Given,
f ( 1 ) = 1 , f ( a ) = 0 f ( 1 ) = 1, f ( a ) = 0 f ( 1 ) = 1 , f ( a ) = 0
And f ( x ) = lim r → x { 2 r 2 [ ( f ( r ) ) 2 − f ( x ) f ( r ) ] r 2 − x 2 − r 3 e f ( r ) r } f\left(x\right) = \sqrt{\lim_{r \to x}\left\{\dfrac{2{r}^{2}\left[( f ( r ) {)}^{2} - f ( x ) f ( r )\right]}{{r}^{2} - {x}^{2}} - {r}^{3}e\dfrac{f ( r )}{r}\right\}} f ( x ) = lim r → x { r 2 − x 2 2 r 2 [ ( f ( r ) ) 2 − f ( x ) f ( r ) ] − r 3 e r f ( r ) }
⇒ f 2 ( x ) = lim r → x ( 2 r 2 ( f 2 ( r ) − f ( x ) f ( r ) ) r 2 − x 2 − r 3 e f ( r ) r ) ⇒ {f}^{2} ( x ) = \lim_{r \to x}\left(\dfrac{2{r}^{2}\left({f}^{2} ( r ) - f ( x ) f ( r )\right)}{{r}^{2} - {x}^{2}} - {r}^{3}e\dfrac{f ( r )}{r}\right) ⇒ f 2 ( x ) = lim r → x ( r 2 − x 2 2 r 2 ( f 2 ( r ) − f ( x ) f ( r ) ) − r 3 e r f ( r ) )
⇒ f 2 ( x ) = lim r → x ( 2 r 2 f ( r ) r + x ( f ( r ) − f ( x ) ) r − x − r 3 e f ( r ) r ) ⇒ {f}^{2} ( x ) = \lim_{r \to x}\left(\dfrac{2{r}^{2}f ( r )}{r + x}\dfrac{( f ( r ) - f ( x ) )}{r - x} - {r}^{3}e\dfrac{f ( r )}{r}\right) ⇒ f 2 ( x ) = lim r → x ( r + x 2 r 2 f ( r ) r − x ( f ( r ) − f ( x )) − r 3 e r f ( r ) )
⇒ f 2 ( x ) = 2 x 2 f ( x ) x + x ( lim r → x ( f ( r ) − f ( x ) ) r − x ) − x 3 e f ( x ) x ⇒ {f}^{2} ( x ) = \dfrac{2{x}^{2}f ( x )}{x + x}\left(\lim_{r \to x}\dfrac{( f ( r ) - f ( x ) )}{r - x}\right) - {x}^{3}e\dfrac{f ( x )}{x} ⇒ f 2 ( x ) = x + x 2 x 2 f ( x ) ( lim r → x r − x ( f ( r ) − f ( x )) ) − x 3 e x f ( x )
⇒ f 2 ( x ) = 2 x 2 f ( x ) 2 x f ′ ( x ) − x 3 e f ( x ) x ⇒ {f}^{2} ( x ) = \dfrac{2{x}^{2}f ( x )}{2x}{f}^{'} ( x ) - {x}^{3}e\dfrac{f ( x )}{x} ⇒ f 2 ( x ) = 2 x 2 x 2 f ( x ) f ′ ( x ) − x 3 e x f ( x )
Now, taking f ( x ) = y f\left(x\right) = y f ( x ) = y we get,
⇒ y 2 = x y d y d x − x 3 e y x ⇒ {y}^{2} = xy\dfrac{dy}{dx} - {x}^{3}e\dfrac{y}{x} ⇒ y 2 = x y d x d y − x 3 e x y
⇒ y x = d y d x − x 2 y e y x ⇒ \dfrac{y}{x} = \dfrac{dy}{dx} - \dfrac{{x}^{2}}{y}e\dfrac{y}{x} ⇒ x y = d x d y − y x 2 e x y
Now, let y = v x ⇒ d y d x = v + x d v d x y = vx ⇒ \dfrac{dy}{dx} = v + x\dfrac{dv}{dx} y = vx ⇒ d x d y = v + x d x d v
⇒ v = v + x d v d x − x v e v ⇒ v = v + x\dfrac{dv}{dx} - \dfrac{x}{v}{e}^{v} ⇒ v = v + x d x d v − v x e v
⇒ d v d x = e v v ⇒ \dfrac{dv}{dx} = \dfrac{{e}^{v}}{v} ⇒ d x d v = v e v
⇒ e − v v d v = d x ⇒ {e}^{- v}vdv = dx ⇒ e − v v d v = d x
Integrating both side
e v ( x + c ) + 1 + v = 0 {e}^{v} ( x + c ) + 1 + v = 0 e v ( x + c ) + 1 + v = 0
Now using f ( 1 ) = 1 ⇒ x = 1 , y = 1 f ( 1 ) = 1 ⇒ x = 1, y = 1 f ( 1 ) = 1 ⇒ x = 1 , y = 1 we get,
⇒ c = − 1 − 2 e ⇒ c = - 1 - \dfrac{2}{e} ⇒ c = − 1 − e 2
Hence, e v ( − 1 − 2 e + x ) + 1 + v = 0 {e}^{v}\left(- 1 - \dfrac{2}{e} + x\right) + 1 + v = 0 e v ( − 1 − e 2 + x ) + 1 + v = 0
⇒ e y x ( − 1 − 2 e + x ) + 1 + y x = 0 ⇒ e\dfrac{y}{x}\left(- 1 - \dfrac{2}{e} + x\right) + 1 + \dfrac{y}{x} = 0 ⇒ e x y ( − 1 − e 2 + x ) + 1 + x y = 0
Now taking, x = a and y = 0 x = a \text{ and } y = 0 x = a and y = 0 we get,
e 0 ( − 1 − 2 e + a ) + 1 + 0 = 0 {e}^{0}\left(- 1 - \dfrac{2}{e} + a\right) + 1 + 0 = 0 e 0 ( − 1 − e 2 + a ) + 1 + 0 = 0
⇒ a = 2 e ⇒ a = \dfrac{2}{e} ⇒ a = e 2
⇒ a e = 2 ⇒ ae = 2 ⇒ a e = 2