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SOLAR THERMAL POWER!
               GEEN 4830 – ECEN 5007!




4. Fundamentals of solar thermal concentrating systems!



                    Manuel A. Silva Pérez
                                        !
                      silva@esi.us.es !
Solar Thermal Concentrating
       Systems
       Systems that make use of solar energy by first
           concentrating solar radiation and then converting it
           to thermal energy
       }  Uses:
         }    Electricity (Solar Thermal Power)
         }    Industrial Process Heat
         }    Absorption cooling
         }    Chemical processes
         }    …




1	

                            GEEN 4830 – ECEN 5007	

   07/07/11
Solar energy

       }    Abundant
       }    High-quality energy

       }    Variable (on time)
       }    Unevenly distributed (on space)
       }    Low density




2	

                         GEEN 4830 – ECEN 5007	

   07/07/11
Why high temperature?




3	

              GEEN 4830 – ECEN 5007	

   07/07/11
The sun as a heat source




4	

               GEEN 4830 – ECEN 5007	

   07/07/11
Why concentrate solar radiation?




5	

               GEEN 4830 – ECEN 5007	

   07/07/11
Ideal concentrating system
                                 }    The receiver (or absorber)
                                       converts concentrated
                                       solar radiation to thermal
                                       energy (heat)
                                 }    An ideal receiver may be
                                       characterized as a
                                       blackbody, which has only
                                       radiative losses




6	

             GEEN 4830 – ECEN 5007	

              07/07/11
Geometrical concentration ratio
       }    The geometrical
             concentration
             ratio, Cg, is
             defined as
                       A                                       Concentrator	
  
                  Cg = C
                      Aabs



       Where Aabs is the
        receiver (or
                                                          Collec'on	
  
        absorber) area                                      area	
  
                                                                             Absorp'on	
  
        and Ac is the                                                           area	
  
        collection area.


7	

                           GEEN 4830 – ECEN 5007	

                   07/07/11
Optical efficiency of the receiver




8	

                 GEEN 4830 – ECEN 5007	

   07/07/11
Ideal concentrator
       }  The maximum theoretical optical efficiency (when
           Tabs≥TSky) is the effective absorptivity of the receiver.
       }  The higher the concentrated solar flux (C*I), the better
           the optical efficiency.
       }  The higher the absorber temperature, the higher the
           radiative loss and, therefore, optical efficiency is lower.
       }  The higher the effective emissivity, ε, the lower the
           optical efficiency.




9	

                        GEEN 4830 – ECEN 5007	

       07/07/11
Global efficiency of the ideal concentrating
system




10	

             GEEN 4830 – ECEN 5007	

   07/07/11
Ideal concentrating system
        }  For each value of the geometrical concentration ratio,
            there is an optimum temperature.
        }  The higher the geometrical concentration ratio, the
            higher the optimum temperature and the global
            efficiency.




11	

                       GEEN 4830 – ECEN 5007	

     07/07/11
Concentration limits

}      The Sun is not a point light source.
        Seen From the Earth, is a disk of
        apparent diameter θS ≈ 32’.
}      The maximum concentration ratio is
        given by                                                                  32’	

                           n′2
              C max,3D = 2 2
                        n sen θ S                              32’	

                                                                                      Focus	
  
Where n and n’ are the refractive indices of
 the media that the light crosses before
 and after the reflection on the
 concentrator surface



      12	

                         GEEN 4830 – ECEN 5007	

            07/07/11
Types of concentrating systems
        }    Line focus (2D)
              }    Parabolic troughs; CLFR


          Cmáx,2 D = 1/ sin θ S

        }    Point focus (3D)
              }    Central receiver systems,
                    parabolic concentrators
                    (dishes)

        Cmáx ,3D = 1 / sin θ S         2



13	

                                      GEEN 4830 – ECEN 5007	

   07/07/11
Real concentrating systems




                                         Theoretical
                                         3D: < 46200
                                         2D: < 215

14	

               GEEN 4830 – ECEN 5007	

           07/07/11

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Cu stp 04_fundamentals

  • 1. SOLAR THERMAL POWER! GEEN 4830 – ECEN 5007! 4. Fundamentals of solar thermal concentrating systems! Manuel A. Silva Pérez ! silva@esi.us.es !
  • 2. Solar Thermal Concentrating Systems Systems that make use of solar energy by first concentrating solar radiation and then converting it to thermal energy }  Uses: }  Electricity (Solar Thermal Power) }  Industrial Process Heat }  Absorption cooling }  Chemical processes }  … 1 GEEN 4830 – ECEN 5007 07/07/11
  • 3. Solar energy }  Abundant }  High-quality energy }  Variable (on time) }  Unevenly distributed (on space) }  Low density 2 GEEN 4830 – ECEN 5007 07/07/11
  • 4. Why high temperature? 3 GEEN 4830 – ECEN 5007 07/07/11
  • 5. The sun as a heat source 4 GEEN 4830 – ECEN 5007 07/07/11
  • 6. Why concentrate solar radiation? 5 GEEN 4830 – ECEN 5007 07/07/11
  • 7. Ideal concentrating system }  The receiver (or absorber) converts concentrated solar radiation to thermal energy (heat) }  An ideal receiver may be characterized as a blackbody, which has only radiative losses 6 GEEN 4830 – ECEN 5007 07/07/11
  • 8. Geometrical concentration ratio }  The geometrical concentration ratio, Cg, is defined as A Concentrator   Cg = C Aabs Where Aabs is the receiver (or Collec'on   absorber) area area   Absorp'on   and Ac is the area   collection area. 7 GEEN 4830 – ECEN 5007 07/07/11
  • 9. Optical efficiency of the receiver 8 GEEN 4830 – ECEN 5007 07/07/11
  • 10. Ideal concentrator }  The maximum theoretical optical efficiency (when Tabs≥TSky) is the effective absorptivity of the receiver. }  The higher the concentrated solar flux (C*I), the better the optical efficiency. }  The higher the absorber temperature, the higher the radiative loss and, therefore, optical efficiency is lower. }  The higher the effective emissivity, ε, the lower the optical efficiency. 9 GEEN 4830 – ECEN 5007 07/07/11
  • 11. Global efficiency of the ideal concentrating system 10 GEEN 4830 – ECEN 5007 07/07/11
  • 12. Ideal concentrating system }  For each value of the geometrical concentration ratio, there is an optimum temperature. }  The higher the geometrical concentration ratio, the higher the optimum temperature and the global efficiency. 11 GEEN 4830 – ECEN 5007 07/07/11
  • 13. Concentration limits }  The Sun is not a point light source. Seen From the Earth, is a disk of apparent diameter θS ≈ 32’. }  The maximum concentration ratio is given by 32’ n′2 C max,3D = 2 2 n sen θ S 32’ Focus   Where n and n’ are the refractive indices of the media that the light crosses before and after the reflection on the concentrator surface 12 GEEN 4830 – ECEN 5007 07/07/11
  • 14. Types of concentrating systems }  Line focus (2D) }  Parabolic troughs; CLFR Cmáx,2 D = 1/ sin θ S }  Point focus (3D) }  Central receiver systems, parabolic concentrators (dishes) Cmáx ,3D = 1 / sin θ S 2 13 GEEN 4830 – ECEN 5007 07/07/11
  • 15. Real concentrating systems Theoretical 3D: < 46200 2D: < 215 14 GEEN 4830 – ECEN 5007 07/07/11