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14 декабря, 2021
2.3 Procedure for Calculating Fuel-Cycle Costs
To calculate fuel-cycle costs, it is necessary to focus attention on individual fuel sublots and determine:
1. The amount and composition of each sublot when charged to the reactor
2. The amount of electricity generated by each sublot in each period in which electricity is paid for
3. The amount and composition of each sublot when discharged from the reactor
4. The cost incurred in each step for preparing fuel before it is charged to the reactor
5. The cost or credit incurred in each step for recovering fuel after it is discharged from the reactor
6. The time at which each cost is paid or each credit is received, and the time at which revenue is received for each increment of electricity generated by each lot of fuel
A somewhat simplified, approximate procedure for calculating fuel-cycle costs will be illustrated by the example of sublot 2A of the PWR whose fuel management was described in
Center line |AB C d E F G H
Fuel Lots 6,7, 8, 9 Initially 3.20 w/o U-235 Key |
Cycle Average Burnup * 10,081 MWd/MT Cycle Thermal Energy = 896.8 GWd |
Assembly Number BOC Burnup, MWd/MT EOC Burnup, MWd/MT BOC Relative Power (Assent)!у /Average)
Center
line
7FG |
9AH |
8GB |
9FG |
9FF |
8AH |
8BG |
10AH |
27841 |
10506 |
22820 |
8021 |
12007 |
20927 |
23452 |
0 |
35997 |
20929 |
31824 |
18967 |
22721 |
29456 |
32601 |
10505 |
0.72 |
0.94 |
0.81 |
1.03 |
1.03 |
0.82 |
0.93 |
1.12 |
9HA |
9BG |
9CH |
8DH |
9DH |
8EG |
10BG |
10BH |
10506 |
12827 |
9884 |
19247 |
8086 |
21118 |
0 |
0 |
20928 |
23454 |
20535 |
28621 |
19249 |
30125 |
12826 |
10847 |
0.94 |
0.97 |
0.98 |
0.86 |
1.08 |
0.88 |
1.36 |
1.16 |
8GB |
9HC |
9GB |
8FG |
9 EG |
8CH |
8DG |
10CH |
22820 |
9884 |
12827 |
18968 |
10514 |
20532 |
23409 |
0 |
31820 |
20530 |
22827 |
27840 |
21117 |
29348 |
32506 |
9883 |
0.81 |
0.98 |
0.91 |
0.81 |
1.02 |
0.86 |
0.92 |
1.03 |
9FG |
8HD |
8GF |
8FF |
98H |
90G |
10DG |
100H |
8021 |
19236 |
19382 |
22722 |
10847 |
12829 |
0 |
0 |
18956 |
28594 |
28183 |
31183 |
21660 |
23410 |
12830 |
8086 |
1.02 |
0.86 |
0.80 |
0.79 |
1.07 |
1.07 |
1.37* |
0.83 |
9FF |
9HD |
9GE |
9HB |
9GF |
8BH |
10EG |
|
12007 |
8086 |
10514 |
10847 |
8021 |
21656 |
0 |
|
22714 |
19238 |
21098 |
21656 |
19382 |
31071 |
10516 |
|
1.03 |
1.08 |
1.02 |
1.07 |
1.15 |
0.95 |
1.10 |
|
8HA |
8GE |
8HC |
9GD |
8HB |
10FF |
10FG |
|
20926 |
21099 |
20527 |
12829 |
21651 |
0 |
0 |
|
29454 |
30105 |
29340 |
23408 |
31067 |
12010 |
8022 |
|
0.82 |
0.88 |
0.86 |
1.07 |
0.95 |
1.25 |
0.82 |
|
8BG |
10GB |
8GD |
10GD |
10GE |
10GF |
||
23452 |
0 |
23407 |
0 |
0 |
0 |
||
32601 |
12825 |
32504 |
12829 |
10516 |
8022 |
||
0.93 |
1.36 |
0.92 |
1.37* |
1.10 |
0.82 |
||
ЮНА |
10HB |
10HC |
10HD |
||||
0 |
0 |
0 |
0 |
||||
10505 |
10847 |
9883 |
8086 |
= Maximum Relative Power |
|||
1.12 |
1.16 |
1.03 |
0.83 |
ABCOHFQH |
Key |
Fuel Lots 7, 8. 9. 10 Initially 3.20 w/o U-235
Assembly Number BOC Burnup, MWd/MT EOC Burnup, MWd/MT BOC Relative Power (Assembly/Average)
Figure 3.24 PWR, assembly power and burnup distribution, cycle 8.
Sec. 4. Information on material quantities and energy production from sublots 1A through 4B in cycles 1, 2, and 3, applicable to this example calculation, is given in Table 3.5.
The 63 assemblies of sublot 2A contain 28,171.8 kg of uranium enriched to 2.8 w/o aU. The average bumup experienced by this sublet is 16,448 MWd/MT in cycle 1 and 8700 MWd/MT in cycle 2, for a total bumup B2a of 25,148 MWd/MT. The total thermal energy produced by this sublot is
(25,148 MWd/MTX28.1718MTX24,000 kWh/MWd)= 17,003 X 106 kWh Calculations by computer code LEOPARD made by Rieck [Rl] predict that this fuel wnen
Table 3.3 Fuel-cycle performance of PWR in successive cycles
^Contains burnable poison. * Sixty-three assemblies from this lot and one from previous lot. |
exposed to burnup of 25,148 MWd/MT will contain 27,991 kg of uranium enriched to 0.920 w/o 235 U and 161.330 kg of the fissile isotopes of plutonium 239Pu and 241 Pu.
To obtain the durations of cycles 1 and 2, and from them the times at which payments are made, credits received, and revenue obtained from the sale of electricity, the total thermal energy per cycle Ht is required and is calculated from burnup increments in the next to the last row of the table. The duration of irradiation during the ith cycle, r,-‘ — /’■, in years is obtained from Hi in the last row of the table, using a rated thermal output of 3.250 GW.
Figure 3.25 is a schematic flow sheet for lot 2A fuel cycle. This shows the fuel-cycle steps to be considered and defines notation for the material and service quantities involved in each step, the total cost or credit associated with each step, and the timing of all transactions (dashed arrows).
Table 3.6 gives numerical values for material quantities, unit costs or credits, and total direct costs or credits involved in each fuel-cycle step and calculates the overall net direct cost for lot 2A as $26.4 million. A total of $27.8 million is paid out for UF6 and fabrication in transactions 1 and 2 before any revenue is received from the sale of electricity. Because of this delay in receiving revenue, the total fuel-cycle cost includes also charges for carrying the $27.8 million advanced several years before it is recovered through revenue from the sale of electricity. Similarly, there is a financing charge on the net credit of $1.4 million in steps 3 through 6, delayed until after revenue is received from the sale of electricity.
The assumptions going into the calculation of direct costs in Table 3.6 will be described first. Then the procedure for calculating financing charges will be described, and finally a value will be given for the complete fuel-cycle cost.
Direct costs. The unit costs used in the examples of this chapter are those anticipated in 1975 for the year 1980. Because of changes since 1975, readers are cautioned to regard these costs more as examples than as firm numbers.
The unit cost of enriched uranium in the form of UF6 depends on the 235 U content of the uranium, the price paid for the natural uranium from which the uranium was enriched, the cost of the separative work expended in enriching the uranium, and the composition of the tails stream containing depleted uranium leaving the uranium enrichment plant. The procedure for calculating the cost of enriched uranium is described in Chap. 12. The unit costs
Сц[6] = $848.66/kg U for uranium enriched to 2.8 w/o 235 U fed to fabrication and cV" = $152.83/kg U for uranium containing 0.920 w/o 235 U recovered from reprocessing are based on the following assumptions:
Price of natural uranium ore concentrates, $31.55ДЬ U308
Price of natural UF6, $89.11/kg U
Cost of separative work, $100/separative work unit
235 U content of enrichment plant tails, 0.3 w/o
Table 3.4 Zion reactor, cycle 8: Relative power and bumup
^Maximum local value. * Maximum assembly average. |
Table 3.5 Example of material quantities and energy production by lot and cycle Cycle i ——————— Fuel discharged
|
Thermal energy per cycle, GWh
Я/ = 24 X 10~6 Ujf ABjic 32,188 20,044 §
Duration of irrad.,yr 8766XJ250X a9 1-2553 0.7817 8 1
Receive Revenue from Sole of Electricity |
Zu- |
ZFa" |
ZSh = |
Zr = |
|||||
о C X |
cShU |
CRU’ |
CpPf’ |
c0.Uf’f" |
||||
Times — ty. |
lFa |
t Ґ |
t2 t2t2 |
lSh |
Ir |
V=tp |
Figure 3.25 Schematic flow sheet for lot 2A fuel cycle, showing material and service quantities and timing of transactions. |
It is assumed that /’ = 0.99 fraction of uranium charged in the form of UF6 will be recovered as fabricated fuel. Hence, to provide U’= 28,171.8 kg of fabricated uranium, 28,171.8/0.99 = 28,456.364 kg uranium in the form of UF6 must be purchased. The direct cost of this UF6 is 28,456.364 X 848.66 = $24,149,778.
A similar procedure is used to calculate the other components of the direct cost shown in Table 3.6. Other assumptions are as follows:
Fraction of uranium and plutonium recovered in reprocessing, f" = 0.99.
Fraction of recovered uranium converted to UF6,/’" = 0.995.
The fabrication unit cost of $130/kg includes cost of converting UF6 to U02 and packaging U02 in fuel assemblies.
The shipping cost of $30/kg includes storage charges at the reactor for around 150 days to permit fuel radioactivity to decrease.
The reprocessing and conversion cost of $180/kg includes charges by the government for perpetual storage of radioactive wastes.
Financing charges. A company generating electricity that pays out Z dollars for fuel-cycle costs t years before it receives revenue from generation of electricity from that fuel must pay to the bondholders and stockholders who advanced the funds for the fuel the return they require on their investment, and must also pay income taxes to the government on the profits from which the stockholders’ return is obtained. It is possible to represent all of these financing charges as the product yZt, where у is known as the annual cost of money before income taxes. For a privately owned U. S. electric company, a value of у = 0.151 per year is representative.
To find the total fuel financing charge, it is necessary to find the amount of money advanced for fuel as a function of time. Figure 3.26 is a schematic plot of the amount of
Figure 3.26 Plot of dollars invested in fuel versus time.
money invested in fuel cycle as a function of time for an example like sublot 2A, in which revenue is assumed received from the sale of electricity at two times during irradiation, from sale of Ex kWh at time r, in cycle 1 and from sale of E2 kWh at time t2 in cycle 2. The generalization to a more realistic case, in which revenue is received at more times, should be clear.
At time fu’, Zxj’ dollars are invested in enriched uranium. This amount of money is invested for tFa — tV’ years, until tFm when ZFa more dollars are paid out to fabricate fuel. The financing cost of carrying the initial investment of Zy> dollars for tFa — ty’ years is the product of the cost of money before income taxes, y, and the area of region A, Zy(tFa — fu’)-
Between tFtt, when fabrication is paid for, and f1; when revenue is received from production of Ex kWh of electricity, the dollars invested in fuel is Zy’ + ZFm and financing costs are the product of у and area B, (Zu’ + ZFa)(tx ~ tFa).
If the total electricity production of the lot of fuel is I, mEm (Ex + E2 for sublot 2A) and the net direct fuel-cycle cost is Z/Z/=Z (where Zj is the direct cost of the /’th fuel-cycle step and ZjZj = $26,439,162 for sublot 2A), the amount of money invested in fuel after tx should be reduced by ZExl(Ex + E2 ). Between fj and t2, when the second (and in this case, the last) revenue is received from production of E2 kWh of electricity, the dollars invested in fuel is Zy + ZFa — ZExl(Ex + E2), and financing costs are the product of у and area C, [Zy< + ZFa-ZEi/(Ex +E2)} (t2-tx).
The amount of electricity generated by sublot 2A in cycle 1, Et, is obtained from the thermal efficiency of the power plant
77 = ilr = 032615 (ЗЛ4)
the average burnup increment of sublot 2A in cycle 1, AB12a = 16,448 MWd/MT from Table 3.5, and the mass of uranium, U2a =28,171.8 kg. Hence
Ex = 24n ABxzaU’ia = (24)(0.32615)(16,448)(28,171.8) = 3.6271 X 109 kWhe (3.15) Similarly, the amount of electricity generated by sublot 2A in cycle 2 is
E2 = (24)(0.32615) (8700)(28,171.8) = 1.9185 X 109 kWhe (3.16)
The total electric generation is
E = Ex +E2 = (3.6271 + 1.9185) X 109 = 5.5456 X 109 kWhe (3.17)
Between t2 and t$h when payment is made for shipping fuel, the dollars invested in fuel is the difference between the initial outlay Zy’ + ZFa and the direct fuel-cycle cost Z, which is equivalent to
Zy’+ ZFa — Z = Zy" + Z? — Zsh — ZR (3.18)
The financing cost for this time interval is the product of у and area D, (Zy" + ZP — Zr —ZSh)(tsh ~h)-
Between tgh and tR, when payment is made for reprocessing fuel and converting uranium to UF6, the dollars invested in fuel is Zy" + Zp — ZR. The financing cost for this time interval is the product of у and area E, (Zy" + ZP — ZR)(tR — tsh).
If credit for plutonium and uranium is received at a time ty“ later than tR, an additional financing charge is incurred on the value of this uranium and plutonium, Zy" + ZP, for the time interval ty" — tR, equal to the product of у and the area F, (Zy" + ZPX? u" — tR).
[*r |
The sum of areas А, В, C, D, E, and F is
+ (Zu" + Zp — ZR —Zsh)(fsh + Zp ~ZR)(tR — tsf,)
+ (Zu — + Zp)(tV" — tR) = Zu — — tl)j
_l *7 (Eiti+E2t2 . ±T {Eiti +E2t2 „
Zf‘ VT^T* Fa) ^{еГ+е, tsh)
* — ‘*) — (z“-+z-> fihrir — —
Thus, the area under the curve is the sum of the product of each expenditure or credit times the difference between the mean time for receipt of revenue t
i= Eiti + E2t2
Ei +E2
and the time when the expenditure or credit is paid. This result generalizes to an expression for the area of
(3.21)
where Zj is the outlay for fuel-cycle step / (negative if a credit) at f;- and tm is the time at which revenue is received, for production of Em kWh of electricity. The fuel-cycle cost e in mills per kilowatt-hour then is
The assumptions of Table 3.7 are made to obtain the times needed to calculate the carrying-charge term for sublot 2A:
{EttT ~'<) й E’- <3-22>
A time basis of zero is taken for the start of cycle 1 (t = 0).
The mean time for receipt of revenue from sale of electricity, t, is
r= EiU +E2t2 _ (3.6271)(0.7920)+ (1.9185)(1.9355) _ , ,0„._
1- ~ЁГПГ~~————————— ШпТШБ 1 1876 yr (3-23)
From the foregoing transaction times and the direct fuel-cycle costs or credits of Table 3.6, the carrying charges and total fuel-cycle costs may be calculated, as shown in Table 3.8 for sublot 2A. Division of the total fuel-cycle cost of $33,173,168 by the electricity generated by sublot 2A, 5.5456 X 109 kWhe, and conversion to mills per kilowatt-hour of electricity by Eq.
(3.21) gives 5.9819 mills/kWhe for the unit fuel-cycle cost of lot 2A.
Table 3.8 shows that more than 20 percent of the fuel-cycle cost arises from carrying charges.