frequency

(noun)

The quotient of the number of times n a periodic phenomenon occurs over the time t in which it occurs: f = n / t.

Related Terms

  • wave speed
  • doppler effect
  • angular frequency
  • transmitter
  • Hertz
  • media
  • interfere
  • superposition
  • classical physics
  • photon
  • wavelength
  • period

(noun)

The quotient of the number of times (n) a periodic phenomenon occurs over a unit of time (t): f = n / t.

Related Terms

  • wave speed
  • doppler effect
  • angular frequency
  • transmitter
  • Hertz
  • media
  • interfere
  • superposition
  • classical physics
  • photon
  • wavelength
  • period

Examples of frequency in the following topics:

  • Frequency of Sound Waves

    • The perception of frequency is called pitch.
    • The perception of frequency is called pitch.
    • The SI unit of frequency is called a Hertz, denoted Hz.
    • Different species can hear different frequency ranges.
    • Three flashing lights, from lowest frequency (top) to highest frequency (bottom). f is the frequency in hertz (Hz); or the number of cycles per second.
  • Radio Waves

    • The lowest commonly encountered radio frequencies are produced by high-voltage AC power transmission lines at frequencies of 50 or 60 Hz.
    • In this case, a carrier wave having the basic frequency of the radio station (perhaps 105.1 MHz) is modulated in frequency by the audio signal, producing a wave of constant amplitude but varying frequency.
    • Other channels called UHF (ultra high frequency) utilize an even higher frequency range of 470 to 1000 MHz.
    • Frequency modulation for FM radio.
    • (a) A carrier wave at the station's basic frequency.
  • Period and Frequency

    • The period is the duration of one cycle in a repeating event, while the frequency is the number of cycles per unit time.
    • The frequency is defined as the number of cycles per unit time.
    • Frequency is usually denoted by a Latin letter f or by a Greek letter ν (nu).
    • Note that period and frequency are reciprocals of each other .
    • Sinusoidal waves of various frequencies; the bottom waves have higher frequencies than those above.
  • Beats

    • The wave resulting from the superposition of two similar-frequency waves has a frequency that is the average of the two.
    • This wave fluctuates in amplitude, or beats, with a frequency called the beat frequency.
    • We can determine the beat frequency mathematically by adding two waves together.
    • One can also measure the beat frequency directly.
    • The number of beats per second, or the beat frequency, shows the difference in frequency between the two notes.
  • RLC Series Circuit: At Large and Small Frequencies; Phasor Diagram

    • Response of an RLC circuit depends on the driving frequency—at large enough frequencies, inductive (capacitive) term dominates.
    • Now, we will examine the system's response at limits of large and small frequencies.
    • At large enough frequencies $(\nu \gg \frac{1}{\sqrt{2\pi LC}})$, XL is much greater than XC.
    • The impedance Z at small frequencies $(\nu \ll \frac{1}{\sqrt{2\pi LC}})$ is dominated by the capacitive term, assuming that the frequency is high enough so that XC is much larger than R.
    • Distinguish behavior of RLC series circuits as large and small frequencies
  • Resonance in RLC Circuits

    • Frequencies at which the response amplitude is a relative maximum are known as the system's resonance frequencies.
    • The reactances vary with frequency $\nu$, with XL large at high frequencies and XC large at low frequencies given as:
    • $\nu_0$ is the resonant frequency of an RLC series circuit.
    • A variable capacitor is often used to adjust the resonance frequency to receive a desired frequency and to reject others. is a graph of current as a function of frequency, illustrating a resonant peak in Irms at $\nu_0 = f_0$.
    • An RLC series circuit with an AC voltage source. f is the frequency of the source.
  • Aliasing

    • Looked at from another point of view, for any sampling interval $\Delta$ , there is a special frequency (called the Nyquist frequency), given by $f_s = \frac{1}{2\Delta}$ .
    • The extrema (peaks and troughs) of a sinusoid of frequency $f_s$ will lie exactly $1/2f_s$ apart.
    • Figure 4.9 shows a cosine function sampled at an interval longer than $1/2f_s$ ; this sampling produces an apparent frequency of 1/3 the true frequency.
    • This means that any frequency component in the signal lying outside the interval $(-f_s,f_s)$ will be spuriously shifted into this interval.
    • Figure 4.9: A sinusoid sampled at less than the Nyquist frequency gives rise to spurious periodicities.
  • Forced Vibrations and Resonance

    • The phenomenon of driving a system with a frequency equal to its natural frequency is called resonance.
    • The phenomenon of driving a system with a frequency equal to its natural frequency is called resonance.
    • When tuning a radio, for example, people are adjusting the resonant frequency of the radio circuit so that it only oscillates to the desired station's broadcast (or driving) frequency.
    • Resonance occurs when the driving frequency equals the natural frequency, and the greatest response is for the least amount of damping.
    • Heavy cross winds drove the bridge into oscillations at its resonant frequency.
  • Microwaves

    • Extremely high frequency (EHF) is the highest microwave frequency band.
    • Super high frequency (SHF) is the designation for electromagnetic wave frequencies in the range of 3 GHz to 30 GHz.
    • Microwaves at a frequency of 2.45 GHz are produced by accelerating electrons.
    • The maser, rather than amplifying visible light energy, amplifies the lower-frequency, longer-wavelength microwaves and radio frequency emissions.
    • The range of frequencies and wavelengths is remarkable.
  • General Case

    • Since the time between waves is reduced, the frequency is increased.
    • If the observer is moving away from the sound source, the frequency will be lowered, and if the observer moves closer to the sound source, the frequency is increased.
    • If the source approaches the observer at an angle (but still with a constant velocity), the observed frequency that is first heard is higher than the object's emitted frequency.
    • If the speeds and are small compared to the speed of the wave, the relationship between observed frequency and emitted frequency is approximately
    • The wave-fronts are produced with the same frequency as before.
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