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This is probably not a good question, since I am at a fairly low level, but I am a little bit confused when the two concepts were described to me and it's bringing discomfort during my study.

What I was told is that, the classical field theory is classical mechanics with infinite degrees of freedom

But on the other hand, I was also told thermodynamic system is also a "large-scale" system with very large degrees of freedom.

It seems be a matter of "scale" that these theories adhere to.

If classical mechanics is considered to be "small-scale" comparing with classical field theory, then what is the "scale" of thermodynamics comparing with CFT?

Can statistical method be applied to field? How to draw the connection & distinction when study these theories?

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I think this is a nice question! I hadn't appreciated before that you could describe both classical field theory and statistical mechanics as different kinds of "large $N$" limits of classical mechanics ($N$=number of degrees of freedom).

The TL;DR:

  • Classical field theory involves an infinite number of classical degrees of freedom at zero temperature.
  • Statistical mechanics involves a finite number of classical or quantum degrees of freedom at finite temperature.
  • Statistical field theory involves an infinite number of classical or quantum degrees of freedom at finite temperature.
  • Quantum field theory involves an infinite number of quantum degrees of freedom at zero temperature.

You will find examples which contradict essentially all of the distinctions I just made :) (You can compute finite temperature effects in quantum field theory, you will find statistical mechanics books covering the infinite number of degrees of freedom of the electromagnetic field at finite temperature, etc) But I think it captures what's going on at a high level, at least morally.

Classical field theory

A typical entry point into classical field theory is to consider an infinite number of coupled harmonic oscillators. In classical mechanics, you study a mass on a spring. In a more advanced treatment, you will study two or more coupled masses, for example two or three masses connected by springs. You can approach classical field theory by filling space with a dense grid, where at every node in the grid there is a mass, and each mass is connected by springs to its nearest neighbors. This "infinite box spring" can describe wavelike solutions that propagate through space if you "ping" one of the point masses. The questions you tend to ask are deterministic. Given some initial condition of the field, you want to know how the field will evolve. The answer to a given question will be based on the configuration of the field at a given time.

Statistical mechanics

The essence statistical mechanics is random motion due to thermal fluctuations that occur at finite temperature. You can imagine taking one mass on a spring, and coupling it to a large thermal bath at some temperature. If we focus on how the mass on a spring behaves, it will undergo random oscillations due to its connection to the thermal bath. The thermal bath is the large system, but we do not need to explicitly model it. Sometimes, people talk about "ensembles" of hypothetical copies of the original system which are coupled together. The questions you ask in statistical mechanics are probabilistic. You want to know how likely it is for the system to have some property. Answers to questions are based on a probability distribution over states of the system.

Statistical field theory

I want to make a few other points about systems displaying random motion.

Imagine a classical field, which is undergoing random motion. Imagine our infinite box spring, coupled to a thermal bath with some temperature. There will be random waves propagating through the mattress. This is statistical field theory. You can use this set of ideas to study states of matter, and in particular phase transitions between different states of matter. You can think of all of the atoms in a magnet, say, as describing a kind of field (imagine each atomic magnet as a point mass in our box spring analogy, and the springs as an analogy for magnetic couplings between the atoms). Then, depending on the temperature, the atomic magnets may line up to form a magnetized state, or be randomly oriented to be a demagnetized state -- statistical field theory lets you quantitatively study this kind of situation. Answers to questions are based on studying the probability distribution of field configurations. This is as opposed to classical field theory, where answers are based on a single, deterministic field configuration, and statistical mechanics, where the answers are based on a probability distribution of some finite number of degrees of freedom.

Quantum field theory

Quantum field theory is like statistical field theory, but where the random motion is driven by quantum mechanics, instead of temperature. A quantum harmonic oscillator exhibits random zero-point motion, and there is a discrete spectrum of excitations above this ground state. Coupling many quantum harmonic oscillators to form a "quantum boxspring mattress" is one way to think about quantum fields (this is the approach Zee takes in his textbook). The discrete spectrum of excitations for one quantum harmonic oscillator, can be interpreted as particles in quantum field theory. Answers to questions in this context are based on the probability amplitudes for the field to achieve certain configurations (a probability amplitude $A$ is related to a probability $P$ by $P=|A|^2$).

Caveats

Finally, I should say that the boundaries between different areas in physics are not always as well-defined as they may seem, especially between statistical mechanics and statistical field theory. In my experience, the factor that really separates statistical mechanics and statistical field theory is what tools are used to solve a problem, rather than whether a classical or quantum field is involved. Blackbody radiation is often covered in a statistical mechanics course, for example, even though you are really studying the statistical mechanics of the electromagnetic field. I think this is just considered "too basic" to be called statistical field theory, even though by my definition above, arguably it should be a topic in statistical field theory. To give you an idea, a central topic in a statistical field theory course is the Ginzburg-Landau approach to phase transitions, where one uses symmetry to motivate an expression for the free energy of a field, and different states of matter correspond to how the minima of the free energy depend on temperature. More generally, statistical field theory courses often use techniques that are also used in quantum field theory -- such as effective field theory, the renormalization group, non-perturbative techniques such as instantons -- but applied to thermal systems (not to say that the techniques originated in QFT; there is a rich interplay where information passes back and forth between the subjects). This is just to say; many of the divisions we make in physics are somewhat arbitrary, and so always take claims that different fields are cleanly separated (like I made in the preceding paragraphs of my answer) with a grain of salt.

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Classical mechanics: the prototype is a set of point particles, or a set of rigid bodies (since the body is perfectly rigid, it is described by a finite set of degrees of freedom). The equations of motion are ordinary differential equations, typically of the form $F= m a$.

Classical field theory the main jump with respect to classical mechanics is that now the equations of motion are (typically) partial differential equations. Instead of having a finite number of degrees of freedom, there are degrees of freedom (namely, some quantity that evolves) at each point in space. Example: temperature is described by a field, that is an entity that assignes a local degree of freedom "temperature" to each point in space. The dynamical equation is the "heat equation", a very famous partial differential equation (PDE). Other examples are:

  • Electromagnetism: we have vectors representing the magnetic and electric "fields" at each point. PDE = Maxwell equations.

  • Gravity: we have the metric tensor "field" at each point, that tells us how spacetime bends. PDE = Einstein equations.

  • Hydrodynamics: at each point we have density, temperature and velocity, that are the typical "fields" in fluid dynamics. PDE = Euler equations (if the fluid is a perfect fluid) or Navier-Stokes equations (if there is viscosity).

  • Elasticity (or more generally deformable solids): at each point you have a "displacement" field.

  • More generally:"continuum mechanis" is based on classical field theory, as long as quantum effects can be ignored. That "continuum" is quite clear: there is a continuum of local degrees of freedom.

NOTE: quantum mechanics is the "quantum version" of classical mechanics, quantum field theory is the "quantum version" of classical field theory.

Now thermodynamics: it is a very different thing. It can blend with classical field theory (e.g. to do hydrodynamics or continuum mechanics you need a "local version" of thermodynamics, that is thermodynamics applied locally to a "matter element"). The idea is that a system comprised of many degrees of freedom can be described by a few variables, that are statistical in nature, under certain (technical) assumptions. Statistical mechanics is the "justification" of the thermodynamic point of view and provides the tools to calculate thermodynamic quantities (like pressure, internal energy, chemical potential etc..) from the microscopic degrees of freedom that constitute the system. Statistical field theory is statistical mechanics applied to systems that are fields in nature and its tools are not very different from the ones of quantum field theory.

In short: classical mechanics and classical field theory are interested in describing the exact dynamics of every degrees of freedom. Thermodynamics deals with a finite set of statistical variables that capture the overall property of a system with many degrees of freedom. Statistical mechanics is the set of methods that can be used to extract those finite set of statistical variables form a more detailed (microscopic) description of the system (it is more than that.. but this is the idea).

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