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Laser Micrometer

Single-Slit Diffraction?
Single-Slit Diffraction
1. You have been asked to measure the width of a slit in a piece of paper. You mount the paper 80 centimeters from a screen and illuminate it from behind with laser light of wavelength 633 nanometers (in air). You mark two of the intensity minima as shown in the figure, and measure the distance between them to be 17.9 millimeters
Express your answer in micrometers, to three significant figures.
2.If the entire apparatus were submerged in water, would the width of the central peak change?
a. The width would increase.
b.The width would decrease.
c.The width would not change.
here's the link to the page
(1) In single slit diffraction ,for position of minima ,path difference d sine theta =n*wavelength, where n is order of minima.In the figure shown 17. 9 mm is total distance between 3 rd minima on either side.
therefore 2y=17.9
y=8.95 mm
sine theta=tan theta=y/screen distance'D'
d sine theta= d * y/ screen distance 'D
d * y/ screen distance 'D= 3 wavelength
d =3wavelength*D / y
=3*633*E-9*0.8/8.95*E-3
=169.743 micro meter.
(2)width in water= width in air / refractive index of water
hence width in water will decrease ( choice b correct)
'
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Digimatic Micrometer Digimatic Micrometer $162.99 No programming needed to start measuring all the way down to .00005" (50 millionths!). User programmable to do all sorts of comparative measurements . . . compare multiple pieces to one original or set the desired dimension as zero and compare all pieces to that. Full black-filled thimble and sleeve markings so can be used even if the battery runs out. Instant conversion from inch to millimeters - better than any chart. Mfg: Mitutoyo SPECS: 5¾" (14.6cm) long x 2-5/8" (6.7cm) high. Carbide tipped measuring faces. Reads 0-1" (2.5cm) 0-25mm. Accurate to .00005" (.0013mm). W/case. |
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Ocular Micrometer $58.94 High Quality Content by WIKIPEDIA articles An ocular micrometer is a glass disk that fits in a microscope eyepiece that has a ruled scale, which is used to measure the size of magnified objects. The physical length of the marks on the scale depend on the degree of magnification. A microscope (from the Greek:, mikros, small and, skopein, to look or see ) is an instrument to see objects too small for the naked eye. The science of investigating small objects using such an instrument is called microscopy. Microscopic means invisible to the eye unless aided by a microscope. Author: Surhone, Lambert M./ Tennoe, Mariam T./ Henssonow, Susan F. Binding Type: Paperback Number of Pages: 74 Publication Date: 2010/08/16 Language: English Dimensions: 6.00 x 9.02 x 0.18 inches |
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Laser Micro QC 1
A laser cavity has a flat mirror and a spherical mirror with radius of curvature of 40 cm. The mirrors are sep
A laser cavity has a flat mirror and a spherical mirror with radius of curvature of 40 cm. The mirrors are separated by 20 cm. The flat mirror is partially transparent, while the spherical mirror is perfectly reflecting. An output of 2 mW at a wavelength of 0.543 um (micrometer, green) is emitted by the laser.
a) Demonstrate that the cavity is stable.
b) What is the half angle of the beam divergence (in radians)?
c) An opaque screen with a circular hole of radius a is placed at a distance of 40 cm from the flat mirror. A total power of 1 mW passes through the hole. Calculate the radius of “a” of the hole. Assume that the center of the hole coincides perfectly with the optical beam axis.
For a stable mode, the wavefront curvature of the mode has to match that of both mirrors, thus it is flat on the flat mirror. Thus take the origin of the z-coordinate on the flat mirror since the beam waist is there. The radius of curvature of the wavefront satisfies
R(z)=z [1 + (zR/z)^2 ],
where zR =k w0^2/2 is the Rayleigh length in terms of the beam radius w0 at the waist. Now, when z=L, R(z)=2 L. Thus
2 L =L[1+ (zR/L)^2 ]
Hence zR=L=20 cm, so that w0= sqrt(2L/k)=sqrt(Lλ /π )=.0186 cm. The cavity is stable because the real part of 1/w0^2 is positive (a negative value describes a field that grows away from the axis , which would clearly be unstable).
Use
w=w0 sqrt(1+z^2/zR^2),
set z=40 cm, that will give w at the location of the disk. Let
I(r) = I0 exp(-2 r^2/w^2).
I leave it to yuo to determine I0 in terms of the total power.
The power passing through a hole of radius a is
P = 2π∫ (r=0 to a) I(r) r dr
= I0 (π /2)w^2 [ 1-exp(-2 a^2/w^2)].
You solve this for a.











































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