The general solution of the differential equation x2 + y2 – 2xy \(\frac {dy}{dx}\) = 0 is (where C is a constant of integration.)
2(x2 – y2) + x = C
x2 + y2 = Cy
x2 – y2 = Cx
x2 + y2 = Cx
Given x2 + y2 – 2xy \(\frac {dy}{dx}\) = 0
\(\frac {dy}{dx}\) = \(\frac {x^2 +y^2}{2xy}\)
\(\frac {dy}{dx}\) = \(\frac {x}{2y} + \frac {y}{2x}\)
Let \(\frac {y}{x}\) = v
\(\frac {dy}{dx}\)= v +x \(\frac {dv}{dx}\)
v + x\(\frac {dv}{dx}\) = \(\frac {v}{2}\) + \(\frac 12\)v
x\(\frac {dv}{dx}\)= -v + \(\frac {v}{2}\)+ \(\frac 12\) v
x\(\frac {dv}{dx}\) = -\(\frac {v}{2}\)+ \(\frac 12\)v
∫ \(\frac {2v}{1-v^2}\) dv = ∫ \(\frac {1}x{}\) dx
ln \(\frac {1}{1-v^2}\) = ln Cx
Where C is a arbitrary constant.
Now put v = \(\frac {y}{x}\)
ln \(\frac {1}{1-(\frac {y}{x})^2}\)= ln Cx
\(\frac {x^2}{x^2 - y^2}\) = Cx
x2 - y2 = Cx is also a constant.
Therefore, the correct answer is (C) x2 – y2 = Cx
Let \( f : \mathbb{R} \to \mathbb{R} \) be a twice differentiable function such that \( f(x + y) = f(x) f(y) \) for all \( x, y \in \mathbb{R} \). If \( f'(0) = 4a \) and \( f \) satisfies \( f''(x) - 3a f'(x) - f(x) = 0 \), where \( a > 0 \), then the area of the region R = {(x, y) | 0 \(\leq\) y \(\leq\) f(ax), 0 \(\leq\) x \(\leq\) 2\ is :