TheHP 200A Audio Oscillator, first built in 1938, was the first product[1] made byHewlett-Packard and was manufactured inDavid Packard'sgarage inPalo Alto, California.
It was a low-distortionaudio oscillator used for testing sound equipment. It used theWien bridge oscillator circuit, that had been the subject ofBill Hewlett's masters thesis. It was also the first such commercial oscillator to use a simplelight bulb as the temperature-dependent resistor in its feedback network.[2] The light bulb was an inexpensive and effectiveautomatic gain control that not only kept the oscillator output amplitude constant, but it also kept the oscillator's loop gain near unity. The latter is a key technique for achieving a low distortion oscillator. Earlier, Larned Meacham had used light bulbs in bridge circuits to stabilize and linearizeoscillators in 1938.[3]
The product code was chosen to give the impression that HP was an established company.[4] A variation, the HP 200B, was customized forWalt Disney, which bought eight units for use in the production ofFantasia.[5]
The circuit diagram is shown in Hewlett's 1939 patent.[6][7][8]
| HP 200A | HP 200B | |
|---|---|---|
| Frequency range | 35 Hz-35 kHz in 3 range X1: 35-350 Hz X10: 350-3500 Hz X100: 3500- 35 000 Hz | 20 Hz-20 kHz in 3 range X1: 20-200 Hz X10: 200-2000 Hz X100: 2000- 20 000 Hz |
| Scale of dialer | 35-350 | 20-200 |
| Calibration accuracy | less than 2% | less than 2% |
| Output power | 1 W 500 Ω load | 1 W 500 Ω load |
| Distortion | less than 1% between 35 Hz and 15 kHz | less than 1% between 35 Hz and 15 kHz |
| Output impedance | less than 75Ω under 15 kHz | less than 75Ω under 15 kHz |
| Power voltage | 115 V 50-60 Hz 60 W | 115 V 50-60 Hz 60 W |
Through the 1940s and into the 1950s, the subsequent versions of the 200A covered different and wider frequency ranges. The latest version was the 200CD.[10] It covered from the subaudio 5 Hz to the low end (Long Wave) of the AM radio band at 600 kilohertz. The 200CD became a ubiquitous audio generator in engineering laboratories worldwide from the 1950s to the 1990s.[11][12]
William R. Hewlett'sWien bridge oscillator can be considered as a combination of a differential amplifier and aWien bridge, connected in a positive feedback loop between the amplifier output and differential inputs. At the oscillating frequency, the bridge is almost balanced and has very small transfer ratio. Theloop gain is a product of the very high amplifier gain and the very low bridge ratio.[13] In Hewlett's circuit, the amplifier is implemented by two vacuum tubes.
The amplifier's inverting input is the cathode of tube V1 and the non-inverting input is the control grid of tube V2. To simplify analysis, all the components other than R1, R2, C1 and C2 can be modeled as a non-inverting amplifier with a gain of 1+Rf/Rb and with a high input impedance. R1, R2, C1 and C2 form abandpass filter which is connected to provide positive feedback at the frequency of oscillation. Rb self heats and increases thenegative feedback which reduces the amplifier gain until the point is reached that there is just enough gain to sustain sinusoidal oscillation without over driving the amplifier.
If R1 = R2 and C1 = C2 then at equilibrium Rf/Rb = 2 and the amplifier gain is 3. When the circuit is first energized, the lamp is cold and the gain of the circuit is greater than 3 which ensures start up. The dc bias current of vacuum tube V1 also flows through the lamp. This does not change the principles of the circuit's operation, but it does reduce the amplitude of the output at equilibrium because the bias current provides part of the heating of the lamp.
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