Use the sine-bar bandwidth pattern:

Engrave it in grayscale mode as a negative image with 0.1 mm line spacing:

Monitor the Ruida KT332N controller’s analog laser power control output:

The traces:
- 1 X axis
DIR
, low = left-to-right (yellow) - 2
L-ON
laser enable, low active (magenta) - 3
L-AN
analog voltage (cyan)
The scope triggers when the top two traces go low during a left-to-right scan with the laser beam active. The trigger point lies far off-screen to the left, with the delay set to pull the interesting part of the scan into view.
Although both the controller’s L-AN
output and the laser’s IN
input specify a signal range of 0 V to 5 V, the analog output voltage never goes below 0.4 V, but (as will seen later) that produces 0 mA from the laser power supply.
Set the X cursors to the top and bottom of the sine wave and read off the 4.36 V peak-to-peak value.
Set the Y cursors to matching points on successive cycles and read off ΔT=33.44 ms. Because each cycle is 1 mm wide, the scan speed is set to 25 mm/s and traveling 1 mm should require 40 ms, puzzle over that number and the related fact that 1/ΔT=29.91 Hz. This seems to happen only for speeds under 50-ish mm/s, for which I have no explanation.
Repeat the exercise at various speeds up through 500 mm/s:

The analog output voltage has dropped to 1.56 Vpp.
The average voltage increases from 2.66 V at 25 (or is it 33?) Hz to 2.78 at 500 Hz, which is reasonably close to the same value.
The signal’s -3dB point would be at √½ × 4.36 Vpp = 3.1 Vpp, which happens at 200 mm/s = 200 Hz:

Which is eerily close to the “around 200 Hz” bandwidth figured from the risetime measurements.
All of the analog output measurements as a slide show:
One might now wonder whether there’s any bandwidth difference between the analog and PWM signals as measured in the laser tube current.
Data! We need more data!
One thought on “CO₂ Laser Tube Current: Controller Bandwidth Measurement”
Comments are closed.