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pro vyhledávání: '"J. Gerhard Müller"'
Autor:
J. Gerhard Müller
Publikováno v:
Entropy, Vol 26, Iss 8, p 619 (2024)
In this paper, we are concerned with the process of experimental information gain. Building on previous work, we show that this is a discontinuous process in which the initiating quantum-mechanical matter–instrument interactions are being turned in
Externí odkaz:
https://doaj.org/article/39ea209ccd08475f8885764773abff91
Autor:
J. Gerhard Müller
Publikováno v:
Entropy, Vol 26, Iss 3, p 255 (2024)
It is argued that all physical knowledge ultimately stems from observation and that the simplest possible observation is that an event has happened at a certain space–time location X→=x→,t. Considering historic experiments, which have been grou
Externí odkaz:
https://doaj.org/article/f53dea38c6094c21aeabcceef4d92a95
Autor:
J. Gerhard Müller
Publikováno v:
Entropy, Vol 22, Iss 7, p 737 (2020)
A thermodynamic approach to mechanical motion is presented, and it is shown that dissipation of energy is the key process through which mechanical motion becomes observable. By studying charged particles moving in conservative central force fields, i
Externí odkaz:
https://doaj.org/article/3d4029cfac074420bf95e46abd7736c8
Autor:
J Gerhard Müller
Publikováno v:
Entropy
Entropy, Vol 22, Iss 392, p 392 (2020)
Volume 22
Issue 4
Entropy, Vol 22, Iss 392, p 392 (2020)
Volume 22
Issue 4
Making use of the equivalence between information and entropy, we have shown in a recent paper that particles moving with a kinetic energy &epsilon
carry potential information i p o t ( &epsilon
T ) = 1 ln ( 2 ) &epsilon
k B  
carry potential information i p o t ( &epsilon
T ) = 1 ln ( 2 ) &epsilon
k B  
Autor:
J Gerhard Müller
Publikováno v:
Entropy
Volume 21
Issue 11
Entropy, Vol 21, Iss 11, p 1052 (2019)
Volume 21
Issue 11
Entropy, Vol 21, Iss 11, p 1052 (2019)
The equivalence between information and entropy is used to interpret the entropy of a molecular gas as missing information about its internal state of motion. Our considerations show that thermodynamic information is principally composed of two parts