The Subcutaneous Transmitter (A3028) is an implantable telemetry sensor for rats and mice that provides high-fidelity amplification and recording of one or two biopotential inputs. The device comes in rechargeable and non-rechargeable versions, as well as fully-implantable and head-mounting versions.
Warning: Check to make sure devices are inactive upon arrival at your facility. Do not store within 10 cm of iron tools, power transformers, computers, or external hard drives. During implantation, take note that stainless steel tools and work surfaces are often magnetic, and can either activate and deactivate your transmitters.
Warning: Rechargeable devices left inactive on the shelf will eventually drain their batteries completely, after which they cannot be recharged to full capacity. Recharge inactive batteries every six months.
The A3028A displaces volume 1.4 ml and provides two EEG channels with bandwidth 160-Hz for fifteen days. The A3028E displaces 2.8 ml, and provides one EEG channel with 160 Hz and 512 SPS for eighteen weeks. Both the A3028A and A3028E are fully-implantable beneth the skin of an animal. The A3028M is a head fixture with replaceable battery that provides two EEG channels with 640-Hz and 2048 SPS for four days. The A3028M may be mounted on the skull of an animal, but may not be implanted beneath the skin. All versions of the A3028 operate within our Subcutaneous Transmitter System. Non-rechargeable versions offer the longest operating life. The rechargeable devices offer one third the operating life for the same volume. They may be recharged between experiments and used a dozen times before their leads and encapsulation show signs of wear. Recharging takes place through the EEG leads with the help of a Battery Recharger A3033. The versions with battery holders are intended to be mounted in head fixtures, and we deliver them with a plastic enclosure that may be cemented to an animal's skull. Their batteries may be replaced at any time.
We turn the transmitter on and off with a magnet. The A3028A comes with three helical stainless-steel leads coated with silicone. The three leads provide us with two biopotential inputs, X and Y, that share a common ground, C. The sensor measures the voltage difference X − C and Y − C. The electrodes at the end of the wires can be stainless steel screws, gold pins, or bare helical wire, as we discuss in Electrodes and The Source of EEG.
|Outer Dimensions||14 mm × 14 mm × 8 mm|
|Operating Life||360 hours|
|Shelf Life||27 months|
|Number of Inputs||2|
|Type of Input||Differential|
|Input Impedance||10 MΩ || 2 pF|
|Sample Rate (Each Input)||512 SPS|
|Input Dynamic Range||20 mV|
|Input Bandwidth||0.3 Hz − 160 Hz|
|Input Noise||≤12 μV rms|
|Input Mains Hum||<1 μV|
|Total Harmonic Distortion||<0.1%|
The A3028D is the same circuit with the same functionality as the A3028A, but with a 255 mA-hr battery instead of the A3028A's 48 mA-hr battery. The A3028D's volume is 3.0 ml and its operating life is 1900 hours.
All versions of the A3028 turn on and off with the application of a magnetic field. We like to use cow magnets. Component U2 is a micro-power hall effect switch. When it detects a magnetic field, it asserts its output. When we remove the field, the transmitter changes state. If it is inactive, it activates. If it is active, it deactivates. The state change does not occur when we bring the magnet close to the transmitter, it occurs when we move the magnet away.
We determine the version of a transmitter during assembly, programming, and encapsulation. We might change capacitors on the board to set the filter frequencies. We might change resistors to set the gain. We program the logic chip to set the sample rate for each channel. We can equip the circuit with various sizes of battery. The larger the battery, the longer the operating life.
The A3028 transmits either one or two signals. Each signal has its own channel number. Each sample of each signal is transmitter by the A3028 with a radio-frequency message. Each message contains a channel number, as we describe in Message Encoding. Channel numbers lie in the range 1-222. A two-channel transmitter transmits on channels n and n+1, where n is an odd number.
The following table presents some existing versions of the A3028. Those marked with an asterisk are not yet in production, but are designed and ready to enter production.
|A3028A||±10 mV, 0.3-160 Hz, 10 MΩ, 512 SPS||±10 mV, 0.3-160 Hz, 10 MΩ, 512 SPS||48 (BR1225)||1.4||14||14||7||360||27|
|A3028B||±10 mV, 0.3-160 Hz, 10 MΩ, 512 SPS||Disabled||48 (BR1225)||1.4||14||14||7||600||27|
|A3028B-R||±10 mV, 0.3-160 Hz, 1 MΩ, 512 SPS||Disabled||19 (PP030112AB)||1.4||14||14||7||240||11|
|A3028C||Disabled||±10 mV, 0.3-80 Hz, 10 MΩ, 256 SPS||48 (BR1225)||1.4||14||14||7||950||27|
|A3028D||±10 mV, 0.3-160 Hz, 10 MΩ, 512 SPS||±10 mV, 0.3-160 Hz, 10 MΩ, 512 SPS||255 (BR2330)||3.0||24||24||8||1900||140|
|A3028E||±10 mV, 0.3-160 Hz, 10 MΩ, 512 SPS||Disabled||255 (BR2330)||3.0||24||24||8||3200||140|
|A3028E-R*||±10 mV, 0.3-160 Hz, 1 MΩ, 512 SPS||Disabled||190 (GM382030)||4.0||32||22||9||2300||100|
|A3028F||±10 mV, 0.3-320 Hz, 10 MΩ, 1024 SPS||±10 mV, 0.3-320 Hz, 10 MΩ, 1024 SPS||48 (BR1225)||1.4||14||14||7||180||27|
|A3028H||±10 mV, 0.3-80 Hz, 10 MΩ, 256 SPS||±10 mV, 0.3-80 Hz, 10 MΩ, 256 SPS||48 (BR1225)||1.4||14||14||7||600||27|
|A3028L||±10 mV, 0.3-320 Hz, 10 MΩ, 1024 SPS||±10 mV, 0.3-320 Hz, 10 MΩ, 1024 SPS||1000 (BR2477)||6.5||27||27||14||4000||550|
|A3028P||±10 mV, 0.3-40 Hz, 10 MΩ, 128 SPS||Disabled||30 (CR1025)||0.8||19||11||4.0||860||17|
|A3028P-R*||±10 mV, 0.3-40 Hz, 1 MΩ, 128 SPS||Disabled||11 (GMB300910)||0.8||19||11||4.0||140||7|
|A3028Q||±10 mV, 0.3-160 Hz, 10 MΩ, 512 SPS||Disabled||560 (CR2354)||5.0||24||24||11||7000||300|
|A3028U||±100-mV, 0.0-160 Hz, 10 MΩ, 512 SPS||±100-mV, 0.0-160 Hz, 10 MΩ, 512 SPS||255 (BR2330)||3.0||24||24||8||1700||140|
|A3028V||±10 mV, 0.3-160 Hz, 10 MΩ, 512 SPS||±10 mV, 30-640 Hz, 10 MΩ, 16 SPS||48 (BR1225)||1.4||14||14||7||600||27|
The shelf life for a non-rechargeable transmitter is how long it takes to exhaust the battery permanently when we leave it inactive on the shelf. The shelf life of a rechargeable transmitter is how often we must re-charge it to keep its battery in good condition. The rechargeable devices provide lower battery capacity per unit volume, but their batteries may be recharged to full capacity before implantation. See below for details of current consumption and how to calculate battery life of new versions of the A3028. The following versions are for head fixtures only. These devices come with their own plastic enclosure for mounting to the animal skull. Their batteries are in holders from which they may be removed and replaced.
|A3028M-H||±10 mV, 0.3-640 Hz, 10 MΩ, 2048 SPS||±10 mV, 0.3-640 Hz, 10 MΩ, 2048 SPS||48 (BR1225)||2.0||16||16||10||100||27|
|A3028N-H||±10 mV, 0.3-160 Hz, 512 SPS||Disabled||48 (BR1225)||2.0||16||16||10||600||27|
All versions provide stimulus protection on both inputs by means of three resistors and two capacitors. The resistors protect against applied voltages up to ±50 V. The capacitors attenuate radio-frequency noise that might otherwise be picked up from the antenna and demodulated in the amplifier inputs. Prior to batch 111, only the A3028R provided stimulus protection. Now that all versions provide this protection, the A3028E and A3028R are identical, and we have retired the A3028R version from our table.
The A3028 electrode leads are color-coded with colors that do not blend with the natural color of animal tissue. The X lead is red, Y is yellow, and C is blue. A dual-channel transmitter produces two radio-frequency message sequences with two separate channel numbers. The lower of the two is X and the higher is Y. A single-channel transmitter may be equipped with only X or only Y. If the single channel is X, the leads will be red and blue. If the single channel is Y, the leads will be yellow and blue.
Each lead of the transmitter has its own terminating electrode. Each electrode type has a one-letter name, as given in the table below. We specify these electrodes with two letters for a single-channel transmitter (X or Y, and C) and three letters for a dual-channel (X, Y, and C). Click on the letter for a data sheet or photograph.
|A||Bare wire, length 2 mm, stainless steel helix.|
|B||Screw, thread 0-80, length 3.2 mm.|
|C||Screw, thread M0.5, length 0.6 mm.|
|D||Pin, diameter 0.30 mm, length 3.1 mm, Mill-Max 4353-0-00-15-00-00-33-0|
|E||Socket, for pin diameters 0.20-0.33 mm, Mill-Max 4428-0-43-15-04-14-10-0|
|F||Pin, diameter 0.64 mm, length 4.1 mm, Mill-Max 5035-0-00-15-00-00-33-0.
Mates with Plastics One socket E363/0.
|G||Pin, diameter 0.51 mm, length 6.0 mm, Mill-Max 5063-0-00-15-00-00-33-0.
Mates with Plastics One socket MS303/6.
|H||Depth electrode, wire 125-μm dia Pt-Ir, insulation 200-μm dia teflon.
Locate with guide cannula, cut wire after cementing.
|J||Depth electrode, wire 125-μm dia 316SS, insulation 200-μm dia teflon.
Locate with guide cannula, cut wire after cementing.
|W||Depth electrode, straight wire 125-μm dia 316SS, insulation 200-μm dia teflon.
Locate with hypodermic tube, cut tube and wire after cementing.
The A3028A-DDC is a two-channel transmitter, sample rate 515 SPS on each channel, volume 1.4 ml, with 1.9-mm long pins on X and Y, and a 0.6-mm long screw on C. The A3028A-HFC has a depth electrode on X, a gold-plated pin on Y, and a screw on C.
We provide some on-line advice on implanting the transmitters here, but most of our advice on this subject we conduct by e-mail with our customers, with assistance between customers, including the exchange of implantation videos, being common.
The following files define the A3028 design. Note that we distribute all these files under the GNU Public License.S3028A_1.gif: 2 channels 0.3-160 Hz, A3028AAV1 and A3028AAV2.
The A3028 provides two amplifiers for recording two channels of EEG, or simultaneous EEG/EMG recording. The photographs below show an early version of the circuit, which is similar to all subsequent versions.
We purchase boards fully-loaded with parts from our assembly house. We change various capacitors and resistors to create new versions of the assembly. The table below shows how we can modify the A3028RV3 assembly to create new versions. We modify only those components that are necessary for the new version to function correctly.
|Version||C7||C8||C9, C10, C11||C12||C13||C14, C15, C16|
|A3028RV3||100 nF||10 μF||1.0 nF||100 nF||10 μV||2.0 nF|
|A3028F||510 pF||510 pF|
|A3028L||510 pF||510 pF|
|A3028U||1.0 kΩ||620 kΩ||1.0 kΩ||620 kΩ||1.0 nF|
|A3028V||100 nF||240 pF|
Versions not listed above cannot be constructed from the A3028RV3, but are based upon newer assembly versions.
The A3028 three input leads are X, Y, and C. They are red, yellow, and blue respectively. You can see all three declared with in the circuit diagram for non-rechargeable and rechargeable devices.
|X||X positive input||Connected to VC by 100 nF in series with 10 MΩ.|
|Y||Y positive input||Connected to VC by 100 nF in series with 10 MΩ.|
|C||shared negative input||Connected directly to VC.|
|OUT||radio-frequency antenna||a flexible stranded steel transmit antenna|
The rechargeable devices provide access to their batteries through the X and C leads. Diodes permit current to enter X and leave through C. The leakage current of the diodes requires that we place a 1 MΩ resistor between X and C, thus reducing the X input impedance from our preferred 10 MΩ. The input impedance of the Y input remains 10 MΩ.
|X||X positive input||Connected to VC by 1 MΩ as well as 100 nF in series with 10 MΩ.|
|Y||Y positive input||Connected to VC by 100 nF in series with 10 MΩ.|
|C||shared negative input||Connected directly to VC.|
|OUT||radio-frequency antenna||a flexible stranded steel transmit antenna|
The A3028 amplifies and filters X and Y to produce XA and YA. The gain of the A3028A amplifier is 100. Its high-pass filter consists of a zero at 0.16 Hz and another at 0.32 Hz. Its low-pass filter is a three-pole, 3-dB ripple Chebyshev filter with 160-Hz cut-off frequency. Both XA and YA are applied to a two-channel sixteen-bit ADC. In the A3028A, the ADC samples the two channels alternately at 512 SPS per channel, for a combined sample rate of 1024 SPS. In the A3028B, sampling from YA is disabled, and XA is sampled at 512 SPS. (We note that the A3028B will replace the A3019A single-channel transmitter.)
The ADC produces sixteen-bit values between 0 and 65535. A value of 0 for X means XA = 0V, and 65535 means XA = VBAT. With a fresh battery, VBAT = 2.7 V. In the A3028A, with its gain of 100, each ADC count represents roughly 400 nV at the X and Y inputs. In the last few days of a transmitter's life, the VBAT drops to 2.2 V, at which point the transmitter fails. During this time, the voltage represented by each ADC count drops in proportion to the battery voltage. When VBAT is 2.2 V, one count represents roughly 350 nV. In theory, the dynamic range of the A3028A is 2.7 V ÷ 100 = 27 mV. But in practice, the amplifier is not able to drive XA all the way up to VBAT or all the way down to 0 V. We quote the dynamic range of the A3028A as ±10 mV. But when we convert ADC counts to input voltage, we multiply by 400 nV.
At each input, most versions of the A3028 provide a DC-blocking capacitor. These are C7 and C12 in the schematic. Together with input resistors R5 and R12, they form two single-pole high-pass filters with time constant 1.0 s. There is another high-pass filter in each amplifier, consisting of R6/C8 for X and R13/C13 for Y. These have time constant 0.5 s in most versions of the A3028. The figure below shows the theoretical step response of the A3028A inputs, and compares it to that of other devices we have manufactured.
The common-mode reference voltage in the amplifier is VC, and VC is derived from the battery voltage by a 1.8-V regulator. Thus VC is 1.8 V, and the average value of both XA and YA are also 1.8 V. Thus the average digital value of X and Y correspond to 1.8 V. This allows us to calculate the battery voltage from the average value of either channel. We have VBAT = 65535 / average(X) × 1.8 V. This relation applies to all versions of the A3028, and both inputs, regardless of the gain and frequency response of its amplifiers, and regardless of what battery we have installed.
The figure below shows the X signal from an un-encapsulated A3028E as we reduce VBAT from 4.2 V to 1.2 V over 300 s. Our formula for VBAT from the average value of X works down to VBAT = 1.9 V. After that, the X decreases, suggesting an increase in VBAT, when in fact the actual VBAT drops to 1.8 V and the transmitter turns off.
The analog input impedance of X and Y is 10 MΩ in the pass-band of the amplifier, with the exception of X in rechargeable devices, for which input impedance is 1 MΩ. Most versions of the A3028 provide a high-pass filter at 0.3 Hz to remove slowly-varying electrochemical potentials so that the gain of the amplifier can be ×100 and the dynamic range is the battery voltage divided by 100. For non-rechargeable devices, the battery voltage is 2.7 V for most of the operating life of the device, so the dynamic range is 27 mA. We quote ±10 mV in our specification table because the dynamic range is not centered about C. The A3028U amplifier, however operates all the way down to 0.0 Hz and accommodates electrochemical potentials by reducing the amplifier gain to ×10 so that the input dynamic range is &plumn;100 mV.
We set the cut-off frequency of the A3028 three-pole, 3-dB ripple, Chebyshev, low-pass filters by our choice of filter capacitance, CF. There are three capacitors in each filter that must have the same value for the filter to function properly. They are C9, C10, and C11 for the X filter and C14, C15, and C16 for the Y filter. With CF = 1.0 nF, the cut-off frequency is 160 Hz. The following graph shows how the gain of the two inputs of an A3028A varies with frequency.
The frequency response in the pass-band shows a slight decrease in gain from 10 Hz to 80 Hz, followed by a bump up at 130 Hz. These two features are the 3-dB ripple of the three-pole Chebyshev filter. By tolerating this non-uniformity of gain in the pass-band, we obtain a far sharper cut-off at the top of the pass-band. Amplitude drops by a factor of ten, or 20 dB from 160 Hz to 256 Hz. Frequencies above 256 Hz when sampled at 512 SPS will produce artificial sin-waves of lower frequency, in a process called aliasing. The purpose of our low-pass filter is to prevent aliasing. It is an anti-aliasing filter. Even with the sharp cut-off of our Chebyshev filter, however, we might still see aliasing of high frequency components in EEG.
The plot above shows what the X and Y digitized signal looks like when we apply a powerful signal above 256 Hz to both inputs. The result is an artificial waveform of frequency 262 − 256 = 6 Hz. Its amplitude is around 700 counts rms, which is one tenth the amplitude it would produce if we reduced the frequency to 25 Hz. The mains hum in the signal is carried in by the signal source when we connect it to the transmitter.
We expect some variation between amplifiers, because the three-pole filter is sensitive to the exact component values. The plot below shows the frequency response of a batch of fourteen A3028E transmitters stimulated with a 30-mV sinusoid through a 20 MΩ resistor.
At 10 Hz, the fourteen channels agree to within ±0.5 dB. At 130 Hz, where we have the bump in the Chebyshev response, they agree to within ±1 dB. These variations are well within the range we expect with 5% capacitors and 1% resistors.
When we apply a pure sinusoidal waveform to the A3028, the sinusoid is amplified, filtered, digitized, transmitted, received, and recorded by the data receiver. The purpose of the A3028 is to provide high-fidelity EEG recordings, so we hope to see only a pure sinusoidal waveform emerge in the frequency spectrum of the recorded signal. We apply a 14-mVpp sinusoid of increasing frequency to the input of an A3028E-R transmitter. We measure the power of the recorded signal after subtracting its fundamental harmonic. This non-fundamental power is a combination of imperfection in the applied sinusoid, noise in the amplifier, and distortion in amplification and transmission of the signal. We divide the non-fundamental power by the total signal power to obtain a measure of the distortion of the sinusoid by the recording process.
For the scattered-sampling devices, distortion remains less than 1% in the 0.3-160 Hz pass-band of the A3028 amplifier. At 10 Hz and below, distortion is less than 0.01%. The distortion power for scattered-sampling devices has a white noise spectrum: it is not distortion of the original sinusoid, but noise added to the sinusoid by the power of the sinusoid. This noise is due to random variation in the sampling instants, which is a feature of the process by which A3028 transmitters avoid systematic collisions with other transmitters. We call it scattering noise. If we sample uniformly, we obtain the second plot shown above, in which distortion is less than 0.003%. With uniform sampling, the non-fundamental power is dominated by periodic signals that may be the result of distortion in the amplifier, or they may be imperfections in the signal produced by our function generator. The figures below show the spectrum of the non-fundamental power with uniform sampling.
Uniform sampling increases current consumption by 10% (for example, the A3028D with regular sampling consumes 152 μA, while the A3028D with scattered sampling consumes 135 μA). Given that scattering noise does not distort the shape of the fundamental sinusoid, and given the chaotic nature of most biopotential signals, there is no practical benefit in reducing the scatter noise below 1%, while there is a practical benefit to increasing operating life by 10%.
The A3028U provides a 200-mV dynamic range and 0.0-160 Hz bandwidth on both inputs. Its EEG amplifier gain is only ×10.
The least significant bit of the 16-bit digitized samples is 4.1 μV for battery voltage 2.7 V. To avoid We enable uniform sampling for all A3028U devices. Total harmonic distortion remains less than 25 ppm (0.0025%) from 0.03 Hz to 160 Hz.
The A3028V provides two channels: one running at 496 SPS and 0.3-160 Hz, and one at 16 SPS and 30-640 Hz. The first is for normal EEG recording, the second is for EMG amplitude measurement. The Neuroarchiver will reconstruct the 496 SPS signal into a 512 SPS signal by filling in the missing samples using the previous sample values, and the result will be an EEG signal almost identical to the one we would obtain with 512 SPS. The Neuroarchiver will leave the 16 SPS signal as it is, provided you enter "16 512" for the default frequency in the Neuroarchiver configuration. The figure below shows the gain versus frequency of the EEG and EMG inputs. Our measurement of the EMG gain between 200-500 Hz is erratic because of aliasing noise produced by under-sampling a non-random periodic sinusoid. With a random EMG input, we expect no such error in our measurement of amplitude.
The figure below shows how the A3028R's 160-Hz low-pass filter responds to pulses applied to the X input.
The low-pass filter introduces the ringing after the pulse, which consists of three maxima and minima in damped harmonic oscillation after the pulse has ended. The figure below shows the response of the A3028R to perforant pathway discharge spikes of amplitude roughly 10 mV.
The ringing we see after the discharge spikes is not generated by the brain itself, but rather by our low-pass filter. The slow, positive pulse following the negative spike is, however, produced by the brain, and the ringing is overlaid on top of this pulse.
[20-SEP-13] Input noise on an un-encapsulated A3028A with no input leads is 20 counts rms on each channel, or 8 μV. This is lower than the 12 μV of the A3019. The decrease is a result of superior distribution of power and decoupling in the A3028.
[08-OCT-13] We look for noise generated by the Hall Effect Switch. This noise existed in the A3019, as we describe here. We have a new Hall Effect Switch, the SL353LT. We find that it, too, generates noise in the 10-30 Hz range in an encapsulated transmitter.
We see the same 20.75 Hz noise in both channels. The amplitude is around 7 counts, or 7 × 0.4 μV = 2.8 μV.
[11-MAR-14] When the A3028 is encapsulated and equipped with leads, these leads pick up radio-frequency power from the antenna. If the C lead is left open-circuit and the X and Y leads are connected to some solid body, the C lead acts like an antenna. The radio-frequency power is demodulated by parasitic diodes in the circuit, and the result is noise visible on the EEG, as shown here. Its amplitude is roughly 100 μV rms. If you see such noise in an implanted transmitter, your C lead has a broken conductor.
[01-DEC-16] We take a two-channel A3028D and put it in water at 40°C. We use 8-s recording intervals to measure the amplitude and frequency of the switching noise in each of the two input channels No3 and No4 as the water cooled to 19°C.
The frequency of the switching noise increases with frequency. We perform the same experiment with four transmitters at once, using this processor to calculate the rms amplitude of the fundamental harmonic of the switching noise.
In No13/14 the noise is far greater in X than in Y. But in No10 the noise is as large as any we have seen, and appears on the Y input. We touch the tip of a ×1 probe to the package of the Hall Effect Switch on a battery-powered, un-encapsulated transmitter. We see no signe of 20 Hz, certainly less than 200 μV. We hope to eliminate switching noise entirely in a future design, but for now we have yet to understand why switching noise appears in some amplifiers and not in others.
Suppose we want to know the root mean square amplitude of a biometric signal, or the mean square amplitude, but we do not need to know its exact shape. When we monitor electromyography (EMG), our chief interest may be the power of the signal, to determine if an animal is awake or asleep, rather than examining the fluctuations in the signal itself.
As we mention above, when we try to represent a continuous, time-varying signal as a sequence of discrete samples, we must make sure that the variation in the time-varying signal between the sample points approximates a straight line. When we plot the sampled signal, we are going to display it by drawing straight lines between the samples, so these straight lines are supposed to represent what the signal actually did between the samples. If the signal varies greatly between samples, we will not see this variation. Failing to see rapid variations between samples may not concern us, but rapid variations can, through sampling, look like much slower variations when we join the samples with lines. If we sample a 100-Hz signal at 48 SPS, for example, our straight-line reconstruction of the signal will be a 2-Hz sinusoid. This generation of slow variation from rapid variation is aliasing. To avoid aliasing, we must filter the signal we want to sample so that it contains no changes of direction between sample points. With a perfect low-pass filter, which has gain 1.0 up to frequency fc and 0.0 above fc, we can sample at 2fc and avoid aliasing. In practice, low-pass filters are not perfect, and avoiding aliasing is not quite sufficient to provide adequate representation. In the A3028, we sample at 3.2fc. Our low-pass filter gain drops by a factor of 10 from fc to 1.6fc. For example, in our 512 SPS transmitter for EEG, we filter at 160 Hz. The filter gain drops by a factor of ten from 160 Hz to 256 Hz.
But aliasing does not change the power of a signal, not unless we somehow miss all the powerful moments of a signal by a spectacularly unfortunate choice of sample instants. For an irregular signal like EMG, sampling at 16 SPS and taking the standard deviation of the samples, will give us a good measure of the EMG signal amplitude. Most EMG power is in the range 40-300 Hz, so we can high-pass filter at 30 Hz and low-pass filter at 320 Hz to separate the EMG from any artifacts that may be generated by our EMG pick-up electrodes, sample at 16 SPS and obtain EMG power at a cost of only 1.8 μA in current consumption. Thus the A3028V monitors EMG on Y and EEG on X and has the same battery life as the single-channel A3028B EEG monitor.
[29-MAR-16] We calibrate the A3028 center frequency to lie in the range 913-918 MHz at room temperature, which is around 22°C. The MAX2624 oscillator that provides the radio-frequency signal has a temperature coefficient of −0.2 MHz/°C. In an animal body at 37°C, the center frequency will drop to 910-915 MHz. Our Octal Data Receivers (A3027) and the older Data Receiver (A3018) are designed to provide reliable message reception in for center frequencies in the range 908-918 MHz. The spectrum of the entire signal spans a ±5 MHz range about the center.
[04-AUG-16] The 50-mm antenna makes a loop roughly 20-mm long. This loop fits easily into a rat. We compared (see here and here) 50-mm and 30-mm antennas moving in air at room temperature on a self-propelled sphere and found that the 30-mm antenna performed just as well as the 50-mm. The 30-mm antenna makes a loop only 13 mm long.
When we immerse an A3028E with 50-mm antenna in water, the radio-frequency power it emits remains constant to within a factor of two as we half-immerse it in water, completely immerse it in water, or press it up agains the wall of a water-filled beaker. The center-frequency of its transmission increases by 1 MHz from air to total immersion in water. The dielectric constant of water is ninety times greater than that of air. Water affects the propagation of radio waves along the antenna, slowig them down, so that the effective length of the antenna is greater. The water also affects the oscillator within the transmitter circuit, changing its resonant frequency.
When we immerse an A3028A with 30-mm antenna in water, the power it emits rises by a factor of ten (10 dB) and the center-frequency rises by 2 MHz. The figure below is the power spectrum we measure when we hang an A3028A by its leads in air, then surround it with a beaker of water.
The antenna is the loop of stranded steel wire insulated with silicone that is attached at one end to the input leads. The antenna connection is marked OUT on the schematic. The antenna transmits the values of X and Y with 7-μs bursts of 902-928 MHz radio waves. The power transmitted during these bursts is roughly 300 μW (−5 dBm). The receiving antenna, which is usually a Loop Antenna (A3015C) connected to an Octal Data Receiver (A3027), must pick up at least 25 pW (−76 dBm) to overcome noise in the receiving antenna amplifiers, and at least four times (12 dB) more than the 902-928 MHz interference power picked up by the receive antenna. In our office, interference power ranges from 100 pW to 100 nW. In order to guarantee reception outside a faraday enclosure, we must receive 1 μW (−30 dBm). Inside an FE2F faraday enclosure, which offers at least ×1000 (30 dB) isolation from interference, we must receive 1 nW (−60 dBm).
For a discusion of body capacitance, see Body Capacitance in the A3019 manual.
[29-SEP-16] The A3028 can run down its battery in two ways. It can sit on the shelf in its inactive state, or it can digitize and transmit its input signals in its active state. In practice, the battery will be consumed by some combination of inactive and active periods.
The inactive current of the A3028 consists of the current consumption its magnetic sensor (U2) and its logic switch (U3). The average inactive current is around 2.0 μA. The shelf life of the transmitter is the time it takes the inactive current to drain the battery. For the 48 mA-hr battery, the shelf life is over two years. For the 255 mA-hr battery, the shelf life is over ten years. The shelf life of the 19 mA-hr rechargeable battery used by the A3028B-R is 11 months. So long as we do not leave the A3028B-R inactive on the shelf for more than 11 months, we can recharge it to its full capacity immediately before implantation.
The active current of the A3028 is its current consumption in the active state. This current depends upon the number of samples the transmitter takes per second. The A3028B provides one channel with 512 SPS. The active current consists of the quiescent current of the logic chip, which is independent of sample rate, and the consumption of the sample and transmit process, which increases linearly with sample rate. The figure below shows active current versus the total sample rate. To obtain the total sample rate, we add the sample rates of both channels.
The linear trend fitted to the data provides us with the following empirical formula for typical active current, Ia, as a function of the total sample rate, R.
Ia = 21 μA + (R × 0.11 μA/SPS)
The operating life of the transmitter is the time it takes the active current to exhaust a fresh battery. As the battery is exhausted, the average value of the analog inputs increases, like this. The A3028B single-channel, mouse-sized transmitter has nominal battery capacity 48 mA-hr. According to the above formula, its typical active current is 77 μA. Its typical operating life is 620 hours. In our version table we specify a typical operating life of 600 hours for the A3028B, based upon measurements rather than the above calculation. The A3028B-R rechargeable transmitter will run for 240 hours before its battery is so exhausted that further operation will cause damage to the battery itself. The A3028E dual-channel, rat-sized transmitter has a 255 mA-hr battery. Its typical operating life is 1900 hours.
The A3028U performs uniform sampling to reduce total harmonic distortion at the cost of higher current consumption. It provides a total of 1024 SPS and its current consumption is 143 μA. The A3028D's current consumption, according to the formula above, is 134 μA. To determine the current consumption of a transmitter with uniform sampling, we use 21 μA + R × 0.12 μA/SPS.
The standard deviation of the active current is 5% of its typical value. But the standard deviation of the battery capacity is closer to 10% the nominal capacity. The operating life is, on average, equal to its typical value, but varies from one transmitter to the next with a standard deviation that is 10% of the typical operating life. Assuming a normal distribution of operating life, we can be 82% certain that the operating life will be >90% of the typical value, and 97% certain it will be >80% of the typical value. In the case of the A3028R single-channel 512 SPS transmitter, we can be 97% sure that it will operate for longer than 2560 hrs, and 18% of the time it will run for longer than 3500 hrs.
If we remove the radio-frequency oscillator from an A3028E transmitter, which runs at 512 SPS, the active current consumption drops from around 80 μA to 40 μA. The sample and transmit activity consumes 60 μA, of which 40 μA is transmission and 20 μA is the quiescent current of the logic chip, amplifiers, and regulators. During the 7-μs burst transmissions, the current drawn by the transmission circuits is 11 mA.
[29-SEP-16] We encapsulate the A3028 in black epoxy, then coat the epoxy with a 1-mm layer of clear silicone. The leads are stainless steel springs coated with dyed silicone. We remove one in ten transmitters from our production line for accelerated aging. These transmitters run until they exhaust their batteries while fully immersed in water at 60°C.
Corrosion is a likely cause of failure in electronic devices in warm, humid environments. Both silicone and epoxy are permeable to water vapor, so that the implanted transmitter's encapsulation becomes saturated with water vapor. Changes in the transmitter temperature provoke condensation in any cavities within the electronic circuit, such as might exist within a cracked ceramic capacitor or beneath a small surface-mount component. Our epoxy encapsulation procedure seeks to eliminate such cavities, but if they exist within the components, the condensed water, combined with the warmth of the animal body and the electrical potential presented by the circuit, result in corrosion that leads to failure of the EEG amplifier and ultimately to premature draining of the battery. At 60°C, corrosion occurs over ten times faster than at 37°C in an animal body.
The typical operating life of the A3028 in 100% humidity at 60°C is over 100 days, with the first artifacts of corrosion appearing in the EEG signal after about 50 days. Implanted in an animal, we expect no sign of corrosion in the EEG until 500 days, and no failure through corrosion until 1000 days. None of the popular versions of the A3028A run for anywhere approaching 500 days, so we claim that our transmitters will not fail due to corrosion while implanted.
We have moved our development to a separate page, Subcutaneous Transmitter Development.