
#1
Nov2212, 11:41 AM

P: 3

I'm actually quite scared of asking this due to my very basic knowledge regarding Quantum Mechanics. Actually, this is my first hiccup: is there a difference between Quantum Physics and Quantum Mechanics?
I always thought one was the theoretical investigation and the other the application but after reading a bit I am not so sure any longer. A quick definition clarifying the conflicting info I am getting would help. My actual question: is Quantum Mechanics bound to the 1st law of thermodynamics? Or any classical thermodynamics restriction for that matter. I've been thinking about this and just when I find I can say: no, I think of a way that can maybe be a: yes. I've tried the Google approach and have given up. I've tried reading here and am now more confused than before. So I hope someone can sort this out explaining it in simple terms  and that there actually is an answer. Thanks 



#2
Nov2212, 12:38 PM

Mentor
P: 10,840

I think "Quantum Physics" and "Quantum Mechanics" are the same.
Modern thermodynamics can be derived from quantum mechanics. 



#3
Nov2212, 01:54 PM

Mentor
P: 28,837

Thermodynamics is statistical mechanics. And in statistical mechanics, you can have quantum statistics. That is when a fermion or a boson matters. And Thus, quantum mechanics is applicable to thermo. For example, you can write the partition function for a quantum system with discrete energy states, and you can derive all the same themo state variables and functions from that. Zz. 



#4
Nov2212, 02:07 PM

P: 3

Do QM and Thermodynamics interact?
Thanks for the explanations.
I understand that quantum mechanics can explain thermodynamics. What about the other way around? My problem is that I don't know whether one can state that the conservation of energy even applies to quantum mechanics. Is this a valid question: does energy conservation work if a particle traverses the Higgs field and picks up mass? 



#5
Nov2212, 03:09 PM

Sci Advisor
Thanks
P: 3,856





#6
Nov2212, 05:18 PM

P: 3

It shows that I was wrong on the first part and misunderstood the function of the Higgs field. I suppose typical layman misconceptions. 



#7
Jan113, 04:36 AM

P: 35

You asked two questions: 1. The difference between Quantum Physics and Quantum mechanics and 2. The relation between Quantum mechanics and the 1st law of thermodynamics (your actual question).
1. 'Mechanics' is only a part of 'physics'. (you have many other parts such as  statics, heat, Sound, Light, electricity and magnetism, to mention a few). In mechanics we use Newton's laws to describe motion of bodies. When we try to describe the (motion) propagation of light, we find Newton's laws do not serve the purpose adequately. In place of Newton's laws we use Laws of Quantum mechanics (QM) OR Wave mechanics (WM). These are much more complicated compared to Newton's laws. That is why people are afraid of QM and WM, just as you were 'quite scared' even to pose your question! Mechanics deals with the study of motion of macroscopic bodies and is simple (relatively speaking) while QM &WM deal with study of motion of light and other particles at atomic level and is complicated. 2. If you had asked the relation between QM and TD it would have been more interesting. you stopped at the fist law of TD! Anyway, in mechanics (dynamics) we have the law of conservation of energy, but that does not include 'heat' as a form of energy. TD includes heat also as a form of energy and must be taken into account while the bookkeeping or accountancy is done for energy. TD deals with conversions of energy in general and heat and other forms of energy in particular. Statistical mechanics (Which is also mechanics) is a boarder case, relating Newton's mechanics, TD and QM. 



#8
Jan113, 09:15 AM

Sci Advisor
HW Helper
P: 11,863

Radhakrishnam, 'wave mechanics' is a term coined to describe Schrödinger's work of 1926 and in modern usage it is a subtheory of Quantum Mechanics in particular or Quantum Physics in general.
Quantum Mechanics is the subtheory of Quantum Physics describing systems of point particles with finite classical (Hamiltonian) DOF (where available). 


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