US2025163692A1PendingUtilityA1

Splash Reducing Surfaces

Assignee: HURD RANDYPriority: Nov 22, 2023Filed: Nov 22, 2024Published: May 22, 2025
Est. expiryNov 22, 2043(~17.3 yrs left)· nominal 20-yr term from priority
E03D 13/005E03D 13/00
43
PatentIndex Score
0
Cited by
0
References
0
Claims

Abstract

Systems and methods for reducing splashing of a liquid impinging on a surface include two sidewalls symmetrically oriented about a vertical plane. The sidewalls are joined along the vertical plane defining a back corner of a splash reducing surface. Each sidewall forms an angle less than a critical angle relative to a horizontal line extending from the sidewall to a vertical axis. The vertical axis is on the vertical plane at a specified distance from the back corner.

Claims

exact text as granted — not AI-modified
What is claimed is: 
     
         1 . A splash reducing surface comprising:
 two sidewalls symmetrically oriented about a vertical plane, the sidewalls being joined along the vertical plane defining a back corner of the splash reducing surface, each sidewall forming an angle less than a critical angle relative to a horizontal line extending from the sidewall to a vertical axis, the vertical axis being on the vertical plane at a specified distance from the back corner.   
     
     
         2 . The splash reducing surface of  claim 1 , wherein the sidewalls form the angle less than the critical angle relative to the horizontal line for a range of rotation angles of the horizontal line relative to the vertical plane. 
     
     
         3 . The splash reducing surface of  claim 1 , wherein the two sidewalls form an upper portion having a cross section in a horizontal plane, and wherein the splash reducing surface further comprises a lower portion joined to the upper portion and wherein a cross-section of the lower portion is continuous with the cross-section of the upper portion translated along a curve. 
     
     
         4 . The splash reducing surface of  claim 3 , wherein the splash reducing surface is a urinal. 
     
     
         5 . The splash reducing surface of  claim 4 , further comprising: a drain formed in the lower portion. 
     
     
         6 . The splash reducing surface of  claim 1 , wherein the sidewalls of the splash reducing surface are defined by 
       
         
           
             
               
                 r 
                 = 
                 
                   B 
                   ⁢ 
                   
                     exp 
                     ⁡ 
                     ( 
                     
                       α 
                       Θ 
                     
                     ) 
                   
                 
               
               , 
             
           
         
         where r is a distance from the vertical axis to the sidewall, B is the specified distance from the back corner, α is an azimuthal angle of r relative to the vertical plane, and Θ=±tan θ is the tangent value of the critical angle θ. 
       
     
     
         7 . The splash reducing surface of  claim 1 , wherein the critical angle is 40 degrees or less. 
     
     
         8 . The splash reducing surface of  claim 1 , wherein the critical angle is 30 degrees or less. 
     
     
         9 . A urinal comprising:
 a bowl comprising:
 a back surface forming an angle less than a critical angle between a line extending from a fluid origination point to the back surface, the fluid origination point being a specified distance from the back surface and a specified height from a bottom of the bowl; 
 two sidewalls, each sidewall forming a sidewall angle between a central vertical plane including the fluid origination point and the sidewall; and 
 a front wall joining the two sidewalls and a bottom portion of the back surface, wherein the two sidewalls and the back surface define an opening. 
   
     
     
         10 . The urinal of  claim 9 , wherein the line is a parabolic curve. 
     
     
         11 . The urinal of  claim 9 , wherein the back surface is defined by 
       
         
           
             
               
                 C 
                 = 
                 
                   
                     
                       3 
                       
                         
                           
                             8 
                             ⁢ 
                             
                               Θ 
                               2 
                             
                           
                           - 
                           1 
                         
                       
                     
                     ⁢ 
                     arc 
                     ⁢ 
                     
                       tan 
                       ⁡ 
                       ( 
                       
                         
                           
                             4 
                             ⁢ 
                             Θ 
                             ⁢ 
                             z 
                           
                           - 
                           r 
                         
                         
                           r 
                           ⁢ 
                           
                             
                               
                                 8 
                                 ⁢ 
                                 
                                   Θ 
                                   2 
                                 
                               
                               - 
                               1 
                             
                           
                         
                       
                       ) 
                     
                   
                   + 
                   
                     
                       1 
                       2 
                     
                     ⁢ 
                     
                       ln 
                       ⁡ 
                       ( 
                       
                         
                           2 
                           ⁢ 
                           Θ 
                           ⁢ 
                           
                             z 
                             2 
                           
                         
                         - 
                         rz 
                         + 
                         
                           Θ 
                           ⁢ 
                           r 
                         
                       
                       ) 
                     
                   
                 
               
               , 
             
           
         
         where and Θ=±tan θ is the tangent value of the critical angle θ, r is a distance between the fluid origination point and the back surface, z is a vertical distance relative to the fluid origination point, and C is a constant related to the specified distance. 
       
     
     
         12 . The urinal of  claim 9 , wherein the critical angle is 30 degrees or less. 
     
     
         13 . A method for forming a splash suppressing surface, the method comprising:
 determining a fluid origination point a specified length from a back portion of the splash reducing surface;   defining a surface that intersects a line extending from the fluid origination point, the line intersecting the surface at an angle less than a critical angle; and   fabricating the defined surface to form the splash suppressing surface.   
     
     
         14 . The method of  claim 13 , wherein fabricating the defined surface comprises fabricating a porcelain casting of the defined surface. 
     
     
         15 . The method of  claim 13 , wherein the critical angle is 30 degrees or less. 
     
     
         16 . The method of  claim 13 , wherein the back surface is defined by 
       
         
           
             
               
                 C 
                 = 
                 
                   
                     
                       3 
                       
                         
                           
                             8 
                             ⁢ 
                             
                               Θ 
                               2 
                             
                           
                           - 
                           1 
                         
                       
                     
                     ⁢ 
                     arc 
                     ⁢ 
                     
                       tan 
                       ⁡ 
                       ( 
                       
                         
                           
                             4 
                             ⁢ 
                             Θ 
                             ⁢ 
                             z 
                           
                           - 
                           r 
                         
                         
                           r 
                           ⁢ 
                           
                             
                               
                                 8 
                                 ⁢ 
                                 
                                   Θ 
                                   2 
                                 
                               
                               - 
                               1 
                             
                           
                         
                       
                       ) 
                     
                   
                   + 
                   
                     
                       1 
                       2 
                     
                     ⁢ 
                     
                       ln 
                       ⁡ 
                       ( 
                       
                         
                           2 
                           ⁢ 
                           Θ 
                           ⁢ 
                           
                             z 
                             2 
                           
                         
                         - 
                         rz 
                         + 
                         
                           Θ 
                           ⁢ 
                           r 
                         
                       
                       ) 
                     
                   
                 
               
               , 
             
           
         
         where and Θ=±tan θ is a tangent value of the critical angle θ, r is a distance between the fluid origination point and the back surface, z is a vertical distance relative to the fluid origination point, and C is a constant related to the specified distance. 
       
     
     
         17 . The method of  claim 13 , wherein the surface is defined by 
       
         
           
             
               
                 r 
                 = 
                 
                   B 
                   ⁢ 
                   
                     exp 
                     ⁡ 
                     ( 
                     
                       α 
                       Θ 
                     
                     ) 
                   
                 
               
               , 
             
           
         
       
       where r is a distance from the fluid origination point to the surface, B is the specified length from the back portion, α is an azimuthal angle of r relative to a central vertical plane, and Θ=±tan θ is a tangent value of the critical angle θ. 
     
     
         18 . The method of  claim 13  wherein the surface is defined by rotating the line through a range of angles relative to a central vertical plane containing the fluid origination point. 
     
     
         19 . The method of  claim 18 , wherein the surface is a first surface, and the method further comprises:
 defining a second surface that is a mirror image of the first surface across the central vertical plane,   wherein fabricating the surface comprises fabricating the first surface and the second surface together to form a unified body.   
     
     
         20 . The method of  claim 19 , wherein the first surface and the second surface form a urinal.

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