This compact unit, powered by an external 24V DC “wall wart” or battery,
provides very high sonic fidelity, no audible noise, and switchable loudness
compensation.
The maximum output power of this phone amp is 137mW into 300 phones, and 218mW
into 32-ohm phones. With the (most excellent; see sidebar) Sennheiser HD 650
300-ohm phones, maximum undistorted SPL is 119dB sine wave, corresponding to
about 105-108dB music waveform aver age, which is about the SPL of a large
orchestra playing full blast.
AMPLIFIER CIRCUIT
The output stage Q3-Q4, biased by constant-current sources Q1-Q2 (and associated
diodes and resistors), is a unity voltage gain power amplifier with a BW (bandwidth)
of about 1.5MHz ( Fig. 1). Q3-Q4 bias is about 30mA, enough to ensure Class
A operation up to full power with 300-ohm phones. With 32-ohm phones, operation
will be class AB at high power, but distortion will still likely be inaudible.
But you can obtain full Class A with 32 phones by increasing Q3-Q4 bias to
about 120mA, by changing R13, R14 to 1.2k-Ohm This, though, increases the dissipation
of Q3 and Q4 from 0.36W to 1.1W, so you should use small TO-220 heatsinks (or
insulated chassis heatsinking).
The TL082 input stage has a Class AB output. However, measurements involving
supply current monitoring established that the TL082 output bias is 0.62mA,
and its operation is Class A up to a load current of about ±1.2mA peak. The
application here draws only about ±0.5mA peak, so the TL082 is always in Class
A. This, plus a 1.3MHz available BW (reduced to 230kHz by C4), ensures high-purity
amplification by the TL082.
INPUT STAGE AND FEEDBACK
The (hail per channel) TL082, operating in Class A as described, provides
stable gain, low DC offset, and low noise (in audible; about 4dB SPL with the
most sensitive phones). Feedback resistors R6, R8 precisely set the gain. C4
applies negative feedback locally around the op amp, above about 230kHz (the
-3dB roll- off frequency of the overall amplifier). This cap is not necessary
for stability; without C4 the amp’s -3dB bandwidth is 1.26MHz and stable, but
this invites AM radio interference, and so on.
50-ohm OUTPUT IMPEDANCE
The feedback is taken from emitter resistors R17, R18, giving this junction
a very low output impedance (<1-ohm) So why the series 50-ohm R20? This,
of course, sets the amp’s output impedance at 50 The reasons for this are:
1. Output is unconditionally stable — open, short, pure reactance.
Above: Fig. 1a: Transistor Pinouts. A-2512-O1 -- 2N3904 TIP 29; 2N3906 TIP
30
2. Output is short- circuit proof.
3. Power delivered to 300-ohm and 32-ohm phones is approximately equal (about
3dB higher with 32-ohm phones, but they tend to be less efficient).
But what about “damping factor”? Unlike speakers, whose bass resonance might
show a 10x impedance rise, phones have a nearly constant, nearly resistive
impedance. The Sennheiser HD 650 (see Table 1) has a resonance Z of 481-ohm
(re 300-ohm nominal). With a 50-ohm amplifier output Z, the signal increase
to the phones at their 12 resonance is only 0.5dB. If this concerns you, you
can delete H20. But then a clipping signal level into 32-ohm phones could deliver
about 2W, blowing the phones and perhaps your ears!
POWER SUPPLY
To eliminate concerns about AC line pollution, I decided on an external “wall
wart” DC supply. The unit specified in Fig. 2 works perfectly and causes no
audible hum, or other noise (Photo 4). The circuit comprising Q1, 2 derives
a stable voltage that’s very close to the midpoint of the incoming single-ended
DC supply voltage.
Basically a push-pull Class AB buffer amp, the output (H5-R6 junction) serves
as the circuit ground, to which is then referenced the desired bipolar (about
±13V) supply. You could add voltage regulators, but they are not necessary
because the amplifier has a very high power supply rejection ratio (PSRR).
Including regulators would lower the supply voltage, and therefore the amplifier’s
maximum output power.
INPUT CIRCUIT
The ALPS 100KAX2 100-kOhm stereo volume control pot ( Fig. 1) is, as of this
writing, available at Radio Shack for about $3. This is a bargain—buy all you
can. Quality appears to be excellent, and they have a 10% tap which I used
for switchable (low) loudness compensation. Of seven units, I measured attenuation
tracking (L/B), from 0 to -40dB, to be between about ±0.2dB and ±1dB (this
does not depend on full-H matching, but rather on matching of the ratios of
wiper-to-ground H to the full H). I suggest purchasing a number of units and
selecting for best attenuation tracking.
R2 and C1 filter HF interference, such as AM radio stations. C2, the only
cap in the audio path, removes any source DC offset that would cause noisy
attenuator operation. I used a 1.0uF 100V metal poly cap from Digi-Key (EF1105),
10 for $7.36. Or, you can spend whatever you like on the audiophile cap of
your choice. 111 keeps C2 discharged with no input connected.
TABLE 1. Characteristics of Sennheiser Headphones. Sennheiser HD 650
Comparing the HD650 with the Grado RS-2 (both about $450), the Grado had some
upper midrange roughness, while the Sennheiser sounded exceptionally smooth
and tonally neutral.
Above: Fig. 2: Power supply for HA-2 headphone amp.
Above: Fig. 3: Loudness compensation responses—attenuator setting 0 to —25dB
in 5dB steps.
The gain (3.2W/300-ohm phones) is such that at full volume (attenuation at
0dB), a 2.0V RMS input (Red Guide CD 0dBFS = full scale) drives the amp to
full power, producing 119dB SPL peaks, and about 107dB average music SPL —about
that of a large orchestra playing full-blast—on the Sennheiser HD650 phones.
But you can easily change the gain (with R6); the circuit maintains stability
and adequate HF response over a gain range of at least 1 to 10.
LOUDNESS COMPENSATION
When S1 activates this, R3, R4, and C3 provide the LF boosts versus attenuation
shown in Fig. 3. Maximum boost occurs at 20dB attenuation and then stays constant
below that level. Down to about -30dB (re full volume), the boost nicely compensates
the loss in LF hearing sensitivity (Fletcher-Munson con tours) from i0OdB
SPL down to 70dB SPL, within about 2dB to 20Hz. The compensation is not adequate
for much lower than 70dB SPL, but with good headphones why listen at lower
volume?
Unlike many attempts at such compensation, that used here does not sound “boomy”
or “muddy.” With a maximum boost of only 3dB at 100Hz, 7dB at 36Hz, and that
only at and below -20dB volume, the compensation simply maintains natural bass
fullness as the volume is decreased.
Note: If you use the ALPS 100k AX2 pot, you can use Photo 2 as a calibrated
dB template. These pots are very unit- to-unit consistent regarding attenuation
versus rotation angle.
CONSTRUCTION
Don’t do what I did—I (barely) stuffed everything into a 5 1/8” x 2 7/8” x
2 1/8” aluminum “Bud Box Clone” from Radio Shack (Photo 5). Fabricating a PC
board, as opposed to the “rat’s nest on balsa wood, lots of glue” construction
I used, might save space, but I think the enclosure should be at least 6” x
3” x 3” in size*.
The DC supply input jack must be insulated from the metal enclosure. As Photo
3 shows, I cut a 3/4” hole (with a Greenlee chassis punch—very precise and
burr-free), then mounted over the hole a piece of the schematics; I used OHS
(on-hand thick plastic, on which the DC jack was mounted.
I didn’t use any shielded cables for the audio input paths, hence the 20kHz
crosstalk of -66dB (not that anyone would notice it). But coax cable input
connections would certainly improve 20kHz crosstalk, if only for the sake of
impressive numbers.
Regarding Photo 5, I didn’t use the transistor types specified in stock) types,
similar enough to those specified. The circuit is very insensitive to transistor
parameters (I’ve verified this by trying very different transistors; no noticeable
degradation).
ADDING A SECOND PAIR OF OUTPUTS
You can connect a second 50 resistor to the R17/R18/R20 junction to drive
a second output. If driving two pairs of 300Q phones, the output stage Q3-Q4
will go into Class AB above about half the full voltage output. I’ve found
that such Class AB loading appears clean (no visible crossover distortion nor
obvious sonic anomalies). But you can achieve full Class A operation with two
pairs of 300-ohm phones by increasing the bias to 6OmA (change R13, R14 to
560-ohm). Small heatsinks on Q3, Q4 may or may not be needed; if Q3, Q4 are
not too hot to touch, they’ll be fine.
===
TABLE 2 HA-2 Headphone Amp Measurements.
Maximum Gain: 3.705 11.4dB, no load
3.176 = 10.0dB, 300-ohm load
1.428 3.1dB, 32-ohm load
At maximum gain, 0dBFS 2.0V RMS (Red Guide CD Full Scale Signal) drives amplifier
to full output.
Loudness Compensation (switchable): Maximum at attenuator —20dB; constant
below —20dB: *3dB at 100Hz, 7dB at 36Hz (close to equal-loudness contours fur
80dG SPL re> 100dB SPL)
===
SENNHEISER HD-650 PHONES
Is $450 expensive for headphones? Well, to quote the Chuck Mangione song title,
“Compared To What?” Most audiophiles wouldn’t blink at spending $450 for a
good pair of speakers, especially if they were almost ruler flat from 20Hz
to 20kHz, could produce 120dB SPL, and reproduced clean 16Hz at 100dB SPL.
Not on this planet for $450!
But these headphones do all of the above, plus they have razor- sharp, time-adjusted,
pristine transient response (not to ion the obvious freedom from room acoustics).
Tonal reproduction is effortlessly and extremely natural, “Coloration” doesn’t
appear to be in these phones’ vocabulary.
As wonderful as this is, there’s something beyond, difficult to describe,
when these phones are driven by a highly transparent, sonically noiseless amplifier,
fed directly from a player, particularly an SACD or DVD-A unit: You will be
repeatedly startled into instinctively looking around as you hear quiet but
clearly-revealed background noises, such as the conductor’s footsteps, musicians’
motions, distant glasses clinking, and everyone breathing. Every subtle sonic
nuance produced by the instruments is revealed with crystal clarity. If an
unexpected, well-recorded xylophone is played, For example, you’ll swear the
resonating metal is right in front of you—downright spooky.
===
The amp (with the pair of 50-ohm output resistors) can drive two pairs of
32-ohm phones, but since it’s not recommended to increase Q3, Q4 bias above
120mA (the level for full Class A driving one pair of 32-ohm phones), operation
about half the full voltage output will be Class AB. But the 120mA bias is
more than enough to ensure the absence of crossover distortion; the sound will
still be very clean
ELECTRICAL PERFORMANCE
Table 2 summarizes the measurements. I don’t have a distortion analyzer, but
THD up to just below clipping is probably no more than the 0.004% typical of
the TL082 (that figure is with its output stage Class AB loaded; here everything
is Class A).
Figure 4 shows square-wave responses (20Hz, 1kHz, 20kHz) while driving the
HD650 phones to 109dB SPL, and also with no load. The 20Hz exponential decay,
and the 20kHz exponential rise time, reflect the -3dB bandwidth of 3.3Hz to
230kHz.
I compared various SACDs (1) with the HD650 phones directly connected to the
player output (the 300-ohm phone impedance and high sensitivity allow that)
and (2) with the head phone amp inserted into the path (loudness compensation
off, volume control set to match the direct connection). I heard no difference.
Some might prefer a headphone amp that imparts a pleasing (euphonic) “sound”—warm,
“romantic,” and so on—but this unit isn’t one of them. If the recording has
natural warmth, you’ll hear it clearly (with good headphones).
* The Hammond 1590 E aluminum enclosure, 7.4” x 4.7” x 3,1”, Digi-Key HM155,
is a good choice.
Headphone Amp Parts List: Total Qty.; Schematic; Ref. Amp; Supply; Description;
Source.