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abraxalito abraxalito is online now

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  • Last Activity: Today 12:53 AM
  • Join Date: 19th September 2007

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Posted 20th October 2015 at 08:49 AM by abraxalito Comments 0
Nowadays with discrete transistors as affordable as they are, the most cost-effective solution for a particular audio application may well be a discrete one when SQ (rather than numbers) is uppermost. Audiophile faddishness about discretes aside.

Here's a case in point - my pic shows a headphone buffer where the design aims were lowest cost, smallest size and lowest battery drain, while maintaining acceptable SQ. There are 28 transistors which go for 0.04rmb each on Taobao. That's 1.12rmb. OK so you can also buy 2 NJM4556s for that, but how do they sound? In my experience of building an O2-alike, not so great. They're also going to take 15mA at 7V whereas this design takes 6.5mA at 3.6V input. So an integrated design will be more than 4X as power hungry. With a 2600mAh single cell LiIon this could run for 400hrs - over two weeks continuous if played at low level.

The power supply is created by an LM2662 which inverts the 3.6V positive input for a -3.6V rail. It...

Posted 14th October 2015 at 03:57 AM by abraxalito Comments 2
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Here's the power supply I've lashed up to feed the balanced SE classA amp.

Its fed from a 5VA EI transformer with a 65VAC secondary. One 390uF cap follows the rectifier, then there's a 30mH choke, two 390uF caps beyond that.

A series regulator is made from a string of 3 TL431s as reference (the max from a single one is 36V - I've gone for a total of 78V) and that's followed by a 2SK213 simply because I had no other high voltage transistor to hand. There's an RC filter feeding the gate of the MOSFET to reduce the output noise from the shunts (68k,200nF).

Output ripple isn't visible on my scope but I plan to feed the output into my AC millivoltmeter and see what its giving out in terms of noise.

Posted 10th October 2015 at 02:55 AM by abraxalito Comments 4
Headphone amps aren't any different from speaker amps in principle - what you hear (apart from a bigger version of the input signal) is the power supply's noise coupled through the inadequate PSRR of the electronics.

SE classA operation is a way to minimize the generation of power supply noise by arranging the current flow to be constant to a first order so that any remaining ripple on the supply is the result of the finite output impedance of the follower's loading current source and those of the driving stages. But how significant are these 2nd order effects? This design is an attempt to find out - by reducing them as far as practicable.

The idea is to run SE classA at a much higher voltage than is needed to drive the 'phones (balanced, with 80V supplies giving 144V peak-peak) then step down the output voltage with a custom-wound output transformer. This has the effect of increasing the PSRR of the amp's output stage. I'm not worried overmuch about the PSRR...

Posted 25th September 2015 at 02:56 PM by abraxalito Comments 2
Since I figured out the reason for needing all those caps in my earlier DAC designs was all brought on by using passive I/V, I'm now a total convert of active I/V in order to do away with the sheer bulk.

Having tried single transistor I/V and loved it, I found there was still some improvement to be gained by biassing the common-base transistor with additional current sources to reduce its input impedance. Since getting down to the region of 1ohm would require some 25mA of bias which isn't well suited to portable applications I decided to have a go at using feedback to obtain the impedance I'm seeking.

I'm not using an off-the-peg CFB amp because they still turn out to be fairly power supply quality susceptible (subjectively speaking) so here's a design I hope that greatly reduces the supply impedance requirements so that it can be used in a portable player.

The picture shows the second prototype I/V stage, coupled to a 6th order Chebyshev anti-imaging...

Posted 21st September 2015 at 12:54 AM by abraxalito Comments 7
I've been getting a lot of use out of Simon Bramble's webpage for designing active filters recently - Its a great resource.

Right down at the bottom of the page the last filter he shows the schematic of is a 9th order Chebyshev, 1dB ripple, with a corner frequency of 1kHz. A textbook frequency response plot is obtained using LTC6241s. I latched on to this and tried changing the corner frequency to 18kHz, wondering if I could use such a design for an anti-imaging filter for my DACs. So I divided all the capacitor values by 18 and ran the sim. Disaster! The frequency response I obtained is below - a 7dB spike at 17kHz.

The problem seems to be inadequate Q - high order filters are composed of sections which increase in Q (more positive feedback) and the chosen opamps aren't fast enough (18MHz GBW). I went to a faster opamp for the highest Q stage which brought about some improvement...
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I read that thread some...
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Hi, maybe your current...
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Looking good, the 30mH...
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