Dynamic Elastic Response of a Ring to Transient Pressure Loading

1966 ◽  
Vol 33 (2) ◽  
pp. 261-266 ◽  
Author(s):  
Shin-Ichi Suzuki

Stress analysis is carried out for distributed impact loads applied along the inner and outer edges of a ring. These loads are assumed to be of the form q(θ)e−αt. The relationships between the stresses at both edges, the dimensions, and time are obtained. The results show that the ratio μ of the stress under impact to that under static load is different from μ = 2. The problem is analyzed by using the Laplace transformation method.

2012 ◽  
Vol 2012 ◽  
pp. 1-15 ◽  
Author(s):  
M. Eshghi ◽  
M. Hamzavi ◽  
S. M. Ikhdair

The spatially dependent mass Dirac equation is solved exactly for attractive scalar and repulsive vector Coulomb potentials including a tensor interaction potential under the spin and pseudospin (p-spin) symmetric limits by using the Laplace transformation method (LTM). Closed forms of the energy eigenvalue equation and wave functions are obtained for arbitrary spin-orbit quantum number κ. Some numerical results are given too. The effect of the tensor interaction on the bound states is presented. It is shown that the tensor interaction removes the degeneracy between two states in the spin doublets. We also investigate the effects of the spatially-dependent mass on the bound states under the conditions of the spin symmetric limit and in the absence of tensor interaction (T=0).


1973 ◽  
Vol 40 (4) ◽  
pp. 1140-1141
Author(s):  
R. A. Bourgois

This Note concerns the use of the generalized Airy stress function, introduced by Radok [1], for dynamic plane-stress and plane-strain problems with axial symmetry. The solution of the basic equations for stress waves may be accomplished by Laplace transformation. The case of the dynamic elastic response of a thick cylinder to internal axial symmetric impact loads will be studied.


2015 ◽  
Vol 75 ◽  
pp. 448-458 ◽  
Author(s):  
Weiqiang Kong ◽  
Bengt Perers ◽  
Jianhua Fan ◽  
Simon Furbo ◽  
Federico Bava

2005 ◽  
Vol 128 (4) ◽  
pp. 680-686 ◽  
Author(s):  
T. Koppel ◽  
L. Ainola

The transition from a laminar to a turbulent flow in highly accelerated start-up pipe flows is described. In these flows, turbulence springs up simultaneously over the entire length of the pipe near the wall. The unsteady boundary layer in the pipe was analyzed theoretically with the Laplace transformation method and the asymptotic method for small values of time. From the experimental results available, relationships between the flow parameters and the transition time were derived. These relationships are characterized by the analytical forms. A physical explanation for the regularities in the turbulence spring-up time is proposed.


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