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Damping capacity is a mechanical property of materials that measure a material's ability to dissipate elastic strain energy during mechanical vibration or wave propagation. When ranked according to damping capacity, materials may be roughly categorized as either high- or low-damping.
Relative damping capacity of various metals [15] Materials Damping capacity † Gray iron (high carbon equivalent) 100–500 Gray iron (low carbon equivalent) 20–100 Ductile iron: 5–20 Malleable iron: 8–15 White iron: 2–4 Steel: 4 Aluminum: 0.47 † Natural log of the ratio of successive amplitudes
The damping ratio provides a mathematical means of expressing the level of damping in a system relative to critical damping. For a damped harmonic oscillator with mass m , damping coefficient c , and spring constant k , it can be defined as the ratio of the damping coefficient in the system's differential equation to the critical damping ...
Damping dissipates energy in the system, which reduces the vibration level which is transmitted at the natural frequency. The fluid in automotive shock absorbers is a kind of damper, as is the inherent damping in elastomeric (rubber) engine mounts. Damping is used in passive isolators to reduce the amount of amplification at the natural frequency.
The ratio of the loss modulus to storage modulus in a viscoelastic material is defined as the , (cf. loss tangent), which provides a measure of damping in the material. tan δ {\displaystyle \tan \delta } can also be visualized as the tangent of the phase angle ( δ {\displaystyle \delta } ) between the storage and loss modulus.
Self-damping (ACSR/SD) is a nearly obsolete conductor technology and is rarely used for new installations. It is a concentric-lay stranded, self-damping conductor designed to control wind induced (Aeolian-type) vibration in overhead transmission lines by internal damping. Self-damping conductors consists of a central core of one or more round ...
In the filtering application, the resistor becomes the load that the filter is working into. The value of the damping factor is chosen based on the desired bandwidth of the filter. For a wider bandwidth, a larger value of the damping factor is required (and vice versa). The three components give the designer three degrees of freedom.
The earliest study of thermoelastic damping can be found in Clarence Zener’s classical work, [1] [2] in 1937, in which he studied thermoelastic damping in beams undergoing flexural vibrations. Flexural vibrations cause alternating tensile and compressive strains to build up on opposite sides of the neutral axis leading to a thermal imbalance.
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