Addendum: Sept. 2, 2022 In the note below we argue that v/c acts as a projection i.e. as cos(theta), but give no direct evidence for this. In a second note posted Sept. 2, 2022 and called Part II we address this issue and show that a photon bouncing back and forth perpendicular to the direction of motion has both a momentum and a rest mass type of term and v/c is cos(theta). Special relativity is often described in terms of a Lorentz transformation. Historically Lorentz considered Maxwell’s electromagnetic equations viewed from a moving frame. Einstein considered motion in a moving frame using light as a measuring device with the assumption that the speed of light is the same in all frames and cannot be surpassed. In this note we...
In a previous note (1) we attempted to derive Newton’s second law d/dt p = F(x) = -dV/dx for a conse...
Considerations on the complementary time-dependent coordinate transformations emboding Lorentz trans...
In Part I we argued that two flow equations for a free particle, namely: d/dx (partial) A(x,t) = p ...
In Part I of this note we considered searching for a single equation which would describe either a p...
In part I of this note we argued that setting p=E(v,mo)v where p is momentum and E energy of a free ...
Addendum Sept. 8, 2022: The conservation of photon momentum parallel to the moving mirror holds i.e....
The Lorentz transformation was discovered by Lorentz by considering the invariance of Maxwell’s ele...
Consider a mass at rest mo at x=0 at t=to. To an observer moving at a constant speed v, the values x...
The classical action (relativistic or nonrelativistic) may be written with v=x/t and x and t varied ...
In a number of previous notes, e.g. (1), we argued that the form of special relativity follows from ...
In simple Newton equation cases, one deals with nonrelativistic kinetic energy and potential energy....
In this note, we consider the classical Action= Integral L dt which is equal to Et - px with E=.5mo ...
We propose here two new transformations between inertial frames that apply for relative velocities g...
Entities in physics involve either mass or energy or both. Projectiles combine both rest mass and ki...
Einstein’s energy-momentum equation EnEn = pp + momo ((1)) allows for at least two very different s...
In a previous note (1) we attempted to derive Newton’s second law d/dt p = F(x) = -dV/dx for a conse...
Considerations on the complementary time-dependent coordinate transformations emboding Lorentz trans...
In Part I we argued that two flow equations for a free particle, namely: d/dx (partial) A(x,t) = p ...
In Part I of this note we considered searching for a single equation which would describe either a p...
In part I of this note we argued that setting p=E(v,mo)v where p is momentum and E energy of a free ...
Addendum Sept. 8, 2022: The conservation of photon momentum parallel to the moving mirror holds i.e....
The Lorentz transformation was discovered by Lorentz by considering the invariance of Maxwell’s ele...
Consider a mass at rest mo at x=0 at t=to. To an observer moving at a constant speed v, the values x...
The classical action (relativistic or nonrelativistic) may be written with v=x/t and x and t varied ...
In a number of previous notes, e.g. (1), we argued that the form of special relativity follows from ...
In simple Newton equation cases, one deals with nonrelativistic kinetic energy and potential energy....
In this note, we consider the classical Action= Integral L dt which is equal to Et - px with E=.5mo ...
We propose here two new transformations between inertial frames that apply for relative velocities g...
Entities in physics involve either mass or energy or both. Projectiles combine both rest mass and ki...
Einstein’s energy-momentum equation EnEn = pp + momo ((1)) allows for at least two very different s...
In a previous note (1) we attempted to derive Newton’s second law d/dt p = F(x) = -dV/dx for a conse...
Considerations on the complementary time-dependent coordinate transformations emboding Lorentz trans...
In Part I we argued that two flow equations for a free particle, namely: d/dx (partial) A(x,t) = p ...