To direct the learning algorithm toward a certain solution for the AS signals, we use the following procedure: for any subgroup of conditions T′ ⊂ {1,…, T} corresponding to a known signal we initialize a matching signal λ c so that sign(λ c, t ) = sign(λ c, t ′) ∀ t, t′ ∈ T′, while λ c, t = 0 ∀ t ∉ T′.
In the absence of the dispersive term and (m=0), model (1.2) reduces to the wave equation u_{tt}-Delta u-Delta u_{t}-Delta u_{tt}+u_{t}=|u|^{p-2}u. (1.4) Xu and Yang [11] established a blow-up result for certain solutions of (1.4) with arbitrary positive initial energy, where (1< p
This observation is consistent with the observation of Burde [14], where it is noted that certain solutions of the boundary layer equations for axially symmetric pipe flow are also exact solutions of the full axially symmetric Navier-Stokes equations.
On the other hand, it was noted in [13], for example, that certain solutions of the GNEP (the normalized Nash equilibria, to be defined later) can be found by solving a suitable standard VI associated to the GNEP.
Under suitable assumptions on relaxation functions, damping terms, and source terms, by using the energy method we proved a global nonexistence result for certain solutions with negative initial energy.
"I explained the situation of the team to the federation of Kazakhstan before the Giro, and I asked certain questions and asked for certain solutions," Bruyneel said.
