Saturday 24 February 2024

The NAD 6040 Cassette Deck

The NAD 6040 Cassette Deck


Purchased off ebay UK, it was clear that this machine needed attention. As always, buying an old machine is always a risk, but I think this risk was worth it since the price was low.
 
Faulty Meters: After opening up the deck, it was found that both meters were faulty. I was aware of this possibility after questioning the seller, but I still decided to take the risk.

On inspection, the left meter dial loading spring had buckled, and the right meter dial loading spring had also buckled, but this meter had also developed an 'open circuit'. Both meters were beyond restoration, so an alternative had to be found.

I had some ideas regarding digitizing the VU meter display, but realizing this was going to be difficult and time consuming, it was decided to drop the idea and search for an exact-fit VU meter replacement.



Original Advert Picture



Original VU Meter with Fascia Removed
 
I came across a set of Chinese made VU meters that were a near exact fit, except for the fascia. The fascia of the original meters had a 'short drop' display, and with this in mind I took another chance and bought these meters, believing that I could swap the fascias. And yes indeed, this proved to be the case - so now I have a set of new VU meters for my 'new' NAD 6040 cassette deck.

The idea of swapping old for new numeric display inserts crossed my mind, but soon realized that the two scales didn't match very well, especially around -10dB and -20dB.
 
Although the meters fit perfectly, I did notice that the numeric display is unfortunately a little high, perhaps as much as 2mm? Still, this is infinitely better then no solution. In fact, I could have intervened here, but doing so may have compromised the meter's long term operating life?
 
Illumination:

The next problem was to establish suitable alternative light. The previous configuration projected light from behind the original meters, but this proved unsatisfactory since the display appeared too vibrant, almost fluorescent in appearance.
 
Shown below is the new VU meter display and the lighting that I eventually settle for, an explanation of what I did follows later.


NAD 6040 with New VU Meters.
Illumination is from under the meters.

(Long exposure photography)



NAD 6040 with new VU Meters.
Illumination is still from under the meters.
(Flash exposure photography)


Manufacturer Meter Specification
135uA FSD, and 650Ω internal resistance.

VU Meter Lighting and Assembly

Once the new fascia was removed, and the former re-employed, the next task was to find some suitable lighting. There was indeed a degree of trial and error methodology at work here, but finally settling for the following configuration.

Here strip-LED-lighting cut to length, wired, and a suitable DC voltage drop from the unregulated motor DC supply, to give just the right amount of lighting. All LEDs are deliberately running at much less than rated current of 20mA, typically about 5mA - 6mA for each of the six LEDs.




Alternative VU Meter Lighting
Strip-LED is at the base of both meters.


To facilitate this new VU meter lighting, the power supply unit had to be modified slightly.

Modified PSU Unit.
PSU was re-capped, additional fuses inserted
into the two secondary winding circuits, for
(a) DC motor and 'new' LED lighting, and
(b) Audio/bias PCB.


Modified PSU Circuit Diagram for the NAD 6040

  • Additional Fuses: Quick Blow (500mA provisionally)
  • Smoothing Capacitor C304: was 2200uF, now 3300uF, voltage rating is higher than 25v.
  • LED Circuit Series Resistance: 330Ω, 2W rated, but even a 1 watt rating will be okay.

Take-up Spool Issue

There was insufficient torque developed by the take-up spool which was accounted for from the lack of driver-to-idler friction. This was resolved by putting the cassette deck into Play mode, 'roughing up' and thus 'cutting' into fresh rubber, the idler tyre with fine sand paper. Any debris resulting was cleaned up, and the idler was later carefully cleaned with IPA, and then later again treated with Rubber Renue.

All other gears and frictional pulleys were cleaned, again with IPA.

All relevant mechanisms were cleaned and lubricated.
There are no signs of cracking plastic - good!

Record/Playback Head

The record/playback head works well, but does show signs of wear on its face. Any resetting of azimuth is out of the question, since the wear grove will probably influence any future azimuth adjustment. So either the head will be lapped, or a replacement will be fitted.

At the time of writing, the original head has been removed.

Head inductance estimated prior to lapping: L-Ch ~ 90mH, R-Ch ~ 83mH. All estimated at 1Khz.


Original NAD 6040 Record/Playback Head Before Removal.


Record/Playback Head Removed


The Original NAD 6040 Record/Playback Head
To be lapped.
There is more head wear and corrosion
than this photograph is suggesting.


Lapped Record/Playback Head

Although I have a small stock of record-playback heads with Metal tape capability, and so could have directly replaced the head, getting the original head lapped was the preferred option. The head was successfully lapped by https://www.summertone.com.
 

 
Once the head was tested for Left/Right channel inductance changes - no significant variations between before and after lapping were found, and so the head was reassembled. Azimuth was provisionally set, and other matters concerning this deck now followed.

Head Height

Only just discovered that the default shim is raising the record/playback head too high. This became apparent when I could hear music in the right channel, deep into the erase noise on the other side (actually the other half) of the tape, but this time playing backwards. The default shim appears to be too thick. In fact when I first observed the said shim, this was my immediate though. Was this the original shim as NAD intended?

This will be resolved later.
 
 
Biasing Problem
 
It became apparent that biasing the NAD 6040 for a reasonably flat frequency response from 1Khz to 10Khz at -20dB (ref: Dolby Level) was difficult. The bias trimming potentiometers could not set the bias low enough to obtain a reasonably flat response to 10Khz.
 
Examining the biasing circuit there were a few options available - change (a) C162 and C262 capacitances (250v or higher rating) to lower values (say 100pF), thus increasing their impedances, or (b) replace with an increased R315 value to supply the bias oscillator with a lower DC voltage. The objective was to effectively lower the amount of high frequency bias voltage, or more importantly - lower bias current.
 
Initially I changed the already 220pF C162/C262 in circuit for 100pF, and although this partially worked, it wasn't enough.

Later, inspecting the DC voltage dropping R315 resistor for the bias oscillator, revealed that during the assembly of this deck, the NAD production line had made a mistake?!

According to the service manual R315=510Ω, but in its place was 390
Ω?  This was the reason why I could not bias Normal (Type I) tapes properly.

Since I have a large stock of 470
Ω (1/2 watt) resistors, these proved to be a suitable replacement. The result of this was that I could now bias the deck so that provisionally the record/playback response goes past 10Khz to >16Khz at -3dB, reference 1Khz.
 



Head Height 

Returning to the head height issue, it was clear that the inner most channel (the right channel) was too high causing some low cross talk interference with the adjacent right channel. Although this cross talk was low, it could be sometimes heard if one side was unrecorded.

After thinking about this, it was decided to lower the plastic head height post on the head assembly in very small increments. Sanding down that said post down by several tens of microns was seemingly the only option?

New Rec/PB Head

There's no doubt that this was proving to be successful as the cross talk lessened each time. However, it came to the point where I decided to  change the head completely - this time cross talk was so low it was barely detectable. Here subjecting the tape to a 333Hz test tone at about +10dB (Ref: Approx 160 nWb/m DIN), the tone could just be heard in the right channel buried deep into the noise - this was as good as it was going to get.

Lowering The Head Post
Photo taken during several careful stages of 'sanding'


New Metal Tape Compatible Record/Playback Head

With the new head finally soldered in, the correct head height, and  azimuth had to be established. This was achieved using my home made Nakamich DR10 made 3Khz reference tape. The process of establishing correct height is a time consuming process of trial and error where various or multiple shims are placed between the head post and the base of the head platform on the right hand side. Here in this initial photograph, there no shims inserted.


With the plastic head height post 'sanded down' by a fraction of a mm, the highest output was achieved using just the one (ironically original) shim. Azimuth was set using an ABEX 10Khz full track reference. The entire head and path were demagnetized before reference tapes were used. Many of the calibration settings that followed were still only provisional.
 
Head Depth

During Play operation, I sense that the depth of the head into the cassette is a little excessive. This I believe also applied to the original head?

Later I will have to carefully ream out a groove in the head support base holes of about 0.5mm ... 1mm in the direction of forward head movement to effectively lessen head depth during Play.

Revised Head Depth

With the locating holes on the platform of the record head 'reamed' slightly to facilitate less head penetration during Play/Record, and with the original shim in place, finally thoughts turn towards calibrating this machine.

Provisional Frequency Response

With the bias circuit modified again to its original factory state from the changes previously mentioned above, a frequency record/response curve was determined using a TDK D46 cassette tape.

On the application of White Noise during record at approximately -20dB (Ref: Dolby Level in this case), the playback plot is shown below.
 
Fast Fourier Transform Plot
of the NAD 6040 Cassette Deck.
PB response is approximately to 15,000Hz,
at -3dB, reference: 1Khz.


Total Harmonic Distortion (on TDK D46)

For an estimation of THD (Total Harmonic Distortion) at 1Khz, a recording was made at Dolby Level, then played back at a level of +1dB above Dolby Level we examine the following Fast Fourier Transform plot -


As can be seen, only the 3rd harmonic dominates, which is very convenient.

This greatly simplifies the expression for THD.

Generally Total Harmonic Distortion is defined as ...



Where V1 is the fundamental frequency, and V2, V3, V4 etc, are harmonic distortions of V1.


However, since it is only the 3rd harmonic we are considering, this simplifies to just THD ~ V3/V1 or THD ~ V@3Khz/V@1Khz.

From the Fast Fourier Transform capture, the Third Harmonic lies at approximately -12dB below the 1000Hz test tone which is at +36dB on this scale. Therefore, this difference is ~ -48dB, and so the THD can be estimated from ...

-48dB = 20⨉LOG(V@3Khz/V@1Khz)

or

10^(-48/20) = V@3Khz/V@1Khz
 
or V@3Khz ~ 0.004×V@1Khz
 
That is, THD ≅ 0.4% at +1dB playback above Dolby Level


VU Meter Amplifier Revision

The gain of the AN6552 OP Amp was modified slightly to allow the VU Meters to be calibrated to '0' at Dolby Level. This small revision gave me about an extra 3dB of voltage output for the meters, which is what was required.


Wow & Flutter and Speed Drift

With a belt 70-72mm in diameter, and 3.5mm in width, early wow and flutter figures were determined over a period of about 9 minutes. The belt was from my stock, not necessarily the one I'll finish with, so it's provisional. (Later discovered that 4mm wide belts tend to get thrown off - they are simply too wide!)

The wow and flutter, and target speed figures are based on a ABEX 3.15Khz full track test tape. Target speed is 3150Hz, the deck was set to around 3155Hz, and drifted to an estimated 3165Hz in about 10-15 minutes, that equates to 0.16% and 0.48% fast respectively, assuming the ABEX tape is precise.




DC Motor Swap

Despite the fair-to-good wow and flutter figures I could still hear occasional very slow-moving speed changes, something that was not going to be detected by the wow and flutter program WFGIU.EXE.

It was decided to disassemble the original and swap it for a NOS Mabuchi ED-550L 12DC, 2400 rpm motor with internal speed controller.

Since sourcing a 2400 rpm, 12V DC brushed motor with 2.5mm shafts is very difficult, the problem here was matching a 2.5mm centered-hole pulley to a 2mm motor shaft. Some reliable adaptation had to made between the new Mabuchi 2mm motor shaft and the 2.5mm centered-hole pulley.

Experimentally, a 2.5mm outer diameter brass tube was cut to length and this was carefully 'hammered' into the original pulley. Next this new adaptation had to be fitted to the 2mm Mabuchi motor shaft. It was a close fit, but not tight enough, and so experimentally the motor shaft was bonded to the inside of the brass tube, which already had the pulley fitted.

After allowing 10 hours for the bond to 'cure' (24 hours recommended), the NAD 6040 was temporarily tested for speed stability, and wow and flutter.



New Mabuchi 12DC, 2400 rpm Motor.
Original pulley fitted via 2mm to 2.5mm adaptation.
So far - very stable, pulley movement is very concentric.
Note: the glue expands as it 'cures'.




Original Pinch Roller Returned to the NAD 6040

Wow and flutter figures continued to be too variable and unpredictable for my liking, and later they even increased significantly from the above figures.

Observing close-up the 'new' pinch roller, I discovered that the said roller's rubber surface was oscillating back and forth along the line of the capstan as it turned!

So again, I had to open up the deck and re-fit the original roller, followed by 'sanding down' the roller, and then cleaning off the residue with IPA.

What happened next surprised me - the wow and flutter figures fell to under a mean value of 0.087% wrms. It seems the newly bought roller was substandard!? (No, I later
discovered that the pinch roller 'tyre' was not seated correctly on its rim, the imperfection was tiny, but enough to cause wow/flutter disturbances)


Original (and 'sanded') Pinch Roller Returned
Mean wow & flutter: ~ 0.087% WRMS.
Observe: increased dispersion in wow/flutter with time.
Possible cause - no apparent back tension on the NAD 6040?
Therefore, as the supply reel 'empties out' it loses mass,
thus less inertia, and less 'drag'.

Finally, the restoration is complete, a summary may follow later.


cassettedeckman@gmail.com

*This write up may be subject to alterations, corrections, and additions without notice. 24/03/2024 

Revision: (08/04/2024)

Thursday 1 February 2024

Mitsubishi DT-4700 Cassette Deck

 Mitsubishi DT-4700 Cassette Deck
 

Bought early January 2024 for just £25 including postage, I decided to gamble on restoring this good-looking, well made deck, rather heavy cassette deck.

Original Advert:
 


 

Today, the Mitsubishi DT-4700 has been fully restored.





Some of the work undertaken is summarized below.

DT-4700 Fascia & Controls: Washed and dried. All chassis screws frequently used had their threads 'bathed' in oil - making them easy to take out, and and return. The tape activation controls were cleaned with a mixture of metal polish and water 'worked in' with a cloth until they were shiny, then finally polishing the controls with a dry cloth.

Switches & Potentiometers: All cleaned with contact cleaners.

Pre-amplifier, Dolby Board, and Record Amplifier:
Completely re-capped, and re-transistorized.

Power Supply Unit: Re-capped, some new diodes, new regulation transistors.

When working through the above, it is always important to periodically check system voltages - PSU, and amplifier stability before moving to the next batch of components.

Mains Switch Failure:

The original mains ON/OFF latching switch eventually failed, internally a plastic pin had broken. It became obvious that repairing this was out of the question; when working with high voltages it is advisable not to take repair risks.
 
Luckily I found some 250v rated single pole, single throw (SPST) switches on ebay that could be adapted. 



Shown below is the original mains switch and transformer circuit. Note the 10nF suppressor capacitor is across the Live and Neutral. I may add an additional suppressor across Live and Neutral later!?





Failing Auto-Stop:
 
At the rear of the cassette transport is a rotating disc that effectively interrupts an infrared beam from an excited, forward-biased LED, which is then picked up by an adjacent photo-transistor. The design is to generate light interruption and hence develop a square wave which then feeds an RC timer circuit. If the period of the wave is too long, then an auto-stop is generated by energizing a solenoid to force a Stop.
 
I had problems with the auto-stop unit, and had to run the deck with this feature disabled for a time until the problems were diagnosed.

After replacing transistors in the auto-stop circuit, it later became apparent that one major source of the problem was the photo-interrupter circuit; this being the light emitting LED and photo transistor combination.

Testing the unit 'offline' suggested that the LED was faulty - I could not forward bias the diode to conduct.

A not-so-perfect solution was then to re-house the unit with a new infrared LED/photo-transistor combination. The unit had to be part-drilled to enlarge the aperture so that both LED and transistor could be fitted. Unfortunately this did not produce a great fit, so gluing the two  semiconductors was the only viable solution - a 'glue gun' was used instead of a permanent 'super glue' bond.






The LED and photo-transistor had little effective depth, and so gluing was the only option, the 3mm bore also proved to be too wide.

Front side of IR LED and Photo transistor Circuit Board


Solder side


An infrared LED, infrared photo transistor, and mounting screws
are 'buried' inside heat-gun glue.
It's not 'pretty', but it's strong and stable.
(I may later re-work this?)


The work done doesn't look professional or 'cool', but it is functional and very stable.

The circuit diagram below illustrates the basic operation of the circuit.

Note - the IR LED is permanently on when the deck is switched on.

The original in-line resistor (1W rating) was 680Ω, but was later replaced by a higher 820
Ω, 2 watt rated resistor.

Since both IR LED and photo transistor are closely coupled, I believe I could still further increase this resistance to 1K
Ω, and hence lower the IR beam intensity, and still maintain a good beam to the photo transistor. I'll try this later.

The value of the IR LED current was initially about 23mA; while it's now around 18.3mA. From general experience with LEDs, I don't see why I couldn't lower the excitation current further, thus reducing the likeliness of later unexpected IR LED failure? Remember, this IR LED is permanently conducting, even if the deck's motor is not active.
 
The oscilloscope trace below shows the collector voltage of the photo-transistor during Rewind operation. Accessing and part-rotating the sensor holder behind the cassette transport will alter the duty-cycle of the waveform; therefore, an ideal 50% duty-cycle was sought.


Auto-stop now runs perfectly, with a switch off time of about 3 seconds.

Auto-Stop Warning:
 
The Mitsubishi DT-4700 cassette deck's auto-stop unit works off the supply reel, and not the take up reel. Which, in my opinion is not a good design.

Reasoning - if the 'take up' spool stops turning, the auto-stop will not detect this event, and so the right hand side of the cassette tape will eventually jam or seize with tape!

Recording Pre-emphasis: Otherwise referred to as Recording Equalization. This sets the level of high frequency recording emphasis (gain) when the audio is applied to the recording head. The objective is to drive a near constant recording current with rising frequency. The deliberate rise in voltage amplitude to the record head begins at around 300Hz to 500Hz. 

Pre-emphasis can be trimmed from a ‘resonance circuit’ in the emitter leg of Q501/Q601 – to increase or decreases this pre-emphasis, the ferrite core L501/L601 inductance can be decreased or increased accordingly.

Here, the pre-emphasis of both channels was set to match each other.

The overall pre-emphasis gain of current signal level is indicated in the service manual - from the chart, the gain over 400Hz at 10Khz is about 7.5dB.

Since some sibilance distortion was noted, pre-emphasis was reduced a little to try to 'kill off' high frequency saturation..

Playback De-emphasis: Originally R114 was a 3.9KΩ fixed resistor, I swapped both channels for a 10KΩ trimmer potentiometer so that both channels could be matched on playback exactly. Prior to removing the old resistors, their values were measured, and the potentiometers that replaced them were also set to the same values. 

The level of de-emphasis on this Mitsubishi is approximately the same as found on many late 1970s decks in my possession.






Dolby Level calibration points as suggested in the
service manual are also shown.

Tape Speed Variability

The deck's transport was surprisingly stable as the graph shows over a period of just over 10 minutes.

The target speed from the ABEX reference tape is 3150Hz, as can be seen, I accidentally neglected to check this! However, this is unimportant since (a) I can rectify this easily, and (b) the objective of the test was to check the deck for speed variations.

Wow & Flutter

Even with the original pinch roller, and a slightly temporary narrow drive belt, wow and flutter figures returned by WFGUI.EXE were very satisfactory, averaging at about 0.065% wrms.

Additional Interior Shots







February 2024.

Tuesday 26 December 2023

Detailed Modelling of a TA7122AP Equivalent Circuit

Detailed Modelling of a
TA7122AP/
ECG1085
Equivalent Circuit

  • Biasing of Q1 is achieved by linking Pin 5 to Pin 2, typically 100KΩ.
  • Voltage-Series Feedback and hence accurate gain is achieved by
    linking a feedback network between Pin 6 and Pin 3.
TA7122/ECG1085 Re-drawn
The TA7122AP or ECG1085 Voltage Amplifier

  • For this analysis, Voltage-Series feedback (in blue) is not added to the circuit, but is designed to be employed later to generate an accurate voltage gain at Vo.

  • To the left of Vin is the signal generator, the signal generator's voltage source is Vs, or for this article 𝚫Vo

  • Some circuit component values differ slightly from the original specification, this will be considered in calculations.

  • Parasitic capacitances will be ignored since we are only concerned with audio frequencies.

 

As promised in my last article, a more detailed analysis of the Toshiba TA7122 voltage amplifier now follows. This is not intended to be an electronics tutorial, but more of an attempt to model this old and interesting amplifier, and compare the analysis with actual measured results. Bear in mind both theoretical and actual measurements will have some inherent errors - the latter especially so since readings will be taken from an oscilloscope screen. Nevertheless, a general comparison can be made between theoretical and (near) actual.

I cannot guarantee that the derivation of an expression here is free of errors, but I am reasonably confident of much of the work. Some simplifications were added at the T3 side of the amplifier, where no reference is made to hie, ri, and hfe on that final stage.

It is important to represent the T1 input side of the amplifier accurately, since this is where the bulk of the gain is generated.

I may offer later, a detailed explanation of my thinking as I attempted to mathematically model the TA7122AP IC.

So then, in summary - the purpose of the work below is to establish the voltage gain of the said amplifier as it stands here; that is without Voltage-Series negative feedback that would be later inserted between Vo and the emitter of T1.

The Derivation of Voltage Gain

I will use the delta symbol '𝚫' to highlight what we seek to find.

A prediction of voltage gain 𝚫Vo/𝚫Vs without Voltage-Series feedback now follows.

Much of this is written from an electrical and electronic engineering perspective, and so assumptions of reader knowledge is presumed.

There will be no proofs of Kirchoff's voltage and current laws as this too lengthy to write out. 

Hand-written 'scribbles' and small alterations are included, but this is because this was a 'first run' at collecting all the ideas together. Word processing the work below on a computer would be fraught with difficulties as many readers will know - circuit drawing, finding the correct symbols, lengthy equation writing etc.

 

G1 is the voltage gain for stage 1
G3 could have been written for stage 3, but wasn't.

Setting RL1 = 470KΩ; any higher and the gain
would cause 𝚫Vo to saturate too easily.
With my limited equipment, it can be
difficult to generate a very low input signal
𝚫Vs which
is stable at around 2mV and less.
 

Feedback Network: Above I 'referred' the feedback circuit RF into the input side with an equivalent Thevenin circuit - as if it were all sourced at the input. This then became just one equivalent signal source (but mathematically mixed) with an equivalent input resistance.
 
No additional Thevenin circuit was referred to the T3 side in parallel with Re3, simply because it would have very little effect on calculations. This holds true as Re3 << Rf.


Below should read 'So far then, EQ 6 yields ...'

  • K1 and K2 were dimensionless definitions
    that made transposition of formulae
    and computation easier.

Labeling 𝚫VRL2 as 𝚫Vo we have





Matching Theory and Practice
 
  • Signal Generator Test Frequencies: 50Hz, 100Hz or 1,000Hz.
  • Vcc = 30 volts.
  • 𝚫Vs was adjusted so that 𝚫VR2 or 𝚫Vo did not saturate, saturation began a little higher than 25v peak to peak.
  • Signal source 𝚫Vs was measured 'offline', ie not connected to the input during 𝚫Vo measurements. Thus effectively creating an accurately measured voltage source.
  • Rs is the resistance of the source, and was measured at around 600Ω.

    The theoretical model above and its computations were performed on a Spreadsheet, with measured comparisons also included, we can finally compare.

Click on this image to see the results.


Increasing Amplifier Gain

To obtain easy control over an effective minute input signal,
a simple potential divider circuit was set up.



A claimed '90dB' gain is quoted for this amplifier if limits of its ability are exploited. With that I decided to push the gain of this near equivalent circuit to as high as I could measure, at least for now. Feedback was reduced, to accomplish this RF was increased from 100KΩ to 1MΩ! This effectively reduces feedback current into the emitter circuit of T1.
 
I needed to set up an additional circuit at the input to create a controllable, but minute driving voltage with my old equipment.
 
With Re1 remaining at 0.22KΩ, and utilizing my old (but calibrated) Hameg 20Mhz oscilloscope to measure the outcome, output was pushed to 10v peak-to-peak, and an effective but new input Vs was measured at a little under 0.25*0.00465 peak-to-peak or 1.1625v p2p. The resultant measured gain was then approximately 20·LOG(10/0.0011625) or 78.7dB.

So how did the mathematical modelling compare? With Rs now being effectively replaced by a Thevenin 0.468K, the spreadsheet computation predicted a gain 9348 with RF = 1MΩ, this equates to 20·LOG(9348) or 79.4dB.

Circuit Issues
 
The amplifier circuit wasn't without problems - with the addition of a 1MΩ feedback resistance, the amplifier's 'switch on' time was delayed, and more so if RF was increased further. 
 
The reason being the base-emitter bias voltage at transistor T1 took more time to reach the Vbe 'cut in' voltage at approximately 0.55v - 0.60volts. What creates this scenario is an effective increased Rf⨉Cbe charging capacitor time constant at the input to T1. With Rf at 1M and transistor base-emitter junction capacitance Cbe (at say ~10pF), we have an increased time constant by a factor of 10. This of course means it will take about ten times as long for T1 to switch on. There may be other factors too why 'switch on' was delayed?
 
To overcome this, use a lower feedback value - recommended 100KΩ or less.


Comment
 
Predicted voltage gain modelling results with actual were good to excellent.
 
Analysis shows that altering hfe, ri (hie), and hfe within the developed equations does not effect the outcomes significantly, and indeed this was verified by the spreadsheet program and so possible variations can largely be ignored.
 
However, dynamic output resistance (1/hoe) or ro can and does effect results. Variations in Re1 also had a strong impact on gain as expected, since this also forms part of a internal current-series negative feedback loop.
 
Regardless of the pleasing accuracy of the mathematical model, ultimately the voltage gain of the TA7122AP/ECG1085 (and their emulation above) will be determined solely by the feedback network from Vo (pin 6) to the emitter of T1 (pin 3). 
 
For official configuration suggestions, see the ECG1085 datasheet online.

------------------------------------------------------------------------

Note: Corrections and modifications to the above article may be periodically made without notice.

29/12/2023

cassettedeckman@gmail.com