optics formula sheet study sheet physicsa 2010

1
DENSER MEDIUM=increased speed Depth Shallow Deep Wavelength Short Long Speed Slow Fast REFLECTION Angle of incidence =Angle of Refration REFRACTION (transmission) 2 1 = 2 1 1 = (1) Direction of propagation the direction in which the energy is travelling Wavelength distance between to poimts in phase distance between 2 successive crests Typical tranverse wave DIVERGING-CONVEX ALWAYS-Virtual, Erect, Smaller than object Behind mirror between F and V Di or f is negative CONCAVE-CONVERGING A: Real, Inverted, Smaller, Between C and F B: Real, Inverted, Same size as object, At C C: No image, Reflected rays are parallel D: Virtual, Erect, Larger than object, Behind mirror = Χ’1 Χ’2 = 1 2 = 1 2 = = 1 Γ— sin = 2 Γ— sin = = = ( ) = = = = = = DENSER MEDIUM=bends toward the normal and slower speed for electromagnetic waves CONVEX-bi convex-CONVERGING c. Magnified, inverted, real, D i is pos, f is pos d. Magnified, upright, virtual, D i is neg, f is pos As an object moves toward F the image increases in size CONCAVE-bi concave-DIVERGING a. Diminished, upright, virtual, D i is neg, f is neg b. Diminished, upright, virtual, D i is neg, f is neg All measurements are made from the optical centre of the lens = + = ( βˆ’) = ( βˆ’) = Γ— ( + ) = = Optical power/ Lens Power = = = = = = = = Critical Angle-Denser medium to lighter medium Medium to air = = = = = = = = = β†’β†’β†’β†’β†’β†’ Wavelengths decrease Refracts more critical angle decreases frequency increases Wavelength of light in a denser medium = For string with mass(m) and length(L) under tension(F), the speed of the wave is given by = Mark Riley [email protected]

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Optics formula sheet- basic as this subject is at this point. Has plenty of diagrams missing lenzmakers equation for some reason I forgot to put him on

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Page 1: Optics Formula Sheet study sheet PhysicsA 2010

DENSER MEDIUM=increased speed

Depth Shallow Deep Wavelength Short Long

Speed Slow Fast

REFLECTION

Angle of incidence =Angle of Refration

REFRACTION (transmission)

π‘ π‘–π‘›πœƒ2

π‘ π‘–π‘›πœƒ1=𝑣2

𝑣1

π‘ π‘–π‘›πœƒ1 = π‘Žπ‘›π‘”π‘™π‘’ π‘œπ‘“ 𝑖𝑛𝑐𝑖𝑑𝑒𝑛𝑐𝑒 (1𝑠𝑑)

Direction of propagation

the direction in which the energy is travelling

Wavelength

distance between to poimts in phase

distance between 2 successive crests

Typical tranverse wave

DIVERGING-CONVEX

ALWAYS-Virtual, Erect, Smaller than object

Behind mirror between F and V

Di or f is negative

CONCAVE-CONVERGING

A: Real, Inverted, Smaller, Between C and F

B: Real, Inverted, Same size as object, At C

C: No image, Reflected rays are parallel

D: Virtual, Erect, Larger than object, Behind mirror

π·π‘‘π·π‘Ž

=Χ’

1

Χ’2

=𝑣1

𝑣2=π‘ π‘–π‘›πœƒ1

π‘ π‘–π‘›πœƒ2=𝐢

𝑣= 𝑛𝐴

𝑛𝐴1 Γ— sin 𝜽𝟏 = 𝑛𝐴2 Γ— sin 𝜽𝟐

𝜽𝟏 = 𝑖𝑛𝑐𝑖𝑑𝑒𝑛𝑑 π‘Žπ‘›π‘”π‘™π‘’

𝜽𝟐 = π‘Ÿπ‘’π‘“π‘Ÿπ‘Žπ‘π‘‘π‘’π‘‘ π‘Žπ‘›π‘”π‘™π‘’

π‘ͺ = 𝑠𝑝𝑒𝑒𝑑 π‘œπ‘“ 𝑙𝑖𝑔𝑕𝑑 𝑖𝑛 π‘£π‘Žπ‘π‘’π‘’π‘š(π‘Žπ‘–π‘Ÿ)

𝒗 = 𝑠𝑝𝑒𝑒𝑑 π‘œπ‘“ 𝑙𝑖𝑔𝑕𝑑 𝑖𝑛 π‘‘π‘•π‘Žπ‘‘ π‘π‘Žπ‘Ÿπ‘‘π‘–π‘π‘’π‘™π‘Žπ‘Ÿ π‘šπ‘’π‘‘π‘–π‘’π‘š

𝒏𝑨 = π΄π‘π‘ π‘œπ‘™π‘’π‘‘π‘’ π‘Ÿπ‘’π‘“π‘Ÿπ‘Žπ‘π‘‘π‘–π‘£π‘’ 𝑖𝑛𝑑𝑒π‘₯ π‘œπ‘“ π‘‘π‘•π‘Žπ‘‘ π‘šπ‘’π‘‘π‘–π‘’π’Ž

π’—πŸ = 𝑆𝑝𝑒𝑒𝑑 π‘œπ‘“ 𝑙𝑖𝑔𝑕𝑑 𝑖𝑛 π‘“π‘–π‘Ÿπ‘ π‘‘ π‘šπ‘’π‘‘π‘–π‘’π‘š

π’—πŸ = 𝑆𝑝𝑒𝑒𝑑 π‘œπ‘“ 𝑙𝑖𝑔𝑕𝑑 𝑖𝑛 π‘ π‘’π‘π‘œπ‘›π‘‘ π‘šπ‘’π‘‘π‘–π‘’π‘š

𝑫𝒕 = π‘‡π‘Ÿπ‘’π‘’ 𝑑𝑒𝑝𝑑𝑕

𝑫𝒂 = π΄π‘π‘π‘Žπ‘Ÿπ‘’π‘›π‘‘ 𝑑𝑒𝑝𝑑

DENSER MEDIUM=bends toward the normal and

slower speed for electromagnetic waves

CONVEX-bi convex-CONVERGING

c. Magnified, inverted, real, Di is pos, f is pos

d. Magnified, upright, virtual, Di is neg, f is pos

As an object moves toward F the image increases in size

CONCAVE-bi concave-DIVERGING

a. Diminished, upright, virtual, Di is neg, f is neg

b. Diminished, upright, virtual, Di is neg, f is neg

All measurements are made from the optical centre of

the lens

𝟏

𝒇=𝟏

𝒅𝒐+𝟏

π’…π’Š

π’…π’Š =𝒇𝒅𝒐

(𝒅𝒐 βˆ’ 𝒇)

𝒅𝒐 =π’‡π’…π’Š

(π’…π’Š βˆ’ 𝒇)

𝒇 =π’…π’Š Γ— 𝒅𝒐

(𝒅𝒐 + π’…π’Š)

𝑴 =π’…π’Šπ’…π’

=π’‰π’Šπ’‰π’

Optical power/ Lens Power 𝟏

𝒇

π’…π’Š = 𝒅𝒗 = 𝒗 = π’…π’Šπ’”π’•π’‚π’π’„π’† 𝒐𝒇 π’Šπ’Žπ’‚π’ˆπ’†

𝒅𝒐 = 𝒅𝒖 = 𝒖 = π’…π’Šπ’”π’•π’‚π’π’„π’† 𝒐𝒇 𝒐𝒃𝒋𝒆𝒄𝒕

π’‰π’Š = π’‰π’†π’Šπ’ˆπ’‰π’• 𝒐𝒇 π’Šπ’Žπ’‚π’ˆπ’†

𝒉𝒐 = π’‰π’†π’Šπ’ˆπ’‰π’• 𝒐𝒇 𝒐𝒃𝒋𝒆𝒄𝒕

Critical Angle-Denser medium to lighter medium

Medium to air 𝐬𝐒𝐧 πœ½π’„ =𝟏

𝒏𝑨𝒉

π¬π’π§πœ½π’‰π¬π’π§πœ½π‘³

= 𝒏𝒓 = π¬π’π§πœ½π’„ =𝒏𝑨𝑳𝒏𝑨𝒉

𝐬𝐒𝐧 πœ½π’‰ = π‘Žπ‘›π‘”π‘™π‘’ π‘œπ‘“ π‘•π‘’π‘Žπ‘£π‘–π‘’π‘Ÿ π‘šπ‘’π‘‘π‘–π‘’π‘š

𝐬𝐒𝐧 πœ½π‘³ =π‘Žπ‘›π‘”π‘™π‘’ π‘œπ‘“ π‘™π‘–π‘”π‘•π‘‘π‘’π‘Ÿ π‘šπ‘’π‘‘π‘–π‘’π‘š

𝒏𝒓 = π‘…π‘’π‘™π‘Žπ‘‘π‘–π‘£π‘’ π‘Ÿπ‘’π‘“π‘Ÿπ‘Žπ‘π‘‘π‘–π‘£π‘’ π‘Žπ‘›π‘”π‘™π‘’

𝒏𝑨𝑳 = π‘Žπ‘π‘ π‘œπ‘’π‘™π‘’π‘‘π‘’ π‘Ÿπ‘’π‘“π‘Ÿπ‘Žπ‘π‘‘π‘–π‘£π‘’ 𝑖𝑛𝑑𝑒π‘₯ π‘œπ‘“ π‘™π‘–π‘”π‘•π‘‘π‘’π‘Ÿ π‘šπ‘’π‘‘π‘–π‘’π‘š

𝒏𝑨𝒉 = π‘Žπ‘π‘ π‘œπ‘’π‘™π‘’π‘‘π‘’ π‘Ÿπ‘’π‘“π‘Ÿπ‘Žπ‘π‘‘π‘–π‘£π‘’ 𝑖𝑛𝑑𝑒π‘₯ π‘œπ‘“ π‘•π‘’π‘Žπ‘£π‘–π‘’π‘Ÿ π‘šπ‘’π‘‘π‘–π‘’π‘š

𝐑 β†’ 𝐎 β†’ 𝐘 β†’ 𝐆 β†’ 𝐁 β†’ 𝐈 β†’ 𝐕

Wavelengths decrease

Refracts more

critical angle decreases

frequency increases

Wavelength of light in a denser medium

𝝀𝒉 =𝝀𝑨𝒏𝒉

For string with mass(m) and length(L) under

tension(F), the speed of the wave is given by

𝑽 = 𝑭𝑳

π’Ž

Mark Riley

[email protected]