In this subsection, we shall solve (3.12).
In this example we shall solve (4.7) on [ 0, 1 / 2 ].
In theorem, we shall solve the Fekete-Szegö problem for f ∈ S.
Now we shall solve the system of triple (q^{2} -integral eq^{2} -integral(4.3).
In equation (4.1), we shall solve it by two types of the Hukuhara derivative, which are defined in Definition 2.2.
For the sake of simplicity we have neglected such collisions, but in our future work, we shall solve the cumbersome problem by taking into consideration these collisions.
The optimization problem that we shall solve is max W ( 1 − λ ) ∑ j, k = 1 j > k N ϱ jk 2 + λ log | det W | s.t.
In the following, we shall solve the q-fractional isoperimetric problem: Given a functional J as in (4.1), find which functions minimize (or maximize) J, when subject to the boundary conditions y(0)=y_{0},qquad y(a)=y_{a} (4.6) and the q-integral constraint I y)= int_{0}^{a}Gbigl x,y, ^{mathrm{c}}D_{q,0^^{alpha}ybigr),d_{q}x=l, (4.7) where l is a fixed real number.
In this section, we shall solve the inverse spectral problem, give the sufficient conditions for three sequences to be the spectra of (L 0,1 0,infty;q)), (L 0,1/2;0,h_;q)) and (L(1/2,1 h_,infty;q)) with (h_neq h_), and further describe the procedure of recovering the potential.
In this paper, we shall solve this problem and explicitly give a new solution of the Neumann problem on (partialmathcal{T}_{n}). Define varepsilon_{0}=limsup_{rrightarrowinfty}tau^{-1}(r)r tau'(r)log r< 1, where (tau(r)) is a nondecreasing and continuously differentiable function satisfying (tau(r geq1) for any (rinmathbf{R}^cup{0}).
