Ax = f (0.1) has a nonempty solution set N in X, x∗ is the normal solution to (1) (a solution with the minimal norm). Under these assumptions one cannot establish a continuous dependence of a solution to (1) on perturbances ofA and f . Therefore one should consider the problem on finding a solution to equation (1) as an ill-posed one and solve it with the help of a certain regularization method. Recently continuous solution methods for ill-posed problems arouse much interest. These methods are reduced to the solution of the Cauchy problem for a differential equation of a certain order. The order of the differential equation is said to be the order of a continuous method. For the case, when X = H is a Hilbert space, continuous methods are investigated rather well [1]–[6]. In [7], [8], one studies the convergence of a continuous method of the first order for equation (1) with a monotone and accretive operator A in a Banach space, assuming that the operator A is differentiable. Note that in the investigation of the convergence of a continuous method in a Banach space not only the properties of the operator A, but also the geometric properties of the spaces X and X∗ play an essential role. The objective of this paper is to establish the conditions which are sufficient for the convergence of a continuous method of the first order in a Banach space without the assumption on the differentiability of the monotone operator A. Let δX(s) be the module of convexity of the space X. Assume that this function is continuous and grows on [0, 2], δX(0) = 0 ([9], p. 49; [10]). Consequently, the inverse function δ−1 X (e) exists. Since the space X is uniformly smooth, we have that X∗ is also uniformly convex ([9], p. 34). Let δX∗(s) be the module of convexity of X∗. Define the function gX∗(s) = δX∗(s)/s. It is well known [10] that this function is continuous and grows on [0, 2], gX∗(0) = 0. Thus we can construct the function g−1 X∗(e). Assume that the operator of the dual mapping J : X → X∗ is defined by the correlations ([11], p. 311) ‖Jx‖ = ‖x‖, 〈Jx, x〉 = ‖x‖ ∀x ∈ X. (0.2) The properties of this operator are defined by the geometric properties of the spacesX andX∗. Note that under the above assumptions about the spaceX the operator J is monotone, bounded, and continuous ([11], pp. 313, 330, 331). In addition, the following inequality is true (see [8], [12])