For Newton’s rings, the interference condition for constructive and destructive interference is based on the thickness t of the air film and the wavelength of light. The pattern of colored rings can only be observed if the light is polychromatic, as monochromatic light will produce a simple fringe pattern without any color.
| 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. |