Next: Analysing the real 3D Up: Computing Wakepotentials Previous: Looking at Wakepotentials

Looking at Wakefields

Since we specified

    -time
        firstsaved= eval(0.1/@clight)
        lastsaved= eval(1/@clight)
        distancesaved= eval(0.01/@clight)

in the inputfile for gd1, gd1 did save the electric and magnetic fields at several times. We look at the 30.th saved electric field:

 -3darrow
     symbol= e_30
     arrows= 30000 # default is 1000
                   # but for wakefields, better take more
     doit

The resulting plot is shown in figure 4.3

**Figure 4.3:** The electric field as induced by a line charge traveling on the axis. The direction of the arrows indicate the direction of the field, and their size is proportional to the absolute value of the field strength.
$\begin{figure}\centerline{ \psfig{figure=wakefield00.PS,width=608pt} }\end{figure}$

Since the field near the line charge is extremely large (it is singular in reality), we see mostly field near the charge. In order to see the field away from the line charge, we specify that we want to magnify the arrows by a factor of 20, but we do not want to have any arrow larger than "2":

 -3darrow
     symbol= e_30
     arrows= 30000    # default is 1000 
                      # but for wakefields, better take more
     lenarrows= 20    # <- magnify
     maxlenarrows= 2  # .. but no arrow larger than "2"
     doit

The resulting plot is shown in figure 4.4

**Figure 4.4:** The electric field as induced by a line charge traveling on the axis. The direction of the arrows indicate the direction of the field. Their size now is not proportional to the field strength, since we did specify that there should be a treshold value of "maxlenarrows= 2".
$\begin{figure}\centerline{ \psfig{figure=wakefield01.PS,width=608pt} }\end{figure}$

Next: Analysing the real 3D Up: Computing Wakepotentials Previous: Looking at Wakepotentials