![]() ![]() Now we place a small vertikal wall, like a noise barrier from floor to a certain height „h“, in the propagation path.Īnd watch three different sound paths red, blue and green. The distance between locations with positive and negative pressure deviation maxima is a half wavelength along the dispersion path. As we know, the signal is carried by sinusoidal varying deviations from atmospheric pressure, traveling forward with sound velocity. Let us take a closer look at our assumed plane wavefront. ![]() Obstacles with a size similar to the wavelength show a much more complicated impact on wave propagation. Obstacles that are very small compared to the wavelength have no influence on wave propagation. The angle of incidence is equal to the exit angle. A ray-tracing model covers this perfectly. Such large obstacles compared to the wavelength indeed act like mirrors to the sound. Think of an ocean wave that hits a rocky beach. At normal incidence, the SPL directly at the wall is twice that of the incoming wavefront. Ray tracingĪ wall that is much larger than the wavelength reflects the wave backwards. To simplify our discussions as before (Link wavelength), we assume the signal carried by the wave to contain only a single frequency. Our consideration starts with a plane wavefront that hits a stiff, heavy and flat wall at normal incidence. Therefore, objects in our daily environment influence sound propagation differently: they both reflect and diffract sound, depending on shape and size relative to the sound signal’s wavelength. The easiest way to describe sound propagation is by comparison with light rays.īut the wavelength of light is far below a millimeter while that of sound ranges from millimeters to meters. Interestingly, sound waves bend around objects. A complex mixture of reflection and diffraction happens to sound that hits an object of similar dimension as the wavelengths of the sound signal. ![]()
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