![]() The plurals of maximum and minimum are maxima and minima, respectively.Įxplain that monochromatic means one color. Both are pronounced the way you would expect from the spelling. It will be useful not only in describing how light waves propagate, but also in how they interfere. Huygens’s principle works for all types of waves, including water waves, sound waves, and light waves. The new wavefront is a line tangent to the wavelets and is where the wave is located at time t. These are drawn later at a time, t, so that they have moved a distance s = v t s = v t. Each point on the wavefront emits a semicircular wave that moves at the propagation speed v. A wavefront is the long edge that moves for example, the crest or the trough. The new wavefront is a line tangent to all of the wavelets.”įigure 17.4 shows how Huygens’s principle is applied. Huygens’s principle states, “Every point on a wavefront is a source of wavelets that spread out in the forward direction at the same speed as the wave itself. He used wavefronts, which are the points on a wave’s surface that share the same, constant phase (such as all the points that make up the crest of a water wave). The Dutch scientist Christiaan Huygens (1629–1695) developed a useful technique for determining in detail how and where waves propagate. Although wavelengths change while traveling from one medium to another, colors do not, since colors are associated with frequency. ![]() It follows that the wavelength of light is smaller in any medium than it is in vacuum. Where λ λ is the wavelength in vacuum and n is the medium’s index of refraction. As it is characteristic of wave behavior, interference is observed for water waves, sound waves, and light waves. Here we see the beam spreading out horizontally into a pattern of bright and dark regions that are caused by systematic constructive and destructive interference. Passing a pure, one-wavelength beam through vertical slits with a width close to the wavelength of the beam reveals the wave character of light. The laser beam emitted by the observatory represents ray behavior, as it travels in a straight line. In Figure 17.2, both the ray and wave characteristics of light can be seen. Interference is the identifying behavior of a wave. ![]() However, when it interacts with smaller objects, it displays its wave characteristics prominently. As is true for all waves, light travels in straight lines and acts like a ray when it interacts with objects several times as large as its wavelength. The range of visible wavelengths is approximately 380 to 750 nm. The source sound is a stick hitting a metal can.Where c = 3.00 × 10 8 c = 3.00 × 10 8 m/s is the speed of light in vacuum, f is the frequency of the electromagnetic wave in Hz (or s –1), and λ λ is its wavelength in m. Sound Example : Multiple echoes produced under a parabolic bridge, Stanley Park, Vancouver, B.C. Sound Example : Reflected sound from the opposite side of a lake, heard as an echo. Compare: ABSORPTION, ACOUSTIC RADIATION, REFRACTION, TRANSMISSION. See also: BINAURAL HEARING, PHASING, SOUND PROPAGATION. Symmetrically-shaped surfaces produce symmetrical reflections, the most striking examples of which are the whispering gallery, where sound travels along the walls via repeated reflections, and the PARABOLIC REFLECTOR where all sound is reflected to the focus of the parabola. In general, concave surfaces focus sound waves, thereby concentrating the sound in specific areas, and convex shapes scatter sound, thereby promoting good diffusion. Different surfaces have different reflecting powers, as measured by their ABSORPTION COEFFICIENT or REFLECTION COEFFICIENT. Sound reflection gives rise to DIFFUSION, REVERBERATION and ECHO. Reflection of a sound wave at a barrier, as if from an imaginary source at an equal distance behind the barrier. See: CANYON EFFECT, DIFFUSE SOUND FIELD, SOUNDING BOARD. However, this law of reflection holds only when the WAVELENGTH of the sound is small compared to the dimensions of the reflecting surface. the angle of INCIDENCE of a SOUND WAVE equals the angle of reflection, just as if it were produced by a 'mirror image' of the stimulus on the opposite side of the surface. The law for reflection is the same as that for light, i.e. ![]() If a sound is not absorbed or transmitted when it strikes a surface, it will be reflected. ![]()
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