 
					
					
						Relativistic Calculations					
				 
				
					
						 المؤلف:  
						E. R. Huggins
						 المؤلف:  
						E. R. Huggins					
					
						 المصدر:  
						Physics 2000
						 المصدر:  
						Physics 2000					
					
						 الجزء والصفحة:  
						74
						 الجزء والصفحة:  
						74					
					
					
						 19-11-2020
						19-11-2020
					
					
						 1811
						1811					
				 
				
				
				
				
				
				
				
				
				
			 
			
			
				
				Relativistic Calculations
Although we have not quite finished with our discussion of Einstein’s special theory of relativity, we have covered two of the important consequences, time dilation and the Lorentz contraction, which will play important roles throughout the text. At this point we will take a short break to discuss easy ways to handle calculations involving these relativistic effects. Then we will take another look at Einstein’s theory to see if there are any more new effects to be discovered.
After our discussion of time dilation, we pointed out the importance of the quantity  which is a number always less than 1. If we wanted to know how much longer a moving observer’s time interval was, we divided by
 which is a number always less than 1. If we wanted to know how much longer a moving observer’s time interval was, we divided by  to get a bigger number. If we wanted to know how much less was the frequency of a moving clock, we multiplied by
 to get a bigger number. If we wanted to know how much less was the frequency of a moving clock, we multiplied by  to get a smaller number.
 to get a smaller number.
With the Lorentz contraction we have another effect that depends upon  . If we see an object go by us, the object will contract in length. To predict its contracted length, we multiply the uncontracted length by
. If we see an object go by us, the object will contract in length. To predict its contracted length, we multiply the uncontracted length by  to get a smaller number. If, on the other hand, an object moving by us had a contracted length l, and we stop the object, the contraction is undone and the length increases. We get the bigger uncontracted length by dividing by
 to get a smaller number. If, on the other hand, an object moving by us had a contracted length l, and we stop the object, the contraction is undone and the length increases. We get the bigger uncontracted length by dividing by  .
.
As we mentioned earlier, first determine intuitively whether the number gets bigger or smaller, then either multiply by or divide by the  as appropriate. This always works for time dilation, the Lorentz contraction, and, as we shall see later, relativistic mass. We will now work some examples involving the Lorentz contraction to become familiar with how to handle this effect.
 as appropriate. This always works for time dilation, the Lorentz contraction, and, as we shall see later, relativistic mass. We will now work some examples involving the Lorentz contraction to become familiar with how to handle this effect.
				
				
					
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