Page 70 - Electric Machinery Fundamentals
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46   ELECTRIC MACHINERY FUNDAMENTALS

                (d)  This task is ideally suited for MATLAB. We can take advantage of MAT LAB's
                   vectorized calculations  to determine the  velocity of the  bar for each value of
                   force.  The MATLAB  code to pelform this calculation is just a version of the
                   steps that were performed by hand in part c. The program shown below calcu-
                   lates the current, induced voltage, and velocity in that order, and then plots the
                   velocity versus the force on the bar.

                   % M- flle '  ex!  10  m
                   % M-f i le  to  calculate  and  plot  the  velocity  of
                   % a  linear  mot or  as  a  func tion  of  load .
                   VB  = 120 i                  %  Batter y  v oltage  (V)
                   r   0 . 3 ;                  % Resist ance  (ohms )
                   1   1 ;                      % Bar  l ength  (m)
                   B   0 . 6 ;                  % Flux  den s i t y  (T)

                   % Sel ect  the  forces  to  apply  t o  the  bar
                   F  =  0 : 10 : 50 ;          %  Fo r ce  (Nl
                                                                              (
                   %  Calculate  the  c u rrents  fl owing  i n  t h e  motor .
                   i  =  F  . f  11  •  B )  ;   % Current  (A)

                   %  Calcul ate  the  induced  voltages  on  t h e  bar .
                   eind  =  VB  - i  •  r;      %  Induced  voltage  (V)

                   %  Calculate  the  velocit ies  of  the  bar .
                   v_bar  =  eind  . f  11  •  B) ;   % Velocity  (rn/ s)

                   % Plot  the  veloc ity  of  t he  ba r  versus  force .
                   plot (F , v_bar) ;
                                                              i
                   t i t l e  ('pl ot  of  Veloci t y  versus  Applied  For ce ) ;
                   xlabe l   (I Force  (N)  I) ;
                   ylabe l  ('Ve loc ity  (rols) I ) i
                   a xis  «(0500  2 00J);
                   The resulting  plot is  shown in Figure 1- 28. Note that the bar slows down more
                   and more as load increases.
                (e)  If the bar is initially unloaded, then  eind  = VB'  If the bar suddenly hits a region
                   of  weaker  magnetic  field,  a  transient  will  occur.  Once  the  transient  is  over,
                   though, eind will again equal V n -
                This fact can be used to determine the final speed of the bar. The initial speed was
           120 m/s. Thejinal speed is
                               VB  =  eind  =  v sfll
                                    VB
                                VSS  =  Bl
                                       l20V
                                    (0.08 T)(IO m) = ISO mI,

           Thus, when the flux in the linear motor weakens, the bar speeds up. The same behavior oc-
           curs in  real dc  motors: When the field flux  of a dc motor weakens,  it turns faster.  Here,
           again, the linear machine behaves in much the same way as a real  de  motor.
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