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The derivation of integration-fragmentation equations in the Becker-Döring case-Döring case. From the continuum integration-fragmentation equation we derived a new equation which we call

Generalized Boltzmann-Type Equations for Aggregation in Gases and fragmentation processes. Dynamic equations for the particle concentrations in the system are derived using

Kinetic Equations for Particle Clusters Differing in Shape and the H-theorem and semidetailed balance). These equations are to generalize the classical coagulation-fragmentation type equations

Kinetic Models of Integration-Fragmentation in the Becker-Do¨ring Case: Derivation of Equations and the H-TheoremKinetic Models of Integration-Fragmentation in the Becker-Do¨ring Case: Derivation of Equations

On equivalence between kinetic equations and geodesic equations in spaces with affine connectionDiscrete kinetic equations describing binary processes of agglomeration and fragmentation

Kinetic models of integration-fragmentation in the Becker-D¨oring case: derivation of equations, the H-theoremWe examined the interconnections between the kinetic equations of evolution of particles

Mathematical model of a two-stage process of laser fragmentation of nitrocompound molecules and subsequent laser-induced fluorescence of characteristic fragments fragmentation of vapors of nitrocompounds and subsequent nitric oxide (NO-fragments) laser-induced fluorescence

Branching processes with infinite collection of particle types and stochastic fragmentation theoryThe stochastic model for the description of the so-called fragmentation process in frameworks

Investigation into the critical domain problem for the reaction-telegraph equation using advanced numerical algorithms traditional reaction–diffusion equations. Being motivated by ecological problems such as habitat fragmentation

Analytical solution for tension-saturated and unsaturated flow from wicking porous pipes in subsurface irrigation: The Kornev-Philip legacies revisited are considered and connected through continuity of pressure along the pipe-soil contact. The first fragment is a

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