Lecture #8 Batteries and thermal energy storage

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1 Lecture #8 Batteries and thermal energy storage PHYS-E0483_ Peter Lund

2 Contents Lecture # 8 Basic principles of batteries Li-ion battery Comparison of battery technologies Application Thermal storage principles Advanced thermal storage Large-scale applications

3 Main components of a battery Anode (negative electrode) Cathode (positive electrode) Electrolyte (ionic conductor) Anions (negative ions) Cations (positive ions) Slides 3-14 from D. Linden: Handbook of Batteries, 2 nd Edition, 1995

4 Operating principle of a battery Charging/discharging of a battery; reversed current flows Example Zn/Cl 2 cell negative electrode (oxidation): Znà Zn 2+ +2e - positive electrode (reduction): Cl 2 +2e - à 2Cl - overall reaction (discharge): Zn+Cl 2 à Zn 2+ +2Cl - (ZnCl 2) negative electrode (reduction): Zn 2+ +2e - à Zn positive electrode (oxidation): 2Cl - à Cl 2 +2e - overall reaction (charge): Zn 2+ +2Cl - à Zn+Cl 2

5 Important battery parameters (1) Theoretical voltage, capacity, energy density Free energy change in the reaction ΔG = n F E 0 n=electrons involved in the reaction F= Faradays constant (26.8 Ah) E 0 = standard cell potential (V) Standard cell potential = anode (ox. potential) +cathode (red. potential) From table (à) Reaction Zn+Cl 2 à ZnCl 2 Znà Zn 2+ +2e - -(-0.76V) Cl 2 +2e - à 2Cl V = 2.12 V

6 Important battery parameters (2) Theoretical voltage, capacity, energy density Capacity = total amount of electricity involved in the electrochemical reactions Theoretical max. : 1gram of material = 26.8 Ah/g Energy density = Theoretical Wh x capacity/ weigth ZnCl 2 battery system: 1.22 g/ah g/ah = 2.54 g/ah= Ah/g 2.12 V x Ah/g = Wh/g = kwh/kg

7 Parameters for major battery systems

8 Performance characterization of major battery systems (primary and secondary batteries)

9 Electrochemical principles of a battery Theore&cal values drop because of inideali&es, e.g. charge transfer limita&ons, contact resistance, etc = Polariza(on effects

10 A battery at equilibrium (E 0 ) One electrode reac,on (forward=reduc,on) aa+ne cc One electrode reac,on (forward=oxida,on) bb-ne dd Total aa+bb cc+dd Free energy change for this reaction ΔG = - n F E 0 Nernst equation for non-standard conditions

11 A battery at non-equilbrium During opera,on current I> 0 à voltage losses (electrode reac,os, charge transport etc) à electrode polariza,on (so-called polariza,on) η ; E =E-η a,b are bakery specific parameters (see Fig) Tafel-equa&on

12 A battery in practice Characterzing bakery discharging/charging by the C-rate: amount of current a bakery delivers when discharged in one hour to the point of 100% depth of discharge I = M x C n ; I (A) = C n (Ah)/1 (h), C n = rated bakery capacity, n=,me based in hours for which the rated capacity is declared, M=mul,ple frac,on of C C/10 discharge rate, e.g. if 10 Ah bakery à I = 1 A for 10 hours C/5 discharge rate, e.g. if 10 Ah bakery à I = 2 A for 5 hours Resistance increases when discharging/charging due to accumula,on of reac,on products, ac,va,on, concentra,on etc. à effec,ve capacity drops

13 Li-ion battery Octavio Salazar: Li-Ion Battery Model

14 Improved Li-ion battery performance through nanocrystals Recent interest in Li 4 Ti 5 O 12 nanocrystals for anodes Accommodation of strain of Li+insertion/ extraction Higher electrode/electrolyte area allows higher charge/discharge rate Short path lengths for electronic transport Short path length for Li+transport Less reactive as bulkli 0.5 CoO 2 +

15 Battery comparison Octavio Salazar: Li-Ion Battery Model

16 Li-ion battery performance Battery performance is temperature dependent, in particular in at low temperatures (up to 50% of capacity lost at -20 C)

17 Flow battery Vanadium redox flow battery Vanadium in 4 different oxidation states Pos. eletrocde: VO 2+ +H 2 O-e - VO H + Neg. eletrocde: V 3+ +e - V 2+ 2 electrolytes in tanks separated by a membrane Wh/L 1 kwh-10 MWh Pilot stage Zinc Bromine flow battery

18 Aluminium-air-battery Al+ alkaline solution+air electrode Al Al 3+ +3e - hydrophobic layer (carbon+pt+ptfe): 2H O 2 + 4e - OH - e - air Anode : 4 (Al+4OH - Al(OH) e- ) Cathode: 3 (O 2 +2H 2 0+4e - 4OH - ) Al Electrolyte: 4 (Al(OH) - 4 Al(OH) 3 + OH- ) total: 4 Al(s) + 6H 2 0(l) + 3O 2 (g) 4Al(OH) 3 (s) Hydrophilic layer Hydrophobic layer 400 Wh/kg, 175 W/kg

19 Battery characteristics PHYS-E0483_ Peter Lund 2015

20 Batteries vs applications vs other storage types PHYS-E0483_ Peter Lund

21 Li-ion battery costs and targets PHYS-E0483_ Peter Lund 2015

22 PHYS-E0483_ Peter Lund 2015

23 Effect on LCOE Battery may increase LCOE with /MWh (past) à in future PHYS-E0483_ Peter Lund 2015

24 PV-EV [Tesla]

25 PV & Tesla battery Hours when PV NOT meeting supply (black) Case Finland: 3 kwp PV for a household (100%) PV not battery PV + 1 Tesla batt. PV + 2 Tesla batt Tammikuu Direct use of PV Heinäkuu 32% 74% 76%

26 Thermal energy storage

27 Sensible thermal storage Q= c p Δ T, where c p =thermal capacitance (kj/kgk) water, rock, ceramics; capacity kwh/m 3 (H 2 O 1.17 kwh/m 3 /K large scale storage 10, ,000 m 3 (steel tanks, subsurface) case OULU: 200,000 m 3 rock cavern water storage, 2-4 bar, o C, 100 MW/10 GWh load levelling, optimal operating strategy heat elec CHP storage Peak boiler

28 Micro-CHP thermal storage (e.g. CHP-DESS)

29 Large-scale water storage

30 Advanced thermal storage - introduction Phase change thermal energy storage phase change absorbs/releases heat (e.g. between solid and liquid) phase change enthalpy ΔH and phase change temperature inorganic salts Na 2 SO 4 x 10 H 2 O (251 kj/kg, 24 C), NaOH x 3.5H 2 0 (272 kj/kg, 64 C) fatty acids (paraffin, stearic acid, ca o C, kj/kg) small scale (up to a few m 3 ) Thermochemical heat storage sorption processes XY+heat X + Y Y=working medium (water, NH 3, ROH, SO 2, SO 3, CO 2, H 2, O 2 ) X=absorbent (e.g. Me, silica gel) storage capacity kwh/m 3 (th), kwh/m 3 (pr)

31 Phase change heat storage heat

32

33 Chemical thermal storage Principles: 1) chemical reactions without sorption, 2) sorption Heat of sorption/ desorption: Wh/kg

34 Classifiction

35 Energy storage densities for sorption storage Water as sorbate, Wh/kg

36 Solid adsorption (silica gel/water) <100 kwh/m3

37 Working principle of thermochemical storage

38 Thermodynamics of thermochemical storage Vapour pressure: sorbent/sorbate

39 Thermochemical heat distribution DH= water in pipe, heat loss & capacity limitiation Chemical DH = thermochemical routes, gas in pipes CH 3 OH +heat CO+H 2 minor losses, high energy density

40 Hydrogen energy storage

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