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1 Carbon Dioxide Zero-Emission Hydrogen System based on Nuclear Power Yukitaka Kato Research Laboratory for Nuclear Reactors Tokyo Institute of Technology Paper #51, 2B2 Innovative Energy Transmutation COE-INES International Symposium, INES-1 1 November, 2004, Tokyo, Japan

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Page 1: Carbon Dioxide Zero-Emission Hydrogen System based on … · hydrogen career system Power plant Power plant output GW 1 Night time operation durationh8 Total Electricity amount GWh

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Carbon Dioxide Zero-Emission Hydrogen System based on Nuclear Power

Yukitaka KatoResearch Laboratory for Nuclear ReactorsTokyo Institute of Technology

Paper #51, 2B2 Innovative Energy TransmutationCOE-INES International Symposium, INES-11 November, 2004, Tokyo, Japan

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Y. Kato, Tokyo Tech

Contents

Back ground: Hydrogen supply for fuel cell vehiclesCO2 zero-emission hydrogen career system using a regenerative reformerExperimental demonstrationEvaluation of the hydrogen career system

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Y. Kato, Tokyo Tech

Hydrogen for FC-A fuel cell is environmental friendly?-

H2Hydrogen

source

1st Energyinput

Problems of H2 supply to a conventional fuel cell vehicleCompressed H2 fuel : high-energy consumptions for production and pressurization, and explosiveness

2nd Energyinput

Explosiveness of H2

H2 cylinder Fuel cell

H2OCompressed

H2

Fig. Subjects for hydrogen supply to a fuel cell vehicle

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Y. Kato, Tokyo Tech

Fuel reforming for hydrogen supply to a fuel cell vehicle

Problems of H2 supply to a conventional fuel cell vehicleFuel Reforming: complex structure, and CO2 emission

Fig. Conventional reforming system for a FC vehicle

CO2, H2

Cat.CH4H2O Reformer Shift

Converter

Cat.Fuel cell

CO2, H2O

Heat input Heat output

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Y. Kato, Tokyo Tech

Regenerative Reforming-Use of chemical absorption-

Fuel reforming for methaneCH4+H2O ↔3H2 +CO, ∆H°1=+205.6 kJ/mol

CO+H2O ↔H2 +CO2, ∆H°2=−41.1kJ/mol

CaO carbonationCaO(s)+CO2(g)↔CaCO3(s),

∆H°3= −178.3 kJ/mol

Regenerative reforming(CO2 absorption reforming, self-heating)

CaO(s)+CH4(g)+2H2O(g)↔4H2(g)+CaCO3(s),∆H°4=−13.3 kJ/mol

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Y. Kato, Tokyo Tech

Non-equilibrium reaction for hydrogen production

Based on fuel reformingSeparation processes for non-equilibrium reforming

Separating CO2 from system using chemical absorptionMerit of non-equilibrium reforming

Enhancement of hydrogen productionUse of exothermic reaction heat for endothermic reformingDrop in reforming temperature

CH4 steam reforming: 700oC -> 500oCEnhancement of high-carbon numbers reactant reforming

Kerosene, C2H5OH and higher hydrocarbonReuse of carbon dioxide

CO2 zero-emission system

Link with nuclear power system

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Y. Kato, Tokyo Tech

CO2 zero-emission FC vehicle using the regenerative reformer

Regenerative reformingCO2 recoverable, self heating, and simple reforming systemthermally regenerative

CO2 zero-emission FC vehicleSafety H2 carrier system

under low-pressure and high-density

CaCO3, Cat. CO2

(2) CaO regeneration/CO2 recovery

CO2 recycleprocess

Surplus heat/electricity for thermal decarbonation

CaO, Cat.CH4H2O

H2

(1) CO2 absorption reforming

Fuel cellH2O

CO2 absorption reforming

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Y. Kato, Tokyo Tech

CO2 zero-emission hydrogen career system

CO2 Hydrogenation

Regeneration Station

CaO regenerator

CO2storage

•Electricity from nuclear power plants•Heat from high-temperature gas reactor(HTGR) and H. T. industries

Recycle

Fuel cell vehicles

CH4

Electrolysis of water H2

Hydrogen system driven by surplus electricity and heat from nuclear power plants, and unstable energy.Safe and compact hydrogen transportationCO2 zero emission energy system

CH4regenerator

Renewable energy system

Electricity/ Heat HTGR

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Y. Kato, Tokyo Tech

Experiment of the regenerative reformer

Demonstration of the possibility of the regenerative reforming systemFor polymer electrolyte fuel cell (PEFC) operated at a hydrogen pressure of less 0.3 MPa.

CH4

Ar

CO2

H2

(1)

(2)

(3)

(4)

(5) (6) (7)

(8)(9)

(10)

(11)

(12)

A quartz tube, 15 mm in inner diameter and an effective heating zone length of 600 mm.

(1) flow meter, (2) evaporator, (3) micro-feeder, (4) water reservoir, (5) electric furnace, (6) reactor tube, (7) reactor bed, (8) thermocouple, (9) furnace heating controller, (10) liquid-gas separator, (11) gas chromatograph, (12) soap flow meter

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Y. Kato, Tokyo Tech

CO2 absorption reforming

0

20

40

60

80

100

0 20 40 60 80 100 120 140

c [m

ol%

]

t [min]

CH4

H2

CO

CO2

Equilibrium H2 concentration of the conventional reforming

Equilibrium H2 concentration of the regenerativereforming

T=550oC

During the initial 60 min, hydrogen production was higher than the equilibrium concentration of conventional reforming. Charged CaO absorbed well CO2by carbonation. CO2 <1%CO was removed, <1%Low-temperature reforming (conventional reform. temp. > 700oC)

Al2O3 Ni cat+CaO Fig. Temporal change of effluent composition of the regenerative reformer at 550°C

(a) regenerative reformer (RGR)

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Y. Kato, Tokyo Tech

CO2 removal from reforming gas

0

5

10

15

20

500 550 600 650 700 750 800

c CO

2 [m

ol%

]

T [oC]

MeasuredEquilibrium

RGRSQRCVR

Effluent CO2 concentration from RGR at 550°C was less than 1%.

Fig. Effect of bed temperature on effluent carbon dioxide concentration of the reformer comparing with other type reformers.

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Y. Kato, Tokyo Tech

H2 productivity

65

70

75

80

85

90

95

100

500 550 600 650 700 750 800

c H2 [m

ol%

]

T [oC]

MeasuredEquilibrium

RGRSQRCVR

94% of H2production was measured by the RGR at 550°C.

Effect of bed temperature on hydrogen production concentration of the reformers.

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Y. Kato, Tokyo Tech

Estimation ofa zero emission vehicle1 kg of H2 in order to drive for 100 km7.46 kg (9.04 liters) of CaO was required for the RGR.

Viehcle mileage km 100Hydrogen requirement kg 1.0Hydrogen production conc mol% 94CaO requirement mass kg 7.94CaO requirement volume liter 9.62

Recovered CO2 kg 5.5

SSR-FC Vehic le

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Y. Kato, Tokyo Tech

Comparison between H2 systemsTable: Scale of energy storage facilities for 100 km mileage, 14.7 kWh, 500 mol-H2 (= Petroleum of 4 L, 2.8 kg)

7.9 L9.6 kg

400 kg100 kg

67 kg

25.6 L

0 50 100 150 200

volume [liter], mass [kg]

Regenerative reformer

Advanced lead-acid battery

Advanced Li-ion battery

Matal hydride, 1.5 wt%

Hydrogen cylinder, 70 Mpa mass [kg] volume [liter]

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Y. Kato, Tokyo Tech

Estimation of the zero-emission hydrogen career system

Power plantPower plant output GW 1Night time operation durationh 8Total Electricity amount GWh 8

GW 2.88E+04FC VehicleViehcle mileage km 100Hydrogen requirement kg 1Hydrogen production conc mol% 94CaO requirement mass kg 7.94CaO requirement volume liter 9.62CO2 kg 5.5CO2 mol 125dH for regeneration kJ/mol-CO2 178

Regeneration stationRequirement reaction heat kJ/piece 2.23E+04Cell piece pieces 1.29E+06CO2 amount kg 7.12E+06

m3(STP) 3.62E+06

Nighttime surplus electricity of 1 GW for 8 hours was used for the regeneration at the regeneration stations.The RGR packages of 1.3 million pieces/dayare able to be regenerated in the stations. CO2 of 7.1×103

ton/day is expected to be recovered from the stations.

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ConclusionsThe regenerative reformer was applicable to a practical CO2 zero-emission reforming with safety hydrogen supply.The required amount of CaO for the reformer was expected to be small enough comparing with other hydrogen storage system or batteries.The system can utilize surplus electricity generated from renewable energy system and nuclear power plant.Electricity of 1 GW for 8 h can regenerate 1.3 million of reforming packages, and recover 7.1 ton of CO2.The hydrogen career system using the regenerative reformer would widen need of those power plants because the system realizes new vehicle system of total CO2 zero-emission.The hydrogen career system also contributes to load leveling of power plant operation.

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Shifting into non-equilibrium by separation

Reforming+H2 separation

Nom-equilibrium

Reforming processes

Nom-equilibrium

(a) Conventional, non-treatment

(b) H2 separation

(c) CO2 separation

CnHmOk+bH2O hydrogen

source

H2, CO2, CO, others

Equilibrium mixture

Pure H2

Pure H2

Exhaust CO2

CO2 fixation

Fuel cell

Reforming+CO2 separation

Reforming

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Y. Kato, Tokyo Tech

Unstable Operation-Load leveling for Economical Plant Operation-

Load change and unstable operation

Low-annual operation rateUneconomic

Load leveling for 100% operation

Energy storageEnergy conversion

Unstable &UneconomicalRegion

Fig. A daily load change in a summer day in JapanTokyo Electric Power Co. http://www.tepco.co.jp/

Peak Electric Load (2001)Japan=181 GWTokyo area=64 GW (24 Jul.), 51 GW (15 Jan.)

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Y. Kato, Tokyo Tech

Diversification of energy supply and demand

DemandSupply

Stable StablePresent

Future Storage

Daily and Seasonal change

Instable

Fig. Forecast of the change of energy flow pattern

Decentralization/ Renewable energy

Diversified

Future society needs high-efficient tech. of,Energy storageEnergy transportationEnergy conversion

Use of chemicalreaction

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0

5

10

15

20

25

0

20

40

60

80

100

0 50 100 150 200 250

c i [m

ol%

]

c H2

[mol

%]

t [min]

CO

CO2

CH4

H2

Pre-breakthrough Post-breakthrough

T=550oCfCH4=106Nml/min

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0

20

40

60

80

100

500o C

pre

550o C

pre

600o C

pre

500o C

pos

t

550o C

pos

t

600o C

pos

t

COCH4

CO2

H2

c [m

ol%

]

fCH4=106Nml/min