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Helped by its innovative energy-capturing capability, engineers say Bose''s semi-active suspension uses less than one-third the power required by a conventional vehicle air conditioner. The system''s responses are generated from mathematical algorithms created during the research project.Using input from sensors around the vehicle, the control unit sends signals to the amplifiers and motor-actuated struts at each corner of the vehicle. The result is a smooth glide over all types of roads.Bose engineers also say the bulky suspension hardware eventually will be reduced to half the current size. An advantage of the Bose suspension is that it can easily be retrofitted into existing production cars with little modification, Bose says.
Interfacing the Blast Pressure TransducerLooking at the dimensions of the pencil probe in Figure 6 relative to the preceding value of ?, it is clear that the probe has the potential to act as a reflecting body to high frequencies in the approaching shock front.In order to minimize reflections, the probe is tapered over approximately its first two-inches of length. It then transitions into a cylindrical body with a flat surface on one side. This flat surface eliminates discontinuities between an embedded, discshaped, radial facing, quartz sensing element and the transducer housing. Ideally, the velocity of the shock front and the spatial averaging of the disc as the front traverses across it will control the measured rise time. The averaging effect associated with any pressure transducer can be envisioned as the distortion that a sine wave would encounter as it passes at right angles to the axis of symmetry that is perpendicular to the plane of the circular diaphragm of the transducer. The diaphragm would cause distortion through spatial averaging of the wave, which results in attenuation.
After briefly describing towing the air-blast environment, some of the historical challenges associated with its measurement were air presented. Problems associated with interfacing a pressure transducer to the air-blast environment shocks were next described, and analysis procedures were provided to calculate the effects of any transducer-mounting compromises. Tools for validation of data were then discussed, and methods to minimize any documented environment-induced noise, if present, were provided. The frequency limitations attributable to long cables runs used in air-blast testing were then described, and some computational tools were identified. Last, a comparison of different transducer technologies was performed.
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