Aksayskiy Vladimir
Landauer's principle as a consequence of the Shannon-Hartley theorem or communication and information in the world of black bodies
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   Communication and information in the world of black bodies. The message, in contrast to the
   information, obeys the Landauer principle, according to which any generator, transmitter, and
   receiver of a message is a source of thermal radiation, which in the case of electromagnetic
   communication is conveniently considered in terms of the Planck black body model. In this
   case, the Shannon - Hartley theorem leads to the well-known formulation of the Landauer
   principle.
   
   According to the Shannon - Hartley theorem [1], the data transmission rate over
   a communication channel or channel capacity is:
   C = B*log_2(1 + S/N)     ,                                  (1)
   where
   C is the channel capacity in bits per second, a theoretical upper bound on the net bit rate; 
   B is the bandwidth of the channel in hertz; 
   S is the average received signal power, watts (or volts squared); 
   N is the average power of the noise, watts (or volts squared); 
   S/N is the signal-to-noise ratio (SNR).
   
   Wien's displacement law [2] allows us to represent the bandwidth in the form of:
   B = f_max = (k*T*a)/h    ,                                (2)
   where
   f_max is the frequency corresponding to the maximum of the black body radiation curve, Hz;
   k is the Boltzmann constant, J/K; 
   h is the Planck constant, J*s; 
   T is temperature, K; 
   a=2.821439 is a constant.
   
   Substituting (2) into (1) and multiplying both sides of the equation by the Planck constant,
   we get:
   W = k*T*a*log_2(1 + SNR)    ,                      (3)
   where
   W - energy of a bit in the communication channel, J.
   
   Taking in (3) SNR = 0.1856, we obtain the well-known expression of the Landauer principle:
   W = k*T*ln(2)    ,                                            (4)
   
   Planck's blackbody model is based on the Bose - Einstein distribution, but in some cases it is
   convenient to use the Fermi - Dirac distribution.
   
   Links
   1_ Shannon-Hartley theorem https://en.wikipedia.org/wiki/Shannon%E2%80%93Hartley_theorem
   2_ Wien's displacement law https://en.wikipedia.org/wiki/Wien%27s_displacement_law
   
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