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  2. Violin acoustics - Wikipedia

    en.wikipedia.org/wiki/Violin_acoustics

    Most strings are wound with metal to increase their mass while avoiding excess thickness. During a bow stroke, the string is pulled until the string's tension causes it to return, after which it receives energy again from the bow. Violin players can control bow speed, the force used, the position of the bow on the string, and the amount of hair ...

  3. String vibration - Wikipedia

    en.wikipedia.org/wiki/String_vibration

    the higher the tension, the higher the frequency of the fundamental; the lighter the string, the higher the frequency of the fundamental; Moreover, if we take the nth harmonic as having a wavelength given by = /, then we easily get an expression for the frequency of the nth harmonic:

  4. Piano acoustics - Wikipedia

    en.wikipedia.org/wiki/Piano_acoustics

    The highest strings must be under the greatest tension, yet must also be thin enough to allow for a low mass density. The limited strength of steel (i.e. a too-thin string will break under the tension) forces the piano designer to use very short and slightly thicker strings, whose short wavelengths thus generate inharmonicity.

  5. Dispersion relation - Wikipedia

    en.wikipedia.org/wiki/Dispersion_relation

    The top electron has twice the momentum, while the bottom electron has half. Note that as the momentum increases, the phase velocity decreases down to c, whereas the group velocity increases up to c, until the wave packet and its phase maxima move together near the speed of light, whereas the wavelength continues to decrease without bound. Both ...

  6. Attenuation - Wikipedia

    en.wikipedia.org/wiki/Attenuation

    Light scattering depends on the wavelength of the light being scattered. Thus, limits to spatial scales of visibility arise, depending on the frequency of the incident lightwave and the physical dimension (or spatial scale) of the scattering center, which is typically in the form of some specific microstructural feature.

  7. Attenuation coefficient - Wikipedia

    en.wikipedia.org/wiki/Attenuation_coefficient

    The attenuation coefficient of a volume, denoted μ, is defined as [6] =, where Φ e is the radiant flux;; z is the path length of the beam.; Note that for an attenuation coefficient which does not vary with z, this equation is solved along a line from =0 to as:

  8. Dispersion (optics) - Wikipedia

    en.wikipedia.org/wiki/Dispersion_(optics)

    Since that refractive index varies with wavelength, it follows that the angle that the light is refracted by will also vary with wavelength, causing an angular separation of the colors known as angular dispersion. For visible light, refraction indices n of most transparent materials (e.g., air, glasses) decrease with increasing wavelength λ:

  9. Distributed Bragg reflector - Wikipedia

    en.wikipedia.org/wiki/Distributed_Bragg_reflector

    Time-resolved simulation of a pulse reflecting from a Bragg mirror. A distributed Bragg reflector (DBR) is a reflector used in waveguides, such as optical fibers.It is a structure formed from multiple layers of alternating materials with different refractive index, or by periodic variation of some characteristic (such as height) of a dielectric waveguide, resulting in periodic variation in the ...