Given 2 = 60o = 30o We know,
sin = n for first minima n = 1, At first minima
sin =
106 sin 30o =
=
m Now after making a new slit, Fringe width, =
given, D = 50 cm and = 1 cm. 1 102 =
d = 25 106 m = 25 m.
Given 2 = 60o = 30o We know,
sin = n for first minima n = 1, At first minima
sin =
106 sin 30o =
=
m Now after making a new slit, Fringe width, =
given, D = 50 cm and = 1 cm. 1 102 =
d = 25 106 m = 25 m.
When white light is used in Young's double slit experiment and one slit is covered by a red filter and the other by a green filter, several effects occur: Different Fringe Widths: Each color will produce fringes of different widths due to their varying wavelengths.
This means that red and green will not overlap perfectly.
Color Overlap: As the fringe patterns develop, some regions will have overlap due to the differing fringe spacings of red and green light.
This overlap will create areas where the colors mix, potentially leading to an appearance of intermediate colors.
Overall, because each color produces its own pattern and these do not align, a clear interference pattern as seen with monochromatic light (a single color) will not be formed.
Instead, there will be a complex pattern where the fringes do not distinctly appear as solid bands of red or green due to the overlapping and different fringe widths.
When electric field vector is completely removed and incident on Brewster's angle then only refraction takes place.
The light wave is propagating with plane wave fronts described by the equation .
The wave propagates in a direction perpendicular to these wave fronts.
This direction is symmetric with respect to the , , and axes.
Since the wave is symmetric about these axes, the angle it makes with each axis is the same.
Let these angles be , , and , which are the angles made by the light with the , , and axes, respectively.
This implies: According to the sum of the squares of the direction cosines: Substituting the equality of direction cosines, we get: Thus, the angle is given by:
In Young's double-slit experiment, the distance between the slits and the screen, , the wavelength of the light, , and the position of the 5th bright fringe from the central maximum, .
The distance between the central maximum and the th bright fringe is given by the formula:
where is the distance between the two slits. We can rearrange this formula to solve for :
Substituting the values given in the question, we get:
Therefore, the separation between the slits is .
Numerical aperature of the microscope is given as
Where d = minimum sparaton between two points to be seen as distinct
= 2.4
To determine the angular spread of the central maximum in a single-slit diffraction pattern, we can use the formula for the angular position of the first minimum (also understood as the boundary of the central maximum) on either side of the center.
For a single-slit diffraction pattern, the angle to the first minimum is given by the condition:
where :
is the width of the slit, is the wavelength of the light (or microwaves in this case),
is the order number of the minimum with
(for the first minimum,
) However, we are only interested in the angle to the first minimum, so we will only consider
. Since the slit width
and the wavelength
, we substitute these values into the equation to find :
The angle whose sine is 0.5 is
. This angle of
is the angle from the center to the first minimum on one side.
The angular spread of the central maximum would cover the range from the first minimum on one side to the first minimum on the other side, totalling twice this angle:
Therefore, the angular spread of the central maxima of the diffraction pattern is
, which corresponds to Option A.
Angular position of nth minima from central maxima, sin =
here n = 2
sin =
=
=
rad.
In a Young's double slit experiment, the intensity at a point on the screen is given by the formula :
where is the intensity at the center of the pattern, is the distance between the slits, is the angle between the line joining the point to the center of the pattern and the line passing through the center of the pattern and the slits, and is the wavelength of the light used.
The phase difference between the waves from the two slits at a point on the screen is given by :
For a phase difference of between the waves from the two slits at point P, we have :
For a phase difference of between the waves from the two slits at point Q, we have :
Solving for in both cases, we get:
Substituting these values in the formula for intensity, we get :
Therefore, the ratio of intensities at points P and Q is 3 : 2
Third bright fringe of known light coincides with the 4th bright fringe of the unknown light.