ISSN 2348-1218 (print) International Journal of Interdisciplinary Research and Innovations ISSN 2348-1226 (online) Vol. 8, Issue 3, pp: (59-64), Month: July - September 2020, Available at: www.researchpublish.com
Radiation – Charge Energy Transference Relations Kush Kabra Kush.kabra16736@gmail.com
Abstract:Change in frequency of radiation is directly proportional to product of charges and inversely proportional to displacement brought from origin. Case (i) from infinity (
) (
Case (ii) from (
)
( (
)
) )
Keywords: Radiation, directly proportional, charges.
1. INTRODUCTION Electrostatic phenomena arise from the forces that electric charges exert on each other. Coulomb’s law quantifies the amount of force between two stationary electrically charged particles. The electric force between charged bodies at rest is conventionally called electrostatic force or Coulomb force1 The electrostatic potential Energy of one point charge q at position r in the presence of an electric field E is defined as negative of work W done to bring it from reference position to that position r2 Law of conservation of energy states that the total energy of an isolated system remains constant; it is said to be conserved over time3 The Planck Constant, or Planck’s constant is the quantum of electromagnetic action that relates a photon’s energy to its frequency. The Planck constant multiplied by a photon’s frequency is equal to a photon’s energy 4 Assumptions: 1. Assume that a photon of energy v
⁄ hits a charge q having initial velocity zero attains instantaneous velocity
2. Consider charge Q at origin stationary and charge q is brought to A without accelerating. 3. Order of charge is out of range of applicable Quantum mechanics. 4. Order of mass of charge is out of range of applicable quantum mechanics 5. 6.
if
take |
| i.e. work is always done against the electric field or field causing attraction forces (if any)
7. Only electrostatic forces is experienced between charges Q and q 8. Consider charge Q at origin stationary and charge q is brought to B from A without accelerating.
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