Interference in a Thin Film: Newton’s rings
Purpose
The purpose of this experiment was to show how light interference works in a thin film
Part 1: Thin wedge consecutive lines of fringes
Part 2: Newton’s Rings circles of fringes
Interference in a Thin Film: Newton’s rings
Theory
Index of refraction glass n = 1.5 air n = 1.0
When nA > nB
rays reflecting from the side where n=nA reflect the same
phase rays reflecting from the side
where n=nB experience a
phase reversal
Interference in a Thin Film: Newton’s rings
Theory
A phase reversal is equivalent to shifting the ray by half a wavelength
Diagram from Physics 294 Laboratory Manual, page 17-1
Interference in a Thin Film: Newton’s rings
Theory
When waves interfere constructively:
Interference in a Thin Film: Newton’s rings
Theory
When waves interfere destructively:
Interference in a Thin Film: Newton’s rings
Theory
When waves interfere destructively:
Interference in a Thin Film: Newton’s rings
Theory Part 1
Diagram from Physics 294 Laboratory Manual, page 17-2
Interference in a Thin Film: Newton’s rings
Theory Part 1
Two glass plates at an angle cause the space between them t to increase with x t = /2 = x tan
Where t is the distance between the two pieces of
glass is the wavelength of the light x is the distance between consecutive fringes is the angle between the glass
tan = t / x Since is constant, t / x should be constant Implies fringes happen at regular intervals
Interference in a Thin Film: Newton’s rings
Theory Part 2
Interference in a Thin Film: Newton’s rings
Theory Part 2
Interference in a Thin Film: Newton’s rings
Theory Part 2
Interference in a Thin Film: Newton’s rings
Theory Part 2
Diagrams from Physics 294 Laboratory Manual, page 17-3
Interference in a Thin Film: Newton’s rings
Theory Part 2
rm2 = xm
2/4 + 2 = mR Where
rm is the actual radius of the mth fringe
xm is the measured diameter is the perpendicular offset from the center of
the ring m is the order of the ring
m=0 for the bulls eye m=1, 2, 3, … for each consecutive ring
is the wavelength of the light R is the curvature radius of the plano-convex lens
Interference in a Thin Film: Newton’s rings
Apparatus
Interference in a Thin Film: Newton’s rings
Apparatus
Diagram from Physics 294 Laboratory Manual, page 17-2
Interference in a Thin Film: Newton’s rings
Procedure
Interference in a Thin Film: Newton’s rings
Procedure Part 1
The distance from an arbitrary (m=0) fringe to 20 consecutive dark fringes was measured
The difference between each fringe was calculated x = xn - xn-1
From x we can calculate /2 = x tan
Interference in a Thin Film: Newton’s rings
Procedure Part 2
Position the microscope over the center of the bulls eye
Measure xL and xR to get xm for 10 rings xm = |xL - xR|
Plot xm2 versus m to find R and 2
xm2/4 + 2 = mR
xm2 = mR/4 - 2/4
y = mx + b
Interference in a Thin Film: Newton’s rings
Analysis
Interference in a Thin Film: Newton’s rings
Analysis Part 1
Error for x x = (x)2 + (x)2
x = 2(x)2 x = 2(0.004 cm)2
x = 0.006 cm
m Xm (cm) error Xm (cm) difference Xm (cm) error difference (cm)0 11.883 0.0041 11.941 0.004 0.058 0.0062 11.990 0.004 0.049 0.0063 12.040 0.004 0.050 0.0064 12.090 0.004 0.050 0.0065 12.141 0.004 0.051 0.0066 12.190 0.004 0.049 0.0067 12.233 0.004 0.043 0.0068 12.290 0.004 0.057 0.0069 12.332 0.004 0.042 0.00610 12.380 0.004 0.048 0.00611 12.432 0.004 0.052 0.00612 12.486 0.004 0.054 0.00613 12.530 0.004 0.044 0.00614 12.580 0.004 0.050 0.00615 12.632 0.004 0.052 0.00616 12.684 0.004 0.052 0.00617 12.734 0.004 0.050 0.00618 12.786 0.004 0.052 0.00619 12.838 0.004 0.052 0.00620 12.888 0.004 0.050 0.006
Interference in a Thin Film: Newton’s rings
Analysis Part 1
Average x = 0.050 Excel “=AVERAGE(x)”
Standard Deviation x = 0.004 Excel “=STDEV(x)”
Interference in a Thin Film: Newton’s rings
Analysis Part 1
t = /2 = x tan /2 = x tan
for sodium light is 589.3 nm = 5.893*10-7m x average was 0.050 cm = 5.0 * 10-4m
Solve for (5.893*10-7m)/2 = (5.0 * 10-4m ) tan = 3.4 * 10-2 degrees
Interference in a Thin Film: Newton’s rings
Analysis Part 1
For small angles (tan) (tan) = (/2) / x
(tan) = (5.893*10-7m )/2 / (6*10-5 m) (tan) = .004
= 0.034 +/- .004 degrees
Interference in a Thin Film: Newton’s rings
Analysis Part 2
Interference in a Thin Film: Newton’s rings
Analysis Part 2
xm2 = xm
2 * (xm/xm)2 + (xm/xm)2
xm2 = xm
2 * 2(xm/xm)2
x12 = (0.062 cm) * 2(0.006/0.248)2
x12 = 0.002
m xr (cm) xl (cm) xm (cm) error xm (cm) xm 2̂ (cm) error xm 2̂ (cm)0 11.9001 11.770 12.018 0.248 0.006 0.062 0.0022 11.721 12.064 0.343 0.006 0.118 0.0033 11.678 12.092 0.414 0.006 0.171 0.0044 11.650 12.124 0.474 0.006 0.225 0.0045 11.618 12.152 0.534 0.006 0.285 0.0056 11.594 12.180 0.586 0.006 0.343 0.0057 11.576 12.202 0.626 0.006 0.392 0.0058 11.550 12.226 0.676 0.006 0.457 0.0069 11.530 12.246 0.716 0.006 0.513 0.00610 11.518 12.260 0.742 0.006 0.551 0.006
Interference in a Thin Film: Newton’s rings
Analysis Part 2Xm^2 versus m
y = 0.0555x + 0.0064
0.000
0.100
0.200
0.300
0.400
0.500
0.600
0 2 4 6 8 10 12
m
Xm
^2 (
cm
^2)
Interference in a Thin Film: Newton’s rings
Used Excel’s LINEST() function to calculate slope and intercept
Slope = 0.0555 +/- 0.0006 Intercept = 0.006 +/- 0.004
0.0555 0.0060.0006 0.004
Interference in a Thin Film: Newton’s rings
Analysis Part 2
xm2 = mR/4 - 2/4
y = 0.0555x + 0.0064 y = mx + b To find 2
- 2/4 = 0.006 2 = -0.024 cm2
2/4 = 0.004 2 = 0.02
2 = -0.02 +/- 0.02 cm2
Interference in a Thin Film: Newton’s rings
Analysis Part 2
xm2 = mR/4 - 2/4
y = 0.0555x + 0.0064 y = mx + b To find R
mR/4 = 0.0555x where x = m = 589.3 nm = 5.893 * 10-5 cm
(5.893 * 10-5 cm)R/4 = 0.0555 R=3.767 * 103 cm
Interference in a Thin Film: Newton’s rings
Analysis Part 2
R/4 = 0.0006 R = 0.0006 * 4 /
R = 0.0006 * 4 / 5.893 * 10-5 cm R = 40 cm
R = 3.77 * 103 +/- 0.04 * 103 cm
Interference in a Thin Film: Newton’s rings
Conclusion
We were able to see how rays of light could interfere causing fringes
Dark fringes: destructive interference Bring fringes: constructive interference Interference explains colours in a thin film
Interference in a Thin Film: Newton’s rings
Conclusion
Measured distance between fringes Able to calculate the thin film’s properties In Part 1 we were able to calculate
= 0.034 +/- .004 degrees In Part 2 we found
2 = -0.02 +/- 0.02 cm2
R = 3.77 * 103 +/- 0.04 * 103 cm
Interference in a Thin Film: Newton’s rings
Conclusion
Errors Error in positioning the travelling microscope over
the same place for each fringe Error in taking measurements from the
micrometer scale Error would arise in Part 1 if the fringes were not
aligned perpendicular to the direction of the travelling microscope
Interference in a Thin Film: Newton’s rings
Conclusion
Experiment could be improved by using a travelling light sensor instead of a
microscope
Interference in a Thin Film: Newton’s rings
Questions?
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