US2009078519A1PendingUtilityA1

Vibration damping device

Assignee: CARCATERRA ANTONIOPriority: Mar 31, 2005Filed: Mar 31, 2006Published: Mar 26, 2009
Est. expiryMar 31, 2025(expired)· nominal 20-yr term from priority
F16F 15/005F16F 7/1028F16F 7/10
45
PatentIndex Score
0
Cited by
0
References
0
Claims

Abstract

The damping device comprises a cluster of resonators with a predetermined frequency distribution, that, when attached to a main or “master” structure, is capable of absorbing irreversibly its vibrational or/and acoustic energy produced by a vi 5 brating body. the density of natural frequencies of the plurality of resonators is comprised within a curve that lies below the envelope curve determined by the formula, e( )=1/−1.

Claims

exact text as granted — not AI-modified
1 . Vibration damping device for damping vibrations of a vibrating or oscillating entity, e.g. a body or a structure or a gas mass, adapted to be connected to the vibrating entity, 
     the vibrating entity defining at least one respective natural frequency (ω M ), 
     the damping device comprises a predetermined plurality (N) of resonators, 
     the plurality (N) of resonators have respective natural frequencies (ω N ), with values close to a curve determined by a first formula 
     
       
         
           
             
               
                 
                   δ 
                   opt 
                 
                 / 
                 N 
               
               = 
               
                 
                   1 
                   
                     
                       2 
                        
                       π 
                     
                   
                 
                  
                 exp 
                  
                 
                   { 
                   
                     - 
                     
                       
                         
                           1 
                           2 
                         
                          
                         
                           [ 
                           
                             
                               ( 
                               
                                 σ 
                                 / 
                                 r 
                               
                               ) 
                             
                             - 
                             
                               ( 
                               
                                 I 
                                 / 
                                 r 
                               
                               ) 
                             
                           
                           ] 
                         
                       
                       2 
                     
                   
                   } 
                 
                  
                 
                   
                      
                     
                       ( 
                       
                         σ 
                         / 
                         r 
                       
                       ) 
                     
                   
                   
                      
                     Ω 
                   
                 
               
             
             , 
             
               
 
             
              
             
               
                 σ 
                 / 
                 r 
               
               = 
               
                 
                   
                     m 
                      
                     
                         
                     
                      
                     
                       ω 
                       M 
                       3 
                     
                   
                   r 
                 
                  
                 
                   Ω 
                   3 
                 
                  
                 sin 
                  
                 
                     
                 
                  
                 
                   Ω 
                    
                   
                     ( 
                     
                       
                         ω 
                         M 
                       
                        
                       
                         t 
                         0 
                       
                     
                     ) 
                   
                 
               
             
           
         
       
     
     where mω M   3 /r, I/r and t 0 =π(4ω M ) are the parameters defining the first formula, 
     the density of natural frequencies of the plurality of resonators is comprised within a curve that lies below the envelope curve determined by a second formula,
     e (Ω)=1/|Ω−1| 
 
     where Ω=ω N /ω M  is a nondimensional frequency. 
   
   
       2 . Damping device according to  claim 1  wherein the value of mω M   3 /r is comprised in the range from 2 to 20. 
   
   
       3 . Damping device according to  claim 1  wherein the value of I/r is comprised in the range from 0.94 to 14. 
   
   
       4 . Device according to  claim 1 , wherein the resonators are five or more. 
   
   
       5 . Device according to  claim 1 , wherein the resonators are fixed to an own support structure. 
   
   
       6 . Device according to  claim 1 , wherein there are provided means for adjusting the natural frequency of the resonators. 
   
   
       7 . Device according to  claim 6 , wherein the resonators comprise electromechanical circuits. 
   
   
       8 . Device according to  claim 6  wherein the resonators comprise acoustic ducts. 
   
   
       9 . Device according to  claim 6 , wherein the resonators comprise solid masses. 
   
   
       10 . Device according to  claim 9 , wherein the solid masses are shaped as beams. 
   
   
       11 . A body or structure made at least partially of a micro-structured material incorporating one or more damping devices according to  claim 1 . 
   
   
       12 . A body or structure according to  claim 12  wherein the damping devices are arranged according to a matrix and are fixed to the microstructured material. 
   
   
       13 . A system for recovering wave energy incorporating the damping device according to  claim 1 . 
   
   
       14 . A system for damping vibrations in floating vessels incorporating the damping device according to  claim 1 . 
   
   
       15 . A system for damping vibrations in buildings incorporating the damping device according to  claim 1 .

Join the waitlist — get patent alerts

Track US2009078519A1 — get alerts on status changes and closely related new filings.

We store only your email — no account needed. See our privacy policy.