What does the frequency sharpness mean?

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Discussion Overview

The discussion centers around the concepts of frequency response and sharpness of resonance, exploring their definitions, mathematical representations, and implications in various physical systems. Participants delve into the characteristics of resonance in mechanical systems, particularly in relation to simple harmonic motion (SHM) and damped oscillators.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants define frequency response as the amplitude of oscillation as a function of frequency, while sharpness of resonance is linked to the Q factor, indicating how quickly energy decays in the system.
  • There is a discussion about the shape of the resonance curve, with some suggesting it resembles a bell curve, while others clarify it is more accurately described by a Lorentzian profile.
  • Participants mention that the sharpness of resonance is influenced by various factors, including system dynamics, losses in cavities, and the characteristics of the gain medium in optical oscillators.
  • One participant notes that resonance peaks can be mathematically described using Gaussian, Lorentzian, or Voigt profiles, with the Q value being determined by the ratio of maximum value to the full width at half maximum (FWHM).
  • There is a contention regarding the occurrence of resonance in simple harmonic oscillators, with some asserting that resonance peaks do not occur in SHM, while others argue that they can be represented as delta functions in ideal cases.
  • Participants discuss the implications of damping on the natural frequency and resonance behavior of mechanical oscillators, emphasizing the differences between damped and undamped systems.

Areas of Agreement / Disagreement

Participants express differing views on the occurrence of resonance in simple harmonic oscillators and the nature of resonance curves. There is no consensus on the definitions and implications of frequency response and sharpness of resonance, indicating multiple competing perspectives.

Contextual Notes

Some claims depend on specific definitions of terms like "sharpness" and "frequency response," and the discussion includes unresolved mathematical steps regarding the representation of resonance in different systems.

apache
what does the 'frequency response' and 'sharpness' of resonance mean ?
thanks
-apache
 
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Frequency response is a measure of the amplitude of an oscillation as a function of frequency.

Sharpness of resonance is defined by the Q factor, which is related to how quickly the energy of the oscillating system decays.
 
thank you..
the frequency response would then be shown with the bell curve right ? with max. amplitude at the natural freq. of the system.
but what would be the determinants of the shapness of resonance?
thank you once again
-apache
 
See here...

http://www.cims.nyu.edu/~barnett/tf/q.pdf
 
Usually by bell curve they mean Gaussian profile exp(-f2). The resonance curve shape is 1/(1-f2) which is usually called Lorents curve.
 
the frequency response would then be shown with the bell curve right

Magnitude vs. frequency is shown via Bode magnitude diagrams.

They do not always have a peak. It depends on the system dynamics.
 
Apache,

The determinants of the sharpness in resonance depends on the system involved. Lots of physical systems undergo resonance peaks, in the case of inhomogenously broadened optical oscillators (lasers) for example, the sharpness depends on the losses in the cavity, the gain medium, the shape and reflectivity of the mirrors and the length of the cavity.

Resonance peaks can be described mathematically using Gaussian, Lorentzian or a combination between the two (convolution) called a Voight profile. All these mathematicals functions have 2 important parameters, the maximum value and the Full width-Half maximum (The width of the curve at 1/2 the maximum value.) The ratio of these two parameters gives the Q values. Tall skinny peaks have high a Q, flat broad peaks have a low Q.

As enigma correctly points out, there need not be a resonant peak at all. Indeed there may be many overlapping resonance peaks (common in the case of lasers).
 
thanks for the replies,
yeah i was wrong on the bell curve lol .. but it kinda looks like a bell, with 0 gradient and max amplitude at f0 ...
anyhow.. i don't think i understand how the sharpness would be affected in mechanical SHM .. like mabye a spring and mass etc..
thanks for all your help
 
Resonance peaks do not occur in Simple Harmonic oscillators, only in mechanical oscillators with some damping constant, r and some sinusoidal driving force, F(t).

The frequency of oscillation you get with SHM is called the natural resonance of the system, so called because it resonates at that frequency without a driving force (i.e. F(t)=0). For damped oscillators, the natural frequency is slightly different than that of an undamped system (i.e r=0, as in SHM).

It is possible to force an oscillator to oscillate at a frequency other than its natural frequency using a driving force, however the amplitude decreases. Plotting the driving force frequency vs amplitude will give a resonance peak.

Some characteristics of mechanical resonance peaks include:-
- Amplitude = F/s as w (drive frequency) approaches 0 (Hooke's Law)
- Amplitude approaches 0 as w approaches infinity.
 
  • #10
Resonance does occur in simple harmonic oscillator, resonance curve is then a delta-function (zero width and infinite amplitude).

Equation of forced oscillations in oscillating system can be written as: x"+(wo/Q)x'+wo2=wo2cos(wt), where wo is own (resonance) frequency of system and w - frequency of external force, 1/Q - damping factor (Q is usually called quality of oscillating system).

Stationary solution of this equation (established oscillations in such system after some time) is: x(t)=xocos(wt), where amplitude of oscillations depends on frequency w of external force: xo={[(1-(w/wo)2]2+(w/Qwo)2}-1

You may see that for ideal oscillator (Q=oo) amplitude xo becomes delta function. For non-infinite Q values the width of resonance curve deltaw/wo (FWHM = width on 1/2 level for energy = width on 0.71 level for amplitude) is equal to 1/Q.

Typical Q values: mass on spring 1-10, radio LC circuit 10-100, mass on a string 100-1000, quarts watch crystal 104-5, spectral lines (in visible range) 105-6, orbiting moons and planets 107-9, good laser 108-9, atomic clock cavity 1011-13.
 
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