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Fig. 1 shows the single ended nature of air.   We can push on it and raise the pressure an
arbitrary amount, but we cannot pull on it.  We can only let it relax and fill a space as it will;
the pressure will never go below "0".  As we push on air, the increase in pressure is greater
than the corresponding decrease when we allow air to expand.  This means that for a given
motion of a diaphragm acting on air, the positive pressure perturbations will be slightly greater
than the negative.  From this we see that air is phase sensitive.

As a result of its single ended nature, the harmonic content of air is primarily 2nd order, that is
to say most of the distortion of a single tone is second harmonic.  The phase of this distortion
reflects the higher positive pressure over the negative.

Air's transfer curve also shows also that it is monotonic, which is to say its distortion products
decrease smoothly as the acoustic level decreases.  This is an important element that has
often been overlooked in audio design and is reflected in the poor quality of early solid state
amplifiers and D/A and A/D converters.  They are not monotonic: the distortion increases as
the level decreases.

The usual electrical picture of an audio signal is as an AC waveform, without a DC
component.  Audio is represented as alternating voltage and current, where positive voltage
and current alternates with negative in a reciprocal and symmetric fashion.  This fiction is
convenient because it lends itself to the use of an energy efficient design for amplifier power
stages known as push-pull,  where a "plus" side of an amplifier alternates operation with a
"minus" side.   Each side of a push-pull amplifier handles the audio signal alternately; the
"plus" side supplying positive voltage and current to the loudspeaker, and the "minus" side
supplying negative voltage and current.

Problems with push-pull amplifier designs associated with crossover distortion have been
discussed elsewhere at length, and one of the primary results is non-monotonicity.  Class B
and many AB designs have distortion products that dramatically increase with decreasing
signal.   This is reduced greatly by Class A mode, but crossover distortion remains as a lower
order discontinuity in the transfer curve.

For reproducing music as naturally as possible, push-pull symmetric operation is not the best
approach.  Air is not symmetric and does not have a push-pull characteristic.  Sound in air is a
perturbation around a positive pressure point.  There is only positive pressure, more positive
pressure, and less positive pressure.

Push-pull circuits give rise to odd ordered harmonics, where the phase alignment reflects
compression at both positive and negative peaks and crossover nonlinearity near the zero
point.

Only one linear circuit topology delivers the appropriate characteristic, and that is the single
ended amplifier.  Single ended amplification only comes in pure Class A, and is the least
efficient form of power stage you can reasonably create, typically idling at more than twice the
rated output power 

under the best of conditions.

Single ended operation is not new.  It is routinely found in the low level circuitry of the finest
preamplifying stages and in the front end circuits of the finest power amplifiers.  The first tube
power amplifiers were single ended circuits using a single tube driving the primary of a
transformer.

Summary of Contents for Aleph 0

Page 1: ...Pass Laboratories Aleph 0 Owner s Manual ...

Page 2: ... Class A circuits to preamps and input stages I feel that in specialized and demanding applications the energy penalty is worth the purity of performance obtainable from single ended Class A operation This purity delivers the most musicality and listening satisfaction per watt of any operating mode Over the years I have remained fascinated by the characteristic sound of the single ended topology b...

Page 3: ...jumper can be used between pins 1 and 3 on the XLR which terminates the pin 3 negative input to ground When running unbalanced input use of this plug will increase the amplifier s gain to 26 dB in the event that you need or prefer higher gain than the standard 20 dB figure If you don t need that extra gain our own preference is to not use the shorting plug If you insert the copper shorting jumper ...

Page 4: ... with the same specs sounded the same We have heard Triodes Pentodes Bipolar VFET Mosfet TFET valves IGBT Hybrids THD distortion IM distortion TIM distortion phase distortion quantization feedback nested feedback no feedback feed forward Stasis harmonic time alignment high slew Class AB Class A Pure Class A Class AA Class A AB Class D Class H Constant bias dynamic bias optical bias Real Life Bias ...

Page 5: ...s in series with the signal path the better This often true even if adding just one more gain stage will improve the measured specs 2 The characteristic of gain devices and their specific use is important Individual variations in performance between like devices is important as are differences in topological usage All signal bearing devices contribute to the degradation but there are some differen...

Page 6: ...serves as a natural benchmark Virtually all the amplifiers on the market are based on a push pull symmetry model The push pull symmetry topology has no particular basis in nature Is it valid to use air s characteristic as a model for designing an amplifier If you accept that all processing leaves its signature on the music the answer is yes One of the most interesting characteristics of air is its...

Page 7: ...amplifier alternates operation with a minus side Each side of a push pull amplifier handles the audio signal alternately the plus side supplying positive voltage and current to the loudspeaker and the minus side supplying negative voltage and current Problems with push pull amplifier designs associated with crossover distortion have been discussed elsewhere at length and one of the primary results...

Page 8: ...reaches the single ended bias point of the Aleph 0 it is considered a single ended Class A amplifier as the bias is provided by a current source attached to the negative power supply Beyond the single ended bias point it will operate as a push pull amplifier in the conventional sense leaving Class A at twice the bias point or about 120 watts peak into 8 ohms A very important consideration in attem...

Page 9: ...at small fractions typically 20 of their ratings For extended life we do not allow chip temperatures to exceed 80 degrees C Regardless of the type of gain device in systems where the utmost in natural reproduction is the goal simple single ended Class A circuits are the topologies of choice While it will not leave Class A on an unclipped positive signal a single ended Class A design would ordinari...

Page 10: ...any environment the amplifier is equipped with balanced inputs featuring a common mode noise rejection of greater than 60 dB Balanced operation is accomplished through a passive network tied directly into the input stage of the amplifier not with additional active input circuitry as in other products This assures that the noise benefits of balanced operation are not accompanied by the degradation ...

Page 11: ...ance 01 ohm Input Impedance 25 Kohm differential XLR 10 Kohm single ended RCA Common mode rejection 60 dB Output Noise 600 microvolts DC offset less than 100 mV after warm up Power Consumption 300 watts at 75 watts output Operating Temperature 50 degrees C Warm up time 1 hour minimum Dimensions 12 W x 12 D x 10 5 H Shipping Weight 68 lb PASS PASS Pass Laboratories 21555 Limestone Way Foresthill CA...

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