19-Solar Thermal Basics. ECEGR 452 Renewable Energy Systems

19-Solar Thermal Basics ECEGR 452 Renewable Energy Systems Overview • • • • • • Introduction Concentrating Solar Power (CSP) Plant Principles CSP T...
Author: Ginger Robinson
2 downloads 0 Views 536KB Size
19-Solar Thermal Basics ECEGR 452 Renewable Energy Systems

Overview • • • • • •

Introduction Concentrating Solar Power (CSP) Plant Principles CSP Technologies Concentration Ratio CSP Efficiency Stagnation

Dr. Louie

2

Introduction • Solar radiation is converted to thermal energy when it is absorbed by an object • Typical irradiance value is 1000 W/m2

Dr. Louie

3

Introduction • Three types of solar-thermal systems  Active solar heating: a separate collector is used  Passive solar heating: collection is integrated into the design of a building  Solar thermal engines: similar to active, but the thermal energy is used to drive an generator

Dr. Louie

4

Concentrating Solar Power (CSP) direct solar radiation optical concentrator concentrated solar radiation

receiver

heat Heat engine

(Brayton/Rankine)

electricity Dr. Louie

5

Solar Thermal Generation • Concentrator: none • Receiver: a small pool (1 m2) laying on the ground containing 100 liters of water • Assume:  no reflection  no energy lost to surroundings

GHI = 1000 W/m2

Dr. Louie

6

Solar Thermal Generation • Ambient water temperature: 15o C • After one hour: 3.6 MJ of solar radiation have been absorbed • Assume:  no reflection  no energy lost to surroundings

• What is the temperature rise?

GHI = 1000 W/m2

Dr. Louie

7

Solar Thermal Generation • How much has the temperature risen? T 

Q 3.6MJ   8.637 C mch (100)(4186) (specific heat of water is 4186 J/K)

• We now have water at 23.6 oC • Can we use this heated water to create electricity?

GHI = 1000 W/m2

horizontal surface

Dr. Louie

8

Solar Thermal Generation • We cannot use it to generate electricity efficiently • Temperature is too low

GHI = 1000 W/m2

horizontal surface

Dr. Louie

9

Carnot Efficiency • Upper limit on the efficiency of a process operating between two temperatures is dictated by the Carnot Efficiency TL TH  TL hc  1   TH TH

• Where  hC: is the Carnot efficiency  TL: is the cold reservoir temperature (K)  TH: is the hot reservoir temperature (K)

Dr. Louie

10

Solar Thermal Generation • Assuming the cold reservoir is at ambient temperature, then the maximum efficiency is TH  TC 296  288 hC    3% TH 296

• Can you think of a more efficient design?

GHI = 1000 W/m2

horizontal surface

Dr. Louie

11

Concentrating Solar Power (CSP) • Concentrator: lens  Assume the area of the lens shadow is 2m2 (note this is NOT the surface area)  Diffuse irradiance (assumed to be 100 W/m2 is not concentrated)

• Only direct radiation is focused • Irradiance on the pool: 1800W/m2

Gb = 900 W/m2

2m2

1m2 Dr. Louie

12

Concentrating Solar Power (CSP) • What is the temperature of the pool after one hour under these conditions?  same assumptions as previous case  Tamb = 15 oC Gb = 900 W/m2

2m2

1m2

Dr. Louie

13

Concentrating Solar Power (CSP) • What is the temperature of the pool after one hour under these conditions? T 

Q 6.48MJ   15.5 C mch (100)(4186)

 TH  30.5 C

hC 

TH  TC  5% TH

increased efficiency

2m2

1m2

Dr. Louie

14

Concentrating Solar Power (CSP) • Concentrator: mirrors • Modeled from Snell’s Law • We will use GDNI, assuming the mirrors track the sun absorber direct irradiance

reflected

1

2

Dr. Louie

15

Direct Normal Irradiance Direct Normal Irradiance: beam irradiance on a surface that is normal to the beam

direct normal irradiance

Dr. Louie

16

Concentrating Solar Power (CSP) Angle of reflected beam determined from Snell’s Law

 

Dr. Louie

17

Concentrating Solar Power (CSP) • Fundamental operating premise: Concentrated Solar Power (CSP) allows for “higher quality” energy to be converted due to the higher operating temperature of the heat engine • What CSP configurations can you think of?

Dr. Louie

18

Types of CSP • Four commercial or pilot project types:    

Parabolic trough collector (PTC) Centralized receiver systems (power towers) Dish/engine systems Linear Fresnel reflector

Dr. Louie

19

PTC

Dr. Louie

20

Power Tower

Dr. Louie

21

Dish

Dr. Louie

22

Concentration Ratio • Geometric concentration ratio AC C  Arec

 AC: area of collector  Arec: area of receiver

• “area” is interpreted as aperture area • To heat a liquid to a high temperature, you need large collector area and/or a small receiver area

Dr. Louie

23

Example • 25 mirrors with dimension 10m x 10m are used to concentrate beam irradiance (DNI) of 1000 W/m2 on a receiver that is 5m x 5m. Find the:  geometric concentration ratio  irradiation received by the receiver

Dr. Louie

24

Example • 25 mirrors with dimension 10m x 10m are used to concentrate beam irradiance (DNI) of 1000 W/m2 on a receiver that is 5m x 5m. Find the:  geometric concentration ratio  irradiation received by the receiver 25  (10  10)  100 (5  5) irradiance  100  1000  100kW C 

Dr. Louie

25

Concentration Ratio • What prevents us from using an arbitrarily small receiver to increase the concentration ratio? C 

AC Arec

• Consider a surface with aperture of 100m2 that focuses solar radiation on a receiver with area 0.001m2 • What is the concentration ratio?

Dr. Louie

26

Concentration Ratio • What prevents us from using an arbitrarily small receiver to increase the concentration ratio? C 

AC Arec

• Consider a surface with aperture of 100m2 that focuses solar radiation on a receiver with area 0.001m2 • What is the concentration ratio? 100 C   100, 000 0.001

Dr. Louie

27

Concentration Ratio • What is the irradiance on the receiver (if GDNI =1,000 W/m2)?

Dr. Louie

28

Concentration Ratio • What is the irradiance on the receiver? 100, 000  1000 W

m

2

 100 MW

m2

• This greater than the irradiance at the surface of the Sun ( about 63 MW/m2)! • Second law of thermodynamics prevents this

Dr. Louie

29

Concentration Ratio • The actual limit is 2

R C     45, 000 r

 R: mean distance from the Earth to the Sun  r: radius of the Sun

Dr. Louie

30

Concentration Ratio • Actual concentration ratios are much smaller (< 5000), depending on the collector arrangement • It is useful to consider the size of the reflected image of the Sun • Sun does not appear as a point, it appears as a disc

Dr. Louie

31

Concentration Ratio subtended solid angle of 0.53o

 s  0.53

Dr. Louie

32

Side Note • Angle subtended by the moon is also about 0.53o • This is why a “Ring of Fire” eclipse can occur

Source: National Geographic

Dr. Louie

33

Reflected Image reflected image of the Sun will always have a target-to-mirror solid angle equal to 0.530 Sun’s rays cannot be focused to a single point! receiver

Sun’s image

Dr. Louie

34

CSP Process • CSPs concentrate irradiation, GDNI, from the collector to receiver GC   CGDNI

 Gc = irradiance from the collector (W/m2)   is the absorptivity (unitless, ≤ 1)

Dr. Louie

35

CSP Efficiency • Temperature of the receiver, Trec, increases  thermal energy, Q, is transferred to a working fluid in the receiver  as Trec increases above the ambient temperature, Tamb, it begins to transfer heat via radiation (convection and conduction heat transfer are ignored)  Thermal energy is lost  How is the radiated power determined?

Dr. Louie

36

CSP Efficiency • Recall the Stefan-Boltzmann Law: G   T 4 W/m2

  5.67  108 J/(sm2K 4 )

• If the object is not a black body, then: G  eT 4 W/m2

 e is the emissivity of the object (unitless)

• Surrounding environment is also radiating energy toward the receiver • net irradiance: 4 4 Grec  e (Trec  Tamb )

Dr. Louie

37

CSP Efficiency • Net flow of heat: Q  AC (GC  Grec ) W 4 4 Q  AC ( CGDNI  e (Trec  Tamb )) W

• Receiver efficiency: hrec  Q

AC CGDNI

Dr. Louie

38

CSP Efficiency • Efficiency: hrec  Q

ACC GDNI

4 4  (Trec  Tamb )     e  CG DNI  

• Assume Trec > Tamb • What happens to the efficiency of the receiver if:  Concentration ratio (C) increases?  Trec increases?

• What is the maximum efficiency?

Dr. Louie

39

CSP Efficiency • Efficiency: hrec

Q

ACGDNI

4 4  (Trec  Tamb )     e  CG DNI  

• assume Trec > Tamb • What happens to the efficiency of the receiver if:  Concentration ratio increases? • efficiency increases

 Trec increases? • efficiency decreases

• What is the maximum efficiency?   Dr. Louie

40

CSP Efficiency

Receiver Efficiency

Efficiency (%)

100 80

C = 1000

60

C = 100

40

C = 10

20 0

0

Stagnation temp

500

1000

1500

2000

Receiver Temp (C)

With: Tamb = 20 C; e =  = .95; GDNI =770 W/m2 Dr. Louie

41

CSP Efficiency • CSPs use heat engines • System efficiency: hCSP  hChrec

• Carnot efficiency increases with temperature hC 

Trec  Tamb Trec

• Which efficiency dominates?

Dr. Louie

42

CSP Efficiency

Total CSP Efficiency

Efficiency (%)

100 80 60

C = 1000

40

C = 100

20 0

C = 10 0

500

1000

1500

2000

Receiver Temp (C)

Dr. Louie

43

CSP Efficiency Example • A typical concentration ratio for a PTC CSP is 70. Find the receiver efficiency, Carnot efficiency and total efficiency if: Trec = 400 oC, Tamb = 20 oC; e =  = 1; GDNI =800 W/m2

Dr. Louie

44

CSP Efficiency Example • A typical concentration ratio for a PTC CSP is 70. Find the receiver efficiency, Carnot efficiency and total efficiency if: Trec = 400 oC, Tamb = 20 oC; e =  = 1; GDNI =800 W/m2

• Receiver efficiency: hrec

4 4  (Trec  Tamb )     e  CG DNI  

Dr. Louie

45

CSP Efficiency Example • A typical concentration ratio for a PTC CSP is 70. Find the receiver efficiency, Carnot efficiency and total efficiency if: Trec = 400 oC, Tamb = 20 oC; e =  = 1; GDNI =800 W/m2

• Receiver efficiency: hrec

4 4  (Trec  Tamb )  (6734  2934 )      e   1     76% CGDNI 70  800    

Dr. Louie

46

CSP Efficiency Example • A typical concentration ratio for a PTC CSP is 70. Find the receiver efficiency, Carnot efficiency and total efficiency if: Trec = 400 oC, Tamb = 20 oC; e =  = 1; GDNI =800 W/m2

• Carnot efficiency: hC 

Trec  Tamb Trec

Dr. Louie

47

CSP Efficiency Example • A typical concentration ratio for a PTC CSP is 70. Find the receiver efficiency, Carnot efficiency and total efficiency if: Trec = 400 oC, Tamb = 20 oC; e =  = 1; GDNI =800 W/m2

• Carnot efficiency: hC 

Trec  Tamb  673  293    56%  Trec  673 

Dr. Louie

48

CSP Efficiency Example • A typical concentration ratio for a PTC CSP is 70. Find the receiver efficiency, Carnot efficiency and total efficiency if: Trec = 400 oC, Tamb = 20 oC; e =  = 1; GDNI =800 W/m2

• Total efficiency: hCSP  hChrec

Dr. Louie

49

CSP Efficiency Example • A typical concentration ratio for a PTC CSP is 70. Find the receiver efficiency, Carnot efficiency and total efficiency if: Trec = 400 oC, Tamb = 20 oC; e =  = 1; GDNI =800 W/m2

• Total efficiency: hCSP  hChrec  42%

Dr. Louie

50

CSP Efficiency

Total CSP Efficiency

Efficiency (%)

100 80 60

C = 70

40 20 0

0

500

1000

1500

2000

Receiver Temp (C) Dr. Louie

51

Suggest Documents