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Jeffery Lewins (MIT ‘56-’59
Some lessons fro early student research (Mistakes I have made)
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Just Three of My Mistakes
The undergraduate paper Reactor kinetics ‘generation time’ Adjoint equations and ‘importance’
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Reactor Kinetics Definitons
Neutron Production rate P Neutron Removal rate R Neutron Lifetime 1/R Neutron Generation time /P k effective P/R k excess (P-R)/P reactivity (P-R)/P Delayed neutron production fraction
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One group of delayed neutrons using the lifetime
1/Removal rate
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Using the Generation time: 1/production rate
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The search for exact solutions with varying .
Time varying reactivity especially ramp and oscillations
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The search for exact solutions with varying .
Time varying reactivity especially ramp and oscillations Step change: converging series solution with infinite radius of convergence (the exponential)
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The search for exact solutions with varying .
Time varying reactivity especially ramp and oscillations Step change: converging series solution with infinite radius of convergence (the exponential) Ramp:the second order (or 1+Ithorder) does not converge!
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Various elegant approximations but not ‘exact’
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Various elegant approximations but not ‘exact’
Henri Smets and the Legendre transform solution for ramp and oscillatory reactivities requiring 1+I independent inverse integral transformations
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Various elegant approximations but not ‘exact’
Henri Smets and the Legendre transform solution for ramp and oscillatory reactivities requiring 1+I independent inverse integral transformations Thought:If it is there in transform space surely it must be there in real space?
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Various elegant approximations but not ‘exact’
Henri Smets and the Legendre transform solution for ramp and oscillatory reactivities requiring 1+I independent inverse integral transformations Thought:If it is there in transform space surely it must be there in real space? Second thought: How about 1+I simultaneous first order equations?
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Various elegant approximations but not ‘exact’
Henri Smets and the Legendre transform solution for ramp and oscillatory reactivities requiring 1+I independent inverse integral transformations Thought:If it is there in transform space surely it must be there in real space? Second thought: How about 1+I simultaneous first order equations? It works!! Finite radius of convergence so solve for 1+I Dirac distributions and step out as far as wanted
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Exact ramp reactivity solution
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Exact oscillating reactivity solution
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Generation time: The time for one neutron to produce neutrons Reproduction time: The time for one neutron to produce one neutron
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Variational theory: deriving the adjoint equation from the “Conservation of Importance’
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Importance, the adjoit equation cummutation
and the detector distribution H Critica: (Ussachev) volume of phase-space
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Importance, the adjoit equation cummutation
and the detector distribution H Critica: (Ussachev) Source-free Time dependent (Lewins)
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Importance, the adjoit equation cummutation
and the detector distribution H Critica: (Ussachev) Source-free Time dependent (Lewins) Steady state With source (Selengut)
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Importance, the adjoit equation cummutation
and the detector distribution H Critica: (Ussachev) Source-free Time dependent (Lewins) Steady state With source The works
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Variational Approximation
Lagrangian for the question of interest Natural boundary conditions First-order error Second-order error 10%,10% gives 1%
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Problem: Non-natural boundary conditions
Natural BC: Outer boundaries Then sources commute Non-natural bc for ? Can non-natural bcs be represented through Dirac distributions as sources?
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Or does it? What about non-naturtal bcs?
?? It does not commute! commutes only Solution: write the non-natural bcs as Dirac distributions in the source S. so that is normal. ?Ho Expectw? Desired relationship Sources?
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Write the non-natural boundary conditions as Dirac distributions ?
Develop a Dirac notation that has to be integrated normal to the boundary surface. Try it on a simple heat conduction problem to see if it works in two dimensions?
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