Lecture 8: Spectroscopic Instruments Flashcards
(36 cards)
chemical composition of stellar body can be
determined by observing its spectrum
velocity determined from
doppler shift of spectral lines
doppler shift observed in light from stars
determine rotation frequency of arms of a spiral galaxy
large planets cause stars to wobble leading to a doppler shift
common components of spectroscopic instruments
slit
collimator
diffraction grating
focusing mirror
detector
in general, spectroscopic instruments
map wavelength to position on detector
resolving power
R= lambda / delta lambda
spectrometer
also ‘monochrometer’
entrance and exit slits
tune wavelength by rotating grating
spectrograph
also ‘spectroscope’
entrance slit
spectrum recorded on camera or CCD array
diffraction gratings - light transmitted by
gaps between lines - apertures
each acts as an independent source
diffraction gratings- secondary wavelets (circular waves) emanate from
each gap
diffraction grating - constructive interference at
certain angles (diffraction orders)
diffraction angle depends on
wavelength
grating equation
sin thetam - sin thetai = m lambda/a
angular dispersion equation
D= dthetam/d lambda = m/a cos thetam
instrumental width equation
delta theta = lambda / Na cos theta m
resolving power equation
R=lambda / delta lambda = mN
free spectral range equation
delta lambda_FSR = lambda/m
intensity maxima occur at
diffraction angles when the path length difference is equal to an integer number of wavelengths
angular dispersion of the grating is the
rate at which the angle changes with wavelength
angular dispersion is derived by
differentiating the grating equation with respect to wavelength
getting from angular to linear dispersion
small angle approx x=Ltheta
dx/dlambda = L d theta/dlambda
sub in angular dispersion
limit of resolution is when
first min of lambda1 coincides with the max of lambda 2
rayleigh criterion
instrumental width delta theta
angular separation to the first min
first min occurs for a phase
thi = 2pi/N