HPA-10 Headphone AmplifierTom Christiansen Audio
The TCA HPA-10 is a nimble, yet powerful, headphone amplifier. It was designed to provide high performance in a small and highly portable package. Its diminutive size allows the HPA-10 to tuck into small spaces, including under the monitor at your workstation.
The HPA-10 has no sonic signature. As result, it offers a precise and fatigue-free rendition of the source material.
Key Features of the HPA-10
The HPA-10 provides 1.25 W into 32 Ω and 250 mW into 300 Ω. This is plenty to reach ear-splitting levels with the vast majority of headphones on the market.
I firmly believe that audio components should have as little impact on the sound quality as possible. This is why I optimize all TCA designs for the lowest possible distortion. The low total harmonic distortion (THD) and intermodulation distortion (IMD) of the HPA-10 result in a realistic, engaging, and fatigue-free listening experience.
The total noise of the HPA-10 measures 1.6 µV RMS (A-weighted) within the audio band. This results in a dynamic range of 130 dB and a signal-to-noise ratio of 131 dB. To put this into perspective, 130 dB is the dynamic range from the quietest perceptible sound to the threshold of pain! Due to this enormous dynamic range, the HPA-10 will allow you to experience an incredible level of detail, both in the quietest passages and in the crescendos of the music.
Designed, Assembled, and Tested in Canada
The HPA-10 is designed, manufactured, and tested in Canada. The raw circuit board is made in Ontario. The circuit assembly and test are performed in Calgary. The chassis is made in Japan. The electronic components are sourced from authorized distributors in the USA and Canada.
A summary of the HPA-10 specifications is provided in the table below.
|Output Power||1.25 W||20 Ω|
|Output Power||1.30 W||32 Ω|
|Output Power||250 mW||300 Ω|
|Total Harmonic Distortion (THD)||< -130 dBc||300 Ω, 100 mW, 1 kHz|
|Total Harmonic Distortion + Noise (THD+N)||
|300 Ω, 100 mW, 1 kHz|
|Intermodulation Distortion (IMD) - SMPTE||< -108 dB||60 Hz + 7 kHz @ 4:1, 300 Ω, 100 mW|
|Intermodulation Distortion (IMD) - DFD||< -120 dB||18+19 kHz @ 1:1, 300 Ω, 100 mW|
|Intermodulation Distortion (IMD) - MOD||< -112 dB||917 Hz + 5.5 kHz @ 1:1, 300 Ω, 1 mW|
|Multi-Tone Intermodulation Residual||<- 140 dBr||AP 32-tone, 300 Ω, 100 mW|
|Gain||10 dB (3.2x)|
|Input Sensitivity||2.4 V RMS||300 Ω, 200 mW|
|Channel Imbalance vs Volume Setting||TBD
||0 – 60 dB attenuation|
|Dynamic Range (AES17)||130 dB|
|Signal-to-Noise Ratio||131 dB|
|Residual Mains Hum & Noise||
1.6 µV RMS
2.1 µV RMS
|Mains Voltage Requirements||
90–264 V AC
|External power supply|
|Size||80 x 32 x 110 mm||(W x H x D), excluding power supply|
|Designed and Manufactured in Canada|
The heart of the output stage in the HPA-10 is a high-speed, high-current buffer with low intrinsic distortion. To further increase the performance of the output stage, the HPA-10 uses a precision audio opamp in a composite amplifier architecture to perform error correction on the output stage. The HPA-10 reaches its high performance, in part, due to the use of this error correcting architecture.
The block diagram of the HPA-10 is shown below.
The volume control is an ALPS RK097-series potentiometer.
The circuit board layout has been optimized for audio performance. Therefore, the circuit board features four copper layers and includes elaborate planes and pours to minimize the error voltages that develop across the various signal conductors and ground connections. In addition, the layout is optimized for high signal integrity. This includes shielding of the high-impedance nodes within the circuit.
The results below are from measurements of the HPA-10 prototype. The final version is expected to perform even better due to improvements in the circuit board layout. As the measurements are expected to improve slightly in the final version, I have opted to show the results from a subset of the usual measurement suite. More detailed measurements will be added when the first batch of HPA-10 arrives from assembly.
The graph below shows the THD+N vs output power with 300 Ω load. The amplifier delivers 250 mW at the onset of clipping. Note that the sharp jumps (aside from when the amplifier clips) are caused by range switching in the Audio Precision APx525 audio analyzer used for the measurement. The THD+N vs output power plots mostly show the THD+N floor of the measurement system.
Single-tone distortion tests, such as THD+N measurements, are useful to determine fundamental amplifier performance and behaviour. However, some criticize these tests as being too simplistic to properly describe the amplifier's behaviour when presented with a more complex signal such as music.
Intermodulation tests address this by using two or more test tones. The gold standard among these tests is the 32-tone test developed by Audio Precision. I was among the first to use this test for amplifier characterization and other vendors have started to follow suit.
The Audio Precision 32-tone IMD test uses 32 test tones of equal amplitude logarithmically spaced in frequency. The phase of the test tones have been designed to provide a crest factor of 10 dB, which is quite representative of music. The signal itself sounds a bit like an out of tune pipe organ.
The graph below shows the result of the 32-tone IMD test with the HPA-10.
The combined amplitude of the 32 tones is the 0 dB reference, and corresponds to 100 mW into 300 Ω. The intermodulation products - i.e. the "grass" between the test tones - are distortion products from the amplifier. These should be as low as possible. As seen in above graph, these distortion products are more than 140 dB (10,000,000×) lower than the reference level, which is truly stellar. This indicates that even with a complex input signal the HPA-10 does not add any audible colouration to the input signal. It is a truly transparent amplifier. The transparency of the HPA-10 is seen in the two-tone IMD tests as well.
Siegfried Linkwitz has proposed a 1 kHz + 5.5 kHz IMD test, which he argues to be highly indicative of the perceived sound quality. He bases his argument on the fact that IMD products in this measurement fall in the frequency range where the ear is the most sensitive (see the Fletcher-Munson curves for more detail). This seems like a reasonable argument so I measured the HPA-10 accordingly.
The result of this measurement is shown below. Note that due to a limitation in the signal source of the APx525, the frequencies used must be an integer multiple of each other. Thus, my test signal consisted of 917 Hz (5500/6) and 5.5 kHz at equal amplitude. I performed this measurement at 1.0 mW as this is representative of typical listening levels with most headphones. The result is shown below.
The IMD products are buried in the noise floor of the measurement equipment. Excellent!
The two more traditional IMD measurements are the SMPTE 60 Hz + 7 kHz (4:1 amplitude ratio) and the 18 kHz + 19 kHz (1:1 amplitude ratio). The former is often used to tease out thermal issues within the amp. The latter often reveals lacking loop gain (so basically lack of control) towards the higher end of the audio frequency range.
The SMPTE IMD test result for the HPA-10 is shown below.
Only the second (d2) and third (3d) order IMD product extend above the noise floor.
The result of the 18+19 kHz IMD measurement for the HPA-10 is shown below. Only the second and third order IMD product (2d and 3d) extend above the noise floor.
The total integrated noise measures 1.6 µV (A-weighted). The HPA-10 shows only a minuscule amount of residual mains hum at 180 Hz. This is what a quiet amp looks like!
The measurements above all characterize the amplifier in the frequency domain. Transient response measurements describe how the amplifier performs in the time domain.
Amplifier stability is paramount and achieving good stability in an amplifier featuring a high-speed composite output stage can be a significant challenge. Therefore, I characterized the transient behaviour of the HPA-10 for various reactive loads.
The oscilloscope images below shows the transient response of the HPA-10 when presented with a 10 kHz square wave and loaded by 300 Ω in parallel with 470 pF of capacitance. This load is representative of a pair of Sennheiser HD-650 with the stock cable and a 2-3 m (~10') extension cord.
As shown above, the transient response of the HPA-1 is exemplary.
Increasing the capacitance to 1.0 nF (Sennheiser HD-650 with the stock cable and an 8 m (~26') extension cord) still shows a clean response.
With 4.7 nF (Sennheiser HD-650 + stock cable + 45 m (~147') extension cord), a very slight degradation of the transient response is observed as a little bit of overshoot develops. The amplifier still shows no signs of instability as no ringing is present in the measurement.
Finally, when loaded with 10 nF, the amplifier finally shows some overshoot and ringing. Note, however, that to obtain such capacitive load in actual use would require approximately 100 m (300') of extension cable on a typical pair of headphones. It is also noteworthy that the HPA-10 remains stable even with 100 nF capacity load. Needless to say, I have full confidence in the stability of the HPA-10.