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Nuclear Energy for District Cooling HUSSEIN ABUSHAMAH, RADEK SKODA, JANA JIŘIČKOVÁ, FACULTY OF ELECTRICAL ENGINEERING, UNIVERSITY OF WEST BOHEMIA 1

Nuclear Energy for District Cooling

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Page 1: Nuclear Energy for District Cooling

Nuclear Energy for District Cooling

HUSSEIN ABUSHAMAH, RADEK SKODA, JANA JIŘIČKOVÁ, FACULTY OF ELECTRICAL ENGINEERING, UNIVERSITY OF WEST BOHEMIA

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Page 2: Nuclear Energy for District Cooling

Heat exchanger

hall

Nuclear heat-only plant

Hot Water

Return Water

Return Water

District heating network

Hot water98 °C

SFAs from VVER

Or

Low enrichment UraniumTEPLATOR

District HeatingConcept

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Page 3: Nuclear Energy for District Cooling

TEPLATOR –Novel Heat-only Nuclear Concept

Reusing spent nuclear fuel

Zero or negative fuel cost

No new radioactive

waste

Saving uranium resources

Low temperature and pressure

Less thickness of the vessel

Higher safety

Low construction

cost

Modular and compact

Construction close to the

demand

Small footprint

Short construction

time

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Page 4: Nuclear Energy for District Cooling

• TEPLATOR Demo reactor is optimized to be fueled by 55 FAs from VVER-440, with thermal capacity of 50-150 MW.

• TEPLATOR solution is especially suitable for countries that have thousands FAs stored either in interim storage casks or spent fuel pools.

TEPLATOR – Fuel

GermanyCzech

RepublicSlovakia

Number

of FAs4,802 10,958 13,955

Total 29,715

10 TEPLATOR

Operation

55 years

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Page 5: Nuclear Energy for District Cooling

TEPLATOR – District Heating Competitivity

District Heating sources

Electric driven technologies

Electric boiler

Compression heat pump

Non-electric based heating

Fossil fuels Natural gas

CoalCHP

RenewableBiomass

Solar

GeothermalNuclear heat-

only

TEPLATORAbsorption heat

pump

8 (€/GJ)

11.4 (€/GJ)

4 (€/GJ)

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Page 6: Nuclear Energy for District Cooling

TEPLATOR –District Cooling ?

TEPLATOR Solution

Pollution Free Energy

&

Neglectable Electricity consumption

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Page 7: Nuclear Energy for District Cooling

TEPLATOR – District Cooling SolutionElectric Driven Cooling

Systems

❖Thermal energy from burning the fuel is converted to electricity in the power plants.

❖The electricity is transmitted through HV/MV/LV grids to the cooling plants or to the consumers.

❖High investments for the expansion of power grid will be necessary due to rapid growth of cooling demand.

❖Pollution emissions will be increased rapidly.

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Page 8: Nuclear Energy for District Cooling

TEPLATOR – District Cooling Feasibility

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Page 9: Nuclear Energy for District Cooling

TEPLATOR – District Cooling Feasibility: Cooling & Heating Demand Model

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Page 10: Nuclear Energy for District Cooling

TEPLATOR – District Cooling Feasibility: Scenarios

Energy SourceDistrict Cooling

System

Scenario 1 Coal Power Plant Electric Driven DCS

Scenario 2 Internal Combustion Power Plant Electric Driven DCS

Scenario 3 Nuclear Power Plant Electric Driven DCS

Scenario 4 Combined Cycle PP with 90% carbon capture Electric Driven DCS

Scenario 5 Heating Plant (TEPLATOR) Heat Driven DCS

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Page 11: Nuclear Energy for District Cooling

TEPLATOR – District Cooling Feasibility: Costs

TEPLATOR District Cooling

Electrical District Cooling

TEPLATOR construction

cost

TEPLATOR Fuel Cost

TEPLATOR O&M Cost

Heat Transmission

Cost

Absorption Cooling Plant Construction

Cost

Absorption Cooling Plant

O&M Cost

Power Plant construction

cost

Power Plant Fuel Cost

Power Plant O&M Cost

Electricity T&D Cost

Compression Cooling Plant Construction

Cost

Compression Cooling Plant

O&M Cost

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Page 12: Nuclear Energy for District Cooling

Strategy 1:Coal Power

Plant

Strategy 1:Internal

CombustionPower Plant

Strategy 1:Nuclear Power

Plant

Strategy 1:Combined

Cycle PowerPlant

Strategy 2:TEPLATOR

Levelized cost of primary energygeneration per MWh cooling demand

($/MWh)21.35 18.17 28.52 18.68 10.44

Levelized cost of primary energytransmission per MWh cooling

demand ($/MWh)12.94 12.94 12.94 12.94 7.64

Levelized cost of DCP per one MWhcooling demand ($/MWh)

15.23 15.23 15.23 15.23 14.02

Levelized cost of cooling energydelivered to district distribution

piping network ($/MWh)49.53 46.35 56.7 46.86 32.1

0102030405060

$/M

Wh

TEPLATOR – District Cooling Feasibility: Results

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Page 13: Nuclear Energy for District Cooling

0

0.5

1

1.5

2

2.5

Coal Power

Plant

Internal

Combustion

Power Plant

Nuclear Power

Plant

Combined

Cycle Power

Plant

TEPLATOR

0.80.44

0

0.04

0

2.42

1.32

0

0.11

0

Ca

rbo

n e

mis

sio

ns

ton

/MW

h

Annual Carbon Emission ton/MWt.h cooling Annual Carbon Emission ton/MWt.h heating

TEPLATOR – District Cooling Feasibility: Results

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Page 14: Nuclear Energy for District Cooling

Annual energydemand (TWt.h)

Annual electricitygeneration - Strategy

1 (TWe.h)

Annual heatgeneration - Strategy

2 (TWt.h)

Total 3.53 1.39 5.68

Heating 0.31 0.35 0.38

Cooling 3.22 1.04 5.30

0.00

2.00

4.00

6.00

8.00

10.00

12.00TW

h

TEPLATOR – District Cooling Feasibility: Costs

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Page 15: Nuclear Energy for District Cooling

Conclusions

❖ Heat driven district cooling/heating systems where the carbon-free heat sources are utilized, are capable to provide:

✓ Economic solution for serving the increasing cooling/heating demand.

✓ Elimination of the unwanted costly energy conversion steps.

✓ Minimization the power system expansion and operation costs.

✓ Fulfilling the pollution reduction targets.

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Page 16: Nuclear Energy for District Cooling

Thank you for your attention