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ANANT BINEKAR
15MSS0020
 Introduction
 Principle
 Operation
 Types
 Application
 Advantages
 Disadvantages
 References
 It is a optical sensor.
 Invented by two scienstists Alfred Perot and
Charles Fabry.
 For measuring small displacements with high
precision in a harsh environment, the so- called
Fabry–Perot optical cavity can be employed.
 The cavity contains two semireflective mirrors
facing each other and separated by distance L.
 The cavity is injected with light from a known
source (a laser, e.g.) and the photons inside the
cavity bounce back and forth between the two
mirrors, interfering with each other in the process.
 In fact, the cavity is a storage tank for light.
At some frequencies of photons, light can
pass out of the cavity.
 The narrow bands of transmitted light are
separated by frequencies that are inversely
proportional to the cavity length:
ν = c/2L
Where, c is the speed of light
v is frequncy
L is length of cavity .
 For practical cavities with a mirror separation
on the order of 1 μm, typical values of ν are
between 500 MHz and 1 GHz.
 Thus, by detecting the frequency shift of the
transmitted light with respect to a reference
light source,changes in the cavity dimensions
can be measured with the accuracy
comparable with the wavelength of light.
 Whatever may cause changes in the cavity
dimensions (mirror movement) may be the
subject of measurements. These include
strain, force , pressure, and temperature.
 This kind of sensor detects changes in optical
path length induced by either a change in the
refractive index or a change in physical
length of the cavity.
Fabry–Perot pressure sensor
 Pressure is applied to the upper membrane.
Under pressure, the diaphragm deflects
inwardly,thus reducing the cavity dimension
L.
 Small size.
 Accurate.
 Insensitive to environmental effect.
 Immune to many electromagnetic and radio-
frequency interferences.
 can operate reliably in harsh environment.
 Indirect contact to mesurend.
 Cost is large.
 Not suitable for high pressure.
 Jacob Fraden, “ Hand Book of Modern
Sensors: physics, Designs and Applications”,
3rd ed., Springer, 2003.
 J.M. Lopez-Higuera, 'Introduction to fibre
optic sensing technology',
in Handbook of optical fibre sensing
technology, J.M. Lopez-Higuera Ed, Wiley,
2002.
Febry perot sensor

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Febry perot sensor

  • 2.  Introduction  Principle  Operation  Types  Application  Advantages  Disadvantages  References
  • 3.  It is a optical sensor.  Invented by two scienstists Alfred Perot and Charles Fabry.
  • 4.  For measuring small displacements with high precision in a harsh environment, the so- called Fabry–Perot optical cavity can be employed.  The cavity contains two semireflective mirrors facing each other and separated by distance L.  The cavity is injected with light from a known source (a laser, e.g.) and the photons inside the cavity bounce back and forth between the two mirrors, interfering with each other in the process.
  • 5.
  • 6.  In fact, the cavity is a storage tank for light. At some frequencies of photons, light can pass out of the cavity.  The narrow bands of transmitted light are separated by frequencies that are inversely proportional to the cavity length: ν = c/2L Where, c is the speed of light v is frequncy L is length of cavity .
  • 7.  For practical cavities with a mirror separation on the order of 1 μm, typical values of ν are between 500 MHz and 1 GHz.  Thus, by detecting the frequency shift of the transmitted light with respect to a reference light source,changes in the cavity dimensions can be measured with the accuracy comparable with the wavelength of light.
  • 8.  Whatever may cause changes in the cavity dimensions (mirror movement) may be the subject of measurements. These include strain, force , pressure, and temperature.  This kind of sensor detects changes in optical path length induced by either a change in the refractive index or a change in physical length of the cavity.
  • 10.  Pressure is applied to the upper membrane. Under pressure, the diaphragm deflects inwardly,thus reducing the cavity dimension L.
  • 11.  Small size.  Accurate.  Insensitive to environmental effect.  Immune to many electromagnetic and radio- frequency interferences.  can operate reliably in harsh environment.  Indirect contact to mesurend.
  • 12.  Cost is large.  Not suitable for high pressure.
  • 13.  Jacob Fraden, “ Hand Book of Modern Sensors: physics, Designs and Applications”, 3rd ed., Springer, 2003.  J.M. Lopez-Higuera, 'Introduction to fibre optic sensing technology', in Handbook of optical fibre sensing technology, J.M. Lopez-Higuera Ed, Wiley, 2002.