Fresnel half period zones are used to describe the contribution of different portions of a wavefront to the intensity at a point in the wave’s path. Each successive zone contributes an equal phase shift but alternates in sign, effectively contributing to the constructive and destructive interference pattern:
- (A) True, as the amplitude of the disturbance from each zone is a function of its area.
- (B) True, as each zone’s radius increases with the square root of its order number.
- (C) True, the area and thus the impact of each zone varies with wavelength, affecting how the wavefront constructs or destructs at a point.
- (D) True, The radii of half period zones are directly proportional to the square root of the wavelength of the light.
| List I | List II |
|---|---|
| (A) The linear momentum of the system remains constant | (IV) The net external force acting on a system of particles is zero |
| (B) The angular momentum of the system remains constant | (III) The external torque acting on a system of particles is zero |
| (C) Inertial frame | (I) The frames relative to which an unaccelerated body appears unaccelerated |
| (D) Non-inertial frame | (II) The frames relative to which an unaccelerated body appears accelerated |
| LIST I | LIST II |
|---|---|
| A. Maxwell's First Equation | I. Modified Ampere's Law |
| B. Maxwell's Second Equation | II. Faraday's Laws of Electromagnetic Induction |
| C. Maxwell's Third Equation | III. Gauss Law in Electrostatics |
| D. Maxwell's Fourth Equation | IV. Gauss Law in Magnetostatics |
| List I | List II |
|---|---|
| (A) (∂S/∂P)T | (I) (∂P/∂T)V |
| (B) (∂T/∂V)S | (II) (∂V/∂S)P |
| (C) (∂T/∂P)S | (III) -(∂V/∂T)P |
| (D) (∂S/∂V)T | (IV) -(∂P/∂S)V |
| List I | List II |
|---|---|
| A. Fraunhofer Diffraction | I. Interaction of the light waves from two different wave fronts. |
| B. Fresnel Diffraction | II. The distance between the source and the screen are effectively at infinite distance. |
| C. Interference of Light | III. It’s a phenomenon in which the wave vibrations are restricted to a particular direction in a plane. |
| D. Polarization of Light | IV. The source and screen or both are at finite distances from the aperture or obstacle. |