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Analysis of Possible Solutions of Some Inverse Dynamical Problem with Regard for Constraint Stabilization
Mukharlyamov R.G., Kaspirovich I.E.
Abstract: Methods for constructing systems of second-order ordinary differential equations whose
Fundamental solution of multidimensional axisymmetric Helmholtz equation
Mavlyaviev R., Garipov I.
© 2016 Informa UK Limited, trading as Taylor & Francis GroupFor axisymmetric Helmholtz equation
Fundamental solution of multidimensional axisymmetric Helmholtz equation
Mavlyaviev R., Garipov I.
© 2016 Informa UK Limited, trading as Taylor & Francis Group.For axisymmetric Helmholtz equation
On the representation of Maxwell's equations in closed waveguides by the help of Helmholtz equations
Malykh M.D., Sevastianov L.A., Tyutyunnik A., Nikolaev N.E.
On the representation of Maxwell's equations in closed waveguides by the help of Helmholtz
Inverse problem of the calculus of variations for systems of differential-difference equations of second order
Popov A.M.
of differential-difference equations is considered. The relationship between the formal potentiality of a linear
An over-determined boundary problem for the Helmholtz equation in a semiinfinite domain with a curvilinear boundary
Tumakov D.
In this paper we consider an over-determined Cauchy problem for the Helmholtz equation in a
Construction of Equations of Dynamics of a Given Structure Based on Equations of Program Constraints
Mukharlyamov R.G.
disturbances. We use modified Helmholtz conditions to represent differential equations in the form of Lagrange
Double-layer potential of axially symmetric Helmholtz lowest term equation
Mavlyaviev R., Khabibullina G., Garipov I.
,which is the generalized Helmholtz equation,both with the lowest term and without it,a double-layer potential is found
Helmholtz potentiality conditions for systems of differential-difference equations
Popov A.M.
-difference equations of muth order of neutral type, we obtain necessary and sufficient conditions for potentiality
Построение уравнений динамики заданной структуры по уравнениям программных связей
Мухарлямов Р.Г.
disturbances. We use modified Helmholtz conditions to represent differential equations in the form of Lagrange

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