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DIFRACTION GRATINGS-use double slit formula

DIFRACTION-Double slit

antinodal โ€“ bright band

๐‘บ๐Ÿ๐‘ทโˆ’ ๐‘บ๐Ÿ๐‘ท = ๐’๐€

๐‘›๐œ† = ๐‘‘ sin๐œƒ ๐‘œ๐‘Ÿ sin๐œƒ =๐‘›๐œ†

๐‘‘

๐‘–๐‘“ ๐œƒ ๐‘–๐‘  ๐‘ ๐‘š๐‘Ž๐‘™๐‘™ ๐‘กโ„Ž๐‘’๐‘›โ€” sin๐œƒ = tan๐œƒ

๐ป๐‘’๐‘›๐‘๐‘’ ๐‘ฅ = ๐ฟ sin๐œƒ ๐‘œ๐‘Ÿ sin๐œƒ =๐‘ฅ

๐ฟ

โˆด ๐’๐€

๐’…=๐’™

๐‘ณ

nodal โ€“ dark band

๐‘บ๐Ÿ๐‘ท โˆ’ ๐‘บ๐Ÿ๐‘ท = (๐’ โˆ’ ๐Ÿ ๐Ÿ )๐€

โˆด (๐‘› โˆ’ 1

2 )๐€

๐’…=๐’™

๐‘ณ

๐‘บ๐Ÿ๐‘ท = number of wave lengths from original1

๐‘บ๐Ÿ๐‘ท = number of wave lengths from original2

n = the number of waves from the original

๐›‰ = the angle for the 1st bright band

x = distance to 1st bright band

L = distance to screen where is being projected

d = distance between slits

WIDTH OF CENTRAL MAXIMUM

๐‘Š๐‘–๐‘‘๐‘กโ„Ž ๐‘œ๐‘“ ๐‘๐‘’๐‘›๐‘ก๐‘Ÿ๐‘Ž๐‘™ ๐‘š๐‘Ž๐‘ฅ =๐‘ณ๐€

๐’…

๐‘ณ โ†‘ ๐‘ฟ โ†‘ ๐‘ฟ โ†“ ๐‘ณ โ†“ ๐’… โ†‘ ๐‘ฟ โ†“ ๐‘ฟ โ†‘ ๐’… โ†“

๐‘ถ๐’“๐’…๐’†๐’“ ๐’๐’‡ ๐’•๐’‰๐’† ๐’๐’‚๐’”๐’• ๐’ƒ๐’“๐’Š๐’ˆ๐’‰๐’• ๐’‡๐’“๐’Š๐’๐’ˆ๐’† ๐’Š๐’” ๐’˜๐’‰๐’†๐’“๐’† ๐œฝ = ๐Ÿ—๐ŸŽยฐ

๐‘จ๐‘ต๐‘ฎ๐‘ผ๐‘ณ๐‘จ๐‘น ๐‘ซ๐‘ฌ๐‘ฝ๐‘ฐ๐‘จ๐‘ป๐‘ฐ๐‘ถ๐‘ต = ๐ฌ๐ข๐ง ๐œฝ โˆ’ ๐ฌ๐ข๐ง ๐œฝ

DIFRACTION-Single slit

Nodal -- Dark Band

๐‘›๐œ† = ๐‘ค sin๐œƒ ๐‘œ๐‘Ÿ sin๐œƒ =๐‘›๐œ†

๐‘ค

๐‘–๐‘“ ๐œƒ ๐‘–๐‘  ๐‘ ๐‘š๐‘Ž๐‘™๐‘™ ๐‘กโ„Ž๐‘’๐‘›โ€” sin๐œƒ = tan๐œƒ

๐ป๐‘’๐‘›๐‘๐‘’ ๐‘ฆ = ๐ฟ tan๐œƒ ๐‘œ๐‘Ÿ sin๐œƒ =๐‘ฆ

๐ฟ

This is the formula for 1st dark band

โˆด n=1

โˆด ๐’๐€

๐’˜=๐’š

๐‘ณ ๐’๐’“ ๐’๐€ =

๐’˜๐’š

๐‘ณ

๐’š = ๐‘ณ๐€

๐’˜

Antinodal -- Bright Band

โˆด (๐’+ ๐Ÿ ๐Ÿ )๐€

๐’˜=๐’š

๐‘ณ ๐’๐’“ (๐’โˆ’ ๐Ÿ ๐Ÿ )๐€ =

๐’˜๐’š

๐‘ณ

๐’š = ๐‘ณ(๐’ + ๐Ÿ ๐Ÿ )๐€

๐’˜

๐›‰ = the angle for the 1st dark band

y = distance to 1st bright band

L = distance to screen where is being projected

w = distance between slits

WIDTH OF CENTRAL MAXIMUM

๐‘Š๐‘–๐‘‘๐‘กโ„Ž ๐‘œ๐‘“ ๐‘๐‘’๐‘›๐‘ก๐‘Ÿ๐‘Ž๐‘™ ๐‘š๐‘Ž๐‘ฅ =๐Ÿ๐‘ณ๐€

๐’˜

WIDTH OF 1ST ORDER BRIGHT FRINGE

(HALF WIDTH OF CENTRAL MAXIMUM)

๐‘Š๐‘–๐‘‘๐‘กโ„Ž =๐‘ณ๐€

๐’˜

--------------------------------------------

For a biconvex lens

๐’‡ =๐’“

๐Ÿ(๐’ โˆ’ ๐Ÿ)

PERIOD T of motion of light spring (where mass

of spring is negligible)

๐‘ป = ๐Ÿ๐… ๐’Ž

๐’Œ

Displacement (x) SI UNIT=metres

Distance from equilibrium

Equilibrium (c)

Amplitude (a) SI UNIT=metres

Max displacement from equilibrium

sometimes reffered to as wave height

Large (a) suggests large amount of energy

Period (T) SI UNIT=seconds

Time it takes to complete 1 oscillation

Time to complete 1 cycle of vibration

๐‘ป = ๐Ÿ

๐’‡

Frequency (f) SI UNIT=Hz

No. of oscillations per second

No. of cycles of vibration per second

๐’‡ = ๐Ÿ

๐‘ป ๐’‡ =

๐’—

๐€

Wavelength (ื’) SI UNIT=metres

Minimum distance between 2 points in phase

ื’ =๐’—

๐’‡

V = speed of the wave (constant) SI m/s

๐’— =๐’…

๐’• ๐‘ฝ = ๐’‡ ๐’—ื’ =

๐Ÿ๐€

๐‘ป

IF FREQUENCY REMAINS UNCHANGED

(as it generally does)

ื’2

ื’1

=๐‘ฃ2

๐‘ฃ1

Reflection of pulses

Boundary Reflected Pulse Transmitted

Pulse

Fixed end Out of phase ---

Free end In phase ---

Light to heavy

medium

Out of phase In phase

Heavy to light medium

In phase Out of phase

Mark Riley [email protected]

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