FREQUENCY is the number of occurrences of a repeating event per unit
time . It is also referred to as TEMPORAL FREQUENCY, which emphasizes
the contrast to spatial frequency and angular frequency . The PERIOD
is the duration of time of one cycle in a repeating event, so the
period is the reciprocal of the frequency. For example, if a newborn
baby's heart beats at a frequency of 120 times a minute, its
period—the time interval between beats—is half a second (that is,
60 seconds divided by 120 beats ).
CONTENTS * 1 Definitions * 2 Units * 3 Period versus frequency * 4 Related types of frequency * 5 In wave propagation * 6 Measurement * 6.1 Counting
* 6.2
* 7 Examples * 7.1
* 8 See also * 9 Notes and references * 10 Further reading * 11 External links DEFINITIONS As time elapses—here moving left to right on the horizontal axis—the five sinusoidal waves vary, or cycle, regularly at different rates . The red wave (top) has the lowest frequency (i.e., cycles at the slowest rate) while the purple wave (bottom) has the highest frequency (cycles at the fastest rate). For cyclical processes, such as rotation , oscillations , or waves , frequency is defined as a number of cycles per unit time. In physics and engineering disciplines, such as optics , acoustics , and radio , frequency is usually denoted by a Latin letter _f_ or by the Greek letter _ {displaystyle nu } _ or _ν_ (nu) (see e.g. Planck\'s formula ). The relation between the frequency and the period T {displaystyle T} of a repeating event or oscillation is given by f = 1 T . {displaystyle f={frac {1}{T}}.} UNITS The
A traditional unit of measure used with rotating mechanical devices is revolutions per minute , abbreviated r/min or rpm. 60 rpm equals one hertz. PERIOD VERSUS FREQUENCY As a matter of convenience, longer and slower waves, such as ocean surface waves , tend to be described by wave period rather than frequency. Short and fast waves, like audio and radio , are usually described by their frequency instead of period. These commonly used conversions are listed below: FREQUENCY 1 mHz (10−3 Hz) 1 Hz (100 Hz) 1 kHz (103 Hz) 1 MHz (106 Hz) 1 GHz (109 Hz) 1 THz (1012 Hz) PERIOD 1 ks (103 s) 1 s (100 s) 1 ms (10−3 s) 1 µs (10−6 s) 1 ns (10−9 s) 1 ps (10−12 s) RELATED TYPES OF FREQUENCY _ Diagram of the relationship between the different types of frequency and other wave properties. For other uses, see Frequency (other) . *
y ( t ) = sin ( ( t ) ) = sin ( t ) = sin ( 2 f t )
{displaystyle y(t)=sin left(theta (t)right)=sin(omega t)=sin(2mathrm
{pi } ft)} _ d d t = = 2 f {displaystyle
{frac {mathrm {d} theta }{mathrm {d} t}}=omega =2mathrm {pi } f}
*
y ( t ) = sin ( ( t , x ) ) = sin ( t + k x )
{displaystyle y(t)=sin left(theta (t,x)right)=sin(omega t+kx)}
d d x = k {displaystyle {frac {mathrm {d} theta
}{mathrm {d} x}}=k}
IN WAVE PROPAGATION Further information:
For periodic waves in nondispersive media (that is, media in which the wave speed is independent of frequency), frequency has an inverse relationship to the wavelength , _λ_ (lambda ). Even in dispersive media, the frequency _f_ of a sinusoidal wave is equal to the phase velocity _v_ of the wave divided by the wavelength _λ_ of the wave: f = v . {displaystyle f={frac {v}{lambda }}.} In the special case of electromagnetic waves moving through a vacuum , then _v = c_, where _c_ is the speed of light in a vacuum, and this expression becomes: f = c . {displaystyle f={frac {c}{lambda }}.} When waves from a monochrome source travel from one medium to another, their frequency remains the same—only their wavelength and speed change. MEASUREMENT See also:
_ This section DOES NOT CITE ANY SOURCES . Please help improve this section by adding citations to reliable sources . Unsourced material may be challenged and removed . (July 2015)_ _(Learn how and when to remove this template message )_ Measurement of frequency can done in the following ways, COUNTING Calculating the frequency of a repeating event is accomplished by counting the number of times that event occurs within a specific time period, then dividing the count by the length of the time period. For example, if 71 events occur within 15 seconds the frequency is: f = 71 15 s 4.7 Hz {displaystyle f={frac {71}{15,{text{s}}}}approx 4.7,{text{Hz}}} If the number of counts is not very large, it is more accurate to measure the time interval for a predetermined number of occurrences, rather than the number of occurrences within a specified time. The latter method introduces a random error into the count of between zero and one count, so on average half a count. This is called _gating error_ and causes an average error in the calculated frequency of _ΔF_ = 1/(2 _TM_), or a fractional error of _ΔF_ / _F_ = 1/(2 _F TM_) where _TM_ is the timing interval and _F_ is the measured frequency. This error decreases with frequency, so it is a problem at low frequencies where the number of counts _N_ is small. A resonant-reed frequency meter, an obsolete device used from about 1900 to the 1940s for measuring the frequency of alternating current. It consists of a strip of metal with reeds of graduated lengths, vibrated by an electromagnet . When the unknown frequency is applied to the electromagnet, the reed which is resonant at that frequency will vibrate with large amplitude, visible next to the scale. STROBOSCOPE An older method of measuring the frequency of rotating or vibrating objects is to use a stroboscope . This is an intense repetitively flashing light (strobe light ) whose frequency can be adjusted with a calibrated timing circuit. The strobe light is pointed at the rotating object and the frequency adjusted up and down. When the frequency of the strobe equals the frequency of the rotating or vibrating object, the object completes one cycle of oscillation and returns to its original position between the flashes of light, so when illuminated by the strobe the object appears stationary. Then the frequency can be read from the calibrated readout on the stroboscope. A downside of this method is that an object rotating at an integral multiple of the strobing frequency will also appear stationary. FREQUENCY COUNTER Main article: frequency counter Modern frequency counter Higher frequencies are usually measured with a frequency counter .
This is an electronic instrument which measures the frequency of an
applied repetitive electronic signal and displays the result in hertz
on a digital display . It uses digital logic to count the number of
cycles during a time interval established by a precision quartz time
base. Cyclic processes that are not electrical in nature, such as the
rotation rate of a shaft, mechanical vibrations, or sound waves , can
be converted to a repetitive electronic signal by transducers and the
signal applied to a frequency counter.
HETERODYNE METHODS Above the range of frequency counters, frequencies of electromagnetic signals are often measured indirectly by means of heterodyning (frequency conversion ). A reference signal of a known frequency near the unknown frequency is mixed with the unknown frequency in a nonlinear mixing device such as a diode . This creates a heterodyne or "beat" signal at the difference between the two frequencies. If the two signals are close together in frequency the heterodyne is low enough to be measured by a frequency counter. This process only measures the difference between the unknown frequency and the reference frequency. To reach higher frequencies, several stages of heterodyning can be used. Current research is extending this method to infrared and light frequencies (optical heterodyne detection ). EXAMPLES LIGHT Complete spectrum of electromagnetic radiation with the visible
portion highlighted Main articles:
Visible light is an electromagnetic wave , consisting of oscillating electric and magnetic fields traveling through space. The frequency of the wave determines its color: 7014400000000000000♠4×1014 Hz is red light, 7014800000000000000♠8×1014 Hz is violet light, and between these (in the range 4-7014800000000000000♠8×1014 Hz) are all the other colors of the visible spectrum . An electromagnetic wave can have a frequency less than 7014400000000000000♠4×1014 Hz, but it will be invisible to the human eye; such waves are called infrared (IR) radiation. At even lower frequency, the wave is called a microwave , and at still lower frequencies it is called a radio wave . Likewise, an electromagnetic wave can have a frequency higher than 7014800000000000000♠8×1014 Hz, but it will be invisible to the human eye; such waves are called ultraviolet (UV) radiation. Even higher-frequency waves are called X-rays , and higher still are gamma rays . All of these waves, from the lowest-frequency radio waves to the highest-frequency gamma rays, are fundamentally the same, and they are all called electromagnetic radiation . They all travel through a vacuum at the same speed (the speed of light ), giving them wavelengths inversely proportional to their frequencies. c = f {displaystyle displaystyle c=flambda } where _c_ is the speed of light (_c _ in a vacuum, or less in other media), _f_ is the frequency and λ is the wavelength. In dispersive media , such as glass, the speed depends somewhat on frequency, so the wavelength is not quite inversely proportional to frequency. SOUND Main article:
The frequencies an ear can hear are limited to a specific range of frequencies . The audible frequency range for humans is typically given as being between about 20 Hz and 20,000 Hz (20 kHz), though the high frequency limit usually reduces with age. Other species have different hearing ranges. For example, some dog breeds can perceive vibrations up to 60,000 Hz. In many media, such as air, the speed of sound is approximately independent of frequency, so the wavelength of the sound waves (distance between repetitions) is approximately inversely proportional to frequency. LINE CURRENT Main article:
In
SEE ALSO See also:
*
NOTES AND REFERENCES * ^ "Definition of FREQUENCY". Retrieved 3 October 2016.
* ^ "Definition of PERIOD". Retrieved 3 October 2016.
* ^ Davies, A. (1997). _Handbook of Condition Monitoring:
Techniques and Methodology_. New York: Springer. ISBN
978-0-412-61320-3 .
* ^ Bakshi, K.A.; A.V. Bakshi; U.A. Bakshi (2008). _Electronic
Measurement Systems_. US: Technical Publications. pp. 4–14. ISBN
978-81-8431-206-5 .
* ^ "Definition of SOUND". Retrieved 3 October 2016.
* ^ Pilhofer, Michael (2007). _Music Theory for Dummies_. For
Dummies. p. 97. ISBN 9780470167946 .
* ^ Elert, Glenn; Timothy Condon (2003). "
FURTHER READING * Giancoli, D.C. (1988). _
EXTERNAL LINKS _ Look up FREQUENCY _ or |

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