. Elements of acoustical engineering. Electro-acoustics; Sound. Fig. Measured directional characteristics of a ribbon microphone with a large circular baffle (see Fig. ) as a function of the radius of the baffle and the wavelength. The polar graph depicts the output, in volts, as a function of the angle, in degrees. The max- imum response is arbitrarily chosen as Fig. Computed directional characteristics of a ribbon microphone with a large circular baffle (see Fig. ) as a function of the radius of the baffle and the wavelength. The polar graph depicts the output, in
. Elements of acoustical engineering. Electro-acoustics; Sound. Fig. Measured directional characteristics of a ribbon microphone with a large circular baffle (see Fig. ) as a function of the radius of the baffle and the wavelength. The polar graph depicts the output, in volts, as a function of the angle, in degrees. The max- imum response is arbitrarily chosen as Fig. Computed directional characteristics of a ribbon microphone with a large circular baffle (see Fig. ) as a function of the radius of the baffle and the wavelength. The polar graph depicts the output, in volts, as a function of the angle, in degrees. The maximum response is arbitrarily chosen as unity. pressure gradient system is very large for values of R/\ greater than f. The phase between the actuating force, equation , and the particle velocity in a plane wave, for a ribbon microphone with a circular baffle, is. Please note that these images are extracted from scanned page images that may have been digitally enhanced for readability - coloration and appearance of these illustrations may not perfectly resemble the original Olson, Harry Ferdinand, 1901-. New York, D. Van Nostrand company, inc.
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