 
					
					
						Light Energy					
				 
				
					
						 المؤلف:  
						Franklin Potter and Christopher Jargodzki
						 المؤلف:  
						Franklin Potter and Christopher Jargodzki					
					
						 المصدر:  
						Mad about Modern Physics
						 المصدر:  
						Mad about Modern Physics					
					
						 الجزء والصفحة:  
						p 119
						 الجزء والصفحة:  
						p 119					
					
					
						 24-11-2016
						24-11-2016
					
					
						 1162
						1162					
				 
				
				
				
				
				
				
				
				
				
			 
			
			
				
				Light Energy
We know that the speed of light is the same for all observers in inertial frames. If so, are the momentum and energy of light as measured by all observers the same even when the light source is moving toward the observer?
Answer
A light source emitting light of frequency f approaching an observer at constant velocity v will appear blue shifted by an amount corresponding to the relativistic Doppler effect formula  because the clock ticking rates will be different for the source reference frame and the observer reference frame, and their separation distance is decreasing. When v << c, we can expand the formula in a Taylor series to obtain f ′ ~ f (1 + v/c – v2/2c2 + . . . ), so the leading term in powers of v/c is positive, corresponding to the blueshift. We assume that an acceleration itself does not produce an additional fundamental frequency shift, although there will be acceleration effects because the source is changing instantaneous comoving inertial frames.
 because the clock ticking rates will be different for the source reference frame and the observer reference frame, and their separation distance is decreasing. When v << c, we can expand the formula in a Taylor series to obtain f ′ ~ f (1 + v/c – v2/2c2 + . . . ), so the leading term in powers of v/c is positive, corresponding to the blueshift. We assume that an acceleration itself does not produce an additional fundamental frequency shift, although there will be acceleration effects because the source is changing instantaneous comoving inertial frames.
For a photon, its energy is E = hf and its momentum is p = E/c, so both energy and momentum are different in different reference frames because the observed frequencies are different. Notice that the recoil of the source on emission of light and of the observer on detection are not accounted for in the discussion and that the energy and momentum input necessary to keep the relative velocity of the source and observer fixed must be considered also. Of course, energy and momentum conservation laws are obeyed in this example.
				
				
					
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