I have a vector field in polar coordinates $(r,\phi)$, which I wish to visualize and better understand. It represents the Electric field vectors for a given field distribution inside a circular boundary: $\hat{r}J_{1}[V_{01}r]+\hat{\phi}0$, with $V_{01}\approx 2.4$ being the first zero of the Bessel function $J_{0}$. We expect such field to be radially directed. So I plotted it as follows to visualize it
TM01ErEnvelope[r_, \[Phi]_] = BesselJ[1, N[BesselJZero[0, 1]] r];
TM01Rec =
TransformedField[
"Polar" -> "Cartesian", {TM01ErEnvelope[r, \[Phi]],
0}, {r, \[Phi]} -> {x, y}]
Show[StreamPlot[TM01Rec, {x, -1, 1}, {y, -1, 1}], Graphics[Circle[]]]
This gave the correct field plot as follows
Then, following a similar line of thinking, I was faced with another (modified) system that have a difference vector field function, now with a complex argument inside the Bessel function: $\hat{r}0+\hat{\phi}J_{1}[V_{01}r (1 - (1 + i) 0.01)]$. So, this is a perturbed version of the argument in the previous case, with the field component $\hat{\phi}$ now present (instead of the $\hat{r}$ component). If the argument were real, one would have expected an azimuthal (concentric circular rings) vector field shape, but since the argument is complex, I am not sure how to interpret, understand or visualize this.
ModifiedTM01ErEnvelope[
r_, \[Phi]_] = BesselJ[1,
r N[BesselJZero[0, 1]] (1 - (1 + I) 0.01)]
ModifiedTM01Rec =
TransformedField[
"Polar" -> "Cartesian", {0,
ModifiedTM01ErEnvelope[r, \[Phi]]}, {r, \[Phi]} -> {x, y}]
And now I have a problem in visualizing it as a StreamPlot
as I did earlier, because the result is complex.
How does one make sense of such case? How can the vector field be interpreted in such case and how can it be visualized (plotted) in a meaningful way?
Any advice is appreciated.