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RESOLVING POWER OF A PLANE
DIFFRACTION GRATING
•The resolving power of a grating is defined as its
ability to show two neighboring lines in a spectrum as
separate.it is measured by the ratio y/dy. where y is the
wavelength of a spectral line and dy is the least
difference in the wavelengths of two neighbouring
spectral lines which can just be resolved.
• Light of two wavelengths y and (y+dy) is incident
normally on the sueface of a plane transmission
grating AB.
i
•The light of each wavelengths would form a
separate diffraction pattern of the silt P1 is the
nth primary maximum of a spectral line of
wavelenghth y at an angle of diffraction 0.Then,
• (a+b)sin θ=ny
•Here (a+b) is the grating element.
•P2 is the nth primary maximum of a second
spectral line of wavelength (y+dy) at an angle of
diffraction ( θ+d θ).Ten,
• (a+b)sin( θ+d θ)=n(y+dy)
•According to rayleigh the two spectral
lines will appear just resolved if the
principal maximum due to (y+dy) falls on
the first minimum of y or vice versa.
•Thus the two lines will appear just
resolved if the angle of diffraction
( θ+dθ)also corresponds to the direction of
first secondary minimum after the nth
primary maximum at P1 corresponds to
wavelength y.
•This is possible if the extra path difference
introduced is y/N.
•Here,N is the total number of lines in the
grating
• (a+b)sin( θ+d θ)=ny+y/N
•Equating the right hand sides of equ(2) and(3),
• n(y+dy)=ny=y/N
or
• Ndy=y/N
• y/dy=nN
The resolving power increases with
•the order n the spectrum
•the total number of lines N on the grating
.The R.b is independent of the grating
element (a+b).
THANK YOU

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RESOLVING POWER OF A PLANE DIFFRACTION GRATING THEORY.pptx

  • 1. RESOLVING POWER OF A PLANE DIFFRACTION GRATING
  • 2.
  • 3. •The resolving power of a grating is defined as its ability to show two neighboring lines in a spectrum as separate.it is measured by the ratio y/dy. where y is the wavelength of a spectral line and dy is the least difference in the wavelengths of two neighbouring spectral lines which can just be resolved. • Light of two wavelengths y and (y+dy) is incident normally on the sueface of a plane transmission grating AB.
  • 4. i •The light of each wavelengths would form a separate diffraction pattern of the silt P1 is the nth primary maximum of a spectral line of wavelenghth y at an angle of diffraction 0.Then, • (a+b)sin θ=ny •Here (a+b) is the grating element. •P2 is the nth primary maximum of a second spectral line of wavelength (y+dy) at an angle of diffraction ( θ+d θ).Ten, • (a+b)sin( θ+d θ)=n(y+dy)
  • 5. •According to rayleigh the two spectral lines will appear just resolved if the principal maximum due to (y+dy) falls on the first minimum of y or vice versa. •Thus the two lines will appear just resolved if the angle of diffraction ( θ+dθ)also corresponds to the direction of first secondary minimum after the nth primary maximum at P1 corresponds to wavelength y. •This is possible if the extra path difference introduced is y/N.
  • 6. •Here,N is the total number of lines in the grating • (a+b)sin( θ+d θ)=ny+y/N •Equating the right hand sides of equ(2) and(3), • n(y+dy)=ny=y/N or • Ndy=y/N • y/dy=nN
  • 7. The resolving power increases with •the order n the spectrum •the total number of lines N on the grating .The R.b is independent of the grating element (a+b).