US2013175013A1PendingUtilityA1

Heat exchanger

Assignee: YOSHIOKA SHUNPriority: Sep 29, 2010Filed: Sep 27, 2011Published: Jul 11, 2013
Est. expirySep 29, 2030(~4.2 yrs left)· nominal 20-yr term from priority
B23K 1/203F28D 1/05383B23K 2103/10F28F 2275/122F28F 9/0243F28F 9/0224F28F 3/086F28D 2021/0068F28D 1/05333B23K 2101/14F28F 1/022F28F 9/002F28F 9/0278B23K 1/0012
35
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Claims

Abstract

A heat exchanger includes a pair of headers extending in an up-and-down direction to carry refrigerant, and plural flat tubes connected to the headers at different height positions and extending along a direction intersecting a longitudinal direction of the headers. Each header includes a first member and a flat tube holding member. The first member has a main flow path, and refrigerant connection flow paths to circulate refrigerant between the main flow path and plural refrigerant flow paths formed in the flat tubes. The flat tube holding member holds the flat tubes. End portions of the flat tubes are adhered to the flat tube holding member. Intermediate flow paths interconnect the refrigerant connection flow paths and the plural refrigerant flow paths in the flat tubes. The intermediate flow paths are formed in at least one of the headers and the flat tubes.

Claims

exact text as granted — not AI-modified
1 . A heat exchanger comprising:
 a pair of headers extending in an up-and-down direction, the pair of headers being configured to carry a refrigerant flow therein; and   plural flat tubes connected to the headers at different height positions, the plural flat tubes extending along a direction intersecting a longitudinal direction of the headers,   each of the headers including
 a first member having a main flow path extending in the up-and-down direction and configured to carry the refrigerant flow therein, and refrigerant connection flow paths extending from the main flow path to an end surface in the direction intersecting the longitudinal direction in order to circulate the refrigerant flow between the main flow path and plural refrigerant flow paths formed in the flat tubes, and 
 a flat tube holding member with end portions of the flat tubes adhered thereto, the flat tube holding member holding the flat tubes, and 
   intermediate flow paths interconnecting the refrigerant connection flow paths and the plural refrigerant flow paths in the flat tubes, the intermediate flow paths being formed in at least one of
 the headers and 
 the flat tubes. 
   
     
     
         2 . The heat exchanger according to  claim 1 , wherein
 a width of the intermediate flow paths is no more than a width of the flat tubes.   
     
     
         3 . The heat exchanger according to  claim 1 , wherein
 each of the headers further includes a second member sandwiched between the first member and the flat tube holding member, and   in a case where the intermediate flow paths are at least partially formed in the headers, the intermediate flow paths are at least partially formed in the second member.   
     
     
         4 . The heat exchanger according to  claim 1 , wherein
 in a case where
 L1 is a length in a direction orthogonal to a longitudinal direction of the first member of a main flow path forming portion forming the main flow path, 
 π is pi, 
 g is a gravitational acceleration, 
 m is a circulating volume of refrigerant in a gas-liquid two-phase state flowing through the main flow path, 
 x is an inlet quality, the inlet quality being a ratio of a mass flow rate of the refrigerant in a gas-phase state with respect to a total mass flow rate of the refrigerant in a gas-liquid two-phase state inside an inlet header of the pair of headers, the refrigerant flows from outside into the inlet header, 
 ρ G  is a density of the refrigerant in a gas-phase state flowing through the main flow path, 
 D is a distance between the uppermost flat tube and a lowermost flat tube, and 
 C 1  and C 2  are constants, 
   
       a relationship 
       
         
           
             
               
                 
                   4 
                   
                     
                       C 
                       2 
                     
                     · 
                     π 
                   
                 
                  
                 
                   
                     m 
                     · 
                     x 
                   
                   
                     
                       ρ 
                       G 
                     
                      
                     
                       g 
                       0.5 
                     
                   
                 
               
               ≤ 
               
                 L 
                  
                 
                     
                 
                  
                 
                   1 
                   2 
                 
                  
                 
                   D 
                   0.5 
                 
               
               ≤ 
               
                 
                   4 
                   
                     
                       C 
                       1 
                     
                     · 
                     π 
                   
                 
                  
                 
                   
                     m 
                     · 
                     x 
                   
                   
                     
                       ρ 
                       G 
                     
                      
                     
                       g 
                       0.5 
                     
                   
                 
               
             
           
         
       
       holds true, and
 C 1 =0.16 and C 2 =1.5. 
 
     
     
         5 . The heat exchanger according to  claim 1 , wherein
 in a case where
 L1 is a length in a direction orthogonal to a longitudinal direction of the first member of a main flow path forming portion forming the main flow path, 
 π is pi, 
 g is a gravitational acceleration, 
 m is a circulating volume of refrigerant in a gas-liquid two-phase state flowing through the main flow path, 
 x is an inlet quality, the inlet quality being a ratio of a mass flow rate of the refrigerant in a gas-phase state with respect to a total mass flow rate of the refrigerant in a gas-liquid two-phase state inside an inlet header of the pair of headers, the refrigerant flows from outside into the inlet header, 
 ρ G  is a density of the refrigerant in a gas-phase state flowing through the main flow path, 
 D is a distance between the uppermost flat tube and a lowermost flat tube, and 
 C 1  and C 2  are constants, 
   
       a relationship 
       
         
           
             
               
                 
                   4 
                   
                     
                       C 
                       2 
                     
                     · 
                     π 
                   
                 
                  
                 
                   
                     m 
                     · 
                     x 
                   
                   
                     
                       ρ 
                       G 
                     
                      
                     
                       g 
                       0.5 
                     
                   
                 
               
               ≤ 
               
                 L 
                  
                 
                     
                 
                  
                 
                   1 
                   2 
                 
                  
                 
                   D 
                   0.5 
                 
               
               ≤ 
               
                 
                   4 
                   
                     
                       C 
                       1 
                     
                     · 
                     π 
                   
                 
                  
                 
                   
                     m 
                     · 
                     x 
                   
                   
                     
                       ρ 
                       G 
                     
                      
                     
                       g 
                       0.5 
                     
                   
                 
               
             
           
         
       
       holds true, and
 C 1 =0.24 and C 2 =1.1. 
 
     
     
         6 . The heat exchanger according to  claim 3 , further comprising
 a securing member sandwiched between the flat tube holding member and the second member, the securing member securing the end portions of the plural flat tubes together with the flat tube holding member.   
     
     
         7 . The heat exchanger according to  claim 3 , wherein
 the second member has a flat panel shape.   
     
     
         8 . The heat exchanger according to  claim 3 , wherein
 the flat tube holding member covers the second member, and both ends of the flat tube holding member are in contact with and brazed to the first member.   
     
     
         9 . The heat exchanger according to  claim 1 , wherein
 plural holes are formed in the that tube holding member.   
     
     
         10 . The heat exchanger according to  claim 1 , wherein
 a length in a direction orthogonal to a longitudinal direction of the first member, of a main flow path forming portion forming the main flow path, is smaller than a width of the flat tubes.   
     
     
         11 . The heat exchanger according to  claim 2 , wherein
 each of the headers further includes a second member sandwiched between the first member and the flat tube holding member, and   in a case where the intermediate flow paths are at least partially formed in the headers, the intermediate flow paths are at least partially formed in the second member.   
     
     
         12 . The heat exchanger according to  claim 2 , wherein
 in a case where
 L1 is a length in a direction orthogonal to a longitudinal direction of the first member of a main flow path forming portion forming the main flow path, 
 π is pi, 
 g is a gravitational acceleration, 
 m is a circulating volume of refrigerant in a gas-liquid two-phase state flowing through the main flow path, 
 x is an inlet quality, the inlet quality being a ratio of a mass flow rate of the refrigerant in a gas-phase state with respect to a total mass flow rate of the refrigerant in a gas-liquid two-phase state inside an inlet header of the pair of headers, the refrigerant flows from outside into the inlet header, 
 ρ G  is a density of the refrigerant in a gas-phase state flowing through the main flow path, 
 D is a distance between the uppermost flat tube and a lowermost flat tube, and 
 C 1  and C 2  are constants, 
   
       a relationship 
       
         
           
             
               
                 
                   4 
                   
                     
                       C 
                       2 
                     
                     · 
                     π 
                   
                 
                  
                 
                   
                     m 
                     · 
                     x 
                   
                   
                     
                       ρ 
                       G 
                     
                      
                     
                       g 
                       0.5 
                     
                   
                 
               
               ≤ 
               
                 L 
                  
                 
                     
                 
                  
                 
                   1 
                   2 
                 
                  
                 
                   D 
                   0.5 
                 
               
               ≤ 
               
                 
                   4 
                   
                     
                       C 
                       1 
                     
                     · 
                     π 
                   
                 
                  
                 
                   
                     m 
                     · 
                     x 
                   
                   
                     
                       ρ 
                       G 
                     
                      
                     
                       g 
                       0.5 
                     
                   
                 
               
             
           
         
       
       holds true, and
 C 1 =0.16 and C 2 =1.5. 
 
     
     
         13 . The heat exchanger according to  claim 2 , wherein
 in a case where
 L1 is a length in a direction orthogonal to a longitudinal direction of the first member of a main flow path forming portion forming the main flow path, 
 π is pi, 
 g is a gravitational acceleration, 
 m is a circulating volume of refrigerant in a gas-liquid-phase state flowing through the main flow path, 
 x is an inlet quality, the inlet quality being a ratio of a mass flow rate of the refrigerant in a gas-phase state with respect to a total mass flow rate of the refrigerant in a gas-liquid two-phase state inside an inlet header of the pair of headers, the refrigerant flows from outside into the inlet header, 
 ρ G  is a density of the refrigerant in a gas-phase state flowing through the main flow path, 
 D is a distance between the uppermost flat tube and a lowermost flat tube, and 
 C 1  and C 2  are constants, 
   
       a relationship 
       
         
           
             
               
                 
                   4 
                   
                     
                       C 
                       2 
                     
                     · 
                     π 
                   
                 
                  
                 
                   
                     m 
                     · 
                     x 
                   
                   
                     
                       ρ 
                       G 
                     
                      
                     
                       g 
                       0.5 
                     
                   
                 
               
               ≤ 
               
                 L 
                  
                 
                     
                 
                  
                 
                   1 
                   2 
                 
                  
                 
                   D 
                   0.5 
                 
               
               ≤ 
               
                 
                   4 
                   
                     
                       C 
                       1 
                     
                     · 
                     π 
                   
                 
                  
                 
                   
                     m 
                     · 
                     x 
                   
                   
                     
                       ρ 
                       G 
                     
                      
                     
                       g 
                       0.5 
                     
                   
                 
               
             
           
         
       
       holds true, and
 C 1 =0.24 and C 2 =1.1. 
 
     
     
         14 . The heat exchanger according to  claim 3 , wherein
 in a case where
 L1 is a length in a direction orthogonal to a longitudinal direction of the first member of a main flow path forming portion forming the main flow path, 
 π is pi, 
 g is a gravitational acceleration, 
 m is a circulating volume of refrigerant in a gas-liquid two-phase state flowing through the main flow path, 
 x is an inlet quality, the inlet quality being a ratio of a mass flow rate of the refrigerant in a gas-phase state with respect to a total mass flow rate of the refrigerant in a gas-liquid two-phase state inside an inlet header of the pair of headers, the refrigerant flows from outside into the inlet header, 
 ρ G  is a density of the refrigerant in a gas-phase state flowing through the main flow path, 
 D is a distance between the uppermost flat tube and a lowermost flat tube, and 
 C 1  and C 2  are constants, 
   
       a relationship 
       
         
           
             
               
                 
                   4 
                   
                     
                       C 
                       2 
                     
                     · 
                     π 
                   
                 
                  
                 
                   
                     m 
                     · 
                     x 
                   
                   
                     
                       ρ 
                       G 
                     
                      
                     
                       g 
                       0.5 
                     
                   
                 
               
               ≤ 
               
                 L 
                  
                 
                     
                 
                  
                 
                   1 
                   2 
                 
                  
                 
                   D 
                   0.5 
                 
               
               ≤ 
               
                 
                   4 
                   
                     
                       C 
                       1 
                     
                     · 
                     π 
                   
                 
                  
                 
                   
                     m 
                     · 
                     x 
                   
                   
                     
                       ρ 
                       G 
                     
                      
                     
                       g 
                       0.5 
                     
                   
                 
               
             
           
         
       
       holds true, and
 C 1 =0.16 and C 2 =1.5. 
 
     
     
         15 . The heat exchanger according to  claim 3 , wherein
 in a case where
 L1 is a length in a direction orthogonal to a longitudinal direction of the first member of a main flow path forming portion forming the main flow path, 
 π is pi, 
 g is a gravitational acceleration, 
 m is a circulating volume of refrigerant in a gas-liquid two-phase state flowing through the main flow path, 
 x is an inlet quality, the inlet quality being a ratio of a mass flow rate of the refrigerant in a gas-phase state with respect to a total mass flow rate of the refrigerant in a gas-liquid two-phase state inside an inlet header of the pair of headers, the refrigerant flows from outside into the inlet header, 
 ρ G  is a density of the refrigerant in a gas-phase state flowing through the main flow path, 
 D is a distance between the uppermost flat tube and a lowermost flat tube, and 
 C 1  and C 2  are constants, 
   
       a relationship 
       
         
           
             
               
                 
                   4 
                   
                     
                       C 
                       2 
                     
                     · 
                     π 
                   
                 
                  
                 
                   
                     m 
                     · 
                     x 
                   
                   
                     
                       ρ 
                       G 
                     
                      
                     
                       g 
                       0.5 
                     
                   
                 
               
               ≤ 
               
                 L 
                  
                 
                     
                 
                  
                 
                   1 
                   2 
                 
                  
                 
                   D 
                   0.5 
                 
               
               ≤ 
               
                 
                   4 
                   
                     
                       C 
                       1 
                     
                     · 
                     π 
                   
                 
                  
                 
                   
                     m 
                     · 
                     x 
                   
                   
                     
                       ρ 
                       G 
                     
                      
                     
                       g 
                       0.5 
                     
                   
                 
               
             
           
         
       
       holds true, and
 C 1 =0.24 and C 2 =1.1. 
 
     
     
         16 . The heat exchanger according to  claim 6 , wherein
 the second member and the securing member have flat panel shapes.   
     
     
         17 . The heat exchanger according to  claim 6 , wherein
 the flat tube holding member covers one of
 the second member and 
 the second member and the securing member 
   
       from outside, and
 both ends of the flat tube holding member are in contact with and brazed to the first member. 
 
     
     
         18 . The heat exchanger according to  claim 7 , wherein
 the flat tube holding member covers one of
 the second member and 
 the second member and the securing member 
   
       from outside, and
 both ends of the flat tube holding member are in contact with and brazed to the first member.

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