Monthly Archives: September 2017

IR Homing Module Integration, Part VIII

Posted 21 September 2017

As I mentioned at the end of the previous post on this subject, there are still some ‘issues’ with the charging station system.

Ambient light flooding, TSAL-6200 LED Power:

AFAIK, there are only two ways to beat the ambient light flooding problem; by reducing the amount of ambient light allowed to hit the phototransistors, or reducing the gain of the phototransistors, or both.   The ‘flat funnel’ sunshade design appears to be effective in reducing the incidence of ambient light from above (i.e. overhead incandescent lighting and sunlight) while preserving off-axis beacon detection ability, but it may not be enough by itself.  The problem with reducing detector gain to a level that would guarantee protection from flooding is that it might make it impossible to detect the charging station signal from far enough (i.e. around 2m away) to maneuver in time to be captured by the charging station lead-in rails.  Thus, the lower limit on the detector gain is set by the beacon field strength at approximately 2m distance.  So, if I want to reduce the detector gain, I have to increase the IR beacon field strength.

With the current setup with a single-TSAL-6200 IR LED transmitter, there’s not much more I can do to increase field strength at 2m.  The flashlight reflector idea significantly increased detection range, but even with the reflector I had to use a gain resistor of over 100K to achieve 2m detection/homing range, and that is probably 2 orders of magnitude greater than the maximum gain for flooding prevention.  The use of a square-wave modulation with it’s 50% duty factor makes this situation even worse, although I can get most of this loss back by running the LED at 200mA instead of 100.

While I was pondering my navel on this subject, someone mentioned that there are now small, cheap IR flashlights available for the tactical and hunting markets, and these flashlights use one or more Cree high-power IR LEDs.  I happened to be familiar with the Cree line of LEDs, as I have used their visual-light models to replace the el-cheapo LEDs in a couple of my bench lamps.  The visual-light models can easily handle 1Amp, and at that current are too bright to look at directly.  A little research showed that the IR models have the same high power rating, making them ideal for this purpose.  In addition to the high power, the IR flashlights typically come with adjustable optics that allow for a broad or spot beam, which would eliminate the requirement for a reflector – cool!

So, I ordered a ‘IR-940’ IR flashlight from eBay, and it looks like it might fill the bill. The flashlight as received is shown below.

IR-940 IR Flashlight

I ran a small series of tests to see if the adjustable optics really made a difference, and discovered that they did.  As shown below, the spot beam is noticeably smaller and more intense than the other settings.  Interestingly, the illumination pattern at the ‘wide’ setting is almost undetectable – it would be easy to conclude that the flashlight was actually turned OFF, when in fact it was still ON, but with a broad-beam pattern.

IR-940 flashlight at the most narrow-beam setting

IR-940 flashlight halfway between the narrowest and widest settings

IR-940 flashlight at the widest setting

After investigating the flashlight’s physical construction for a bit, I figured out that I could simply hacksaw off the battery compartment, leaving only the front optics adjustment section, and of course the 3-LED module itself.  The following photos show the result

IR flashlight LED and optics section wired into charging station transmit module. The black plastic piece is a prototype of the holder to be used in place of the current reflector

I ran some simple distance tests using my digital camera as an IR sensor.  With the room lights off, I could easily detect the flashlight output from up to 5 m (this was as far away I could get without too much trouble), as shown below

IR flashlight from across the room

Then I redesigned the charging station module to accoMmodate the IR flashlight head, as shown below.

Charging station module with IR flashlight head installed

After getting the flashlight head installed on the charging station module, I ran some azimuth tests with the V10 sunshade, as shown below

-90 to +90 degree azimuth scan at 1m: 2ea SFH-314 phototransistors with 1KΩ Rc using the V10 sunshade and the IR flashlight head

-90 to +90 degree azimuth scan at 2m: 2ea SFH-314 phototransistors with 1KΩ Rc using the V10 sunshade and the IR flashlight head

-90 to +90 degree azimuth scan at 3m: 2ea SFH-314 phototransistors with 1KΩ Rc using the V10 sunshade and the IR flashlight head

As can be seen from the above plots, the IR flashlight idea is definitely a winner.  Even with the detector Rc reduced to 1KΩ the square-wave modulated IR signal can be successfully demodulated from at least 3m away.  All three plots above are essentially identical, except for the scale.   So, if needed, the Rc value could probably be further reduced, and/or the flashlight drive current could be lowered.

 

Phototransistor azimuth pattern alignment:

In the ‘original’ (V9) ‘crushed funnel’ sunshade design, the phototransistors were aligned with about 70º offset, i.e with a 110º internal angle between the two back walls.  This resulted in the following azimuth plot

Azimuth scan using 2ea SFH-314 photo transistors

This indicated to me that I needed to bring the two phototransistor boresight angles more in parallel, thereby moving the two individual azimuth responses toward each other, filling the gap between them.  To accomplish this, I printed up another ‘crushed funnel’ sunshade (V10), with the phototransistors offset 50º instead of 70º (i.e. an internal angle of 130º).  This piece was used for the 1m, 2m, and 3m plots above (repeated below for comparison purposes)

-90 to +90 degree azimuth scan with SFH-314 phototransistors using the V10 sunshade and the IR flashlight head, 1m distance

Comparing these two plots, it looks like I overshot a bit with my adjustment, as now the two individual phototransistor responses are too close together to produce a decent slope on the ‘steering’ (L-R)/(L+R) curve shown above in gray.  Fortunately, it costs essentially zero to produce yet another ‘crushed funnel’ design, this time with an offset midway between the V9 (about 70º) and V10 (about 50º) versions, i.e. an offset of about 60º (V11).  The image below shows the result on my 1m range

-90 to +90 degree azimuth scan with SFH-314 phototransistors using the V11 sunshade and the IR flashlight head, 1m distance

The above plot definitely shows an improvement in the phototransistor azimuth response alignment, and this might well be the one that I want to go with.  However, it makes me a little suspicious of the original V9 data, as the V9 and V11 offsets are almost the same (70º for V9 vs 60º for V11).  Maybe the only real difference between V11 & V9 is the Rc value?  To test this theory, I re-ran the V9 setup with a 1K vs 10KΩ, with the following results.

-90 to +90 degree azimuth scan with SFH-314 phototransistors using the V9 sunshade and the IR flashlight head, 1m distance

As can be seen from the above, my suspicions about the original data were well-founded; the V9  scan with the 1KΩ is just about perfect; the two detector az responses cross at about 1/2 amplitude, and the steering curve is smooth and steep in the boresight region.  So it appears that something else was responsible for the anomalous V9 results – either the use of a 10K Rc or the fact that the original V9 results were acquired with the TSAL-6200/reflector setup versus the IR flashlight setup.  Just for completeness, here’s a shot of all three ‘crushed funnel’ designs.

All three ‘crushed funnel’ sunshade designs. As it turns out, V9 was the winner

At this point, I think I have just about everything I need to integrate the square-wave modulation detection/homing scheme onto the robot; I’ve got a good (V9) sunshade, an excellent IR source with the modified IR flashlight, and a well-tested Teensy 3.2-based demod/homing module.  I think the next step will be to mount the sunshade/detector unit and the demod module on the robot, modify the main robot controller software to acquire steering data via an I2C channel, and then do some homing tests.

Stay tuned,

Frank

 

 

 

 

 

 

 

 

IR Homing Module Integration, Part VII

Posted 18 September 2017

So now that I have the Teensy 3.2-based IR Homing module working on the robot end, I shifted my attention to the charging station end.  Now that I’m using a square-wave modulated IR beacon signal, I needed to separate the LED drive and charging probe circuits; the charging probe needs a constant +5VDC, but the LED circuit needs a pulsed signal.

So, I pulled an IRF-510 power MOSFET from my supplies and wired it up to switch about 200mA through the TSAL-6200 IR LED, driven from the output of my Teensy 3.2-based sweep generator.  I needed to mount the Teensy and the IRF-510 on the charger/beacon module, so I used a 1950’s era terminal strip, some hot glue, and some double-sided foam tape – see the photo below.

Teensy waveform generator and IRF-510 MOSFET mounted on charging station module

I used my CCD camera to verify that the TSAL-6200 IR LED was indeed LED-ing, as shown in the following photo

CCD camera shot of square-wave modulated IR beam from TSAL-6200 mounted in a flashlight reflector. Note the direct and reflected energy.

Then I used my Teensy-based rotary table controller and IR Beacon Homing Module to generate an azimuth scan, as shown below.

Setup for azimuth scan acquisition

Azimuth scan using 2ea SFH-314 photo transistors

And here’s a scope photo showing the square-wave modulation waveform at the Charging Station Module and the received waveform at the IR Homing Module

Square-wave transmit modulation (bottom trace) and received waveform at the IR Homing Module (upper trace)

So, at this point I have both the transmit and receive halves of the square-wave modulated beacon system working, but (as usual) there are still some significant flies in the ointment.

  • I’m still worried about the ambient light interference issue, although my initial tests with the improved sunshade have been encouraging.  With the setup as shown in the above scope photo, turning the overhead incandescent indoor spots on and off just caused a barely perceptible DC drop in the upper waveform.
  • In the same vein, I’m concerned that the TSAL-6200 LED, even pulsed at 200mA, won’t give me the detection range I need for successful homing to the charging station capture basket, especially if I further reduce the phototransistor Rc values to make the system less susceptible to IR ‘flooding’.
  • The azimuth scan data indicates that the SFH-314 phototransistors may not be optimally aligned.  It looks like they should be oriented a little more parallel to each other to close the central response gap.

Stay tuned!

Frank

 

 

The Evolution of an Outside Shot – Part IV

Posted 14 September 2017

It has been almost exactly one year since I last posted about my ongoing Quixotic quest to develop an outside basketball shot.  In the intervening period I have had to deal with chronic pain in both knees.

Fortunately I have gotten significant relief from cortisone shots, but unfortunately the relief is fairly short-lived; I get about 2-3 months of relatively pain-free activity, and then another month or so of increasing pain until I am forced to go back for more drugs.  The orthopod tells me that I can continue to do 3-4 shots/year, but eventually I’ll be in the market for new knees.

As it turns out, I have an appointment in about a week to see a joint replacement specialist, and I suspect the result of this visit will be a knee replacement surgery appointment :-(.

In the meantime, I have been making some actual visible progress on developing an outside shot, and just today I hit two 3’s in a 3-on-3 game, one of which was the game winning shot – wowee!!

Here’s a short video showing front and side views of the current shot technique

 

23 Sept 2017 Update:

Here are a couple more short videos taken on my home b-ball court.  My technique is (slowly!) improving, to the point where I hit 22 of 27 foul shots and most of the medium range ones.  These videos focus on my release and follow-through, from the side (first video) and then the front/back (second video)

IR Homing Module Integration, Part VI

Posted 13 September 2017

While I was doing the work that led to the last post, I realized that my el-cheapo stepper motor was just barely able to get out of its own way.  This worked OK for the previous setup,  but when I moved to a larger sunshade arrangement, I started having problems with the torque – or lack thereof.  As I normally do when faced with this sort of obstacle, I hopped onto the Adafruit site and ordered a couple of NEMA17 stepper motors and companion driver modules.  When these arrived a few days ago, I started playing around with them in preparation for testing the upgraded sunshade.

NEMA17 200 steps/rev stepper motor from Adafruit

This stepper model is the one used widely in 3D printers, and they have excellent speed and torque specs.  The only downside is they run very hot – hot enough to burn fingers :-(.

After receiving the units from Adafruit, I spent some quality time on the web figuring out how to drive them. I discovered that I could use the same L289 motor drivers that I am using for my robot motor driver, so that was cool.  Here’s a short video showing it running an example sketch using the L289 driver

 

Next I printed up an adapter so I could mount my new, improved sunshade (with OSRAM SFH-314 phototransistors installed), and soon had the whole thing running, as shown in the short video below

Then I ran my IRBeaconHomingModule program in conjunction with my TeensySweepGen and Teensy_NEMA17_L289_RotaryTable programs to perform an azimuth scan of the new sunshade with OSRAM SFH-314 photo transistors installed in a crossover configuration, as shown in the following short video

 

Next, I modified my little IRBeaconStepperMotorTracker sketch for compatibility with the L289 motor driver, and used it to demonstrate IR beacon tracking with the new sunshade design and the OSRAM SFH-314 phototransistors, as shown in the following short video