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newton rings

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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
Transcript
Page 1: newton rings

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

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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

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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

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Interference in a Thin Film: Newton’s rings

Theory

When waves interfere constructively:

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Interference in a Thin Film: Newton’s rings

Theory

When waves interfere destructively:

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Interference in a Thin Film: Newton’s rings

Theory

When waves interfere destructively:

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Interference in a Thin Film: Newton’s rings

Theory Part 1

Diagram from Physics 294 Laboratory Manual, page 17-2

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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

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Interference in a Thin Film: Newton’s rings

Theory Part 2

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Interference in a Thin Film: Newton’s rings

Theory Part 2

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Interference in a Thin Film: Newton’s rings

Theory Part 2

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Interference in a Thin Film: Newton’s rings

Theory Part 2

Diagrams from Physics 294 Laboratory Manual, page 17-3

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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

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Interference in a Thin Film: Newton’s rings

Apparatus

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Interference in a Thin Film: Newton’s rings

Apparatus

Diagram from Physics 294 Laboratory Manual, page 17-2

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Interference in a Thin Film: Newton’s rings

Procedure

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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

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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

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Interference in a Thin Film: Newton’s rings

Analysis

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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

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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)”

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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

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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

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Interference in a Thin Film: Newton’s rings

Analysis Part 2

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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

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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)

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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

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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

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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

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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

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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

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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

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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

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Interference in a Thin Film: Newton’s rings

Conclusion

Experiment could be improved by using a travelling light sensor instead of a

microscope

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Interference in a Thin Film: Newton’s rings

Questions?

Additional pictures at www.goldenratio.ca


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