Heat |

**In General: Thermodynamics and Heat**

* __Idea__: Heat is energy transferred between two systems
purely as the result of a difference in temperature (no work done).

* __Value__: In an infinitesimal reversible transformation
the heat absorbed by a system can be expressed as δQ = *T* d*S* (> see Heat Theorem).

* __History__: Late 1600s,
Guillaume Amontons intuitively surmised that heat flowed in solids in the direction
of decreasing temperature; Early 1700s, Daniel Fahrenheit invented a mercury
thermometer capable of reproducible measurements; 1761, Joseph
Black introduced the concepts of latent heat and specific heat;
1780s, Invention of the calorimeter by Antoine Lavoisier and Pierre Simon Laplace,
and use of the latent heat of melting ice as a standard for quantifying
heat; The nature of what had been quantified,
though, would elude comprehension throughout the 19th century; 1807–1811,
Joseph Fourier conducted experiments and devised mathematical techniques that
together yielded the first estimate of a material’s thermal conductivity;
1842, Robert Meyer, heat is not a fluid that can penetrate material bodies but a
form of energy; 1843–1849, James Joule, experiments on the equivalence of
heat and energy.

* __Status of theory__:
It is empirically well tested for fluids and crystals, but there is little theoretical understanding.

@ __Historical / conceptual__: Narasimhan PT(10)aug-a1005 [measurement,
historical]; Votsis & Schurz SHPSA(12) [caloric and kinetic theories, and structural realism]; Hari Dass a1306 [caloric theory and Carnot's work].

@ __Related topics__:
Salazar et al EJP(10) [thin plate vs thick slab];
Schittny et al PRL(13) + news bbc(13)may [heat cloaking].

>
__Related concepts__: see inertia; Kinetic
Theory; specific heat [heat capacity]; Thermal Bath.

> __Heat transport__: see Heat Flow [mechanisms – conduction, convection, radiation]; thermal radiation; Transport Phenomena.

> __Other related phenomena__: see Heat Engine; Thermal Expansion.

**Mathematical Theory of Heat Transfer: Heat Equation / Operator** > s.a. spectral geometry; QED phenomenology [for nanoscale objects].

* __Idea__: The heat equation is the diffusion
equation, applied to the temperature in a heat conductor; When the density *ρ*,
specific heat *c* and thermal conductivity *k* are
constant, and setting *a*^{2}:= *k*/*c**ρ* (the thermal diffusivity) and
*f*:= *F*/*cρ*,

*u*_{, t} = *a*^{2} ∇^{2} *u* + *f* ; more
generally, *u*_{, t} = *L**u* ,

with *L* a second-order differential operator; It is related
to the Schrödinger equation by an analytic continuation in *t*.

@ __General references__: Widder 75; in Gilkey 84.

@ __Relativistic__: López-Monsalvo & Andersson PRS(11)-a1006; Mendez & García-Perciante AIP(10)-a1010 [kinetic-theory approach]; Andersson & López-Monsalvo CQG(11)-a1107 [consistent first-order model]; López-Monsalvo PhD(11)-a1107; Govender & Thirukkanesh MPLA(14)-a1404 [causal heat flow in Bianchi V spacetimes]; Duong PhyA(15)-a1501 [and relativistic kinetic Fokker-Planck equation].

@ __Related topics__: Gilkey et al NPPS(02)mp/01 [asymptotics]; Bustamante & Hojman
mp/01/JPA
[Lagrangian, Hamiltonian, Poisson brackets]; Hall in(06)m.DG/04
[range of time-*t* heat operator]; Gibou & Fedkiw JCP(05)
[Dirichlet boundary conditions, 4th-order discretization]; Iliev SelMath(08)mp/06 [discrete,
and Toda hierarchy]; Hall in(08)-a0710 [in
infinite dimensions]; He & Lee PLA(09)
[constrained variational principle]; Smerlak EPJP(12)-a1202 [thermal diffusivity as space-dependent]; Deconinck et al PRS(14) [non-steady-state heat flow]; Ramm a1601 [in a complex medium].

**Heat Kernel **> s.a. effective
action in quantum field theory.

$ __Def__: The solution to
(∇^{2} +
∂_{t}) *u* =
0 with initial condition *U*_{0}(*x*)
= δ(*x*); In
1D, it is given by *u*(*x*,* t*) = exp{–*x*^{2}/2*t*}/(2π*t*)^{1/2}.

$ __Generalization__: It
can be generalized to the equation (Δ + ∂_{t})
*u*_{t}(*g*)
= 0, for a function *u*_{t} defined
on a group *G*, on which the Laplacian is
Δ = ∑_{i} *X*_{i} *Y*_{i},
where *X*_{i} and
*Y*_{i} are
respectively right- and left-invariant vector fields, with solution

*u*_{t}(*g*)
= ∑_{r}* d*_{r} exp{–*t λ*_{r} /2}*χ*_{r}(*g*)
,

where *r* is an irrep of *G*, *d*_{r} its
dimension, *λ*_{r} the
eigenvalue of Δ, and *χ*_{r} the characteristic.

* __Applications__: It is
used in the coherent state transformation for quantum theory, and is a convenient
tool for studying one-loop divergences and
renormalization, anomalies and various asymptotics of the effective action;
It is also the transition density of a Brownian motion.

@ __General references__: Fulling ed-95 [and quantum gravity]; Booth ht/98 [heat
kernel coefficients with Mathematica]; Moss & Naylor CQG(99)gq/01 [diagrammatic
expansion technique]; Maher m.RT/06-proc
[on compact Lie groups].

@ __In curved spacetime__: Martin & McKeon ht/96;
Salcedo PRD(07)-a0706 [to
4th order in derivative expansion]; > s.a. effective field theories.

@ __Calculation of coefficients__: Nesterenko et al CQG(03)
[corner contributions]; Vassilevich PRP(03)
[tools]; Bordag & Vassilevich
PRD(04)ht [with
discontinuous backgrounds]; Iliev AIF(05)mp,
PAMS(07)mp/05 [and
KdV hierarchy].

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jun 2016