US2004176680A1PendingUtilityA1

Assembly for heat treatment of biological tissues

Priority: Apr 20, 2001Filed: Apr 19, 2002Published: Sep 9, 2004
Est. expiryApr 20, 2021(expired)· nominal 20-yr term from priority
A61N 7/02A61B 2017/00084A61B 2090/374A61B 2017/0084
28
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Claims

Abstract

The invention concerns an assembly for heat treatment of a region of a biological tissue ( 410 ) comprising energy-generating means ( 100 ) to supply energy to the region; means ( 200 ) for measuring and recording spatial temperature distribution in said region; a control unit ( 300 ) comprising means for point-to-point digital processing of the temperature distribution in the region. The invention is characterised in that the energy-generating means comprise means( 110 ) for spatial and temporal distribution of the power available to them on said region, the control unit ( 300 ) comprising means ( 330, 350 ), based on the temperature distribution, for controlling the amount and distribution of energy supplied by the generating means ( 100 ).

Claims

exact text as granted — not AI-modified
1 . An assembly for the heat treatment of a region of biological tissue ( 410 ) comprising: 
 energy-generating means ( 100 ) to supply energy to the region,    means ( 200 ) for measuring and recording the spatial temperature distribution in said region,    control unit ( 300 ) comprising numerical processing means for the point-by-point processing of the spatial temperature distribution in the region, characterized in that the energy-generating means comprise means ( 110 ) for spatially and temporally distributing the power that they apply to the aforesaid region, the control unit ( 300 ) comprising means ( 330 ,  350 ) for, on the basis of the temperature distribution, controlling the amount and distribution of the energy supplied by the generating means ( 100 ).    
     
     
         2 . The heat treatment assembly as claimed in  claim 1 , characterized in that the control unit ( 300 ) further comprises means ( 340 ) for estimating the energy losses in the region of the tissue ( 410 ) on the basis of an estimate of the thermal conductivity and of the spatial temperature distribution in the region and its surroundings.  
     
     
         3 . The heat treatment assembly as claimed in one of the preceding claims, characterized in that the control unit ( 300 ) comprises processing means ( 330 ,  350 ) to take account of the thermal conductivity at each point in the region.  
     
     
         4 . The heat treatment assembly as claimed in  claim 3 , characterized in that the control unit ( 300 ) comprises means ( 320 ) for measuring the temperature at each point of a plurality of points sampling the region and at regular time intervals and to deduce therefrom an estimate of the change in temperature as a function of thermal conductivity from one point of the spatial sample to another.  
     
     
         5 . The heat treatment assembly as claimed in one of the preceding claims, characterized in that the energy-generating means ( 100 ) emit focused ultrasound.  
     
     
         6 . The heat treatment assembly as claimed in one of the preceding claims, characterized in that the means ( 200 ) for measuring and recording the spatial temperature distribution comprise a magnetic resonance imaging apparatus.  
     
     
         7 . The heat treatment assembly as claimed in one of the preceding claims, characterized in that the amplitude pw of the power to be supplied at a point {right arrow over (r)} at an instant t+Δt is calculated using a relationship of the type:  
       
         
           
             
               pw 
               = 
               
                 
                   
                     Tp 
                      
                     
                       ( 
                       
                         
                           r 
                           → 
                         
                         , 
                         
                           t 
                           + 
                           
                             Δ 
                              
                             
                                 
                             
                              
                             t 
                           
                         
                       
                       ) 
                     
                   
                   - 
                   
                     
                       FT 
                       
                         - 
                         1 
                       
                     
                      
                     
                       ( 
                       
                         T 
                         * 
                         
                           ( 
                           
                             
                               k 
                               → 
                             
                             , 
                             t 
                           
                           ) 
                         
                          
                         
                            
                           
                             
                               - 
                               
                                 k 
                                 2 
                               
                             
                              
                             D 
                              
                             
                                 
                             
                              
                             Δ 
                              
                             
                                 
                             
                              
                             t 
                           
                         
                       
                       ) 
                     
                   
                 
                 
                   
                     FT 
                     
                       - 
                       1 
                     
                   
                    
                   
                     ( 
                     
                       α 
                        
                       
                         
                           1 
                           - 
                           
                              
                             
                               
                                 - 
                                 
                                   k 
                                   2 
                                 
                               
                                
                               D 
                                
                               
                                   
                               
                                
                               Δ 
                                
                               
                                   
                               
                                
                               t 
                             
                           
                         
                         
                           Dk 
                           2 
                         
                       
                        
                       S 
                       * 
                       
                         ( 
                         
                           k 
                           → 
                         
                         ) 
                       
                     
                     ) 
                   
                 
               
             
           
           
           
               
           
         
       
       where Tp({right arrow over (r)},t+Δt) is the reference temperature at that point at the moment t+Δt, FT −1  is an inverse Fourier transform, T*({right arrow over (k)},t) is the Fourier transform of the temperature measured at the moment t, D is the heat diffusion coefficient for the tissue, α is the energy absorption coefficient for the tissue, S*({right arrow over (k)}) is the Fourier transform of the spatial distribution of the applied energy S({right arrow over (r)}).  
     
     
         8 . Heat treatment assembly according to one of the preceding claims, characterized in that the energy-generating means ( 100 ) comprise energy sources of the ultrasound, laser, microwave or radiofrequency type.

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