Ed Nisley's Blog: Shop notes, electronics, firmware, machinery, 3D printing, laser cuttery, and curiosities. Contents: 100% human thinking, 0% AI slop.
A little over a year ago, I bought two Sony 64 GB MicroSDXC cards (let’s call them A and B). Both cards failed after less than six months in service and were replaced under warranty with Cards C and D:
Sony 64 GB MicroSDXC cards – front
The top card (C) is the most recent failure, the bottom (D) is the as-yet-unused replacement for Card D. Note that the difference: SR-64UY vs. SR-64UX, the latter sporting a U3 speed rating.
Note that the failure involves the card’s recording speed, not its read-write ability or overall capacity. Card C still has its nominal 64 GB capacity and will store-and-replay data just fine, but it can’t write data at the 25 Mb/s rate required by the camera… which is barely a third of the card’s speed rating. Also note that the writing speed is always a minute fraction of the reading speed that you see on the card.
I use these in a Sony HDR-AS30V action camera on my bike, so it’s pure Sony all the way. Although I don’t keep track of every trip, I do have a pretty good idea of what happened…
In service: about 2015-07-10
Failed to record 1920×1080 @ 60 f/s video: 2015-09-22
In round numbers, that’s 70 days of regular use.
My NAS drive has room for about a month of video, depriving me of a complete record of how much data it absorbed, but from 2015-08-21 through 2015-09-22 there’s 425 GB from 25 trips in 30 days. Figuring the same intensity during the complete 70 days, it’s recorded 800 to 900 GB of data (including my verification test). With 60 GB available after formatting, that amounts to filling the card 14 times.
That’s reasonably close to the 1 TB of data I’d been estimating for the failures of Cards A and B, so these Sony cards reliably fail their speed rating after recording 750 GB, more or less, of data.
The simplest possible electrometer amplifier that might work:
Electrometer amp – LMC6081 schematic
The general idea is that the op amp will drive the (essentially) open-circuited inverting input to match the 2 V offset at the noninverting terminal, so that the output will stabilize above the LMC6081’s minimum useful output voltage (of about 1 V) and the gamma-ray pulses will go downward from there (it’s an inverting amp). The rebiasing network downstream from the output cap doesn’t appear in the hardware.
The small cap across the feedback resistor that would compensate / roll off the high-frequency response isn’t possible, unless you have a stockpile of teeny glass vacuum capacitors: the leakage resistance must be far more than 100 GΩ and my collection lacks anything like that. A Teflon-insulated gimmick capacitor wouldn’t be stable enough and would probably still leak crazy current.
Normal electrometer amps operate at essentially DC and amplify an actual current from the ionization chamber. In this case, the radiation level is zero, there’s no chamber current, I’m looking for small pulses generated by gamma ray events, and the amplifier must have reasonable AC response. It’s not clear that circuit can work, but it’s a starting point.
It turned into a hairball:
Electrometer Amp – 10 Gohm Rf
The LMC6081IN is socketed, with the inverting input pin bent outward and soldered to the flying junction of the 100 kΩ input / OMG resistor (which prevents inadvertent shorts from the 24 V chamber bias) and the glass-body feedback resistor. The socket sits end-on in a puddle of epoxy, so I can swap op amps as needed.
The 100 GΩ feedback resistor didn’t work well at all:
LMC6081 100 G – out – noninv level – matched
The lower trace shows the 10.2 VDC offset at the noninverting input, which is what it took to drive the output from near 0 V to the 11.4 V in the upper trace, with no proportional change in between. I replaced the schematic’s 1 MΩ / 220 kΩ resistors with the 20 turn trimpot shown in the photo in order to find that bias condition. Obviously, the op amp acts as an open-loop comparator, not a linear amplifier, and no amount of waiting for it to stabilize would change that outcome.
It’s possible the resistor has failed open, but, frankly, the difference between “100 GΩ” and “open circuit” probably doesn’t amount to much. Note, however, that there’s absolutely no 60 / 120 Hz interference or noise, which continues to surprise me; removing the shield cap and teasing the twiddlepot slams the output with a 60 Hz trapezoid:
LMC6081 100 G – out – noninv level
Swapping in a 10 GΩ resistor produced a smoothly changing output for biases between about 1 V and 8 V, so it’s behaving like an op amp should. Setting the non-inverting terminal to 8 V puts the output voltage at 6.3 V, which means the 10 GΩ resistor drops about 1.7 V to pull 170 pA from the inverting input (which is presumably at 8 V give-or-take a bit) and the chamber electrode. The LMC6081 spec says a maximum of 4 pA (for the I version, which is what I have), so:
My cleanliness isn’t up to par
The chamber delivers quite a bit more zero-radiation current than I expected
The op amp’s input got toasted despite my efforts toward a static-free installation
Hard to choose among those options, it is, indeed.
With the bias set to produce a 6 VDC output, the AC coupled signal doesn’t seem promising:
LMC6081 10 G Rf – out and Vplus in – AC 2 mV div
The lower trace is the bias voltage applied to the noninverting input, which looks reasonably clean. The sweep triggers from the power line; there’s still no 60 Hz interference.
All those flying components are, as you’d expect, microphonic beyond belief: jumping on the concrete basement floor produces a corresponding bounce in the trace that may be due to air currents or noise, for all I can tell. Even with the chamber sitting on a loose cloth pad, tapping the workbench produces 10 s of slowly decaying oscillation, admittedly at a much lower frequency than the noise in that trace.
A single gamma ray event producing an unreasonably high 10 fA chamber current will cause a downward (it’s an inverting amplifier) pulse that amounts to a mere 100 µV, a pulse that obviously isn’t visible against all that racket. You might convince yourself that the event at the center of the top trace comes from a gamma ray, but you’d probably be wrong.
In a normal electrometer amp, a stiff low-pass filter discards all the noise and isolates the DC signal corresponding to the steady-state chamber current from the ionizing radiation. Given that the pulses are on the order of 5 ms wide, there’s no obvious way to discard most of the noise without also tossing the signal.
Pending more thought, I’d say this was definitely fun while it lasted…
The big bag o’ new-old-stock Inmac ball-point plotter pens had five different colors, so I popped a black ceramic tip pen in Slot 0 and ran off Yet Another Superformula Demo Plot:
HP 7475A – Inmac ball pens – weak blue
All the ball pens produce spidery lines, but the blue pen seemed intermittent. Another blue pen from the bag behaved the same way, so I pulled the tip outward and tucked a wrap of fine copper wire underneath. You can see the wire peeking out at about 5 o’clock, with the end at 3-ish:
HP 7475A – Inmac ball pen – wire spacer
The wire holds the tip slightly further away from the locating flange and, presumably, makes it press slightly harder against the paper:
HP 7475A – Inmac ball pen – stock vs. extended
A bit more pressure helped, but not enough to make it dependable, particularly during startup on the legend characters:
HP 7475A – Inmac ball pens – extended blue
That black line comes from an ordinary fiber-tip pen that looks like a crayon on a paper towel by comparison with the hair-fine ball point lines.
Delicacy doesn’t count for much in these plots, so I’ll save the ball pens for special occasions. If, that is, I can think of any…
A stray sunflower seed decided that the spot just outside the garden gate was perfect and gave Mary’s garden an attractive marker. It will eventually have a dozen blossoms, each one serving as a buffet for the local bumblebees:
Sunflower with bumblebee
Each bee makes several complete circuits of the florets, draining the nectar and collecting pollen as she goes:
Sunflower with bumblebee – detail
Mary tucks the open gate inside the garden to avoid disturbing the pollinators, as wasps tend to have short fuses and multiple-strike stingers:
Sunflower with wasp
The bumblebee traveled clockwise and the wasp went counterclockwise, but I don’t know if that’s the general rule. I certainly won’t dispute their choices!
In a few weeks, long after the petals fall away, a myriad small birds will harvest the dried seeds…
An undrilled double-sided circuit board with the edges bonded together doesn’t look like much:
Electrometer amp – undrilled shield planes
Soldering a smaller hex to the center of the bonded plate produces an isolated plane:
Electrometer amp – finished shield planes
The copper fabric tape wrapped around a brass tube soldered to the isolated plane contacts the ionization chamber shell around the central contact and (should) provide complete shielding. Kapton tape around the edges reduces the likelihood of inadvertent shorts.
Working with a shield at +24 V gave me the shakes, so this one confines the chamber bias to the isolated hex and shell, with the larger hex at circuit common (a.k.a. ground). The isolated plane has about 275 pF to the ground plane, which isn’t a Bad Thing at all. In principle, the chamber bias doesn’t need a switch, because there’s no current drain, but I vastly prefer having cold circuitry before popping the lid.
If I had a small DPST switch, I’d use it:
Electrometer amp – chamber – shield planes
As it stands, one switch controls the +24 V chamber bias and the other switches +12 V power to the electrometer amp front end, with simpleminded connectors so I can separate the pieces.
We’ll see how well all that works in practice.
An alert reader will notice the tiny difference between the blue PETG shapes in the two pictures. The bottom one comes from the revised code, of course.
The Smell of Molten Projects in the Morning 