Copyright © 2018 by Wayne Stegall
Created May 15, 2018. See Document History at end for
details.
One-Bend Amplifier
Part 5: Set bias for class B/AB and
evaluate results
Introduction
Because class-a amplifiers are so inefficient and often low-powered, I
thought it would be interesting if the one-bend amplifier would produce
similar results in an efficient class b. Now in class-b more
power is possible so I sought to raise the power supply voltage to the
output stage to 60V and the driver stages to 75V to support 250W into
4Ω with 50% headroom. Note that this is an evaluation not a
redesign, if the results are acceptable the input and driver stages
would possibly be adjusted to ensure that no components are out of
their safe ranges in a later exercise.
Circuits
Note: Component values can be obtained from the SPICE models for
now.
Figure
1:
Amplifier
Schematic
|
|
SPICE
model
Figure
2:
Regulated
power
supply |
|
SPICE model
Spice Results
Forgo hum analysis for now. Instead begin with error transfer
curves.
Figure
3:
Small
signal
error
curve.
Shows dominance of second harmonic and some third.
|
|
Figure
4:
Large
signal
error
curve.
Shows dominance of second harmonic then third.
|
|
|
|
These error curves plotted with convergence difficulties. I think
the following distortion analysis would suggest that they are smoother
than they appear.
Continue with full-power distortion analysis at 1kHz.
Fourier analysis for vout:
No. Harmonics: 16, THD: 0.0408884 %, Gridsize: 200,
Interpolation Degree: 3
Harmonic
|
Frequency |
|
Magnitude |
|
Norm. Mag |
|
Percent |
|
Decibels |
|
|
|
|
|
|
|
|
|
|
1 |
1000 |
|
44.7200000 |
|
1.0000000 |
|
100.0000000 |
|
0.00 |
2 |
2000 |
|
0.0181631 |
|
0.0004062 |
|
0.0406151 |
|
-67.83 |
3 |
3000 |
|
0.0019576 |
|
0.0000438 |
|
0.0043776 |
|
-87.18 |
4 |
4000 |
|
0.0003447 |
|
0.0000077 |
|
0.0007708 |
|
-102.26 |
5 |
5000 |
|
0.0004991 |
|
0.0000112 |
|
0.0011161 |
|
-99.05 |
6 |
6000 |
|
0.0000647 |
|
0.0000014 |
|
0.0001448 |
|
-116.79 |
7 |
7000 |
|
0.0003209 |
|
0.0000072 |
|
0.0007176 |
|
-102.88 |
8 |
8000 |
|
0.0000362 |
|
0.0000008 |
|
0.0000808 |
|
-121.85 |
9 |
9000 |
|
0.0002477 |
|
0.0000055 |
|
0.0005538 |
|
-105.13 |
10 |
10000 |
|
0.0000288 |
|
0.0000006 |
|
0.0000644 |
|
-123.83 |
11 |
11000 |
|
0.0001972 |
|
0.0000044 |
|
0.0004410 |
|
-107.11 |
12 |
12000 |
|
0.0000240 |
|
0.0000005 |
|
0.0000537 |
|
-125.40 |
13 |
13000 |
|
0.0001604 |
|
0.0000036 |
|
0.0003588 |
|
-108.90 |
14 |
14000 |
|
0.0000208 |
|
0.0000005 |
|
0.0000465 |
|
-126.64 |
15 |
15000 |
|
0.0001320 |
|
0.0000030 |
|
0.0002952 |
|
-110.60 |
Certainly we are interested in frequency response
Figure
5:
Bode
shows
frequency
response
down
3dB
at
524kHz
|
|
For stability the open loop phase margin at the closed-loop -3dB
frequency should be more than 45º.
Figure
6:
Stability
analysis
showing
80.9º
of
phase
margin. |
|
Conclusions
The desired predominance of second harmonic expected as a result of the
inner feedback loop is the same as the previous class--a result.
After that the harmonic profile does not taper off like class-a but
rather odd-harmonics are preferred perhaps an expected result.
Perhaps a less pure class-a sound would result than previously. I
think the class-b version is worth further investigation.
1Note: Raw Fourier
analysis data has been processed in spreadsheet to calculate related
results and reformatted.
3See related article: Floating Source-follower Regulator.
Document History
May 15, 2018 Created.