Resonance

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In physics , resonance is the tendency of a system to oscillate at a greater amplitude at some Frequency|frequencies than at others. These are known as the system's resonance frequencies (or, erroneously, resonant frequencies ). At these frequencies, even small Periodic function|periodic driving forces can produce large amplitude oscillations, because the system stores vibrational energy.

Resonance occurs when a system is able to store and easily transfer energy between two or more different storage modes (such as kinetic energy and potential energy in the case of a pendulum). However, there are some losses from cycle to cycle, called damping . When damping is small, the resonance frequency is approximately equal to the natural frequency of the system, which is a frequency of unforced vibrations. Some systems have multiple, distinct, resonance frequencies.

Resonance phenomena occur with all types of vibrations or waves : there is mechanical resonance , acoustic resonance , Electromagnetic radiation|electromagnetic resonance, nuclear magnetic resonance (NMR), electron paramagnetic resonance|electron spin resonance (ESR) and resonance of quantum wave function s. Resonant systems can be used to generate vibrations at a specific frequency (e.g. musical instruments), or pick out specific frequencies from a complex vibration containing many frequencies (e.g. filters).

Resonance was recognized by Galileo Galilei with his investigations of pendulum s and strings (music)|musical strings beginning in 1602.

Examples

One familiar example is a playground Swing (seat)|swing , which acts as a pendulum . Pushing a person in a swing in time with the natural interval of the swing (its resonance frequency) will make the swing go higher and higher (maximum amplitude), while attempts to push the swing at a faster or slower tempo will result in smaller arcs. This is because the energy the swing absorbs is maximized when the pushes are 'in phase (waves)|phase ' with the swing's oscillations, while some of the swing's energy is actually extracted by the opposing force of the pushes when they are not.

Resonance occurs widely in nature, and is exploited in many man-made devices. It is the mechanism by which virtually all sinusoidal wave s and vibrations are generated. Many sounds we hear, such as when hard objects of metal, glass, or wood are struck, are caused by brief resonant vibrations in the object. Light and other short wavelength electromagnetic radiation is produced by resonance on an atomic scale, such as electrons in atoms. Other examples are:

; mechanical resonance|Mechanical and acoustic resonance

the timekeeping mechanisms of all modern clocks and watches: the balance wheel in a mechanical watch and the quartz crystal in a quartz watch

the tidal resonance of the Bay of Fundy

acoustic resonance s of musical instruments and human vocal cords

the shattering of a crystal wineglass when exposed to a musical tone of the right pitch (its resonance frequency)

Electrical resonance

electrical resonance of tuned circuit s in radio s and TV s that allow radio frequencies to be selectively received

Optical cavity|Optical resonance

creation of Coherence (physics)|coherent light by optical resonance in a laser Optical cavity|cavity

Orbital resonance in astronomy

orbital resonance as exemplified by some natural satellite|moons of the solar system 's gas giants

Atomic, particle, and molecular resonance

material resonances in atomic scale are the basis of several spectroscopy|spectroscopic techniques that are used in condensed matter physics .

* Nuclear Magnetic Resonance

* Mössbauer effect

* Electron Spin Resonance .

Theory

The exact response of a resonance, especially for frequencies far from the resonance frequency, depends on the details of the physical system, and is usually not exactly symmetric about the resonance frequency, as illustrated for the simple harmonic oscillator above.
For a lightly damping|damped linear oscillator with a resonance frequency O, the intensity of oscillations I when the system is driven with a driving frequency ? is typically approximated by a formula that is symmetric about the resonance frequency:

:

I(\omega) \propto \frac{\left(\frac{\Gamma}{2}\right)^2}{(\omega - \Omega)^2 + \left( \frac{\Gamma}{2} \right)^2 }.

The intensity is defined as the square of the amplitude of the oscillations. This is a Lorentzian function , and this response is found in many physical situations involving resonant systems. G is a parameter dependent on the harmonic oscillator|damping of the oscillator, and is known as the linewidth of the resonance. Heavily damped oscillators tend to have broad linewidths, and respond to a wider range of driving frequencies around the resonance frequency. The linewidth is Proportionality (mathematics)|inversely proportional to the Q factor , which is a measure of the sharpness of the resonance.

In electrical engineering , this approximate symmetric response is known as the universal resonance curve , a concept introduced by Frederick E. Terman in 1932 to simplify the approximate analysis of radio circuits with a range of center frequencies and Q values.

Resonators

A physical system can have as many resonance frequencies as it has degrees of freedom (engineering)|degrees of freedom ; each degree of freedom can vibrate as a harmonic oscillator . Systems with one degree of freedom, such as a mass on a spring, pendulum s, balance wheel s, and RLC circuit|LC tuned circuits have one resonance frequency. Systems with two degrees of freedom, such as Double pendulum|coupled pendulums and resonant transformer s can have two resonance frequencies. As the number of coupled harmonic oscillators grows, the time it takes to transfer energy from one to the next becomes significant. The vibrations in them begin to travel through the coupled harmonic oscillators in waves, from one oscillator to the next.

Extended objects that experience resonance due to vibrations inside them are called resonators , such as organ pipe s, vibrating string s, quartz crystal s, microwave cavities, and laser rods. Since these can be viewed as being made of millions of coupled moving parts (such as atoms), they can have millions of resonance frequencies. The vibrations inside them travel as waves, at an approximately constant velocity, bouncing back and forth between the sides of the resonator. If the distance between the sides is

d\,

, the length of a round trip is

2d\,

. In order to cause resonance, the phase of a sinusoidal wave after a round trip has to be equal to the initial phase, so the waves will reinforce. So the condition for resonance in a resonator is that the round trip distance,

2d\,

, be equal to an integer number of wavelengths

\lambda\,

of the wave:

:

2d = N\lambda,\qquad\qquad N \in \{1,2,3,\dots\}

If the velocity of a wave is

v\,

, the frequency is

f = v / \lambda\,

so the resonance frequencies are:

:

f = \frac{Nv}{2d}\qquad\qquad N \in \{1,2,3,\dots\}

So the resonance frequencies of resonators, called normal modes , are equally spaced multiples of a lowest frequency called the fundamental frequency . The multiples are often called overtone s. There may be several such series of resonance frequencies, corresponding to different modes of vibration.

Q factor

The quality factor or Q factor is a Dimensionless quantity|dimensionless parameter that describes how damping|under-damped an oscillation|oscillator or resonator is, or equivalently, characterizes a resonator's bandwidth (signal processing)|bandwidth relative to its center frequency.
Higher Q indicates a lower rate of energy loss relative to the stored energy of the oscillator, i.e. the oscillations die out more slowly. A pendulum suspended from a high-quality bearing, oscillating in air, has a high Q , while a pendulum immersed in oil has a low Q . In order to sustain a system in resonance in constant amplitude by providing power externally, the energy that has to be provided within each cycle is less than the energy stored in the system (i.e. the sum of the potential and kinetic) by a factor of

Q/(2\pi)

. Oscillators with high quality factors have low damping which tends to make them ring longer.

sine wave|Sinusoidally driven resonator s having higher Q factors resonate with greater amplitudes (at the resonance frequency) but have a smaller range of frequencies around the frequency at which they resonate. The range of frequencies at which the oscillator resonates is called the bandwidth. Thus, a high Q RLC circuit|tuned circuit in a radio receiver would be more difficult to tune, but would have greater selectivity (electronic)|selectivity , it would do a better job of filtering out signals from other stations that lie nearby on the spectrum. High Q oscillators operate over a smaller range of frequencies and are more stable. (See oscillator phase noise .)

The quality factor of oscillators vary substantially from system to system. Systems for which damping is important (such as dampers keeping a door from slamming shut) have Q & nbsp;=& nbsp;½. Clocks, lasers, and other systems that need either strong resonance or high frequency stability need high quality factors. Tuning forks have quality factors around Q & nbsp;=& nbsp;1000. The quality factor of atomic clock s and some high-Q optical cavity|lasers can reach as high as 10¹¹ and higher.

There are many alternate quantities used by physicists and engineers to describe how damped an oscillator is that are closely related to its quality factor. Important examples include: the damping ratio , bandwidth (signal processing)|relative bandwidth , oscillator linewidth|linewidth and bandwidth measured in Octave (electronics)|octave s.

Types of resonance

Mechanical and acoustic resonance

Mechanical resonance is the tendency of a mechanics|mechanical system to absorb more energy when the frequency of its oscillations matches the system's natural frequency of vibration than it does at other frequencies. It may cause violent swaying motions and even catastrophic failure in improperly constructed structures including bridges, buildings, trains, and aircraft. When designing objects, Engineer s must ensure the mechanical resonance frequencies of the component parts do not match driving vibrational frequencies of motors or other oscillating parts, a phenomenon known as mechanical resonance#Resonance disaster|resonance disaster .

Avoiding resonance disasters is a major concern in every building, tower and bridge construction project. As a countermeasure, shock mounts can be installed to absorb resonance frequencies and thus dissipate the absorbed energy. The Taipei 101 building relies on a — a tuned mass damper — to cancel resonance. Furthermore, the structure is designed to resonate at a frequency which does not typically occur. Buildings in seismic zones are often constructed to take into account the oscillating frequencies of expected ground motion. In addition, engineer s designing objects having engines must ensure that the mechanical resonance frequencies of the component parts do not match driving vibrational frequencies of the motors or other strongly oscillating parts.

Many clock s keep time by mechanical resonance in a balance wheel , pendulum , or Quartz clock|quartz crystal

Acoustic resonance is a branch of mechanical resonance that is concerned with the mechanical vibrations across the frequency range of human hearing, in other words sound . For humans, hearing is normally limited to frequencies between about 20& nbsp; Hertz|Hz and 20,000& nbsp;Hz (20& nbsp; kHz ), Harry F. Olson|Olson, Harry F. Dover Publications, 1967, pp. 248–249. "Under very favorable conditions most individuals can obtain tonal characteristics as low as 12 Hz."

Acoustic resonance is an important consideration for instrument builders, as most acoustic Musical instrument|instruments use resonator s, such as the string resonance|strings and body of a violin , the length of tube in a flute , and the shape of, and tension on, a drum membrane.

Like mechanical resonance, acoustic resonance can result in catastrophic failure of the object at resonance. The classic example of this is breaking a wine glass with sound at the precise resonance frequency of the glass, although this is difficult in practice.

Electrical resonance

Electrical resonance occurs in an electrical network|electric circuit at a particular resonance frequency when the Electrical impedance|impedance of the circuit is at a minimum in a series circuit or at maximum in a parallel circuit (or when the transfer function is at a maximum).

Optical resonance

An optical cavity or optical resonator is an arrangement of mirror s that forms a standing wave cavity resonator for light wave s. Optical cavities are a major component of laser s, surrounding the gain medium and providing feedback of the laser light. They are also used in optical parametric oscillator s and some interferometer s. Light confined in the cavity reflects multiple times producing standing wave s for certain resonance frequencies. The standing wave patterns produced are called modes. Longitudinal mode s differ only in frequency while transverse mode s differ for different frequencies and have different intensity patterns across the cross section of the beam. Optical ring resonators|Ring resonators and whispering galleries are examples of optical resonators that do not form standing waves.

Different resonator types are distinguished by the focal lengths of the two mirrors and the distance between them. (Flat mirrors are not often used because of the difficulty of aligning them precisely.) The geometry (resonator type) must be chosen so the beam remains stable, i.e. the beam size does not continue to grow with each reflection. Resonator types are also designed to meet other criteria such as minimum beam waist or having no focal point (and therefore intense light at that point) inside the cavity.

Optical cavities are designed to have a very large Q factor ; a beam will reflect a very large number of times with little attenuation . Therefore the frequency line width of the beam is very small compared to the frequency of the laser.

Additional optical resonances are guided-mode resonance s and surface plasmon resonance, which result in anomalus reflection and high evanescent fields at resonance. In this case, the resonant modes are guided modes of a waveguide or surface plasmon modes of a dielectric-metallic interface. These modes are usually excited by a subwavelength grating.

Orbital resonance

In celestial mechanics , an orbital resonance occurs when two orbit ing bodies exert a regular, periodic gravitational influence on each other, usually due to their orbital period s being related by a ratio of two small integers. Orbital resonances greatly enhance the mutual gravitational influence of the bodies. In most cases, this results in an unstable interaction, in which the bodies exchange momentum and shift orbits until the resonance no longer exists. Under some circumstances, a resonant system can be stable and self correcting, so that the bodies remain in resonance. Examples are the 1:2:4 resonance of Jupiter 's moons Ganymede (moon)|Ganymede , Europa (moon)|Europa , and Io (moon)|Io , and the 2:3 resonance between Pluto and Neptune . Unstable resonances with Saturn 's inner moons give rise to gaps in the rings of Saturn . The special case of 1:1 resonance (between bodies with similar orbital radii) causes large Solar System bodies to clear the neighborhood around their orbits by ejecting nearly everything else around them; this effect is used in the current definition of planet|definition of a planet .

Atomic, particle, and molecular resonance

Nuclear magnetic resonance ( NMR ) is the name given to a physical resonance phenomenon involving the observation of specific quantum mechanics|quantum mechanical magnetism|magnetic properties of an atom ic atomic nucleus|nucleus in the presence of an applied, external magnetic field. Many scientific techniques exploit NMR phenomena to study molecular physics , crystallography|crystal s and non-crystalline materials through NMR spectroscopy . NMR is also routinely used in advanced medical imaging techniques, such as in magnetic resonance imaging (MRI).

All nuclei containing odd numbers of nucleon s have an intrinsic magnetic moment and angular momentum . A key feature of NMR is that the resonance frequency of a particular substance is directly proportional to the strength of the applied magnetic field. It is this feature that is exploited in imaging techniques; if a sample is placed in a non-uniform magnetic field then the resonance frequencies of the sample's nuclei depend on where in the field they are located. Therefore, the particle can be located quite precisely by its resonance frequency.

Electron paramagnetic resonance , otherwise known as Electron Spin Resonance (ESR) is a spectroscopic technique similar to NMR, but uses unpaired electrons instead. Materials for which this can be applied are much more limited since the material needs to both have an unpaired spin and be paramagnetic .

The Mössbauer effect is the resonant and recoil -free emission and absorption of gamma ray photons by atoms bound in a solid form.

Resonance (particle physics) : In quantum mechanics and quantum field theory resonances may appear in similar circumstances to classical physics. However, they can also be thought of as unstable particles, with the formula above valid if the

\Gamma

is the Particle decay#Decay rate|decay rate and

\Omega

replaced by the particle's mass M. In that case, the formula comes from the particle's Propagator (Quantum Theory)|propagator , with its mass replaced by the complex number

M+i\Gamma

. The formula is further related to the particle's Particle decay#Decay rate|decay rate by the optical theorem .

Failure of the original Tacoma Narrows Bridge

The dramatically visible, rhythmic twisting that resulted in the 1940 collapse of "Galloping Gertie," the original Galloping Gertie|Tacoma Narrows Bridge , has sometimes been characterized in physics textbooks as a classical example of resonance. However, this description is misleading. The catastrophic vibrations that destroyed the bridge were not due to simple mechanical resonance, but to a more complicated interaction between the bridge and the winds passing through it — a phenomenon known as aeroelasticity#Flutter|aeroelastic flutter . Robert H. Scanlan , father of bridge aerodynamics, has written an article about this misunderstanding.

Resonance causing a vibration on the International Space Station

The rocket engines for the International Space Station are controlled by autopilot . Ordinarily the uploaded parameters for controlling the engine control system for the Zvezda module will cause the rocket engines to boost the International Space Station to a higher orbit. The rocket engines are hinge-mounted, and ordinarily the operation is not noticed by the crew. But on January 14, 2009, the uploaded parameters caused the autopilot to swing the rocket engines in larger and larger oscillations, at a frequency of 0.5& nbsp;Hz. These oscillations were captured on video, and lasted for 142 seconds.

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Undetermined Music Artists

Resonance

Biography

Examples

Theory

Resonators

Q factor

Types of resonance

Mechanical and acoustic resonance

Electrical resonance

Optical resonance

Orbital resonance

Atomic, particle, and molecular resonance

Failure of the original Tacoma Narrows Bridge

Resonance causing a vibration on the International Space Station

See also

References

External links

Copyright Citations