Showing posts with label Light. Show all posts
Showing posts with label Light. Show all posts

Normal Shift and Lateral Shift due to Refraction of Light

Normal shift

When the object and the observer are in two different media,the image of the object appears like shifted from original position and it is called normal shift.

In this case we have to imagine the object in one medium and the observer in the other media. When we are seeing the object normally, image appears different from the position of the object. This is called normal shift.

When the object is in the denser medium and observer is in the rarer medium the first case is discussed.

When the light Ray moves from the object towards the observer, it has to move from wherever medium to denser medium. As it is moving from denser medium to rarer medium, it moves away from the normal and angle of refraction is more than that of the angle of incidence. Therefore for the observer the object appears nearer to the surface. This we can notice even in the real life also. If a coin is placed in a glass of water, for a human eye the coil appears nearer than where it is.

Similarly when the object is in the rarer medium and observer is in the denser medium it appears away from its original position and hence apparent height is more than that of the real height.



In both these cases we had calculated the shift of the image as shown.When the object is the denser medium,the image appears nearer to the surface and vice-versa.

Lateral shift on passing through a glass slab

Let us consider a light ray passing through a glass slab of certain thickness t. There is a change of the medium in this case twice. When the light Ray is entering from a into the glass slab it moves towards the normal. Again when it is moving away from the glass slab into the air it moves towards the normal.

This is happening as per the laws of refraction. According to the law when the light Ray is moving from rarer medium to denser medium it has to move towards the normal and vice versa.

After two reflections, it is quite possible that the emergent light Ray is parallel to the incident light Ray. The perpendicular distance between the two light rays within the glass slab is called lateral shift. We can determine the value of the lateral shift in terms of the thickness of the glass slab, angle of incidence and angle of refraction as shown below. Here we have used basic trigonometric definitions to get the required proof.



Problem and solution on normal shift

A mark at the bottom of a liquid appears to be rise by 0.1 m. The depth of the liquid is one meter. What is the refractive index of the liquid with respect to vacuum?

The object is in the denser medium and observer is in the rarer medium. As the light ray is passing from the denser medium rarer medium it moves towards the normal. Therefore for the observer the coin appears nearer to the surface by a given value. What is given in the problem means the apparent shift in the path with respect to the normal direction. Basing on definition and the derivation that we made in the previous post we can derive the equation and solve the problem as shown below.



The above diagram is also having one more problem.

A underwater swimmer is at a depth of 12 meter from the surface of water. The bird is at a height of 18 meter from the surface of water directly about his eyes. At what totally height does the swimmer locates the bird?

Here swimmer is the observer and the birdies the object. As the observer is in the rarer medium and the object is in the denser medium, for the observer object appears for than where it is. Using the concept of apparent shift we can solve the problem as shown above.

Problem one lateral shift




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Problems and solutions on Refraction of Light

Problem and solution

In the following attracted paper two problems are solved. Both of them depend on the basics of definition of effective index.

There are helpful in calculating the refractive index of one medium with the other medium and in calculating the velocity of the lighting a medium basing on the value of refractive index.

We can define velocity of the light in any medium as ratio of velocity of the light in the vacuum to the refractive index of the medium.



Again we are going to solve to more problems basing on the concept of refractive index and its definition.

Being the light travelling in the form of a straight line with can write the displacement is the product of velocity and time.

In the place of the velocity of the medium we can write the ratio of the last of the light is a vacuum to the refractive index of the medium.



In solving the second problem that is attached, we are going to follow a little bit different approach. It is given in the problem that in two different media with two different thickness number of the waves are same. We know that each wave consists of a particular lent is called wavelength. As the wave spreads over the entire thickness, we can say the total thickness of medium is the product of   certain number of the waves multiplied by the wavelength.



Problem and solution

A Ray of light entering from air to glass is partly reflected and partly refracted. If the reflected and the reflected light rays are at right angles to each other, it is the angle of reflection?

We can solve the problem as shown below. We are simply taking the basic mathematics and the definition of the refractive index into consideration while we are solving the problem.




The above attached paper consists of another problem also. It is based on angle of deviation. When there is no change of the medium, light will continue in its path without any deviation. When there is a change of the medium it will refract. As angle of incidence is different from angle of refraction and there is a change in the path of the light Ray. The difference between angle of incidence to angle of refraction is called angle of deviation. Again by applying the Snell’s law, we can solve the above problem.


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Refraction of Light and Snell's Law

The phenomena of the light going into the other medium after striking a boundary separating the two media is called refraction.

When a light travels from one medium to another medium, its speed and wave length will change. But the frequency of the light is not going to change even when the medium is changed. It is just because frequency is the characteristic property of the source and it is independent of the medium. Frequency can be changed only when the source is changed.

The direction of the propagation of the light also changes when the light changes its medium. The phenomenon of transmission of light from one medium to another with the change in speed is called refraction.

Refraction at a plain surface

The reflected light will change its path as per the change of the medium.

When a light rays moving from a rarer medium to denser medium it moves towards from the normal. It means angle of incidence is more than angle of refraction.

When a light rail is moving from denser medium to rarer medium, it moves away from the normal. In this case angle of refraction is more than angle of incidence.

In the following diagram the path followed by the light on the angle of deviation is shown.



Laws of refraction

The incident ray, reflected ray and the normal lies in the same plane.

During refraction the ratio of sin angle of incidence to the sin angle of the fraction remains constant for a given pair of media and for a given wavelength. This la is called Snell’s law.

This ratio is also called refractive index. This refractive index is defined for a pair of media. When no second medium is given by default, it can be understood that the second medium is vacuum.

The ratio is the refractive index of the second medium to where the light is going with respect to refractive index of the first medium from where the light is coming.
The angle of incidence shall be taken in the first medium from where the light is coming and angle of refraction shall be taken in the second medium to where the light is going.

Being frequency is constant, the ratio of refractive indices can be written in the inversely proportional to the velocity of the light in the corresponding media. It is simply because if the refractive index is more velocity of the light is less in that medium and vice versa.

If the second medium is taken as vacuum than the refractive index is called a absolute refractive index of the medium.



If the light is taking equal time in travelling different distances in different medium, then we can prove that the product of refractive index in the distance is constant. It is proved in the following diagram.

If the light travels same distance into different media into different times then we can prove that the time taken to travel is directly proportional to refractive index.

Refraction doesn't takes place if angle of incidence and angle of refraction are equal to 0.
Refraction don’t takes place when the two mediums are having same refractive index that means there shall be a change in the media for the reflection to takes place.

Optical path is defined as the distance traveled by the light in vacuum in the same time in which the travels in a medium.




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Problems and Solutions on Refraction of Light

Problem and solution

A 2 cm high object is placed on the principal axis of a concave mirror at a distance of 12 cm from the pole. If the image is inverted, real and 5 cm in height, find the location of the image and the focal length of the mirror?

We can solve this problem basing on the very definition of magnification and the mirror formula. Magnification is defined as the ratio of height of the image to the height of the object. The other way of defining the magnification is as the ratio of distance of the image to the distance of the object. The sign of the magnification is negative which means that object and image are in the different directions. The problem is solved as shown below.



An object is placed in the principal axis of a concave mirror at a distance X  from a principal focus. The images formed at a distance Y the focus. What is the focal length of the mirror ?

This problem also has to be solved basing on the mirror formula. Being both object and the major place to before the mirror they shall be treated as negative and a concave mirror focal length is also negative.The solution is shown in the above diagram.

Problem and solution

An object is placed in front of a concave mirror at a distance of 50 cm. A plain mirror is introduced covering the lower half of a convex mirror. The distance between the object and the plain mirror is 30 cm. It is found that there is no gap between the image formed by the two mirror. Then what is the radius of curvature of the convex mirror?

In the problem object is placed at a distance of 50 cm from a concave mirror. Between the object and the mirror at a distance 30 cm from the object a plain mirror is placed. That means the plain mirror is a distance of 20 cm from the convex mirror. The image of the object due to the plain mirror will be farmed again at the 30 cm as a virtual image in the backward direction as shown. And hence it is going to be 10 cm behind the convex mirror.

The same shall be the image of the convex mirror also as it is given in the problem that both the images are coinciding with each other.

Therefore we know that the object is in front of the mirror at a distance of 50 cm and the image is behind the concave mirror at a distance of 10 cm and using the mirror formula we can calculate the focal as shown below.



Problem and solution

Two blocks each of mass m lies on a smooth table. They are attracted to the two other masses as shown. The pullies are straight and light. An object to is kept on the table as shown. The surfaces of the two blocks are made are reflecting surfaces. Find the acceleration of the two images by the two reflecting surfaces with respect to each other?

We shall try equations of motion using Newton’s laws. We shall draw  free body diagram and identify the direction of motion. The forces along the direction of motion shall be treated as positive and vice versa. As shown in the below diagram, we can write the equations of motion and derive acceleration of the individual images.

As per the law of optics, the acceleration of the image is twice the acceleration of the mirror.

As the two images are moving in the opposite direction, we can calculate the relative acceleration is the sum of the two accelerations.




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Sign Convention and Image Tracing of Light in Ray Optics

Sign convention

We shall follow certain sign convention in measuring the distances while we are solving the problems are dealing the concepts in Ray optics.

For the sign convention, pole is taken as the origin and the principal axis as the x-axis.
We shall assume that light is always coming from left to right in the given diagram.

All the distances are measured from the pole.

If the distance of the object is measured along the direction of the incident light, it shall be treated like a positive.

If the distance of the object is measured against the direction of incident light, then it is treated as negative.

The same rules are valid even when we are measuring the distance of the image.

The heights measured upward normal to the principal axis are treated as positive and the height measured in the downward direction is treated as negative.

Focal length and the radius of curvature for a convex mirror are treated as positive and for a concave mirror they are treated as negative. It is simply because these values, when measured from the pole appear along the same direction of the incident light as shown in the diagram below.



Image tracing

When a point object is placed before a spherical mirror, a point images formed. The point of intersection of the incident rays is called object and the point of intersection of reflected light rays is called image.

To measure object distance, image distance, focal length and radius of curvature we need to follow certain sign convention. If the reflected light rays intersect with each other, then at the point of intersection is the place a real images formed. If the reflected light rays diverged from the surface of the reflection, the image is a virtual image. It is going to form at the point from where these light rays are appearing like diverging.
Basing on the sign convention we can take their values as positive or negative as shown in the diagram below.



Problem and solution

A rod of length 10 cm lies along the principal axis of a concave mirror of focal length 10 cm in such a way that its one end close to the pole is 20 cm away from the mirror. What is the length of the image formed in this case?

We have to solve this problem in  two different parts. Let us consider the rod as combination of two points where one is the starting point and other one is the ending point.

We can apply mirror formula for both the points with appropriate sign convention as shown below.



Radius of curvature is numerically double to the value of the focal length. Basing on the values of object distance, image distance and the focal length of a mirror, we can derive a relation for magnification. Magnification is simply defined as the ratio of heat of the image to the height of the object. It can be also defined as the ratio of image distance to the object distance.

Relation between them can be shown as



Problem and solution

An object is placed on the principal axis of a concave mirror of focal length 10 cm at a distance 8 cm from the pole. Find the position and the nature of the image?

While solving this problem, we shall apply the proper sign convention. Being the mirror is a concave mirror; its focal length is negative.

Object is placed before the concave mirror as shown. As the object distance is measured from the pole which is against the direction of the incident light Ray, it shall be treated as negative. We don’t know the value of the image location therefore we are not going to assign any specific sign to it. We will take it as it there in the formula and basing an answer will conclude that what is the location and the nature of the image is.
As for the formula it can be identified that the image distances +40 cm. It means that it is developed at the other end of the mirror and then only can be treated as positive. It means the image is a virtual image.



Problem and solution

The above diagram is having another problem with the solution.

At what distance from the concave mirror of focal and 25 cm boy shall stand so that his image as a high equal to half of its original height?


The magnification of the concave mirror is negative which means to say that object and image will never be along the same direction. If object distances positive image distances negative and vice versa. By applying the basic formula of magnification as ratio of image distance to the object distance and the mirror formula with can solve the problem as shown above.


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Ray Optics Introduction and Reflection of Light

Light is a form of energy and it satisfies law of conservation of energy. Light travels like a electromagnetic wave. Human eye has a sensitivity to detect the electromagnetic waves of certain wavelength ranging from 4000 Å to 8000 Å.

Light travels with a very high velocity that is equal to 3 into 10 power 8 m/s in vacuum. The velocity of the light is maximum in vacuum and in any other medium it is less than that value. When the light falls on the objects whose size is much larger than that of the wavelength of the light, it appears like a straight line. Further properties of this and its applications are called ray optics.

Optics is a known subject for us for many years and it is a part of classical physics. We are able to see any objects because sunlight falls on the body and the body absorbs some particular colors, and reflects the other colors. What is the color that the body reflects is the color we see as the color of the body.

Light is a form of energy and it exhibits a wide variety of properties. To understand all these properties of the light we shall follow different theories of light that are evolved over the time.

Initially we have Newton’s corpuscular theory according to which light consists of  tiny particles called carpuscules. The size of the particle decides the color of the light. They travel in straight lines with high velocities.

Further we have different theories like Huygen’s wave theory, Maxwell’s electromagnetic theory and Plank’s quantum theory. Each theory is successful in explaining some properties of light and failed to explain to some other properties.

Finally we have a concept of dual nature. Here we assume that light travels like a wave and interacts with objects like a particle.

A ray of light gives the direction of propagation of light. In the absence of the obstacle, light advancing straight line without changing its direction.

 Reflection of light

The phenomena of the light coming back to the same medium after striking an obstacle is called as reflection. A light ray is reflected by the smooth surface in accordance to the rules of reflection. There are two laws of reflection.

The first law is that the angle of incidence is equal to angle of reflection. Here the angle of incidence is the angle between the incident ray and the normal. The point at which the light ray strikes the surface is called point of incidence. A line drawn through the point of incidence perpendicular to the surface is called normal.

The angle between the reflected and the normal is called angle of reflection. As per the first law angle of incidence is equal to angle of reflection.

As per the second law the incident ray, the reflected ray and the normal lies in the same plane.

The angle of deviation is the angle between the original path of the light and the path taken by of the light. We can derive the equations for the as shown below.

From the diagram it is clear that the reflected ray moves away from a plain surface. It is very clear from the diagram that the reflected ray is diverging from the obstacle and it is not going to form a real image. By extending these two light rays we can identify the location of the image and this kind of the images is called virtual image. From the obstacle the distance of the object in this case is equal to the distance of the virtual image.



Spherical mirror

A spherical mirror is a part that is cut from a hollow sphere and in general made up of the glass. One surface of the glass is silvered therefore it can behave like a mirror. The reflection of the light takes place on the other surface. If the reflection takes place at the convex surface then the mirror is called a convex mirror. If the reflection of the tile light takes place at the concave surface then the mirror is called as concave mirror. There were as shown in the diagram below.


Definitions

The Centre of the sphere from which the mirror is drawn is called Centre of curvature of the mirror.

The radius of the sphere is called radius of curvature of the mirror.

The point of the mirror at the middle of the surface is called as pole.

The line joining the pole and the Centre of the curvature is called principal axis.

The point where all the reflected light rays converge or from where the reflected light rays appears like diverging is called principal focus.

The distance between the principal focus and the pole of the mirror is called focal length.

The light rays that are close to the principal axis are called paraxial light rays.

The area of the spherical surface which is available for the reflection of the light is called Aperture.




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