So, let's say the particle is moving along the y axis at velocity v, so ##x=0##, ##y=vt##. You want to draw the field at ##t=0##, so you drew a circle of radius ##1c## centered on ##(x,y)=(0,-v)## with vectors all around it pointing at its center. Then you drew a circle of radius ##2c## centered on ##(0,-2v)##, with vectors all around it pointing at its center. And so on. And then you tried to draw the integral curves of this field?
No, that won't work. There is also a time varying magnetic field in the frame where the charge is moving which is not present when the charge is stationary. That makes the E field different from some stitched-together slices of a Coulomb field.
Well, you don't know that it hasn't accelerated. I wouldn't say that the field points at where the particle is now. Rather, it points at the forecast of where the charge should be now if it maintained its inertial motion in the time since our delayed image of it. The forecast happens to be correct in this case.