A second order Jupiter-Saturn planetary theory

1982 ◽  
Vol 27 (4) ◽  
pp. 417-430 ◽  
Author(s):  
Osman M. Kamel ◽  
Abdel Aziz Bakry

2020 ◽  
Vol 22 (4) ◽  
pp. 871-874
Author(s):  
Osman M. Kamel ◽  
Adel S. Soliman

AbstractA concise lemma is given for the construction of a semi – analytic Hamiltonian second order secular J–S planetary theory using the Jacobi – Radau system of origins and in terms of the non-singular variables of H. Poincaré. We truncate our expansions at the desired power in the eccentricities and the sines of the inclinations.





1984 ◽  
Vol 31 (2) ◽  
pp. 123-134 ◽  
Author(s):  
Osman M. Kamel ◽  
Abdel Aziz Bakry


1983 ◽  
Vol 28 (2) ◽  
pp. 113-123 ◽  
Author(s):  
Osman M. Kamel ◽  
Abdel Aziz Bakry


Author(s):  
W. L. Bell

Disappearance voltages for second order reflections can be determined experimentally in a variety of ways. The more subjective methods, such as Kikuchi line disappearance and bend contour imaging, involve comparing a series of diffraction patterns or micrographs taken at intervals throughout the disappearance range and selecting that voltage which gives the strongest disappearance effect. The estimated accuracies of these methods are both to within 10 kV, or about 2-4%, of the true disappearance voltage, which is quite sufficient for using these voltages in further calculations. However, it is the necessity of determining this information by comparisons of exposed plates rather than while operating the microscope that detracts from the immediate usefulness of these methods if there is reason to perform experiments at an unknown disappearance voltage.The convergent beam technique for determining the disappearance voltage has been found to be a highly objective method when it is applicable, i.e. when reasonable crystal perfection exists and an area of uniform thickness can be found. The criterion for determining this voltage is that the central maximum disappear from the rocking curve for the second order spot.





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