Click to Chat
1800-2000-838
+91-120-4616500
CART 0
Use Coupon: CART20 and get 20% off on all online Study Material
Welcome User
OR
LOGIN
Complete Your Registration (Step 2 of 2 )
Live Classes IITIAN Teachers
Unlimited Practice & Doubt Removal
Classes 5 Days/Week 3 Hours/Day
All India Test Series with Analysis
Class Recordings for Revision
WAVE NATURE OF LIGHT Huygens’ Wave Theory Huygen, a Dutch mathematician, in 1678, gave a theory regarding nature of light. The theory is popularly known as Huygen’s wave theory. According to this theory, light is a sort of disturbance. The particles of the medium, vibrate in a direction, at right angle to the direction of propagation of disturbance. The process is called wave motion. Considering light to be a wave-motion following properties of light could be explained: (a) Rectilinear propagation of light (b) Reflection (c) Refraction (d) Interference (e) Diffraction (f) Polarisation Photoelectric effect could not be explained on the basis of this theory. A more serious objection to this theory was regarding the nature of medium, through which the light travels while coming from sun to earth, since major portion of space in between has vacuum. This hurdle was overcome by proposing a hypothetical medium ‘ether’. the properties of ‘ether’ as imagined by the supporters of this theory are self-contradicting. Moreover any attempt to test the presence of this medium has not been successful. The theory was, later on, modified by Max Planck by saying that the source of light does not give out continuous disturbance. Instead, it emits certain packets of energy consisting of vibratory energy. The modified theory is called Planck’s quantum theory and the packet of energy is treated to be the fundamental particle of light known as photon. Huygen’s Principle The following constructions were proposed by Huygen's to explain the wave propagation of light. Primary source – The geometrical center or axis of the actual source of light which is either a point or a line is called the primary source. Wavelets – All points lying on small curved surfaces, that receive light at the same time from the same source (primary or secondary) are called wavelets. Secondary source – Any point on a wavelet, acts as the source of light for further propagation of light. It is called a secondary source. Wave front – The envelope of all wavelets in the same phase- having received light from sources in the same phase at the same time is called a wave front. Wave normal – The normal at any point drawn outward on a wave front is called the wave normal. Further propagation of light occurs along the wave normal. In isotropic media the wave normal coincides with the 'ray of light'. Spherical, cylindrical and plane wave fronts The wave fronts from a point of the primary source are spherical wave fronts. The wave fronts from the line primary source are cylindrical wave fronts. At large distances from the primary source the radius of curvature of the wave fronts is negligibly small. Small portions of such wave points are essentially flat or plane. These are called plane wave fronts. Construction of Wave front Wave-front of a wave, at any instant, is defined as the locus of all the particles in the medium which are being disturbed at the same instant of time and are in the same phase of vibration. How to construct a wave-front at any instant (say t + dt) if a wave-front at a slightly earlier instant (t) is known? The answer is that Huygen’s principle gives us the guide lines to do so. Steps to be followed, in this process, are called the basic postulates of the principle and they are stated below. (a) Consider all the points on a primary wave-front (of instant ‘t’) to be the sources of light, which emit disturbances known as secondary disturbance. (b) Tangent envelope to all the secondary wave-lets gives the position of a new wave-front. Consider a point source ‘S’. Light emitted by ‘S’ travels in all directions. Let AB be a section of the position of wave-front, at any instant, of time ‘t’ as shown in figure. The secondary disturbances emitted by all the points on AB are shown by dotted circles. A_{1}B_{1} and A_{2}B_{2} are the two tangent envelopes touching all these secondary disturbances. According to Stoke’s law, the intensity at each point of the secondary wave is proportional to (1 + cosθ). Here ‘θ’ is angle between normal and central line. For backward wave-front ‘A_{2}B_{2}’ (shown dotted), θ = π So, cosθ = cosπ = -1 Thus, intensity at any point on backward wave = k (1+cosπ) = k (1-1) = 0 Therefore back wave-front does not exist. Hence, ‘A_{1}B_{1}’ which is the forward wave-front gives the position of wave-front at the later instant. Every point on a wave-front may be considered a source of secondary spherical wavelets which spread out in the forward direction at the speed of light. The new wave-front is the tangential surface to all of these secondary wavelets. Straight wave front Huygens's principle applied to a straight wave front. Each point on the wave front emits a semicircular wavelet that moves a distance s=vt. The new wavefront is a line tangent to the wavelets. Huygen’s Refraction Huygens's principle applied to a straight wavefront traveling from one medium to another where its speed is less. The ray bends toward the perpendicular, since the wavelets have a lower speed in the second medium. Huygen’s Reflection Huygens's principle applied to a straight wave front striking a mirror. The wavelets shown were emitted as each point on the wave front struck the mirror. The tangent to these wavelets shows that the new wave front has been reflected at an angle equal to the incident angle. The direction of propagation is perpendicular to the wave front, as shown by the downward-pointing arrows. Refer this video to know more about on, “Huygens’ Wave Theory”
Huygen, a Dutch mathematician, in 1678, gave a theory regarding nature of light. The theory is popularly known as Huygen’s wave theory. According to this theory, light is a sort of disturbance. The particles of the medium, vibrate in a direction, at right angle to the direction of propagation of disturbance. The process is called wave motion. Considering light to be a wave-motion following properties of light could be explained:
(a) Rectilinear propagation of light (b) Reflection (c) Refraction (d) Interference (e) Diffraction (f) Polarisation
Photoelectric effect could not be explained on the basis of this theory. A more serious objection to this theory was regarding the nature of medium, through which the light travels while coming from sun to earth, since major portion of space in between has vacuum. This hurdle was overcome by proposing a hypothetical medium ‘ether’. the properties of ‘ether’ as imagined by the supporters of this theory are self-contradicting. Moreover any attempt to test the presence of this medium has not been successful. The theory was, later on, modified by Max Planck by saying that the source of light does not give out continuous disturbance. Instead, it emits certain packets of energy consisting of vibratory energy. The modified theory is called Planck’s quantum theory and the packet of energy is treated to be the fundamental particle of light known as photon.
The following constructions were proposed by Huygen's to explain the wave propagation of light.
Primary source – The geometrical center or axis of the actual source of light which is either a point or a line is called the primary source.
Wavelets – All points lying on small curved surfaces, that receive light at the same time from the same source (primary or secondary) are called wavelets.
Secondary source – Any point on a wavelet, acts as the source of light for further propagation of light. It is called a secondary source.
Wave front – The envelope of all wavelets in the same phase- having received light from sources in the same phase at the same time is called a wave front.
Wave normal – The normal at any point drawn outward on a wave front is called the wave normal. Further propagation of light occurs along the wave normal. In isotropic media the wave normal coincides with the 'ray of light'.
Spherical, cylindrical and plane wave fronts
The wave fronts from a point of the primary source are spherical wave fronts. The wave fronts from the line primary source are cylindrical wave fronts.
At large distances from the primary source the radius of curvature of the wave fronts is negligibly small. Small portions of such wave points are essentially flat or plane. These are called plane wave fronts.
Wave-front of a wave, at any instant, is defined as the locus of all the particles in the medium which are being disturbed at the same instant of time and are in the same phase of vibration.
How to construct a wave-front at any instant (say t + dt) if a wave-front at a slightly earlier instant (t) is known?
The answer is that Huygen’s principle gives us the guide lines to do so. Steps to be followed, in this process, are called the basic postulates of the principle and they are stated below.
(a) Consider all the points on a primary wave-front (of instant ‘t’) to be the sources of light, which emit disturbances known as secondary disturbance.
(b) Tangent envelope to all the secondary wave-lets gives the position of a new wave-front.
Consider a point source ‘S’. Light emitted by ‘S’ travels in all directions. Let AB be a section of the position of wave-front, at any instant, of time ‘t’ as shown in figure. The secondary disturbances emitted by all the points on AB are shown by dotted circles. A_{1}B_{1} and A_{2}B_{2} are the two tangent envelopes touching all these secondary disturbances.
According to Stoke’s law, the intensity at each point of the secondary wave is proportional to (1 + cosθ). Here ‘θ’ is angle between normal and central line.
For backward wave-front ‘A_{2}B_{2}’ (shown dotted), θ = π
So, cosθ = cosπ = -1
Thus, intensity at any point on backward wave = k (1+cosπ) = k (1-1) = 0
Therefore back wave-front does not exist.
Hence, ‘A_{1}B_{1}’ which is the forward wave-front gives the position of wave-front at the later instant.
Every point on a wave-front may be considered a source of secondary spherical wavelets which spread out in the forward direction at the speed of light. The new wave-front is the tangential surface to all of these secondary wavelets.
Straight wave front
Huygens's principle applied to a straight wave front. Each point on the wave front emits a semicircular wavelet that moves a distance s=vt. The new wavefront is a line tangent to the wavelets.
Huygen’s Refraction
Huygens's principle applied to a straight wavefront traveling from one medium to another where its speed is less. The ray bends toward the perpendicular, since the wavelets have a lower speed in the second medium.
Huygen’s Reflection
Huygens's principle applied to a straight wave front striking a mirror. The wavelets shown were emitted as each point on the wave front struck the mirror. The tangent to these wavelets shows that the new wave front has been reflected at an angle equal to the incident angle. The direction of propagation is perpendicular to the wave front, as shown by the downward-pointing arrows.
Diffraction is the concept that is explained using Huygens's Principle, and is defined as the bending of a wave around the edges of an opening or an obstacle.
This principal can be used to define reflection, as shown in the figure. It can also be used to explain refraction and interference. Anything the experiences this phenomenon is a wave. By applying this therory to light passing through a slit, we can prove it is a wave.
From Huygen's construction we learn that while the medium is homogeneous (i.e., optical properties of the medium are same everywhere) light moves forward and does not reflect back.
We also assume that the secondary wavelets are emitted only in forward direction i.e., in the direction of advancement of the wave.
If there is a sudden obstruction or charge in medium as discussed below, the wave may be reflected from the discontinuity. The secondary wavelets on the backward side should also be considered.
Two waves of same frequency and same amplitude from two monochromatic sources are allowed to suppose at a certain point. If in one case the phase difference is 0º and in other case is π/2. Then find the ratio of the intensities in the two cases.
As, A_{1} = 2A
So, I_{1} = 4I
A_{2} = √2A
Thus, I_{2} = 2I
Therefore, I_{1}/I_{2} = 2/1
Thus from the above observation we conclude that, the ratio of the intensities in the two cases would be 2/1.
Many phenomena in Modern Physics such as Photo-electric effect, Compton effect, etc. could not be explained by wave theory.
The propagation of waves through vacuum could not be accounted for, hence a hypothetical medium called ether was assumed to be present. However, the presence of ether could not be detected. It was experimentally shown that medium like ether does not exist.
(a) interference (b) diffraction
(c) photoelectric effect (d) polarisation
Light appears to travel in straight lines since
(a) it is not absorbed by the atmosphere
(b) It is reflected by the atmosphere
(c) its wavelength is very small
(d) its velocity is very large
When light travels from an optically rare medium to optically denser medium, the velocity decreases because of change in
(a) wavelength (b) frequency
(c) amplitude (d) phase
The transverse nature of light is shown by
(a) interference of light (b) refraction of light
(c) polarization of light (d) dispersion of light
Which of the following does not support the wave nature of light.
(c) polarisation (d) photoelectric effect
c
a
You might like to Young’s Double slit Experiment.
For getting an idea of the type of questions asked, refer the Previous Year Question Papers.
Click here to refer the most Useful Books of Physics.
To get answer to any question related to wave nature of light click here.
Signing up with Facebook allows you to connect with friends and classmates already using askIItians. It’s an easier way as well. “Relax, we won’t flood your facebook news feed!”
Post Question
Dear , Preparing for entrance exams? Register yourself for the free demo class from askiitians.
DIFFRACTION Diffraction Sound is propagated in the...
YOUNG’S DOUBLE SLIT EXPERIMENT Conditions...
POLARISATION Polarisation The phenomena of...
Questions and Solutions part 2 11. Angular width...
Questions and Solutions part 3 1. When light is...
INTERFERENCE BY THIN FILM Colours of thin films...
Questions and Solutions Part 1 1. In Young's...
Displacement of Fringes When a film of...