“…Returning to equations (2)(3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17) it is possible to obtain analytic solutions for those flux levels such that Then equations (2)(3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17) With a precise definition of mathematical stability given, the phase plane analysis of equations , , and (2-29) may now be made. Since the model under investigation is spacially independent and thus meant to be informative only, an exhaustive phase plane analysis will not be rendered.…”
Section: S ' =mentioning
confidence: 99%
“…It will be shown that the material buckling for criticality to exist that results 13 from equation (3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17) when high flux levels ($o > 10 ) a r e considered is the same a s equation . Diffusion theory, when the diffusion coefficient and absorption cross section a r e modified to include xenon absorption at high flux, leads to the following for the material buckling.…”
Section: Substituting Original Parameters Into Equation (3-24) Givesmentioning
confidence: 99%
“…Now returning to equation (3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)' under the assumption of large flux values 13 (p3 10 , ), the term "Ln(s+l)' will be neglected compared to the "sn term.…”
Section: Substituting Original Parameters Into Equation (3-24) Givesmentioning
confidence: 99%
“…A technique to obtain quasi-solutions for the spacially dependent, perturbed flux a s given by equation (5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18)(19) can be devolved from a more general mathematical technique called modal analysis. The general application of modal analysis to reactor problems has been discussed by Kaplan (23) and others.…”
Section: Modal Analysis Of the Linear Kinetic Equationsmentioning
confidence: 99%
“…Since the fundamental mode and the first few harmonics contribute most to the flux distribution the series expansion for the Laplace transformed flux will be truncated a s follows: Now the following inequalities must all be satisfied for stability of the perturbed flux a s given by equation (5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18)(19)(20)(21)(22)(23)(24).…”
“…Returning to equations (2)(3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17) it is possible to obtain analytic solutions for those flux levels such that Then equations (2)(3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17) With a precise definition of mathematical stability given, the phase plane analysis of equations , , and (2-29) may now be made. Since the model under investigation is spacially independent and thus meant to be informative only, an exhaustive phase plane analysis will not be rendered.…”
Section: S ' =mentioning
confidence: 99%
“…It will be shown that the material buckling for criticality to exist that results 13 from equation (3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17) when high flux levels ($o > 10 ) a r e considered is the same a s equation . Diffusion theory, when the diffusion coefficient and absorption cross section a r e modified to include xenon absorption at high flux, leads to the following for the material buckling.…”
Section: Substituting Original Parameters Into Equation (3-24) Givesmentioning
confidence: 99%
“…Now returning to equation (3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)' under the assumption of large flux values 13 (p3 10 , ), the term "Ln(s+l)' will be neglected compared to the "sn term.…”
Section: Substituting Original Parameters Into Equation (3-24) Givesmentioning
confidence: 99%
“…A technique to obtain quasi-solutions for the spacially dependent, perturbed flux a s given by equation (5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18)(19) can be devolved from a more general mathematical technique called modal analysis. The general application of modal analysis to reactor problems has been discussed by Kaplan (23) and others.…”
Section: Modal Analysis Of the Linear Kinetic Equationsmentioning
confidence: 99%
“…Since the fundamental mode and the first few harmonics contribute most to the flux distribution the series expansion for the Laplace transformed flux will be truncated a s follows: Now the following inequalities must all be satisfied for stability of the perturbed flux a s given by equation (5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18)(19)(20)(21)(22)(23)(24).…”
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