Page 343 - Electrical Engineering Dictionary
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uniform strength or to measure the magnetic  F  m×n  [z 1 ][z 2 ] if
                              moment of a magnet.
                                                                                              
                                                                                    a 11 a 12 ... a 1n
                                                                                
                                                                                
                                                                                
                                                                                   0 a 22 ... a 2n  
                                                                                
                                                                                              
                                                                                
                              Helmholtz equation  a partial differential           ... ... ... ...  
                                                                                
                                                                                 
                                                                                                
                                                                                
                              equation mathematically described by                 0  0 ... a nn    if m>n
                                                                                
                                                                                 
                                                                                                
                                                                                
                                                                                   0  0 ... 0  
                                                                                
                                                                                              
                                                                                
                                                                                  ... ... ... ... 
                                                                                
                                                                                
                                                                                
                                                                                    0  0 ... 0
                                                                                
                                                                                              
                                                                                
                                                                                    a 11 a 12 ... a 1n
                                         2
                                       ∇ + k 2  φ = 3Df ,            A H (z 1 ,z 2 ) =         
                                                                                    0 a 22 ... a 2n
                                                                                                if m = n
                                                                                
                                                                                  ... ... ... ... 
                                                                                
                                                                                
                                                                                
                                                                                    0
                                                                                       0 ... a nn
                                                                                                    
                                                                                
                                                                                
                                                                                   a 11 a 12 ... a 1m ... a 1n
                                                                                
                                                                                                     
                                                                                
                                    2
                              where ∇ is the Laplacian, k is the wavenum-           0 a 22 ... a 2m ... a 2n  
                                                                                
                                                                                
                                                                                  ... ... ... ... ... ... 
                              ber, f is the forcing function, and φ is the      
                                                                                
                                                                                
                                                                                    0  0 ... a mm ... a mn
                              equation’s solution.                              
                                                                                
                                                                                
                                                                                   if m<n
                                                                     where deg a ii > deg a ki for k 6= i (deg
                              HEMT       See high electron mobility          z 2      z 2             z 2
                                                                     denotes the degree with respect to z 2 ). In a
                              transistor.
                                                                     similar way, the Hirmite form of A(z 1 ,z 2 )
                                                                     with respect to F [z 1 ][z 2 ] can be defined.
                                                                     A(z 1 ,z 2 ) can be reduced to its Hermite form
                              Henry, Joseph   Henry is best known as  A H (z 1 ,z 2 ) by the use of elementary row
                              the first Director (1846) of the Smithsonian  operations or equivalently by premultiplica-
                              Institution, and President of the National  tion by suitable unimodular matrix U(z 1 ,z 2 )
                              Academy of the Sciences. Henry was largely
                                                                     (det U(z 1 ,z 2 ) ∈ F(z 1 )), i.e., A H (z 1 ,z 2 ) =
                              self-taught, but his early experiments gar-  U(z 1 ,z 2 )A(z 1 ,z 2 ).  See for example, T.
                              nered him sufficient recognition to become a  Kaczorek, Two-DimensionalLinearSystems,
                              Professor of Natural Philosophy at New Jer-  Springer-Verlag, Berlin, 1985.
                              sey College (now Princeton). Henry’s early
                              experiments resulted in the development of a  Hermite Gaussian beam  electromag-
                              practical electric motor and a relay later quite  netic beam solution of the paraxial wave
                              important in telegraphy.               equation in which the field is a product of
                                                                     a Hermite-polynomial and a Gaussian func-
                                                                     tion of distance from the beam axis.
                              hermetic seal  a seal that is such that the
                              object is gas-tight (usually a rate of less than  Hermitian matrix  a square matrix that
                              1 × 10 −6  cc/s of helium).            equals its conjugate transpose.
                                                                     hertz   a measure of frequency in which
                              Hermite form of 2-D polynomial matrix  the number of hertz measures the number of
                               denote by F m×n (z 1 ) [z 2 ] (F  m×n  [z 1 ][z 2 ])  occurrences (of whatever is being measured)
                              the set of m × n polynomial matrices in z 2  per second.
                              with coefficients in the field F(z 1 ) (poly-
                              nomial coefficients in z 1 ).  2-D polyno-  Hertz dipole  a straight, infinitesimally
                              mial matrix A(z 1 ,z 2 ) ∈ F m×n  [z 1 ,z 2 ] of  short and infinitesimally thin conducting fil-
                              full rank has Hermite form with respect to  ament with uniform current distribution. The
                              c 
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