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Thermal Energy Storage : Methods and Materials Thermal Energy Storage : Methods and Materials Dr. P. Muthukumar Associate Professor Department of Mechanical Engineering Indian Institute of Technology Guwahati Guwahati 781039 INDIA Guwahati - 781039, INDIA Email: [email protected] 1

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Page 1: Thermal Energy Storage : Methods and MateThermal …€¦ · Thermal Energy Storage : Methods and MateThermal Energy Storage : ... 8 Engg and 4 Science Departments About 6000 students,

Thermal Energy Storage : Methods and MaterialsThermal Energy Storage : Methods and Materials

Dr. P. MuthukumarAssociate Professor

Department of Mechanical EngineeringIndian Institute of Technology Guwahati

Guwahati 781039 INDIAGuwahati - 781039, INDIAEmail: [email protected] 1

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About IITGLocated in the Gateway ofLocated in the Gateway of North – Eastern Part of India

Started 1995, established during 2005.

Beautiful campus among other IITS. Located on the river bank on Brahmaputra. Campus is surrounded by many Hills and Lakes. y

Campus size about 700 acr.

8 Engg and 4 Science Departments

About 6000 students, 300 faculty and 500 supporting

IIT M

faculty and 500 supporting staffs

Over million migratory bi d ild t t

2

birds, wild cats, etc.

Dept. of Mechanical Engineering, Indian Institute of Technology Guwahati

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3

Dept. of Mechanical Engineering, Indian Institute of Technology Guwahati

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Out line of Presentation

TES concepts and methods

Types TES techniques

Steam accumulatorSteam accumulator

Reversible chemical heat storage (Metal hydride based thermal energy storage)

World wide status of TES systemsWorld wide status of TES systems

Proposed TES system for Solar PAN IIT

4

Dept. of Mechanical Engineering, Indian Institute of Technology Guwahati

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Thermal Storage Systems

Thermal energy storage (TES) systems correct the mismatch between the supply and demand of energy.

Types : Sensible, Latent and Reversible Chemical Storage

BenefitsBenefits

Increase system reliability: To reduce the peaks of energy generation

Increase generation capacity: The excess generation availableduring low demand periods can be used to charge a TES in order toincrease the effective generation capacity during high demandincrease the effective generation capacity during high-demandperiods. The result is a higher load factor for the plants, helping togenerate energy in a stable way.

Reduction of costs of generation: Seasonal demands can bematched with the help of TES systems that operate synergistically.

5

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Sensible Heat Storage Materials Essential requirements

o High thermal capacity (ρCp)o High melting point (large operating temperature)o High melting point (large operating temperature)o High thermal conductivityo Stability

L to Low cost

Commonly used sensible storage materials (Solid)Storage medium Operating

temperature, °CHeat capacity, kJ/kg-K

[k]

y g ( )

Reinforced concrete 400 0.85 [1.5]NaCl (solid) 500 0.85 [7]Cast iron 400 0.56 [37]Cast steel 700 0.6 [40]Silica fire bricks 700 1.00 [1.5]Magnesia fire bricks 1200 1.15 [5]

Low costHigh thermal conductivity and volumetric storage capacity

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Molten Salts (Sensible liquid Heat Storage Materials)

Best: 60% NaNO3 + 40% KNO3Solar Salt : Freezing point 220°C

Source: Hoshi et al., Solar EnergySolar Energy 79; 332-339, 2005.

A t H t t f fl id f l t t t to Acts as Heat transfer fluid from solar concentrator to steam generator and also heat storage medium

o Heat storage : Active storage

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Latent Heat Storage Materials

Requirements# High heat of fusion # High thermal conductivity #Low cost

MgCl2/KCl/NaCl; KOH; KNO3; KNO3/KCl; NaNO3

Suffer from low thermal conductivityKNO3; KNO3/KCl; NaNO3

Yet to be exploredy

Integration of graphite enhance k up to 10 W/mK.

Source: Hoshi et al., Solar Energy 79; 332-339, 2005.

Features: High energy density ; Temperature ranges are flexible, Optimal utilization of the storage materials

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Proposed phase change materials (PCM) forcascade heat storage in the temperature range up to380°C are NaNO3, KNO3/ KNO3, KOH and MgCl2 isproposedproposed.

A schematic of the cascade latent heat storage9

A schematic of the cascade latent heat storage

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Techniques of Thermal Storage

Active Heat storage : C f fo Characterized by forced convection heat transfer.

o Heat storage medium circulates in the solar fieldo High heat transfer rate, more effectiveo But, high cost; freezing in solar panels

Direct Active storage : Heat transfer fluid itself serves asDirect Active storage : Heat transfer fluid itself serves as storage (Hot and cold tank)

Indirect Active storage : Heat transfer fluid which isIndirect Active storage : Heat transfer fluid which is circulated in the solar panel is different from the one used in storage. i.e. heat transfer fluid transfer heat to secondary fluid which acts as storagefluid, which acts as storage

Passive Heat Storage : Storage medium is fixed. Heat transfer fl id th h t di l d i h i dfluid passes through storage medium only during charging and discharging time. e.g. solid storage and PCM.

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Direct active Two –Tanks Thermal Storage Systemo Hot and cold fluids are stored separately

o Freezing of salt (120-220°C)o Auxiliary heater is required

to maintain the temperature

o No additional heat exchangero Fast heat transfer

~450°C

~450°C

60% NaNO3 + 40% KNO3 above freezing during night time and adverse weather conditions

Schematic of Solar Thermal Power Plant with direct active two –tanks thermal storage system (Solar Tres, Sevilla; source: Gil et al. (2010), Renewable and Sustainable Energy Reviews 14; 31-35.)

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Active indirect single tank thermal storage system

o Hot and cold fluids are stored in the same tanko Hot and cold fluids are stored in the same tanko Hot and cold fluids are separated because of the stratification effecto Controlled charging and discharging are necessary to maintain the stratificationo Filler material such as quartzite and silica sand used to help thermocline

12Gil et al. (2010), Renewable and Sustainable Energy Reviews 14; 31-35

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STEAM ACCUMULATORSSteam accumulators are specially suited to meet the requirements for p y qbuffer storage in solar steam systems, providing saturated steam at pressures up to 100 bar.

Direct steam generation (DSG) inparabolic troughts with integrated steam

DSG with integrated steamaccumulator also used ash t

13

parabolic troughts with integrated steamaccumulator (Direct heat storage) phase separator

W.D. Steinmann and M.Eck, Solar Energy 80 (2006) 1277–1282

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During the discharge there is a

STEAM ACCUMULATORS

Steam accumulators provide saturated steam. If superheated steam is needed, a

d t t t b

During the discharge there is adrop in the pressure of the steam. To avoid this, the integration ofPCM into the storage vessel tosecond storage system must be

connected to the exit of the steam accumulator

PCM into the storage vessel to replace partly the liquid water

Saturated Steam

St l t ith i t t d14

Steam accumulator with integrated latent heat storage material

Steam accumulator and sensible storage material

W.D. Steinmann and M.Eck, Solar Energy 80 (2006) 1277–1282

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Ammonia-based solar thermochemical energy storage system

2NH3 + Heat → N2 +3H2 (Charging mode)N 3H 2NH H (Di h i d )

Operating temperature: 500–860°COperating pressure : 10 25 Mpa

N2 +3H2→ 2NH3 + Heat (Discharging mode)

15H. Kreetz and K. Lovegrove, Solar Energy Vol. 73, No. 3, pp. 187–194, 2002

Operating pressure : 10-25 Mpa

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Reversible Chemical Heat Storage: Metal Hydride • Intermetallic compounds formed alloying of different metals by• Intermetallic compounds formed alloying of different metals by

ball milling or melting.Absorption (Exothermic)Absorption (Exothermic)

Desorption (Endothermic)2Intermetallic H Metal Hydride Heat+ → +

15-75 Desorption (Endothermic)2Intermetallic H Metal Hydride Heat+ ← + kJ/mole H2

Ab ti i

Metal Hydride ApplicationsH d St

Absorption Desorption

Hydrogen StorageHydrogen Compressor RefrigeratorH t

H2

Heat pumpThermal Energy StorageHeat transformer Heat Heat

Heat driven mass transfer phenomenon

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Metal Hydride Based Heat Storage

o High storage capacity up to 2.2 MJ/kg of hydrideo No thermal insulationo No thermal insulationo Long term storageo Easy regeneration

H t ho High exergy efficiency Heat exchange

MH Reactor

Alloy ΔH

V

V1

Pd

P

y(kJ/mol. H2)

Mg+2% 74 V2Pr

Ps

H Supply

Mg+2% Ni

-74

MgNi -64.88

17

H2 SupplyMg -74.46

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Schematic of a Metal Hydride Reactor

18

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Test Setup of Heat Storage Device 

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Effect of supply pressure on the amount of heat stored

430 bar

3

J/kg

)

25 bar

Mg + 30%MmNi4Ta = 150 ˚Cm = 280 g

stor

ed (k

J

20 bar

15 bar2

t of h

eat s

10 bar

1

Am

ount

00 5 10 15 20

20

0 5 10 15 20Time (min)

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Effect of supply pressure on thermal energy storage coefficient

0.8

C)

0.7

cien

t (TE

SC

0 5

0.6

T 150 oCage

coef

fic

0.4

0.5 Ta = 150 oCTa = 140 oCTa = 130 oCTa = 120 oCne

rgy

stor

a

0.3

0 Ta 120 C

Mg + 30%MmNi4m = 280 g

Ther

mal

en

0.20 5 10 15 20 25 30 35 40

T

21

0 5 10 15 20 25 30 35 40Supply pressure (bar)

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Schematic of a Pre industrialPre-industrial Sacle Metal Hydride ReactorHydride Reactorfor Heat Storage A li iApplication

22

Page 23: Thermal Energy Storage : Methods and MateThermal …€¦ · Thermal Energy Storage : Methods and MateThermal Energy Storage : ... 8 Engg and 4 Science Departments About 6000 students,

3

3.5

4

350

400

450

wt%

)

C)20 bar

Ps

Effect of supply pressureon hydrogen storagecapacity and average bed2

2.5

3

200

250

300

age

capa

city

(w

empe

ratu

re(°

20 bar

10 bar15 bar

temperature (Ta = 250°C)

0 5

1

1.5

100

150

200

Hyd

ogen

stor

a

vera

ge b

ed te

Mg2NiT = 250°C

10 bar15 bar

0

0.5

0 200 400 600 800 1000 1200 1400 1600

Absorption time (s)

0

50H Av

Hydrogen storage capacityAverage bed temperature

Ta 250 Cma = 0.375 kg

Carried out at IIT Madras, 2004

3

3.5

4

350

400

450

e(°C

)

t%)

10 bar15 barPs=20 bar

Absorption time (s)

2

2.5

3

200

250

300

d te

mpe

ratu

re

ge c

apac

ity (w

t

10 bar15 barPs=20 bar

Effect of supply pressureon hydrogen storagecapacity and average bed

0.5

1

1.5

50

100

150

Ave

rage

bed

Hyd

ogen

stor

ag

Mg2NiTa = 300°Cm 0 375 kg

Hydrogen storage capacityAverage bed temperature

10 bartemperature (Ta = 300°C)

(Muthukumar et al., J. Alloys and C )

00 200 400 600 800 1000 1200 1400 1600 1800

Absorption time(s)

0

50H ma = 0.375 kg Compd., 452, 2008)

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Effects of heat release temperature and supply pressure on heat stored (Qr)

1.2

1.4

1.6

oy)

pressure on heat stored (Qr)

0.70.80.9

loy)

0 4

0.6

0.8

1

1.2

r (M

J/kg

of a

llo

2 bar3 bar4 bar

mr = 1.5Th = 650 KTa = 298 K

0 20.30.40.50.6

(MJ/

kg o

f all

2 bar3 bar4 bar

mr = 1.5Th = 650 KTa = 298 K

0

0.2

0.4

510 520 530 540 550 560 570 580 590 600

Heat release temperature (K)

Qr

00.10.2

510 520 530 540 550 560 570 580 590 600

Qr (

Qr vs Tr for Mg2+%Ni at different supply pressures

Heat release temperature (K)

Qr vs Tr for MgNi at different supply pressures

Heat release temperature (K)

0 81

1.21.41.6

g of

allo

y)

2 bar

00.20.40.60.8

Qr (

MJ/

kg 3 bar4 bar

mr = 1.5Th = 650 KTa = 298 K

24Qr Vs Tr for Mg at different supply pressures

0500 520 540 560 580 600

Heat release temperature (K)

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Comparison of performances at 3 bar supply pressure

14161820

y/cy

cle)

2

2.5

lloy)

468

101214

oles

/kg

of a

lloy

MgMg + 2% Ni mr = 1.5

T = 650 K 0 5

1

1.5

(MJ/

kg o

f a MgMg2%NiMgNi

mr = 1.5Th = 650 KTa = 298 KPS = 3 bar

024

500 520 540 560 580 600

Heat release temperature (K)

N (m

o

MgNiTh = 650 KTa = 298 KPS = 3 bar 0

0.5

500 520 540 560 580 600

Heat release temperature (K)

Qin

PS 3 bar

No Of hydrogen moles transferred Vs Tr Heat input Vs heat release temperature

Heat release temperature (K)

1 41.6

y)

0.60.8

11.21.4

J/kg

of a

lloy

MgMg+2%Ni

mr = 1.5T 650 K

00.20.4

500 520 540 560 580 600

Qr (

M Mg+2%NiMg2Ni

Th = 650 KTa = 298 KPS = 3 bar

25Heat release vs Heat release temperature

Heat release temperature (K)

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Operating temperature ranges of different metal hydrides

Material Usable temperature range (oC )

Mg±Ni/Mg2NiH4 250±350g g2 4

Mg/MgH2+2 wt% Ni 290±420

Mg/MgH2 350±450Mg/MgH2 350±450

Mg/MgH2+10 wt% Fe 350±450

Mg±Fe/Mg FeH 450±550Mg±Fe/Mg2FeH6 450±550

Mg±Co/Mg2CoH5 450±550

26

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Storage characterictics of different metal hydrides

Properties Mg/MgH2+2 wt%Ni

Mg/ MgH2

Mg-Fe/ Mg2FeH6

Mg-Co/Mg6CoH1

Mg-Co/Mg2CoH5

metal hydrides

1Enthalpy, kJ/mol 74 74 77.2 89 76Filling Density,

g/cm30.8 0.8 1.22 1.1 1.1

g/cm3

Capacity, wt% 6 5 5 3.5 3.5Energy to weight,

kJ/kg2257 1837 1817 1472 1260

kJ/kgEnergy to volume,

kJ/dm31806 1469 2217 1527 1386

Storage properties of Mg; (25–40) µm,

Temperature (oC) Absorption Desorption S pressure (bar) pressure (bar)

403 19.71 19.68422 27 74 27 54

Source:Bogdanovic et al., J Alloys and Compo nds 282

27

422 27.74 27.54441 39.16 38.85461 54.24 53.76

Compounds ,282; 84-92, 1999.

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Country Location Plant Features/Technology

Operational solar thermal power station in the worldy

capacitygy

AppliedUSA Mojave Desert

California354 parabolic trough

Spain Sevilla 150 parabolic troughSpain Sevilla 150 parabolic troughSpain Granada 100 parabolic troughUSA Boulder City, Nevada 64 parabolic troughSpain Puertollano, Ciudad

R l50 parabolic trough

RealSpain Badajoz 50 parabolic troughSpain Torre de Miguel

Sesmero (Badajoz)50 parabolic trough

Spain Alvarado (Badajoz) 50 parabolic troughSpain Sevilla 20 solar power towerIran Yazd 17 parabolic troughSpain Sevilla 11 solar power towerSpain Sevilla 11 solar power towerUSA Bakersfield, California 5 fresnel reflectorUSA Lancaster, California 5 solar power towerItaly near Siracusa, Sicily 5 parabolic troughAustralia New South Wales 2 fresnel reflectorAustralia New South Wales 2 fresnel reflectorUSA Peoria, Arizona 1.5 dish stirlingGermany Jülich 1.5 solar power towerSpain Murcia 1.4 fresnel reflectorUSA R d R k A i 1 b li t h

28

USA Red Rock Arizona 1 parabolic troughUSA Hawaii 2 parabolic troughIran Shiraz 0.25 CSP

940.65

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Summary of different thermal storage technologies and materials used in the solar power plant (Trough plant)

Storage concept

Experiences/projects

Year Thermalcapacity(MWhth)

Totalcapacity(MWe)

Operating temperature (°C)

HTF TES media

(MWhth) (MWe) re ( C)

Passive system LS3-SSPS-PSA, Spain

2004 0.48 n.a. n.a. Mineral Oil

High-temperature concretee concrete

Active Indirect system (Two-Tanks)

ANDASOL I-SENER/Cobra, Guadix, Spain

2008 1010 n.a. 384–291 Steam Molten salts (60% NaNO3 + 1010 50 560–260

880 382 296 40% KNO3) 880 n.a. 382–296

Active Indirect system (Two-T k )

ANDASOL II-SENER/Cobra, G di S i

2009 n.a. n.a. n.a. Steam Molten salts

Tanks) Guadix, SpainActive Indirect system (Two-Tanks)

EXTRESOL I-SENER/Cobra

2010 (12 h) 50 n.a. Synthetic Oil

Molten salts

Tanks) n.a. SOLANA,

Phoenix, AR, USA 2011 n.a. 280 n.a. n.a. n.a.

Source: Medrano et al., Renewable and Sustainable Energy Reviews 14; 56-72, 2010.

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Summary of different thermal storage technologies and materials used in the solar power plant (Central receiver plant)

Active Indirect system (Two-Tanks)

CESA I-PSA, Spain

1983 7 12 340–220 Steam Molten salts 1982 n.a. 1 n.a. Steam Molten salts

(nitrate) 12 520 Steam (100 bar) Molten saltsTanks) 12 520 Steam (100 bar) Molten salts

Active Indirect system (Two-

CERS-SSPS PSA, Spain

1981 2.7 0.5 n.a. Molten salt (liquid sodium)

Molten salt (sodium)

Tanks) Active Direct system (Two-Tanks)

THEMIS, Targasonne, France

1982 40 2.5 450–250 Molten salt (High technology)

Molten salt (High technology)Tanks) France technology)

Active Direct system (Direct steam generation)

PS10-Abengoa, Sevilla, Spain

2007 15(50 min)

11 n.a. Steam Steam–ceramic

generation) Active Direct system (Direct steam

PS20-Abengoa, Sevilla, Spain

2007 n.a. 20 n.a. Steam Steam–ceramic

generation) Active Direct system (Two-Tanks)

SOLAR TRES-PSA, Spain

2002–2007

588(16 h)

17 565–288 Molten salts (NaNO3 + KNO3)

Molten salts (NaNO3 + KNO )

30

Tanks) Spain(SENER)

KNO3)

Source: Medrano et al., Renewable and Sustainable Energy Reviews 14; 56-72, 2010.

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Solar PAN IIT : Research Proposal

Schematic of proposed 1 MW Solar Thermal Power Plant

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Objectives of Heat Storage

To ensure continuous generation of stream for 8 hrs with 95% reliability and to extend the possibility of steam generation during night time

Proposed Heat Storage Capacity

Technique Capacity App. Cost (USD)

Steam Accumulator 14 GJ 4,20,000

Sensible Heat Storage 1 GJ 1,20,000

Latent Heat Storage 1 GJ 1,80,000

32

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Proposed Thermal Energy Storage Systems

o It is proposed to store the excess energy absorbed during theday time in the form of high pressure water up to 80 bar. Theapproximate capacity of high pressure steam storage vessel isapproximate capacity of high pressure steam storage vessel is150 m3 and the estimated amount of heat stored in the form ofhigh pressure water is about 14 GJ.

o Heat generated from the parabolic solar collector is first stored inthe form of sensible heat in the temperature range up to 350-500°C Thi t d l i l d t t500°C. This storage module is also used to generate superheated steam.

o It is also proposed to store 1 GJ heat in the form of latent heatusing phase change materials (PCM) of temperature range up to400°C. Cascade latent heat storage consists of NaNO3, KNO3/g 3, 3KNO3, KOH and MgCl2 is proposed. The use of a cascade ofmultiple phase change materials (PCM) shall ensure the optimalutilization of the storage material

33

utilization of the storage material.

o Application of metal hydrides as heat storage will be also tested.

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Thanks for your kind attention

34