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The function g ( x ) = f ( x ) + x satisfies the differential equation: g ′ ( x ) = 1 + 1 + x 2 ( g ( x ) / x − 1 ) 2 1 − ( g ( x ) / x − 1 ) 2 . This implies that g ′ ( x ) > 0 for all x > 1 , so the limit L 1 = lim x → + ∞ g ( x ) exists. In addition, we cannot have L 1 < + ∞ , or else we would have lim x → + ∞ g ′ ( x ) = 0 whereas the differential equation forces this limit to be 1. Hence g ( x ) → + ∞ as x → + ∞ .
Similarly, the function h ( x ) = − f ( x ) + x satisfies the differential equation h ′ ( x ) = 1 − 1 + x 2 ( h ( x ) / x − 1 ) 2 1 − ( h ( x ) / x − 1 ) 2 . This implies that h ′ ( x ) ≥ 0 for all x , so the limit L 2 = lim x → + ∞ h ( x ) exists. In addition, we cannot have L 2 < + ∞ , or else we would have lim x → + ∞ h ′ ( x ) = 0 whereas the differential equation forces this limit to be 1. Hence h ( x ) → + ∞ as x → + ∞ .
For some x 1 > 1 , we must have g ( x ) , h ( x ) > 0 for all x ≥ x 1 . For x ≥ x 1 , we have ∣ f ( x ) ∣ < x and hence f ′ ( x ) > 0 , so the limit L = lim x → + ∞ f ( x ) exists. Once again, we cannot have L < + ∞ , or else we would have lim x → + ∞ f ′ ( x ) = 0 whereas the original differential equation (e.g., in the form given in the first solution) forces this limit to be 1 / ( 1 + L 2 ) > 0 . Hence f ( x ) → + ∞ as x → ∞ , as desired.