There are two ways of deriving the asymptotic expansion of J ν (νa), as ν → ∞, which holds uniformly for a ≥ 0. One way starts with the Bessel equation and makes use of the turning point theory for secondorder differential equations, and the other is based on a contour integral representation and applies the theory of two coalescing saddle points. In this paper, we shall derive the same result by using the three term recurrence relation J ν+1 (x) + J ν−1 (x) = (2ν/x)J ν (x). Our approach will lead to a satisfactory development of a turning point theory for second-order linear difference equations.