People hi !
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dr_mick51: You got it all figured out
The 220pF capacitors are a modification identical to the one proposed by Lester (SYLPH AUDIO) on its PCB in order to correct the appearance of the frequency response for the extreme treble which have a very slight rise ->
View attachment 406201
If soldering the legs of the FKP2 220pF is a problem for you in this area then you can use SMD components otherwise the other solution is to solder the FKP2 directly on the pins of the OPAMPS located below the PCB, it is much more convenient. Regarding the original input resistor, it's a 22K (it's easier for me to say because I have the O-NOORUS original diagrams
). It must be replaced by a 220K for obvious reasons of adaptability of the output impedance of the device that will be connected to it.
I will try to explain: the NJW-1194 volume control has an input impedance of 15 to 20 k, which is probably variable depending on the level setting, and which comes in parallel with this 22 k R... So it's in your best interest to increase this R, you can go up to 220 kO.
Reminder:
In electronics (not limited to audio), any active system has a resistance (input, output, etc.) that is never linear but varies +/- depending on the frequency of the signal. We therefore use the notion of impedance to differentiate from pure resistance. To come back to the pairing of devices. In the case of HiFi, the ideal is for the output impedance of a device to be very small compared to the input impedance of the device to which it sends its signal. The smaller the output impedance, the more current the device can "send", and therefore not be disturbed "too much" by its load (the load, here, is the device to which it is connected). Conversely, the smaller the input impedance of a device, the more current it will "consume", and potentially disturb the source device.
If output = low impedance --> not easily disturbed If input = high impedance --> doesn't disturb much We quickly understand that the 2 together is even better! On the contrary, if the output impedance is high and the input impedance is low, very large signal disturbance in perspective (attenuation, distortion,....) If the impedances are more or less equal, we will experience a good attenuation (math shows that if the impedances are equal, the amplitude of the signal is divided by 2 exactly), and we also run the risk of disturbance (distortion).
Here is an explanation by an image of the PCB for a better understanding of the MOD ->
View attachment 406181
In this photo, the amplifier's gain is increased to 27.6dB with the 24K resistors. On my diagram (with the resistors of 15K instead of 24K) the amplifier's gain is 23.5dB.
As you have understood: the changes are in orange. The two capacitors are removed because they are absolutely useless since link capacitors are already present upstream of the TPA3255 and concerning the NJW194, nothing is indicated in the datasheet. It is good to remember that the use of bipolar type operational amplifiers is not recommended with this diagram since the resistance to the inputs will have a high impedance and its impedances will not be equal elsewhere, which will cause OFFSET! So, we will use FET or JFET type operational amplifiers because they are almost insensitive to this imbalance and are adapted to high impedances (it's not me who says it but TI). References such as OPA1656 or OPA1642 are well suited for this tour. I chose the OPA1642 not because of the measurements but for their "subjective" sound rendering...
... I find that the OPA1656 created a kind of "spacialization" effect on certain tracks or channels, which is not the case with the OPA1642 which seemed more natural to me and also has a softer extreme treble that will avoid possible "phenomena" of sibilance. This cannot be measured, it is a personal feeling (which my friends also share), however these two references will have very good results that are also very close to the measurements if we want to remain objective
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FanatNsk::
You
absolutely have to put the 4
capacitors of 220pF because as it is, you create an imbalance of the signals that are expected as "symmetrical" by the TPA3255 chip.
PS: I take advantage of this post to talk about the "heating problems" with the D1: there is none! This feeling is felt by the fact that the material (and its thickness) of the case used is different from those of the competition (FOSI., AIYIMA,...). I invite readers to read TI's datasheet about the TPA3255 amplifier chip and to look carefully at the temperatures measured for a given voltage: on the tables it is indicated 75°C for a voltage of 51V and the Tjmax.de the chip is 125°C. So with the 42°C that I read with the laser thermometer in the center of the top of the case of my D1 powered by 42V/8.3A, I am in completely normal conditions of use even if the feeling of heat is slightly greater than with other amplifiers on the market. Another explanation comes from the use of PFFB which leads to a higher heating rate unlike amplifiers which are not equipped with it.
NOTE: my sytem
with 8 Ohms speakers -> (42 VDC x 0.707)^2 / 8 Ohms =
110 Watts
View attachment 406198
For example, to "counteract" this feeling effect, AIYIMA on its A70 model which has the PFFB used a large aluminum "cube" as a contact sink in its case. However, the TPA3255 chip still works under the same conditions as the O-NOORUS D1 amplifier ->
View attachment 406279
It's a bit like I gave you a pair of insulated gloves with the amp to reassure you (LOL).
In addition, the advertisement for the A70 model is false because even with a 48V 10A Gan power supply, the 300W advertised is not reached with 4 Ohm speakers ->
(48 VDC x 0.707)^2 / 4 Ohms = 287.91 Watts.
It's not me who says it but the
mathematical formulas
Have a good day and happy listening to all.