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A fundamental problem in analysis is to decide whether a smooth solution exists for the Navier-Stokes equations in three dimensions. In this paper we shall study this problem. The Navier-Stokes equations are given by: $u_{it}(x,t)-ρ\triangle u_i(x,t)-u_j(x,t) u_{ix_j}(x,t)+p_{x_i}(x,t)=f_i(x,t)$ , $div\textbf{u}(x,t)=0$ with initial conditions $\textbf{u}|_{(t=0)\bigcup\partialΩ}=0$. We introduce the unknown vector-function: $\big(w_i(x,t)\big)_{i=1,2,3}: u_{it}(x,t)-ρ\triangle u_i(x,t)-\frac{dp(x,t)}{dx_i}=w_i(x,t)$ with initial conditions: $u_i(x,0)=0,$ $u_i(x,t)\mid_{\partialΩ}=0$. The solution $u_i(x,t)$ of this problem is given by: $u_i(x,t) = \int_0^t \int_ΩG(x,t;ξ,τ)~\Big(w_i(ξ,τ) + \frac{dp(ξ,τ)}{dξ_i}\Big)dξdτ$ where $G(x,t;ξ,τ)$ is the Green function. We consider the following N-Stokes-2 problem: find a solution $\textbf{w}(x,t)\in \textbf{L}_2(Q_t), p(x,t): p_{x_i}(x,t)\in L_2(Q_t)$ of the system of equations: $w_i(x,t)-G\Big(w_j(x,t)+\frac{dp(x,t)}{dx_j}\Big)\cdot G_{x_j}\Big(w_i(x,t)+\frac{dp(x,t)}{dx_i}\Big)=f_i(x,t)$ satisfying almost everywhere on $Q_t.$ Where the v-function $\textbf{p}_{x_i}(x,t)$ is defined by the v-function $\textbf{w}_i(x,t)$. Using the following estimates for the Green function: $|G(x,t;ξ,τ)| \leq\frac{c}{(t-τ)^μ\cdot |x-ξ|^{3-2μ}}; |G_{x}(x,t;ξ,τ)|\leq\frac{c}{(t-τ)^μ\cdot|x-ξ|^{3-(2μ-1)}}(1/2<μ<1),$ from this system of equations we obtain: $w(t)<f(t)+b\Big(\int_0^{t}\frac{w(τ)}{(t-τ)^μ} dτ\Big)^2$; $w(t)=\|\textbf{w}(x,t)\|_{L_2(Ω)}, f(t)=\|\textbf{f}(x,t)\|_{L_2(Ω)}.$ Further, using the replacement of the unknown function by \textbf{Riccati}, from this inequality we obtain the a priori estimate. By the Leray-Schauder's method and this a priori estimate the existence and uniqueness of the solution is proved.