The equation is nonlinear because of the square root and the dependence on y'. Our task is to find a solution for y(x) under the given conditions.
To make the equation more manageable, let’s introduce a substitution. Define: v = y'. Then, y''=dv/dx, and the equation becomes: x dv/dx = sqrt(1 + v^2)
We can now separate the variables to integrate. Rewrite the equation as: dv/sqrt(1 + v^2) = dx/x
We can now integrate both sides. The integral of dv/sqrt(1+v^2) is a standard form, which is: ∫ dv/sqrt(1 + v^2) = sinh^(-1)(v)
And the integral of dx/x is ∫ dx/x = ln|x|
So after integration, we get: sinh^(-1)(v) = ln|x| + C
Now, solve for v by taking the hyperbolic sine of both sides:
v = sinh(ln|x| + C)
Using the identity for the hyperbolic sine function, sinh(a+b)=sinh(a)cosh(b)+cosh(a)sinh(b), you can expand this, but it's simpler to treat this as: v = sinh(ln|x| + C)
^this is the expression for v=y'
We know that y'(25)=0, so 0 = sinh(ln|25| + C), which implies ln|25| + C = 0 -> C = -ln|25|
v = sinh(ln|x| - ln|25|)
v = sinh(ln(x/25))
v = (x^2 - 625) / (50x) [using sinh(ln(a))=(a^2-1)/(2a)]
Thus, y' = (x^2 - 625) / 50x
y(x) = ∫ (x^2 - 625) / (50x) dx
y(x) = (1/50) ∫ (x - 625/x) dx
y(x) = (1/50) (x^2 / 2 - 625 ln|x|) + D where D is another constant of integration
0 = (1/50) (25^2 / 2 - 625 ln|25|) + D
0 = (1/50) (625/2 - 625 ln 25) + D
D = (625/50) ln 25 - (625/100)
Thus, final solution:
y(x) = (1/50) (x^2 / 2 - 625 ln|x|) + (625/50 ln 25 - 625/100)
You can simplify this further to y = x2/100 - 25lnx/2 + 25ln25/2 - 25/4