Why Can't the Speed of Light Exceed 300,000 km/s?

vikrant_cbapat
Messages
1
Reaction score
0
I would like to know if there is any logical/mathematical explanation as to why the speed of light can't be greater than c ...

Have also read a few reports that the speed of light has been reduced, and infact stopped ..how authentic are these reports? and if they are, would other effects, like those of gravitation also slow down? in other words, is 300,000km/s the max speed attainable or the speed of light, whatever it may be is the max speed? and WHY?
 
Physics news on Phys.org
Since "c" is defined as the speed of light, the speed of light cannot be greater then c. Its like asking if a dog can be more then a dog.

You can slow down the speed of light to the point of stopping it in its path and it has been done many times. Light slows down as it passes into a new medium and you can infact stop it.
 
Thread 'Why is there such a difference between the total cross-section data? (simulation vs. experiment)'
Well, I'm simulating a neutron-proton scattering phase shift. The equation that I solve numerically is the Phase function method and is $$ \frac{d}{dr}[\delta_{i+1}] = \frac{2\mu}{\hbar^2}\frac{V(r)}{k^2}\sin(kr + \delta_i)$$ ##\delta_i## is the phase shift for triplet and singlet state, ##\mu## is the reduced mass for neutron-proton, ##k=\sqrt{2\mu E_{cm}/\hbar^2}## is the wave number and ##V(r)## is the potential of interaction like Yukawa, Wood-Saxon, Square well potential, etc. I first...
Toponium is a hadron which is the bound state of a valance top quark and a valance antitop quark. Oversimplified presentations often state that top quarks don't form hadrons, because they decay to bottom quarks extremely rapidly after they are created, leaving no time to form a hadron. And, the vast majority of the time, this is true. But, the lifetime of a top quark is only an average lifetime. Sometimes it decays faster and sometimes it decays slower. In the highly improbable case that...
I'm following this paper by Kitaev on SL(2,R) representations and I'm having a problem in the normalization of the continuous eigenfunctions (eqs. (67)-(70)), which satisfy \langle f_s | f_{s'} \rangle = \int_{0}^{1} \frac{2}{(1-u)^2} f_s(u)^* f_{s'}(u) \, du. \tag{67} The singular contribution of the integral arises at the endpoint u=1 of the integral, and in the limit u \to 1, the function f_s(u) takes on the form f_s(u) \approx a_s (1-u)^{1/2 + i s} + a_s^* (1-u)^{1/2 - i s}. \tag{70}...
Back
Top