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Basic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger-Wilckens Centre for Hydogen & Fuel Cell Research University of Birmingham 2 nd Joint European Summer School on Fuel Cell and Hydrogen Technology Crete, 17 th – 28 th Sept. 2012

Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

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Page 1: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Basic Thermodynamics and System Analysis for Fuel Cells

Prof. Dr. Robert Steinberger-Wilckens Centre for Hydogen & Fuel Cell Research University of Birmingham

2nd Joint European Summer School on Fuel Cell and Hydrogen Technology Crete, 17th – 28th Sept. 2012

Page 2: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 2/61 JESS 2 / 2012

Overview

• Basics of Thermodynamics

• Thermodynamics applied to fuel cells and electrolysis

• System analysis

Page 3: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 3/61 JESS 2 / 2012

A very brief Introduction to Thermodynamics

Page 4: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 4/61 JESS 2 / 2012

The Model Thermodynamic World

Consider a volume and ist boundary:

It has a given state of being, quantified by the ‚inner energy state‘ U.

It exchanges activities with the surroundings by transporting mass and energy across the boundary.

U

system variables: T temperature p pressure V volume m mass Q, W T, p, V, m

Page 5: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 5/61 JESS 2 / 2012

Example Representation

Ideal gas law:

p V = n R T

U

system variables: T temperature p pressure V volume m mass Q, W T, p, V, m

piston intake/release valves

V

Page 6: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 6/61 JESS 2 / 2012

The 4 Laws of Thermodynamics

1. Existance of temperature („0th“ Law)

2. Conservation of energy (1st Law)

3. Definition of Entropy (2nd Law)

4. Entropy at T = 0 (3rd Law)

Page 7: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 7/61 JESS 2 / 2012

1st Law of Thermodynamics

Any change of inner energy U is balanced by the exchange of heat Q and work W

U = Q + W

or rather

dU = dQ + dW

Consequences:

- conservation of energy, d U = 0 in isolated system

- impossibility of perpetuum mobile of the first kind (delivering work)

Page 8: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 8/61 JESS 2 / 2012

Steady State and Transitions

Strictly speaking, all thermodynamic laws are only valid in the steady state (equilibrium).

A transition from one state to another must therefore be calculated in infinitesimal steps. These are assumed to be in balance. Between two states at times t1 and t2 going through a transition, a process takes place. If the process can be reversed and the state at t1 be achieved again, the process is reversible.

Page 9: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 9/61 JESS 2 / 2012

2nd Law of Thermodynamics

Every system possesses a property S (entropy) that can be calculated from

d S = d Q / T

In irreversible processes d S ≥ d Q / T

Consequences:

- creation of entropy,

- impossibility of perpetuum mobile of the second kind (converting heat to work)

Page 10: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 10/61 JESS 2 / 2012

1st + 2nd Law of Thermodynamics

Combining we get

d U = d W + d S · T

or

d W = d U - d S · T

or

ΔH = ΔG + T ΔS

ΔG = ΔH - T ΔS

with H …. ‚enthalpy‘ G …. ‚free enthalpy‘ or ‚Gibb‘s energy‘

Page 11: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 11/61 JESS 2 / 2012

Thermodynamic Machines

The relevant thermodynamic processes can mostly be considered as circular processes or ‚machines‘.

p

V

A

B

C

D

S

T

A

B

C

D

Page 12: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 12/61 JESS 2 / 2012

The Carnot Machine: Volume Reaction

1. isothermal compression 2. adiabatic compression 3. isothermal expansion 4. adiabatic expansion

Page 13: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 13/61 JESS 2 / 2012

The Carnot Machine (2)

heat source T1

heat sink T2

work

Q1

Q2

efficiency: ηc = W / Q1

from Q1 - Q2 - W = 0 (1st Law) and dS = dQ / T (2nd Law) it follows that ηc = 1- T2 / T1

Page 14: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 14/61 JESS 2 / 2012

Ele

ctro

lyte

porous anode

porous cathode

O2 (air)

Surplus air

H+

Fuel Cell Principle: Surface Reaction

+ H2O

H2

Surplus fuel

Page 15: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 15/61 JESS 2 / 2012

Hydrogen Production: Electrolysis Splitting of water by electric current

Question: Definition of ‚cathode‘ and ‚anode‘?

Cathode side 2H2O + 2e- H2 + 2OH-

Anode side 2OH- 1/2 O2 + H2O + 2e-

Overall reaction H2O H2 + 1/2 O2

F ... Faraday constant = 96.587 C/mol

2F

Page 16: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 16/61 JESS 2 / 2012

Electrolysis Thermodynamics

Free enthalpy ΔGo = 237 kJ/mol (at 25°C, 1 bar = ‚standard‘ conditions) = 2F Uo

o It follows that Uo

o = 1,23 V which is the voltage necessary for water splitting (ideal case at standard conditions).

2F H2O -----> H2 + 1/2 O2

Page 17: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 17/61 JESS 2 / 2012

Electrolysis Overpotential

Due to kinetic processes and competition of ion reactions at the electrodes the technically necessary Voltage for electrolysis is considerably higher, generally at the order of 1,7 to 1,9 V. The ideal amount of energy needed per Nm³ H2 is ΔGo / VN = 237 kJ/mol / 22,41 l/mol = 3 kWh/Nm³ Standard electrolysers require about 4,2 to 4,8 kWh/Nm³

Question: lower or higher heating value? (LHV or HHV)

Page 18: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 18/61 JESS 2 / 2012

Electrolysis Temperature Dependency

Due to the relationship Δ Go = Δ Ho - T ΔS The energy for splitting water can also be supplied by heat, not only electricity.

Graphics from Winter/Nitsch,1988

Page 19: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 19/61 JESS 2 / 2012

Gibbs free energy for H2 - O2 reaction Form of water product Temperature [°C] G [kJ/mol] Liquid 25 -237,2 Liquid 80 -228,2 Gas 80 -226,1 Gas 100 -225,2 Gas 200 -220,4 Gas 400 -210,3 Gas 1000 -177,4

Uo [V] 1,23 1,18 1,17 1,14 1,09 0,92

Other fuels Temperature [°C] G [kJ/mol]

Methanol 25 -698,2 Methane 25 -802,7 Alkali (battery) 25 -277

Uo [V] 1,21 1,04 1,44

Page 20: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 20/61 JESS 2 / 2012

Generating Entropy? Loosing Energy?

T = 0 ΔH = ΔG

T > 0 ΔH = ΔG + TΔS vibrational energy

consequence: - less energy needed for electrolysis - less energy reclaimed in fuel cell

Page 21: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 21/61 JESS 2 / 2012

Electrode Definition

Electrolysis

+ - e- e

-

2 H2O 2 OH- 1/2 H2

O2

- + e- e

-

H2O 2 OH-

H2 1/2 O2

Fuel Cell (=battery!)

Where are cathode and anode?

reverse reaction:

Page 22: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 22/61 JESS 2 / 2012

Reaction Equilibrium: Fuel Cell Case

Cathode side

H2 + 2 OH- 2 H2O + 2e- Anode side

1/2 O2 + H2O + 2e- 2 OH-

Overall reaction H2 + 1/2 O2 H2O

Uo (open circuit) is identical to that of electrolysis (but negative!) ΔGo = 2F Uo

o = -237 kJ/mol (at STP, for H2 - O2 cell) Uo

o = 1,23 V (for convenience, U is not marked as negative) i.e. energy is released.

Page 23: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 23/61 JESS 2 / 2012

Schematic Voltage Characteristics: Electrolysis and Fuel Cell

Uoo (T)

I [A]

U [V]

I * Ri

I * Ri

I * Re

electrolysis

fuel cell

internal resistance due to non-ideal conductibility resulting in heat produced a.o.

work delivered to external circuit

Page 24: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 24/61 JESS 2 / 2012

Fuel Cell Efficiency

1. Efficiency = useful output / total input

η = Qel / - ΔH

2. Ambiguity: HHV or LHV?

3. Maximum possible efficiency (thermodynamic efficiency)

η = ΔG / ΔH

assuming that all change in Gibbs free energy can be transformed to electricity

alternative: η = U / Uoo (since U = - ΔH / 2F)

Compare to Carnot efficiency (T1 - T2) / T1 (T1,2 in [K]) and Betz efficiency (58%)

Page 25: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 25/61 JESS 2 / 2012

Maximum Efficiency as Function of Temperature

Form of Temperature [°C] G [kJ/mol] water product Liquid 25 -237,2 Liquid 80 -228,2 Gas 80 -226,1 Gas 100 -225,2 Gas 200 -220,4 Gas 400 -210,3 Gas 1000 -177,4

Uo [V] η 1,23 83% 1,18 80% 1,17 79% 1,14 77% 1,09 74% 0,92 62%

Page 26: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 26/61 JESS 2 / 2012

Some Fuel Cell Principal Properties

1. not limited by Carnot efficiency (~ (T1-T2)/T1), only by electrochemical, kinetic and ohmic losses

2. modular 3. low noise 4. exhaust emission predominantely water (and maybe CO2) 5. no moving parts

ergo: • efficient and low-emission energy conversion technology

Page 27: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 27/61 JESS 2 / 2012

00,10,20,30,40,50,60,70,80,9

1

373

573

773

973

1173

1373

1573

1773

1973

T1 [K]

eta

Increasing Efficiencies

lim T1 -> ∞

lim T2 -> 0

0

0,1

0,2

0,3

0,4

0,5

0,6

0,7

0,8

0,9

0,6 0,65 0,7 0,75 0,8 0,85 0,9 0,95 1

U(jo)

eta

lim U -> Uoo

ηc = 1- T2 / T1

T2 = 273 K

Page 28: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 28/61 JESS 2 / 2012

High Efficiency Electricity Production

Power Plant Capacity / MW

20

30

40

50

60

70

10005001005010510,50 ,10

10

Efficiency /%

G asturb ine

G U D - P ow er P lant

D iesel E ngine

Upper Limiting Curve: Future Technology.(Development tendency: GT / GUD: 2000 ; SOFC: 2010).Lower Limiting Curve: Actual Technology.

Steam Power P lant

S pa rk-Ign itionE ng ine

S O FC

P A FC

Fuel Cells

Page 29: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 29/61 JESS 2 / 2012

An Introduction to Energy and Efficiency

Page 30: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 30/61 JESS 2 / 2012

Overview of Indicators • Efficiency * of a single process * of a process chain * of energy services

• Primary energy consumption * direct * cumulative energy

• Fossil energy consumption

• Direct emissions

• Direct & indirect emissions (LCA)

• Energy payback (harvest factor)

• Externalities

Page 31: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 31/61 JESS 2 / 2012

Energy Efficiency Definitions

conventional: energy input given as lower heating value (LHV) result (example): out of 1 Nm³ of natural gas equivalent to 10 kWh, 1 kWh is disregarded reason: 10% of the combustion energy is contained in the exhaust gas as water vapour and not sensible heat is calculated approx. 10% higher than corresponds to the factual chemical energy content of the fuel

= (desired) energy output / (necessary) energy input

Page 32: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 32/61 JESS 2 / 2012

Energy Efficiency Definitions /2

= energy output / energy input (HHV)

correct (but unconventional): energy input given by higher heating value (HHV) corresponds to the factual chemical energy content of the fuel and gives the full picture of the conversion technology

Page 33: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 33/61 JESS 2 / 2012

Efficiency and Efficiency Chains PE primary energy UE useful energy CO combustion

CO

NOx CO2

LHV = 0,90 UE (heat)

1 PE

Conventional boiler

Condensing boiler

HHV = 0,81 UE (heat)

CO

CO2

1 PE

LHV = 1,05 UE (heat)

HHV = 0,95 UE (heat)

therm = 105 % LHV

therm = 95 % HHV

Page 34: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 34/61 JESS 2 / 2012

Efficiency and Efficiency Chains /2 PE primary energy UE useful energy EG electricity generation

EG

NOx CO2

0,33 UE 1 PE

Coal or Nuclear power plant

EG

NOx CO2

0,42 UE 1 PE

Combined Cycle power plant

EG 1 UE ( = 1 PE)

Renewable Energy power plant

Page 35: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 35/61 JESS 2 / 2012

Efficiency and Efficiency Chains /3 PE primary energy UE useful energy EG electricity generation

EG

NOx CO2

0,33 UE 1 PE

Average German Electricity Grid

CHP

NOx CO2

0,3 UE electricity 1 PE

Gas Engine CHP 0,6 UE heat 0,7 PE

0,91 PE

reference case

∑= 1,61 PE

condensing boiler

electricity grid

Page 36: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 36/61 JESS 2 / 2012

FC FP

CO2

η = 0,87 η = 0,85 1 PE

H2O

Natural Gas PEFC Residential System

PE primary energy UE useful energy FC fuel cell FP fuel processing

FC η = 0,80

1 PE

H2O

Natural Gas SOFC Residential System

0,50 UE electricity

0,33 UE heat

CO2

0,34 UE electricity

0,41 UE heat 0,43 PE

1,03 PE

Efficiency and Efficiency Chains /4

reference case

∑ = 1,46 PE

cond. boiler

electricity grid

0,35 PE

1,51 PE

reference case

∑ = 1,86 PE

cond. boiler

electricity grid

Page 37: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 37/61 JESS 2 / 2012

Efficiency and Efficiency Chains /5

FC 1 PE ηel = 0,45

H2O

0,27 UE FP ELY η = 0,67

O2

FC

Hydrogen Fuel cell, wind energy

EG

CO2

ηel = 0,45 η = 0,35

FP

η = 0,85 (CH)

ELY η = 0,67

O2

1 PE η = 0,85 (CH)

H2O

Hydrogen Fuel cell, grid electricity

PE primary energy UE useful energy EG electricity generation FP fuel processing CH compressed hydrogen

NOx

0,08 UE

Page 38: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 38/61 JESS 2 / 2012

Efficiency and Efficiency Chains /6

ICE

CO2

Internal combustion motor η = 0,15

FP η = 0,9

1 PE

NOx CO

0,13 UE (propulsion)

PE primary energy UE useful energy EG electricity generation ICE internal combustion engine FP fuel processing CH compressed H2 LH liquid H2

ICE EG

CO2

η = 0,15 η = 0,35 0,024 UE FP ELY

η = 0,67

O2

1 PE η = 0,85 (CH)

H2O

H2 Internal combustion motor, grid electricity

NOx NOx

η = 0,1 (LH) 0,004 UE

Page 39: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 39/61 JESS 2 / 2012

Efficiency and Efficiency Chains /7

FC 1 PE η = 0,40

H2O

0,23 UE FP ELY η = 0,67

O2

FC

H2 FC vehicle, wind energy

EG

CO2

η = 0,40 η = 0,35

NOx

0,08 UE FP

η = 0,85 (CH)

ELY η = 0,67

O2

1 PE η = 0,85 (CH)

H2O

H2 FC vehicle, grid electricity

PE primary energy UE useful energy EG electricity generation FC fuel cell FP fuel processing CH compressed H2

Page 40: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 40/61 JESS 2 / 2012

Efficiency and Efficiency Chains PE primary energy UE useful energy EG electricity generation FP fuel processing ICE internal combustion engine

EG

NOx CO2

0,33 UE 1 PE

Coal or Nuclear power plant + grid

ICE

CO2

Internal combustion engine η = 0,15

FP η = 0,9

1 PE

NOx CO

0,13 UE (propulsion)

Page 41: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 41/61 JESS 2 / 2012

Combined Heat and Power (CHP)

Condensing boiler

Electricity grid

Water supply

Natural gas

Fuel Cell (CHP)

Hot water storage tank use of waste heat from

electricity generation for heating purposes etc.

Page 42: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 42/61 JESS 2 / 2012

SenerTec ‚Dachs‘ Hot water storage and buffer

photographs courtesy SenerTec

Page 43: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 43/61 JESS 2 / 2012

Micro-CHP – Stirling engine

graphics courtesy KWB

gearbox

heater

cooling

cylinder

insulation

Page 44: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 44/61 JESS 2 / 2012

Efficiency and Efficiency Chains /2 PE primary energy UE useful energy EG electricity generation

CHP

NOx CO2

0,3 UE electricity 1 PE

Gas Engine CHP

0,6 UE heat 0,7 PE

0,91 PE

reference case

∑= 1,61 PE

condensing boiler

electricity grid

FC η = 0,83

1 PE

H2O

Natural Gas SOFC Residential System

0,50 UE electricity

0,33 UE heat

CO2

0,35 PE

1,51 PE

reference case

∑ = 1,86 PE

cond. boiler

electricity grid

η = 0,90

Page 45: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 45/61 JESS 2 / 2012

CHP Unit Efficiencies

25%

30%

35%

40%

45%

50%

55%

60%

65%

70%

0 2 4 6 8 10 12 14 16Electrical power output [MWe]

Elec

trica

l the

rmal

effi

cien

cy

graph courtesy of RollsRoyce FCS

300 MW

Page 46: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 46/61 JESS 2 / 2012

Efficiency and Efficiency Chains /3

FC 1 PE η = 0,40

H2O

0,23 UE FP ELY η = 0,67

O2

FC

H2 FC vehicle, wind energy

EG

CO2

η = 0,40 η = 0,35

NOx

0,08 UE FP

η = 0,85 (CH)

ELY η = 0,67

O2

1 PE η = 0,85 (CH)

H2O

H2 FC vehicle, grid electricity

PE primary energy UE useful energy EG electricity generation FC fuel cell FP fuel processing CH compressed H2

Page 47: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 47/61 JESS 2 / 2012

Vehicle Requirement Profile

New European Driving Cycle example

source: EU

Page 48: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 48/61 JESS 2 / 2012

CUTE Results: Total system efficiency

source: CUTE

Page 49: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 49/61 JESS 2 / 2012

Change in On-Board E-Power Generation

100% 20 – 25%* 50 – 70% (Generator) 70 – 90 % (KSG)

10 – 17% 14 – 22 %

Today:

* Average efficiency

Future:

100% 35 – 50% 35 – 50% (FC-APU) Graph: BMW

Page 50: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 50/61 JESS 2 / 2012

Cumulative Energy: Definitions

b = total chain energy efficiency = (end) energy output / (primary) energy input ‚Energy input‘ includes all input, i.e. not only for operating the system, but also for building it. EF = energy harvest factor = energy output / fossil energy input

Page 51: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 51/61 JESS 2 / 2012

Cumulative Energy: NG Steam Reforming primary energy

natural gas supply

production appliances NatGas

steam reforming

appliances, transport

national distribution

b = UE / Σ E input

source: FfE

Page 52: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 52/61 JESS 2 / 2012

Cumulative Energy: PV-Hydrogen production

insolation PV panels

PV Africa

electricity appliances, demin water

electrolysis

appliances

pipeline transport

appliances, transport

national distribution

source: FfE

Page 53: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 53/61 JESS 2 / 2012

LCA Elements

Definition of boundaries

Page 54: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 54/61 JESS 2 / 2012

LCA Procedure

• Analysis of all process steps involved • Cumulation of all specific emission and impact factors, i.e. kg CO2 / kWh energy kg CO2 / kg of building material kg SO2 / kWh energy etc. Detail given by inclusion or omission of secondary, tertiary etc. sources (system boundary).

Goal: Comparison of base case with alternative variants

Page 55: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 55/61 JESS 2 / 2012

Well-to-Wheel Analysis (1)

FC vehicle, various hydrogen production paths, base case: Diesel

CO2 equiv. per 100 km

0

100

200

300

400

500

600

700

Referenz:Diesel

1. Methanol-Rreformierung

2. Erdgas-Reformierung

3. Netzstrom 4. Wind Energie 5. Grüner Strom 6. Wasserkraft

[kg C

O2 e

q. /

100

km

]

FahrzeugTreibstoffVehicle Fuel

1. MeOH reforming 2. NG reforming 3. Grid electr. 4. Wind energy 5. Green electr. 6. Hydro

Page 56: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 56/61 JESS 2 / 2012

Well-to-Wheel Analysis (2)

FC vehicle, various hydrogen production paths, base case: Diesel

Fossil fraction of energy

0%

20%

40%

60%

80%

100%

Referenz: Diesel 1. Methanol-Rreformierung

2. Erdgas-Reformierung

3. Netzstrom 4. Wind Energie 5. Grüner Strom 6. Wasserkraft

Fossiler Anteil Erneuerbarer Anteilfossil fraction renewable fraction

1. MeOH reforming 2. NG reforming 3. Grid electr. 4. Wind energy 5. Green electr. 6. Hydro

Page 57: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 57/61 JESS 2 / 2012

Total Balance of Conversion: kg CO2 / kWh

kg CO2 / kWh NG producing • electricity and • heat

kg CO2 / kWh electricity from grid

kg CO2 / kWh conventional heating

kg CO2 / kWh balance

alternative

reference

biogas X example: natural gas drivenCHP unit (engine or fuel cell)

Page 58: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 58/61 JESS 2 / 2012

Internal versus External Costs examples for vehicle traffic

Internal costs: • costs of production and delivery of vehicles and fuels • taxes and levys • market price (as a sum of the above plus company profit)

External costs • costs caused for the society, but not attributed or attributable to single products or services • health services due to environmental pollution • health and other services due to noise pollution • public services in safety, accident prevention etc. • general costs of land use, rain run-off management etc.

Page 59: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 59/61 JESS 2 / 2012

Including External Costs

H2

Diesel 3:1

ext. costs

ext. costs

3:2 Internal costs /

market price

17,47 €

5,12 €

Page 60: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 60/61 JESS 2 / 2012

External Costs of Electricity Generation

source: DLR

Page 61: Basic Thermodynamics and System Analysis for Fuel · PDF fileBasic Thermodynamics and System Analysis for Fuel Cells Prof. Dr. Robert Steinberger -Wilckens Centre for Hydogen & Fuel

Thermodynamics & System Analysis Slide 61/61 JESS 2 / 2012

Thanks for your Attention!

Any Questions?