US2019316998A1PendingUtilityA1

Evaluating device of flexural property of material, and evaluation method using thereof

Assignee: SAMSUNG ELECTRONICS CO LTDPriority: Nov 23, 2016Filed: Jun 25, 2019Published: Oct 17, 2019
Est. expiryNov 23, 2036(~10.3 yrs left)· nominal 20-yr term from priority
G01N 2203/0682G01N 2203/0075G01N 2203/0003G01N 2203/0012G01N 2203/028G01N 3/20G01N 2203/0218G01N 2203/0023G01N 2203/0282G01M 5/0041G01N 3/14G06F 17/10
63
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Claims

Abstract

An evaluating device of a flexural property includes a holder, a body disposed on the holder and capable of being moved along with a length of direction of the holder, a clamp coupled to the body to be rotated on the body and fixing a first side of the specimen to be evaluated, and a pressing part disposed over the clamp and pressing a second side of the specimen opposite to the first side and disposed upper than the first side of the specimen to bend the specimen, and an evaluation method of a flexural property of the bent specimen using the same.

Claims

exact text as granted — not AI-modified
What is claimed is: 
     
         1 . A method of evaluating flexural property of a bent specimen using a device for evaluating flexural property comprising:
 a holder,   a body disposed on the holder and capable of being moved along with a length direction of the holder,   a clamp coupled to the body and capable of being rotated on the body and fixing a first side of a specimen to be evaluated, and   a pressing part disposed on the clamp and pressing a second side of the specimen opposite to the first side and disposed upper than the first side of the specimen to bend the specimen,   the method comprising:   evaluating at least one of a strain L of the bent specimen, a folding stress σ f  applied to the bent specimen, a folding modulus Mf applied to the bent specimen, by using:   a thickness h of the bent specimen,   a length L″ of a first arc connecting a first point and a second point which are different from each other and applied with a principal stress corresponding to a half of a maximum principal stress applied to the bent specimen,   a length L′ of a first straight line connecting a shortest distance between the first point and the second point,   a curvature radius p of a virtual circle when the first arc is extended to set the virtual circle, and   a bending angle θ between the clamp and the lower surface of the pressing part.   
     
     
         2 . The method of  claim 1 , wherein the length L″ is represented by Equation 1: 
       
         
           
             
               
                 
                   
                     
                       L 
                       ′′ 
                     
                     = 
                     
                       
                         
                           ρ 
                            
                           
                               
                           
                            
                           π 
                            
                           
                               
                           
                            
                           θ 
                         
                         540 
                       
                       . 
                     
                   
                 
                 
                   
                     Equation 
                      
                     
                         
                     
                      
                     1 
                   
                 
               
             
           
         
       
     
     
         3 . The method of  claim 1 , wherein the length L′ is represented by Equation 2: 
       
         
           
             
               
                 
                   
                     
                       L 
                       ′ 
                     
                     = 
                     
                       2 
                        
                       ρ 
                        
                       
                           
                       
                        
                       sin 
                        
                       
                         
                           θ 
                           6 
                         
                         . 
                       
                     
                   
                 
                 
                   
                     Equation 
                      
                     
                         
                     
                      
                     2 
                   
                 
               
             
           
         
       
     
     
         4 . The method of  claim 1 , wherein the strain L is a parameter depending on only the bending angle θ. 
     
     
         5 . The method of  claim 1 , wherein the strain L is represented by Equation 3: 
       
         
           
             
               
                 
                   
                     
                       Δ 
                        
                       
                           
                       
                        
                       L 
                     
                     = 
                     
                       
                         ( 
                         
                           
                             
                               π 
                                
                               
                                   
                               
                                
                               θ 
                             
                             
                               1080 
                                
                               
                                   
                               
                                
                               sin 
                                
                               
                                 θ 
                                 6 
                               
                             
                           
                           - 
                           1 
                         
                         ) 
                       
                       × 
                       100. 
                     
                   
                 
                 
                   
                     Equation 
                      
                     
                         
                     
                      
                     3 
                   
                 
               
             
           
         
       
     
     
         6 . The method of  claim 1 , wherein the folding stress ρ f  is represented by Equation 4: 
       
         
           
             
               
                 
                   
                     
                       σ 
                       f 
                     
                     = 
                     
                       
                         3 
                          
                         
                           y 
                           ′ 
                         
                          
                         
                           L 
                           ′ 
                         
                          
                         F 
                       
                       
                         
                           whd 
                            
                           
                               
                           
                         
                         ′2 
                       
                     
                   
                 
                 
                   
                     Equation 
                      
                     
                         
                     
                      
                     4 
                   
                 
               
             
           
         
         wherein, in Equation 4, y′ is a parameter considering stress asymmetry of a specimen at each point, F is a force of the pressing part pressing the specimen, w is a length direction width of the specimen, and d′ a length of a second straight line connecting a halfway point of the first straight line with a halfway point of the first arc. 
       
     
     
         7 . The method of  claim 6 , wherein the parameter y′ is represented by Equation 5: 
       
         
           
             
               
                 
                   
                     
                       y 
                       ′ 
                     
                     = 
                     
                       
                         
                           
                             
                               ( 
                               
                                 10 
                                  
                                 h 
                               
                               ) 
                             
                             2 
                           
                            
                           
                             ( 
                             
                               1 
                               - 
                               
                                 cos 
                                  
                                 
                                   θ 
                                   6 
                                 
                               
                             
                             ) 
                           
                         
                         
                           
                             ρ 
                             2 
                           
                            
                           
                             ( 
                             
                               1 
                               - 
                               
                                 cos 
                                  
                                 
                                     
                                 
                                  
                                 30 
                                  
                                 ° 
                               
                             
                             ) 
                           
                         
                       
                       . 
                     
                   
                 
                 
                   
                     Equation 
                      
                     
                         
                     
                      
                     5 
                   
                 
               
             
           
         
       
     
     
         8 . The method of  claim 6 , wherein the length d′ is represented by Equation 6: 
       
         
           
             
               
                 
                   
                     
                       d 
                       ′ 
                     
                     = 
                     
                       
                         ρ 
                          
                         
                           ( 
                           
                             1 
                             - 
                             
                               cos 
                                
                               
                                 θ 
                                 6 
                               
                             
                           
                           ) 
                         
                       
                       . 
                     
                   
                 
                 
                   
                     Equation 
                      
                     
                         
                     
                      
                     6 
                   
                 
               
             
           
         
       
     
     
         9 . The method of  claim 1 , wherein the folding modulus M f  is a parameter depending on the thickness h, the curvature radius ρ, and the bending angle θ. 
     
     
         10 . The method of  claim 1 , wherein the folding modulus M f  is represented by Equation 7: 
       
         
           
             
               
                 
                   
                     
                       M 
                       f 
                     
                     = 
                     
                       
                         
                           4.8 
                           × 
                           
                             10 
                             4 
                           
                            
                           
                               
                           
                            
                           hF 
                            
                           
                               
                           
                            
                           sin 
                            
                           
                             θ 
                             6 
                           
                         
                         
                           w 
                            
                           
                               
                           
                            
                           
                             
                               ρ 
                               3 
                             
                              
                             
                               ( 
                               
                                 1 
                                 - 
                                 
                                   cos 
                                    
                                   
                                     θ 
                                     6 
                                   
                                 
                               
                               ) 
                             
                           
                         
                       
                       × 
                       
                         
                           ( 
                           
                             
                               sin 
                                
                               
                                 θ 
                                 6 
                               
                             
                             
                               πθ 
                               - 
                               
                                 1080 
                                  
                                 
                                     
                                 
                                  
                                 sin 
                                  
                                 
                                   θ 
                                   6 
                                 
                               
                             
                           
                           ) 
                         
                         . 
                       
                     
                   
                 
                 
                   
                     Equation 
                      
                     
                         
                     
                      
                     7 
                   
                 
               
             
           
         
       
     
     
         11 . The method of  claim 1 , wherein the bending angle θ is greater than 0 degree and equal to or less than 180 degrees.

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