dispersing properties of prism and optical cavity in liquids

50
1

Transcript of dispersing properties of prism and optical cavity in liquids

Page 1: dispersing properties of prism and optical cavity in liquids

1

Page 2: dispersing properties of prism and optical cavity in liquids

Dispersing properties of Prism and optical activity in solutions

Page 3: dispersing properties of prism and optical cavity in liquids

3

Dispersion

• The dependence of wave speed and index of refraction on wavelength is called dispersion.

• Therefore the index of refraction of a material depends on wavelength.

• n decreases with increasing wavelength and decreasing frequency

Page 4: dispersing properties of prism and optical cavity in liquids

4

wavelength in the material is given by

λ = λ0 /namount of dispersion is

large in silicate flint glass

Page 5: dispersing properties of prism and optical cavity in liquids

5

prism

• prism is a transparent optical element with flat, polished surfaces that refract light.• A prism can serve as a dispersive element, a beam splitter and a polarizing device.

Page 6: dispersing properties of prism and optical cavity in liquids

6

History

• On February 6, 1672, Newton presented a classic theory at royal academy

of London in his book opticks• He concluded that white light consisted of a mixture of various colors.

Page 7: dispersing properties of prism and optical cavity in liquids

7

𝜃 𝑖2𝜃 𝑡 1𝜃 𝑖 𝜃 𝑡 2

𝛿

Ray diagram

Page 8: dispersing properties of prism and optical cavity in liquids

8

derivation

t1+ A1 + 90 = 180

i2+ A2 +90 = 180

(t1 +i2) + A1 + A2 =180o (1)

A1+ A2 + A = 1800(2)

comparing (1) n (2) (i1 +i2) = A = i1 +i2- A

𝛿

Page 9: dispersing properties of prism and optical cavity in liquids

9

Using snells law n1sin t2 = n2sini2

i2 = sin-1(n2sint2)

i2 = sin-1(n2sin(A- t1))

i2 = sin-1[n2sinA(n2 – sin2i1)1/2 – cos A sin i1]

=i1 + sin-1[n2sinA(n2 – sin2i1)1/2 – sin i1 cos A] -A𝛿

Page 10: dispersing properties of prism and optical cavity in liquids

10

• Apparently, increases with n. which is itself a function of frequency, so we designate the deviation as (v) or (lambda)𝛿 𝛿

• The smallest value of is known as the minimum deviation. Differentiating Eq. (a) and setting it equal to zero yields

Taking the derivative of Snell's Law at each interface

𝜖 ∀

Page 11: dispersing properties of prism and optical cavity in liquids

11

• Dividing the last two equations and substituting

using of Snell's Law once again

The value ofi1for which this is true is the one for which = 0Inasmuch as n is not = 1, it follows that

Page 12: dispersing properties of prism and optical cavity in liquids

12

And therefor

This means that the ray for which the deviation is a minimum traverses the prism symmetrically, that is, parallel to its base.

Page 13: dispersing properties of prism and optical cavity in liquids

13

Deviation versus incident angle

50

45 n = 1.5 40 A = 600

35 30 40 50 60 70 80i1

Page 14: dispersing properties of prism and optical cavity in liquids

14

Pellin-Broca prism

Page 15: dispersing properties of prism and optical cavity in liquids

15

Conti..

• a single monochromatic ray of wavelength A traverses the component prism DAE symmetrically

• thereafter to be reflected at 45" from face AB• The ray will then traverse prism CDB

symmetrically, having experienced a total deviation of 90".

Page 16: dispersing properties of prism and optical cavity in liquids

16

• The ray can be thought of as having passed through an ordinary 60“ prism (DAE combined with CDB) at minimum deviation

• If the prism is now rotated slightly about an axis normal to the paper, the incoming beam will have a new incident angle.

• A different wavelength component, say AZ, will now undergo a minimum deviation, which is again 90"-hence the name constant deviation.

Page 17: dispersing properties of prism and optical cavity in liquids

17

Abbe prism

Page 18: dispersing properties of prism and optical cavity in liquids

18

• Refractive index can be used as a base for studying the properties of light and deviation of the light and its components.

• This may also find its application various purposes as in case of cars, satellites, aircrafts, appropriate refractive index of glass for the human eye, glass made utensils and many others.

Applications

Page 19: dispersing properties of prism and optical cavity in liquids

Optical activity in liquids

Page 20: dispersing properties of prism and optical cavity in liquids

20

Optical activity

A substance is optically A substance is optically active if it rotates the plane of polarized light.

In order for a substance to exhibit opticalactivity, one enantiomer must be present in excess of the other

Page 21: dispersing properties of prism and optical cavity in liquids

21

Introduction

Any material that causes the E-field of an incident linear plane wave to appear to rotate is said to he optically active .The plane-of-vibration appears to have revolved clockwise, the substance is referred to as dextro-rotatory (from the Latin dextro, meaning right). If E appears to have been displaced counterclockwise, the material is levo-rotatory l-rotatory (from the Latin levo,meaning left)

Page 22: dispersing properties of prism and optical cavity in liquids

22

History

• In 18 1 1 the French physicist Dominique F. J. Arago first observed the phenomenon of optical activity.

• Jean Baptiste Biot (1774-1862) saw this same effect while using both the vaporous and liquid forms of various natural substances. .He for the first time distinguish between right- and left-handed rotation.

• In 1825 Fresnel said that linear wave can be represented as a superposition of R-state and L-states.

Page 23: dispersing properties of prism and optical cavity in liquids

23

Lactic acid

Page 24: dispersing properties of prism and optical cavity in liquids

24

Analine

Page 25: dispersing properties of prism and optical cavity in liquids

25

glucose

Page 26: dispersing properties of prism and optical cavity in liquids

26

Rotation of plane-polarized light

Page 27: dispersing properties of prism and optical cavity in liquids

27

Enantiomorphic substance

The substances having same external appearance but internally they are mirror image of each other such substances are enantiomorphs of each other ,these substances are called enantiomorphic substance

Page 28: dispersing properties of prism and optical cavity in liquids

28

Analytical treatment

Two waves represent R and L state are given by

The final disturbance is given by E=Eocos[(KR+KL)z / 2-ωt][ icos(KR+KL)z /2 +jsin(KR+KL)z / 2]

Page 29: dispersing properties of prism and optical cavity in liquids

29

Conti…..

• At the position where the wave enters the medium (z = 0) it is linearly polarized along the x-axis, that is

E=Eocos ωt i If• nR > nL or equivalently kR > kL,E will rotate

counterclockwise• kL > kR the rotation is clockwise

Page 30: dispersing properties of prism and optical cavity in liquids

30

Diagram

Page 31: dispersing properties of prism and optical cavity in liquids

Measuring the Optical rotation of compounds

Page 32: dispersing properties of prism and optical cavity in liquids

32

Polarimetry♦ Polarimetry is the measurement of the polarization of light

♦ Anisotropic crystalline solids, and samples containing an excess of one enantiomer of a chiral molecule, can rotate the orientation of plane-polarized light. Such substances are said to have optical activity.

♦ Measurement of this change in polarization orientation is called polarimetry, and the measuring instrument is called a polarimeter.

♦ These measurements are useful for studying the structure of anisotropic materials, and for checking the purity of chiral mixtures.

Page 33: dispersing properties of prism and optical cavity in liquids

33

Optical Rotation and Polarimetry

Chiral molecules will rotate polarized light:

monochromatic light source

randomly oriented light

optical polarizer - only allows "vertical" light to pass through

optical polarizer - only allows "horizontal" light to pass through

No light emitted

monochromatic light source

randomly oriented light

optical polarizer - only allows "vertical" light to pass through optical polarizer - only allows "horizontal" light to pass through

chiral material detector

Page 34: dispersing properties of prism and optical cavity in liquids

34

monochromatic light source

randomly oriented light

optical polarizer - only allows "vertical" light to pass through optical polarizer - only allows "horizontal" light to pass through

chiral material detector

monochromatic light source

randomly oriented light

optical polarizer - only allows "vertical" light to pass through

optical polarizer

chiral materialdetector

The maximum signal will be optained if the second polarizer is rotated to match the light rotation:

maximum signal

Optical Rotation and Polarimetry

Page 35: dispersing properties of prism and optical cavity in liquids

35

Rotation of plane-polarized light

Page 36: dispersing properties of prism and optical cavity in liquids

36

Rotation of plane-polarized light

Page 37: dispersing properties of prism and optical cavity in liquids

37

a

Rotation of plane-polarized light

Page 38: dispersing properties of prism and optical cavity in liquids

38

The amount of optical rotation is determined by the molecular structure

and concentration of chiral molecules in the substance by Biot’s Law:

Page 39: dispersing properties of prism and optical cavity in liquids

39

What is a Polarimeter?

♦ Polarimeter is the scientific instrument used to make the polarimetry measurements.

Page 40: dispersing properties of prism and optical cavity in liquids

40

Schematic of a Polarimeter

The simplest polarimeter consists of a monochromatic light source, a polarizer, a sample cell, a second polarizer, which is called the analyzer, and a light detector.If the analyzer is oriented 90o to the polarizer so that no light reaches the detector.

Page 41: dispersing properties of prism and optical cavity in liquids

41

Light: electromagnetic radiation

Optical activity is usually measured using light having a wavelength of 589 nm; this is the wavelength of the yellow light from a sodium lamp and is called the D line of sodium.

Page 42: dispersing properties of prism and optical cavity in liquids

42

Examples

• The direction and magnitude of rotation must be determined experimentally.– There is NO CORRELATION between (R) and (S)

configuration and the direction of rotation.

C

CH3

CH2CH3HHO

C

C

CH3

CH2CH3HHO

HOH

CH3

CH3CH2

(+)-2-butanol (-)-2-butanol+13.5o rotation -13.5o rotation

(S)-(+)-2-butanol (R)-(-)-2-butanol

Page 43: dispersing properties of prism and optical cavity in liquids

43

Examples

(S)-(-)-thyroxinebiologically activeO CH2

CCO2H

HH2NI I

II

HO

O CH2HO

I

I I

IC

CO2H

NH2H

(R)-(+)-thyroxineinactive

O CH2

CCO2H

HH2NI I

II

HO

O CH2HO

I

I I

IC

CO2H

NH2H

Unlike (R)-(-)-2-butanol, (R)-thyroxine rotates light to the right.

Page 44: dispersing properties of prism and optical cavity in liquids

44

Polarimetry Aplications

Research and Technological aplications: • Distinguishing between optical isomers • Isolating and identifying unknowns crystallized from various solvents or

separated by high performance liquid chromatography• Monitoring changes in concentration of an optically active component in a

reaction mixture, as in enzymatic cleavage. • Analyzing molecular structure by plotting optical rotatory dispersion curves

over a wide range of wavelengths. • Investigating kinetic reactions by measuring optical rotation as a function of

time.• Liquid crystal displays and polarized sunglasses.• All radio transmitting and receiving antennas are intrinsically polarized, special

use of which is made in radar.• Polarizing filters are used in photography

Page 45: dispersing properties of prism and optical cavity in liquids

45

Pharmaceutical industry

• Determines product purity by measuring specific rotation and optical rotation of:

· Amino acids

· Amino sugars

·Analgesics

· Antibiotics · Cocaine · Codeine

· Dextrose · Diuretics · Serums

· Steroids •Tranquilizers · Vitamins

Page 46: dispersing properties of prism and optical cavity in liquids

Flavor, Fragrance and Essential Oil Industry

Utilizes polarimetry for materials inspection of:

·Camphors

· Citric acid

· Glyceric acid

· Gums · Lavender oil

· Lemon oil

· Orange oil

·Spearmint oil

46

Page 47: dispersing properties of prism and optical cavity in liquids

Food Industry

Ensures product quality by measuring the concentration and purity of the following compounds in sugar based foods, cereals and syrups:

·Carbohydrates

·Fructose

·Glucose

· Lactose ·Levulose

·Maltose

· Raffinose ·Sucrose ·

Xylose

· Various Starches

· Natural mono-saccharides

47

Page 48: dispersing properties of prism and optical cavity in liquids

Chemical Industry

• Analyzes optical rotation as a means of identifying and characterizing:

Biology:

· Biopolymers · Natural polymers · Synthetic

polymers

48

Page 49: dispersing properties of prism and optical cavity in liquids

49

Medicine

• Research of glucose in urine - Diabetes Mellitus

• Research of albumin in urine - Renal diseases

• Hormone research Analysis of: -steroid hormon -testosterone Enzymology and toxicology research.

Page 50: dispersing properties of prism and optical cavity in liquids

Thank you