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Reactor Kinetics-2.. 1
Laboratory for Reactor Physics and Systems Behaviour
Neutronics
Lesson 13: Reactor Kinetics-2
Step Change in Reactivity (Constant Reactivities) • Reactivity Equation (Inhour Equation)
Roots of Reactivity Equation
Stable Reactor Period (for positive reactivity) • Delayed, Prompt Criticality
“Prompt Jump” Approximation
Negative Reactivities
Control Rod Calibration
Reactor Kinetics-2.. 2
Laboratory for Reactor Physics and Systems Behaviour
Neutronics
Step Change in Reactivity (Constant Reactivity)
Important specific application of point kinetics equations • Illustrative, analytical solution possible
Constant (±) introduced at t = 0
• E.g. quick movement of a control rod
Point kinetics eqns.:
For solution, one may apply method of Laplace transforms
• Differential equations replaced by algebraic eqns.
Reactor Kinetics-2.. 3
Laboratory for Reactor Physics and Systems Behaviour
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Laplace Transforms
Useful method for study of time-dependent behaviour of a system • Differential eqn. (in time) converted to algebraic eqn. (in frequency)
Transform:
After certain manipulations, one “reconverts” to obtain solution of original eqn. (in time)
Often needed information got directly from algebraic eqn. itself (e.g. via graphical soln.)
N.B.: not necessary to affect
transformations analytically:
• One can use “tables” of
Laplace transforms
Reactor Kinetics-2.. 4
Laboratory for Reactor Physics and Systems Behaviour
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Solution of Point Kinetics Eqns.
From ,
where are the Laplace transforms of
Eliminating ,
If the reactor was critical at t = 0,
Reactor Kinetics-2.. 5
Laboratory for Reactor Physics and Systems Behaviour
Neutronics
Solution of Point Kinetics Eqns. (contd.)
Thus,
where j are the roots of the denominator
i.e. of
Reactivity Equation (Inhour Equation)
The sought solution:
(from inversion of the Laplace-transform equation (1) above)
Reactor Kinetics-2.. 6
Laboratory for Reactor Physics and Systems Behaviour
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The Roots j
Characteristic equation:
gives the relationship between , (and the kinetics parameters , i , i )
One may solve the equation (Reactivity Eqn.) graphically (Ligou considers: - = …)
o R.H.S…. function of ,
L.H.S.… (±) , constant
o
o
For +ive (supercritical reactor), one value of is +ive, the others -ive
For -ive (subcritical reactor), all 7 roots are -ive
Reactor Kinetics-2.. 7
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Stable Period … positive
For > 0 , after a certain time:
• All the other terms disappear (negative i ’s)
Stable period:
• Time (in stable region) for P (or )
to increase by factor of e
Solution 1 obtained graphically
• For a given set of kinetics parameters
( , i , i ), each specific 1
• E.g. with
transitory region: negative terms which vanish rapidly
Reactor Kinetics-2.. 8
Laboratory for Reactor Physics and Systems Behaviour
Neutronics
Stable Period (contd.)
Without delayed n’s, one had:
i.e.
Delayed n’s render the reactor controllable
For “U235 systems” ( i , i ):
For , no dependence on
In absence of delayed n’s ( = 0),
• For small ’s, differences with/
without delayed n’s, very large
• For ~ , differences decrease strongly (role of becomes much more important)
a factor of ~ 24 on period (for this example)
Reactor Kinetics-2.. 9
Laboratory for Reactor Physics and Systems Behaviour
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Delayed, Prompt Criticality
Normally, reactor is “delayed critical”:
If = , reactor is critical only with prompt n’s (T becomes very short)
For >> , delayed neutrons no longer important
• - vs - curves become asymptotic to = . +
Extremely important that all reactivity insertions are significantly less than +
• Withdrawal of a control rod
• Effects of temperature, voidage (e.g. due to boiling of a liquid moderator)
= important enough limit to provide a special unit for reactivity, the dollar
• = 0.65% (U235 system) 1 dollar (100 cents)
• For U233 , Pu239 , 1$ ~ 0.2 to 0.3%
Reactor Kinetics-2.. 10
Laboratory for Reactor Physics and Systems Behaviour
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Delayed, Prompt Criticality (contd.)
For systems with Pu239 , U233 , reactivity insertions have to be smaller • It is which matters, i.e. the value of in $ or ¢ …
Fast reactors (with Pu239 as primary fuel material), more sensitive because of their
lower value of , not because of their very small • However, abs values are also generally lower in fast reactors
Comments
Normally, change not sudden, e.g. could be ~ linear ramp in reactivity: (t) = K.t
• Point kinetics equations need to be solved numerically
Often, changes in not uniform… require consideration of spatial effects
• Much more complicated eqns. than for Point Reactor model (which remains useful…)
Change in power changes thermal balance, affects temperatures, hence ’s and
• Feedback effects: have to be negative (act as “brakes”)… safety studies involve coupling of
thermal-hydraulics, neutron kinetics
Reactor Kinetics-2.. 11
Laboratory for Reactor Physics and Systems Behaviour
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“Prompt Jump” Approximation
One has seen… rapidly at beginning, before stable period is established • What is the rapid increase in flux value during the transitory phase?
An approximation one can make sometimes: Ci’s remain constant immediately after the change (“prompt jump” approxn.)
i.e.
Thus, from one has:
Solution:
For << , exponential term decreases rapidly
“Prompt jump”:
Reactor Kinetics-2.. 12
Laboratory for Reactor Physics and Systems Behaviour
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“Prompt Jump” Approxn. (contd.)
Result valid for << , i.e. for small +ive ’s, as well as for all -ive ’s
Notions of stable period and “prompt jump” (or “prompt drop”, for -ive ’s)
provide all information necessary for describing reactor response to sudden
change in (<< )
Considering ~ P :
Reactor Kinetics-2.. 13
Laboratory for Reactor Physics and Systems Behaviour
Neutronics
Stable period … negative
For a “prompt drop”
For the stable period, one needs to consider the roots of the Reactivity Equation
• All the values are negative with
• The stable region is where only term - 1 remains and the flux is:
For negative with , 1 1 (decay const. of 1st gp.)
• Thus, a reactor cannot be shut down more quickly than with a -ive period of ~ 80s
• The “neutronic” power is determined by the prompt jump and T (80s)
• After a certain time, thermal power ~ fission-product “decay power” (residual heat)
Flux immediately after drop:
Reactor Kinetics-2.. 14
Laboratory for Reactor Physics and Systems Behaviour
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Calibration of a Control Rod
Reactivity “worth” of a control rod… function of its insertion in the core
For insertion z , effect
i.e.
For calibrating a control rod, one may make a step z
(small +ive ) and measure stable period…
Another method: “rod drop”, large -ive yielding:
(“S-curve”)
Reactor Kinetics-2.. 15
Laboratory for Reactor Physics and Systems Behaviour
Neutronics
Summary, Lesson 13
Reactivity Equation (constant reactivities)
Roots of Reactivity Equation • Stable Reactor Period
Delayed, prompt criticality • Dollar
“Prompt jump” (small +ive, all -ive ’s)
Negative reactivities
Control rod calibration