1985
DOI: 10.1007/978-3-642-70249-5_8
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Radio Wave Propagation in the Magnetosphere

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Cited by 2 publications
(3 citation statements)
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“…According to [15], we can assume δ eff ∼ = 2 × 10 −3 . The transmission coefficient for a weakly ionized plasma layer with sharp boundaries and thickness d is defined by the formula [16]…”
Section: Discussion Of Experimental Resultsmentioning
confidence: 99%
“…According to [15], we can assume δ eff ∼ = 2 × 10 −3 . The transmission coefficient for a weakly ionized plasma layer with sharp boundaries and thickness d is defined by the formula [16]…”
Section: Discussion Of Experimental Resultsmentioning
confidence: 99%
“…2 shows the dependence the pitch of deflection on time for different values of the load.As seen from the graph, our solution is consistent with the solution obtained in [2], which confirms the reliability of the results. Next we consider the problem stability of a rod from high density polyethylene.As the constraint equation will use the Maxwell-Gurevich equation [6] In [4] for the stability problems are limited to only "older" rubbery component of the deformations The graphs show that the "younger" high elastic component of deformation begins to occur even when time is short, especially when the value of the load close to the Euler force.…”
Section: Advanced Materials and Technologiesmentioning
confidence: 99%
“…In matrix form (6) 7) approaches under any constraint equation and allows obtaining a solution regardless of method of fixing, cross-sectional shape, the function changes of initial deflection.Algorithm for determining the strain at each time point is given in [8,9]. For hinge-supportedrod we accept .…”
mentioning
confidence: 99%