US2015285534A1PendingUtilityA1

Solar collector with optimal profile for energy distribution on a tubular receiver

Assignee: UNIV KING FAHD PET & MINERALSPriority: Apr 2, 2014Filed: Apr 2, 2014Published: Oct 8, 2015
Est. expiryApr 2, 2034(~7.7 yrs left)· nominal 20-yr term from priority
F24J 2/12F24J 2002/1028Y10T29/49355F24S 23/70F24S 20/20F24S 2023/833Y02E10/40
47
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Claims

Abstract

The solar collector with optimal profile for energy distribution on a tubular receiver collects and distributes solar energy. Solar energy received from the sun can be modified by either being re-directed (reflection) or being redistributed. In the present invention energy is reflected and redistributed in a manner that yields a required energy variation over a surface. The receiver is a cylinder of known length and diameter. Longitudinal distribution of energy is specified by a user defined function. Circumferential distribution is assumed to be constant. Energy distribution is required to vary along the z axis of the receiver but remain constant in the circumferential direction. An axi-symmetric approach is used in which only one plane of the receiver in r and Z plane is considered. A geometric solution determines a reflecting surface that gives a required energy distribution along the z-axis. A complete reflector is designed by expanding the axi-symmetric behavior.

Claims

exact text as granted — not AI-modified
We claim: 
     
         1 . A solar collector with optimal profile for energy distribution on a tubular receiver, comprising:
 a reflector formed by a single, continuous parametric curve, the reflector having only one smooth reflecting surface;   a receiver through which heat carrying fluid circulates; and   wherein the receiver comprises at least one tube disposed along a focal axis defined by an aperture of the reflector to receive reflected solar energy directed by the reflector along the focal axis.   
     
     
         2 . The solar collector with optimal profile for energy distribution on a tubular receiver according to  claim 1 , wherein the single, continuous parametric curve of the reflector has a contour that conforms to a calculated solution using a system of equations characterized by the relations, 
       
         
           
             
               
                 
                   
                     r 
                     ab 
                   
                    
                   
                     B 
                     x 
                   
                 
                 = 
                 
                   
                     
                       Br 
                       2 
                     
                      
                     
                       sin 
                        
                       
                         ( 
                         θ 
                         ) 
                       
                     
                      
                     
                       cos 
                        
                       
                         ( 
                         θ 
                         ) 
                       
                     
                      
                     
                       
                          
                         θ 
                       
                       
                          
                         x 
                       
                     
                   
                   + 
                   
                     Br 
                      
                     
                       
                          
                         r 
                       
                       
                          
                         x 
                       
                     
                      
                     
                       
                         sin 
                         2 
                       
                        
                       
                         ( 
                         θ 
                         ) 
                       
                     
                   
                 
               
               , 
               
                 
 
               
                
               and 
             
           
         
         
           
             
               
                 
                   cot 
                    
                   
                     ( 
                     
                       θ 
                       / 
                       2 
                     
                     ) 
                   
                 
                 = 
                 
                   
                     
                       sin 
                        
                       
                         ( 
                         θ 
                         ) 
                       
                     
                     + 
                     
                       r 
                        
                       
                           
                       
                        
                       
                         cos 
                          
                         
                           ( 
                           θ 
                           ) 
                         
                       
                        
                       
                         
                            
                           θ 
                         
                         
                            
                           r 
                         
                       
                     
                   
                   
                     
                       
                          
                         x 
                       
                       
                          
                         r 
                       
                     
                     - 
                     
                       cos 
                        
                       
                         ( 
                         θ 
                         ) 
                       
                     
                     + 
                     
                       r 
                        
                       
                           
                       
                        
                       
                         sin 
                          
                         
                           ( 
                           θ 
                           ) 
                         
                       
                        
                       
                         
                            
                           θ 
                         
                         
                            
                           r 
                         
                       
                     
                   
                 
               
               , 
             
           
         
         where B is the solar flux falling on the aperture of the reflector, r ab  is the outer radius of a tubular receiver having length L, B x  is a specific profile of heat flux required over the surface of the tubular receiver, dx is a small length portion of the tubular receiver, r is the length of reflected solar ray, which falls on the tubular receiver at a distance x along the tubular receiver, becoming r+dr at a length of x+dx. 
       
     
     
         3 . The solar collector with optimal profile for energy distribution on a tubular receiver according to  claim 1 , wherein the tubular receiver is substantially cylindrical in shape. 
     
     
         4 . The solar collector with optimal profile for energy distribution on a tubular receiver according to  claim 1 , wherein the solar collector has an opening at its apex. 
     
     
         5 . The solar collector with optimal profile for energy distribution on a tubular receiver according to  claim 1 , wherein the heat carrying fluid is methane undergoing a steam methane reforming (SMR) reaction. 
     
     
         6 . The solar collector with optimal profile for energy distribution on a tubular receiver according to  claim 1 , wherein a horizontal lineal distance from an apex of the solar collector to an outer edge of the solar collector is approximately 6.7 meters to facilitate a quadratic energy distribution along the tubular receiver. 
     
     
         7 . The solar collector with optimal profile for energy distribution on a tubular receiver according to  claim 1 , wherein a horizontal lineal distance from an apex of the solar collector to an outer edge of the solar collector is approximately 0.043 meters to facilitate a constant energy distribution along the tubular receiver. 
     
     
         8 . A method for manufacturing a solar collector, the method comprising the steps of:
 (a) accumulating polynomial energy distribution requirement inputs, local solar flux density input, initial radius of the reflecting surface input, and length of the reactor input;   (b) feeding the inputs of step (a) to a computer executing a procedure that calculates a solution of a system of equations characterized by the relations,   
       
         
           
             
               
                 
                   
                     r 
                     ab 
                   
                    
                   
                     B 
                     x 
                   
                 
                 = 
                 
                   
                     
                       Br 
                       2 
                     
                      
                     
                       sin 
                        
                       
                         ( 
                         θ 
                         ) 
                       
                     
                      
                     
                       cos 
                        
                       
                         ( 
                         θ 
                         ) 
                       
                     
                      
                     
                       
                          
                         θ 
                       
                       
                          
                         x 
                       
                     
                   
                   + 
                   
                     Br 
                      
                     
                       
                          
                         r 
                       
                       
                          
                         x 
                       
                     
                      
                     
                       
                         sin 
                         2 
                       
                        
                       
                         ( 
                         θ 
                         ) 
                       
                     
                   
                 
               
               , 
               
                 
 
               
                
               and 
             
           
         
         
           
             
               
                 
                   
                     
                       sin 
                        
                       
                         ( 
                         θ 
                         ) 
                       
                     
                     + 
                     
                       r 
                        
                       
                           
                       
                        
                       
                         cos 
                          
                         
                           ( 
                           θ 
                           ) 
                         
                       
                        
                       
                         
                            
                           θ 
                         
                         
                            
                           r 
                         
                       
                     
                   
                   
                     
                       
                          
                         x 
                       
                       
                          
                         r 
                       
                     
                     - 
                     
                       cos 
                        
                       
                         ( 
                         θ 
                         ) 
                       
                     
                     + 
                     
                       r 
                        
                       
                           
                       
                        
                       
                         sin 
                          
                         
                           ( 
                           θ 
                           ) 
                         
                       
                        
                       
                         
                            
                           θ 
                         
                         
                            
                           r 
                         
                       
                     
                   
                 
                 = 
                 
                   cot 
                    
                   
                     ( 
                     
                       θ 
                       / 
                       2 
                     
                     ) 
                   
                 
               
               , 
             
           
         
       
       where B is the solar flux falling on the aperture of the reflector, r ab  is the outer radius of a tubular receiver having length L, B x  is a specific profile of heat flux required over the surface of the tubular receiver, dx is a small length portion of the tubular receiver, r is the length of reflected solar ray, which falls on the tubular receiver at a distance x along the tubular receiver, becoming r+dr at a length of x+dx wherein said system of equations produces a set of reflecting surface profile data points; and
 (c) feeding the set of reflecting surface profile data points to a computer aided numerically controlled manufacturing system, said computer aided numerically controlled manufacturing system producing a desired reflecting surface based on said inputs of step (a). 
 
     
     
         9 . The solar collector manufacturing method according to  claim 8 , further comprising the step of determining B x  according to an optimal heat flux profile for a steam methane reforming (SMR) reaction wherein the SMR reaction is approximated by a third order polynomial characterized by the relation,
     B   x =0.1281 x   3 −0.871 x   2 +2.806 x+ 49.7.
   
     
     
         10 . The solar collector manufacturing method according to  claim 9 , wherein the input step (a) further comprises:
 inputting radius of tubular absorber, r ab =0.00865 m;   inputting length of tubular absorber, L=12 m;   inputting initial radius r i =0.04 m; and   inputting solar flux, B=1 KW/m 2 .

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