Article 7 IMECE2011-65819 Solar

7
1 Copyright © 2011 by ASME Proceedings of the ASME 2011 International Mechanical Engineering Congress & Exposition IMECE2011 November 11-17, 2011, Denver, Colorado, USA IMECE2011-65819 VIRTUAL HEIGHT AIDED SOLAR CHIMNEY: A NEW DESIGN Khaled I.E. Ahmed Mechanical & Industrial Engineering Department, Faculty of Engineering, Qatar University, Doha (2713), Qatar. [email protected] Ali K. Abdel-Rahman Mechanical Engineering Department, Faculty of Engineering, Assiut University, Assiut (71516), Egypt. [email protected] Mahmoud Ahmed Mechanical Engineering Department, Faculty of Engineering, Assiut University, Assiut (71516), Egypt. [email protected] Wael M. Khairaldien Mechanical Engineering Department, Faculty of Engineering, Assiut University, Assiut (71516), Egypt. [email protected] ABSTRACT Renewable energy source deployment is growing rapidly as it reduces CO2 emissions and increases diversity and security of supply. Solar chimney (SC) is a promising large- scale power technology, which absorbs solar radiation and converts parts of solar energy into electric power free of CO2 emissions. A major problem of Solar Chimney Power Plant (SCPP) is its low conversion efficiency as determined by the thermal performance of the system. However, the conversion efficiency of SCPP significantly increases with the SC height increase. The current paper proposes a new design of a virtual height aided solar chimney. In this new system the solar chimney is aided with a passive cooling system at the top of the chimney and a passive solar heater at its base to virtually mimic larger heights of the chimney. The new design has been simulated numerically for development and optimization. The numerical study is done in two stages to examine this concept. In the first stage, numerical results are obtained for the effect of the chimney height on the inside air flow speed. Then, in the second stage, the effect of decreasing the temperature at the chimney exit and the effect of increasing the temperature at the chimney base on the air flow speed are examined separately for small chimney heights. Then the combined effect of the two actions is investigated at a wide range of chimney heights. The numerical results have shown that the localized base heating and exit cooling have significantly enhanced the chimney performance for chimney heights up to 500m. A chimney with height of 300m gains an increase in the air velocity more than 25% due to the heating and cooling actions. Virtual height aided Chimney with original height of 300m acts similarly to a conventional chimney with height of 500m due to the effect of base heating and exit cooling actions. This air flow velocity increase reflects 100% increase in the expected generated electric power. Further detailed results are presented and discussed. INTRODUCTION In Qatar and despite of low average wind speed for on- shore energy harvesting, off-shore can be a good alternative. The wind energy becomes visible if the solar power chimney concept is employed in Qatar. Qatar is blessed with more than 2200 kWh/m 2 annual solar radiation as shown in Fig. 1. Solar chimney (SC) power technology is a promising large-scale power technology [1], which absorbs direct and diffused solar radiation and then converts parts of these solar energies into electric power free of emissions. Fig 1. Annual global solar radiation [5] 1700 < SR < 2200 SR > 2200

Transcript of Article 7 IMECE2011-65819 Solar

Page 1: Article 7 IMECE2011-65819 Solar

1 Copyright © 2011 by ASME

Proceedings of the ASME 2011 International Mechanical Engineering Congress & Exposition IMECE2011

November 11-17, 2011, Denver, Colorado, USA

IMECE2011-65819

VIRTUAL HEIGHT AIDED SOLAR CHIMNEY: A NEW DESIGN

Khaled I.E. Ahmed Mechanical & Industrial Engineering Department,

Faculty of Engineering, Qatar University, Doha (2713), Qatar.

[email protected]

Ali K. Abdel-Rahman

Mechanical Engineering Department, Faculty of Engineering,

Assiut University, Assiut (71516), Egypt. [email protected]

Mahmoud Ahmed

Mechanical Engineering Department, Faculty of Engineering,

Assiut University, Assiut (71516), Egypt. [email protected]

Wael M. Khairaldien

Mechanical Engineering Department, Faculty of Engineering,

Assiut University, Assiut (71516), Egypt. [email protected]

ABSTRACT

Renewable energy source deployment is growing rapidly as it reduces CO2 emissions and increases diversity and security of supply. Solar chimney (SC) is a promising large-scale power technology, which absorbs solar radiation and converts parts of solar energy into electric power free of CO2 emissions. A major problem of Solar Chimney Power Plant (SCPP) is its low conversion efficiency as determined by the thermal performance of the system. However, the conversion efficiency of SCPP significantly increases with the SC height increase. The current paper proposes a new design of a virtual height aided solar chimney. In this new system the solar chimney is aided with a passive cooling system at the top of the chimney and a passive solar heater at its base to virtually mimic larger heights of the chimney. The new design has been simulated numerically for development and optimization. The numerical study is done in two stages to examine this concept. In the first stage, numerical results are obtained for the effect of the chimney height on the inside air flow speed. Then, in the second stage, the effect of decreasing the temperature at the chimney exit and the effect of increasing the temperature at the chimney base on the air flow speed are examined separately for small chimney heights. Then the combined effect of the two actions is investigated at a wide range of chimney heights. The numerical results have shown that the localized base heating and exit cooling have significantly enhanced the chimney performance for chimney heights up to 500m. A chimney with height of 300m gains an increase in the air velocity more than 25% due to the heating and cooling actions. Virtual height aided Chimney with original height of 300m acts similarly to a conventional chimney with height of 500m due to the effect of

base heating and exit cooling actions. This air flow velocity increase reflects 100% increase in the expected generated electric power. Further detailed results are presented and discussed. INTRODUCTION

In Qatar and despite of low average wind speed for on-shore energy harvesting, off-shore can be a good alternative. The wind energy becomes visible if the solar power chimney concept is employed in Qatar. Qatar is blessed with more than 2200 kWh/m2 annual solar radiation as shown in Fig. 1. Solar chimney (SC) power technology is a promising large-scale power technology [1], which absorbs direct and diffused solar radiation and then converts parts of these solar energies into electric power free of emissions.

Fig 1. Annual global solar radiation [5]

1700 < SR < 2200

SR > 2200

Page 2: Article 7 IMECE2011-65819 Solar

Tcombsituatunit (The treliabefficisystemwith t

Fig

S

structup anthe pimprotime, researseconsystemundertherm

Pturbinhorizopassacore caxial base the Sinstal[6] fo

Sby mprotoreferemeasumodevisibishow

The solar chimnbines three comted in the cen(PCU) which technologies f

ble. The majorency as determm. However, tthe SC height.

2. Schematic o

Solar collectoture, and transp

nd transfers its periphery to thove the opera

several suggerchers. These

ndary roof undm such as clor the collector

mal storage of SPCU of a largne generators, ontal-to-vertica

age from colleccomponents offlow type. Th[5]. Mostly, th

SC base mainllation and maior large-scale SSCPP performmany researchtypes. The mence base for aure that can b

els, many theorility of buildinn that SC heig

ney power planmponents suchter of the collincludes one ofor the SCPP r problem of mined by the the conversion

overview of thprincip

or consists oparent roof. Thheat to the air

he center driveational performestions were psuggestions a

der the first rooosed water-fillr roof [3], anSCPP [4]. ge-scale SCPP

power electroal transition sector exit to SCf any SCPP. Thhe SC turbinese SC turbines ly because ofintenance of tu

SCPP. ance has beeners [7-12] us

main objectives a theoretical wbe scaled up. retical studies ng a large scalght plays the m

nt (SCPP), as sh as a solar lector, and poor several turbcomponents SCPP is its thermal perfoefficiency of

he solar chimneple

of support mhe ground undeabove it flowinen by buoyan

mance of SCPpreviously propare including aof [2], to add led tanks on tnd a use of s

P consists of onics, a grid ection (HTVTSC inlet. Turbinehe typical SC t are usually pwere proposed

f inconveniencurbine generato

n experimentasing small to

of these studiwork and to get

Utilizing thes[12-22] have

le SCPP. Theost significant

shown in Fig. 2collector, a Swer conversiobine generatorare simple anlow conversioormance of thSCPP increase

ey power plant

matrix, columer the roof heatng radially from

ncy. In order tPP during nighposed by manan intermediatthermal storagthe natural sosolar ponds fo

one or severainterface and S), i.e., the flowe generators arturbine is of thlaced at the S

d to be placed ace arising fromors at the SC to

lly investigatemedium size

ies are to find t a performancse experimentainvestigated th

ese studies havrole in definin

2

2, C

on rs. nd on he es

mn ts m to ht ny te ge oil or

al a

w re he C at m op

ed ed a

ce al he ve ng

the oupractic

TengineSC bdiffereproporheight[23], wthe coProcesthrougProcesthrougnegatithermalossesThe aincludshown

Fig

Tlower exit ocollectempelevel meter increa5,000mchimnspeedschimnincrea

Inunit abase odue to

utcome of the cally visible fo

The SC situatede of the SCPP,base by comence. The martional to the ct. The air cyclwhere 02–03 pollector inlet wss 03–03te degh the turbiness 03te–04 dgh the SC whive work of gral energy of ai

s through the paerodynamic loded in the collen in Fig. 3.

g 3. Temperatuanal

01: atmospher03: col

The air flow in temperature, l

of the solar chctor. It was reerature decreasand the atmoover the sea

ases graduallym. These da

ney heights wos. Artificially

ney will enhaased. n the present aat the top of thof chimney to vo large chimney

SCPP. Largeor research word in the collecto, which drives

mbining with ass flow of ucollector air tele with losses process denoteswhen its tempeenotes the air e when the temdenotes the aihen the temperavitational forir flow are releaower system a

osses of PCU ector and in the

ure–entropy dialysis with systeric air at SC outletllector outlet air,

n the solar chimlower pressure himney when eported by NAses by 6.5oC aospheric pressulevel till 2750

y showing speata show that ould deliver ay creating theance its perfo

article a novel he chimney anvirtually simulay heights is pro

Copyright ©

e heights (> 5rk. or center is thethe air to the the effect o

updraft air is emperature risefor SCPP is shs the heated aierature and enflow at the c

mperature decir behind the erature decrearce. Finally, thased into the at

are also includecomponents a

e SC except tu

agram of air staem losses [23]t, 02: collector i 04: SC outlet air

mney is mainly and higher wicompared to

ASA [24] that tat 1000m heighure decreases 0m. Furthermoeed of 60m/ssolar chimney

air flows with ese driving fo

ormance as if

concept of adnd a solar heatate the temperaoposed.

2011 by ASME

500 m) are no

e actual thermacollector to th

of temperaturapproximately

e and to the SChown in Fig. ir entering fromntropy increasecollector outle

creases slightlyturbine flow

ses due to thhe dynamic antmosphere. Thed in this cycleare respectivelyurbine losses, a

andard cycle

inlet air, r.

y driven by thind speed at ththat under th

the atmospherht from the se10Pa for each

ore wind spees at height oys with highehigher airflow

orces for suchf its height i

dding a coolingting unit at thature differenc

E

ot

al e e y C 3

m e. et y.

ws e d e

e. y

as

e e e e a h d

of er w h is

g e e

Page 3: Article 7 IMECE2011-65819 Solar

DEVV

decreconcetempeabsorcoolinHowegenerpressuchimnheatinschemat the

passi

I

phaseresultchimnphaseexit aspeedconclvirtua

aA

conce10m cchimnmodewith eleme10cm

Urook

ELOPMENT Virtually increeasing the tempept to be aerature at the rption refrigerng concept is ever, absorptiorally addressedure at the chimney base, jusng system simmatic diagram e top of the chim

Fig 4. Schemaive cooling at c

In the current es to examine ts are obtainedney height one, the effect ofand the effect od is examined sluded with relaal height at the

a- The CFD A CFD model iept. A solar chchimney diameney heights froel. A 2-D axisy

mapped meshent size is cont

m. Under the collebed that absor

OF THE NEWeasing the heiperature and pddressed in chimney exit

ation solar drnot addressed

on refrigeratiod for general comney exit cout over the tu

milar to that usfor the new demney and heat

atic overview ochimney top an

base

paper a prelimthis concept.

d as referencen the air flow f decreasing thof heating the separately and ations betweenairflow speed.

Model is built for a pr

himney, Fig. 5, eter, 3m collecom 50m to 100ymmetric modh to get the trolled to be le

ector a thick rb solar radiati

W DESIGN ight of a solapressure at its the current

t could be redriven system. d before for son solar driveooling systems

uld be reducedurbine section,sed in [26]. esign of addingting unit at the

of a solar chimnnd passive heate

minary study In the first p

e frame for thspeed. Then

he temperature chimney base combined. Th

n the chimney .

reliminary examwith 200m col

ctor largest heig00m is assumeddel is built usin

most accurateess than 20cm

layer of higheon during suns

ar chimney bexit is a noveproposal. Th

duced using a This positiv

solar chimneyen systems ars [25]. Also th

d by heating th, using passivFig. 4 shows g a cooling unchimney base.

ney aided withting at chimney

is done in twphase numericahe effect of th, in the seconat the chimneon the air flow

hen the study ireal height an

mination of thllector diameteght, and varioud for the curren

ng ANSYS-CFDe results. Thand higher tha

er heat capacitshine hours an

3

by el he an ve s. re he he ve

a nit

h y

wo al he nd ey w is

nd

is er, us nt D he an

ty nd

releaseduringduringthe copressupressube adimodeldepenatmosto be for com

Fig 5.

a-T

modelsolar veloci

e the stored eng non-sunshineg day time). Tollector is assuure at the collecure. The colleiabatic. The bled based on t

ndent pressure spheric pressur101325Pa andmpressible and

Schematic dra

- The regulaThe preliminaryl have shown tchimney perf

ity significant

C

Chimn

VerticaTurbin

nergy to the fle periods (nigThus, the temp

umed to be 60o

ctor entrance isector and the cboundary condthe chimney hand temperatu

re and temperad 300oK respecd turbulent ther

awing of a solaCFD mo

ar chimney ry results for the great effectformance, Figtly increases

Chimney

Collector

ney

al ne

Copyright ©

lowing air inleght time and cperature of theoC constant alls bounded by thimney walls dition at the c

height and the ure given by NAature at sea levctively. The mrmal fluid anal

ar chimney witodel

the first phast of the chimneg. 6. The a

with the in

Location oTur

LocationTu

C

H

2011 by ASME

et to the turbincloudy intervae ground undel the time. Ththe atmospheriare assumed t

chimney exit iaverage heigh

ASA [24]. Thvel are assumemodel is solvelysis.

th its simulation

se of the CFDey height on thverage airflow

ncrease of th

of Horizontal rbines

n of Vertical urbine

Collector

Horizontal Turbines

E

e al er e c o is ht e d d

n

D e

w e

Page 4: Article 7 IMECE2011-65819 Solar

chimnmodeat higfurtheeffectheighpressucomp

Fig 6

Fig 7

bI

chimnchimnheatinchimn

ney height, Fiel, for simplicigh altitudes is ner decrease thet. This effect

hts. Furthermoure drop afte

parative analysi

6. The airflowturbine re

7. The effect ovelocity enter

b- Cooling thIn the second pney height by hney exit is conng the chimneney base is ex

g. 7. It is woty, the airflownot counted ine pressure at thwill increase

ore, the currener the horizois.

w pattern in m/sgions for chim

of the chimney ring to vertical

he chimney exphase, the concheating the chi

nsidered. The ley base. Thenxamined witho

orth noting thaw speed of the n the current mhe chimney exisignificantly a

nt study does nontal turbines

s at the horizonmney height of 2

height on the al and horizonta

it cept of virtuallyimney base andlatter is examinn the concept out cooling the

at in the currenatmospheric a

model which wiit due to ventuat high chimnenot consider th

since it is

ntal and vertica200 m

airflow averageal turbines

y increasing thd by cooling thned first withou

of heating the chimney exi

4

nt air ill

uri ey he a

l

e

he he ut he it.

Finallyperforbound25oCheightvelociby 1%Both chimn

c-T

movesof prefor a cexit. the croof turbimpaccoolin

Fig

y both effectsrmance under tdary conditions

to simulate dts of 50m andity entering the

% for each 5K chimney heig

ney exit cooling

- Heating thThe second tecs the air up tow

essure drop at tchimney heighFig. 9 shows oss sections ofbines. Fig. 9, act on increasinng.

8. The effect oentering t

s are combinethese effects. Ts have been reddifferent coold 100m. As e vertical and reduction in th

ghts experiencg.

he chimney bachnique which wards the chimthe chimney exht of 50m with/

the profile of f the collector also, shows tha

ng the airflow

of cooling the to vertical and

Copyright ©

ed to comparThe chimney educed with raning conditionshown in Fighorizontal turhe chimney exce the same

se is heating the

mney exit increxit. This conce/without coolin

f the airflow vand chimney at heating the bvelocity than

chimney exit ohorizontal turb

2011 by ASME

e the chimneyexit temperaturnge from 5oC ts for chimney. 8 the airflowrbines increasexit temperatureeffect for th

e chimney baseasing the effecept is examineng the chimneyelocity throughat the locationbase has highethat of the exi

on the airflow bines

E

y e o y w s

e. e

e ct d y h

ns er it

Page 5: Article 7 IMECE2011-65819 Solar

5 Copyright © 2011 by ASME

d- Combined cooling and heating About a 25% increase in the airflow velocity is realized

with the combined actions of heating the chimney base and cooling the chimney exit. Such increase in the air velocity results in a 95% increase in the harvested energy from such arrangement due to the cubic relation between the harvested energy and airflow velocity.

The effects of the combined cooling and heating are examined for chimney heights ranging from 50 – 1000m. It is

worth noting that the cooling and heating is applied at the chimney cross sectional area within height less than 20cm. These localized heating and cooling have shown significant performance enhancement for chimney heights up to 500m, Fig. 10. Chimneys with heights up to 400m gain an increase in the air velocity more than 20% due to the heating and cooling actions, Fig. 11. Chimney with height 300m with heating and cooling actions acts similarly to a chimney with height 500m without these modifications, Fig. 10.

Fig 9. Airflow velocity profile through the cross sections of the collector and chimney at the turbines locations

Fig 10. Airflow average velocities Vx entering horizontal turbines and Vy entering vertical turbine before and after applying heating

chimney base and cooling chimney exit

b) Entering to horizontal turbines a) Entering to vertical turbine

Page 6: Article 7 IMECE2011-65819 Solar

6 Copyright © 2011 by ASME

Fig 11. Percentage increase in the air flow velocity and in virtual height due to the action of heating the chimney base and cooling the

chimney exit.

CONCLUSIONS Solar chimneys are significant source of clean electrical

energy. The performance of the solar chimney power plant depends mainly on the height of its chimney. The chimney height has to be at least 500m to gain cost effective power. In the current work a new design concept of heating the chimney base and cooling the chimney exit has been presented. The new proposed design has worked as a chimney with virtual added height. This virtually added height has shown double the generated electrical power for a chimney with original height up to 400m.

The current preliminary results of the current CFD model require few modifications to include all boundary and environmental conditions to confidently relay on. Moreover, comparisons with experimental results are required for the model to gain confidence in its achieved results and in the claimed enhancements.

REFERENCES

[1] Dennis C. Solar energy: radiation nation. Nature 2006; 443:23–24.

[2] Pretorius JP. Optimization and control of a large-scale solar chimney power plant. Ph.D. thesis. South Africa: University of Stellenbosch; 2007.

[3] Schlaich J, Bergermann R, Schiel W, Weinrebe G. Design of commercial solar updraft tower systems—utilization of

solar induced convective flows for power generation. J Solar Energy Eng 2005;127:117–24.

[4] Davey RC. Device for generating electricity from solar power. WO 2008/ 022372 A1; 28 February 2008.

[5] Schlaich J. The solar chimney: electricity from the sun. Stuttgart, Germany: A. Menges; 1995.

[6] Pasumarthi N, Sherif SA. Experimental and theoretical performance of a demonstration solar chimney model. Part I: Mathematical model development. Int J Energy Res 1998; 22:277–88.

[7] Zhou XP, Yang JK. Temperature field of solar collector and application potential of solar chimney power systems in China. J Energy Inst 2008; 81:25–30.

[8] Zhou XP, Yang JK, Xiao B, Hou GX. Experimental study of the temperature field in a solar chimney power setup. Appl Therm Eng 2007; 27:2044–50.

[9] Ketlogetswe C, Fiszdon JK, Seabe OO. Solar chimney power generation project—the case for Botswana. Renewable Sustain Energy Rev 2008;12: 2005–12.

[10] Ferreira AG, Maia CB, Cortez MFB, Valle RM. Technical feasibility assessment of a solar chimney for food drying. Solar Energy 2008; 82:198–205.

[11] Maia CB, Ferreira AG, Valle RM, Cortez MFB. Theoretical evaluation of the influence of geometric

Page 7: Article 7 IMECE2011-65819 Solar

7 Copyright © 2011 by ASME

parameters and materials on the behavior of the airflow in a solar chimney. Comput Fluids 2009; 38:625–36.

[12] Maia CB, Ferreira AG, Valle RM, Cortez MFB. Analysis of the airflow in a prototype of a solar chimney dryer. Heat Transfer Eng 2009; 30:393–9.

[13] Zhou XP, Yang JK, Xiao B, Hou GX. Simulation of a pilot solar chimney power equipment. Renewable Energy 2007; 32:1637–44.

[14] Zhou XP, Yang JK, Xiao B, Long F. Numerical study of a solar chimney thermal power setup using turbulent model. J Energy Inst 2008; 81:86–91.

[15] Zhou XP, Yang JK, Xiao B, Hou GX, Xing F. Analysis of chimney height for solar chimney power plant. Appl Therm Eng 2009; 29:178–85.

[16] Zhou XP, Yang JK, Xiao B, Li J. Night operation of solar chimney power system using solar ponds for heat storage. Int J Global Energy Issues 2009; 31:193– 207.

[17] Nizetic S, Ninic N, Klarin B. Analysis and feasibility of implementing solar chimney power plants in the Mediterranean region. Energy 2008; 33:1680–90.

[18] Ming TZ, Liu W, Xu GL, Xiong YB, Guan XH, Pan Y. Analytical and numerical investigation of the solar chimney Numerical simulation of the solar chimney power plant systems coupled with turbine. Renewable Energy 2008; 33:897–905.

[19] Ming TZ, Liu W, Pan Y, Xu GL. Numerical analysis of flow and heat transfer characteristics in solar chimney power plants with energy storage layer. Energy Convers Manage 2008; 49:2872–9.

[20] Koonsrisuk A, Lorente S, Bejan A. Constructed solar chimney configuration. International Journal of Heat and Mass Transfer 2010; 53:327–33.

[21] Larbi S, Bouhdjar A, Chergui T. Performance analysis of a solar chimney power plant in the southwestern region of Algeria. Renewable Sustain Energy Rev 2010; 14:470–7.

[22] Chergui T, Larbi S, Bouhdjar A. Thermo-hydrodynamic aspect analysis of flows in solar chimney power plants—A case study. Renewable Sustainable Energy Rev 2010; 14:1410–8.

[23] Gannon AJ, von Backstro¨mTW. Solar chimney cycle analysis with system loss and solar collector performance. J Solar Energy Eng 2000; 122:133–7.

[24] COESA, 1976: U.S. Standard Atmosphere, 1976. U.S. Government Printing Office, 227 pp.

[25] Ahmed Hamza H. Ali, Peter Noeres and Clemens Pollerberg. “Performance Assessment of an Integrated Free Cooling and Solar Powered Single-Effect Lithium Bromide-Water Absorption Chiller” Solar Energy Vol. 82, No.11, pp. 1021–1030, November (2008)

[26] Amara S., Nordell, B., Benyoucef, B. and Benmoussat, A., (2011), "Concentration Heating System with Optical Fiber Supply," Energy Procedia, 6, 805–814