Williamson amplifier

rdf:langString Williamson amplifier

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rdf:langString Commercial amplifier with an inferior transformer, US NRL measurements

rdf:langString Williamson's 1949 design. Dashed lines: open loop response, solid lines: closed loop response. Resonant bumps at low and high extremes indicate narrow phase margins

rdf:langString Commercial amplifier with a high quality transformer, US NRL measurements

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rdf:langString Frequency, phase and transient response of various Williamson amplifiers

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rdf:langString Williamson amplifier with Audio Development 314E transformer.png

rdf:langString Williamson amplifier with Peerless S265Q transformer.png

rdf:langString Williamson amplifier 1949 frequency and phase response.png

rdf:langString The Williamson amplifier is a , push-pull, Class A triode-output valve audio power amplifier designed by D. T. N. Williamson during World War II. The original circuit, published in 1947 and addressed to the worldwide do it yourself community, set the standard of high fidelity sound reproduction and served as a benchmark or reference amplifier design throughout the 1950s. The original circuit was copied by hundreds of thousands amateurs worldwide. It was an absolute favourite on the DIY scene of the 1950s, and in the beginning of the decade also dominated British and North American markets for factory-assembled amplifiers. The Williamson circuit was based on the 1934 by , with an additional error amplifier stage and a global negative feedback loop. Deep feedback, triode-connected KT66 power tetrodes, conservative choice of standing currents, and the use of wide-bandwidth output transformer all contributed to the performance of the Williamson. It had a modest output power rating of 15 Watts but surpassed all contemporary designs in having very low harmonic distortion and intermodulation, flat frequency response throughout the audible frequency range, and effective damping of loudspeaker resonances. The 0.1% distortion figure of the Williamson amplifier became the criterion for high fidelity performance that remains valid in the 21st century. The Williamson amplifier was sensitive to selection and matching of passive components and valves, and prone to unwanted oscillations at infrasonic and ultrasonic frequencies. Enclosing four valve stages and an output transformer in a negative feedback loop was a severe test of design, resulting in a very narrow phase margin or, quite often, no margin at all. Attempts to improve stability of the Williamson could not fix this fundamental flaw. For this reason, and due to high costs of required quality components, manufacturers soon abandoned the Williamson circuit in favour of inherently more stable, cheaper and efficient three-stage, ultralinear or pentode-output designs.