In this work we present the details of calculations we previously performed for the large j behavior of certain 3j and 9j symbols.In this paper we focus on equations (11 and 13), and (23 and 24) of the work of Kleszyk and Zamick [1]. In particular we consider the case when the total angular momentum I is equal to I max − 2n and I max ≡ 4j − 2, and n = 0, 1, 2, ... We take the limit of large j where n becomes much smaller than j. For convenience, we also define J = 2j, where j is the total angular momentum of a single particle.We first address the 3j coefficient, using the formula Eq. (13) We express the total angular momentum I using a new variable m such that I = 4j − 2m, where this time m = 1, 2, 3, .... We can separate parts of the 3j which now becomeswhere the 6 factors N i are:We use the Stirling approximation,and it should be noted that the approximation approaches the true value asymptotically. Now we can write: N i = (α i + β i m + γ i J) with differing constant coefficients. In Eq.(2a) we give the contribuition of −N, ln √ 2πN , α ln N, mβ ln N, and γJ ln N . For the latter we break things up into (a) "extreme" and (b) "next order". This is necessary because "next order" has contributions comparable to those in "−N ". (6) 1 arXiv:1406.4495v4 [nucl-th]