The given differential equation is:
\(\frac{dy}{dx} = \frac{(x^2 + y^2 + 1)}{(2xy)}\)
This is a non-linear differential equation and cannot be solved by simple integration techniques. However, we can make use of the fact that the given differential equation is a homogeneous equation.
To solve this differential equation, we can make the substitution \(y=vx\). Then, we have:
\(\frac{dy}{dx} = v + x\frac{dv}{dx}\)
Substituting this in the given differential equation, we get:
\(v + x\frac{dv}{dx} = \frac{(x^2 + v^2x^2 + 1)}{(2x^2v)}\)
Multiplying both sides by \(\frac{2v}{x}\) and simplifying, we get:
\(\frac{2v}{(v^2 - 1)} dv= \frac{(x^2 + 1)}{x^2} dx\)
Integrating both sides, we get:
\(ln|v - 1| - ln|v + 1| = ln|x| + C\)
where C is the constant of integration. Rearranging and using the initial condition \(y(1) = 0\) (which implies \(v(1) = 0\), we get:
\(v = \frac{y}{x} = \frac{(1 - x^2)}{(1 + x^2)}\)
Substituting this value of v in the equation \(y = vx\), we get:
\(y = x \times \frac{(1 - x^2)}{(1 + x^2)}\)
This is the solution of the given differential equation, satisfying \(y(1) = 0\).
Now, we can rewrite the equation in terms of y and x as:
\(y(1 + x^2) = x(1 - x^2)\)
This can be simplified to:
\(x^2 + y^2 = x\)
This is the equation of a circle with center at \((\frac{1}{2}, 0)\) and radius \(\frac{1}{2}\).
Therefore, the solution of the given differential equation, satisfying \(y(1) = 0\), is a circle.
The representation of the area of a region under a curve is called to be as integral. The actual value of an integral can be acquired (approximately) by drawing rectangles.
Also, F(x) is known to be a Newton-Leibnitz integral or antiderivative or primitive of a function f(x) on an interval I.
F'(x) = f(x)
For every value of x = I.
Integral calculus helps to resolve two major types of problems: