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Quantifying Heat02:46

Quantifying Heat

Thermal Energy Microscopically, thermal energy is the kinetic energy associated with the random motion of atoms and molecules. Temperature is a quantitative measure of “hot” or “cold”, which depends on the amount of thermal energy. When the atoms and molecules in an object are moving or vibrating quickly, they have a higher average kinetic energy (KE) (or higher thermal energy), and the object is perceived as “hot”, or it is described as being at a higher temperature. When the atoms and...
Spontaneity02:21

Spontaneity

A spontaneous process is one that occurs naturally under certain conditions. A nonspontaneous process, on the other hand, will not take place unless it is “driven” by the continual input of energy from an external source. Processes have a natural tendency to occur in one direction under a given set of conditions. Water will naturally flow downhill (spontaneous process), but uphill flow (nonspontaneous process) requires outside intervention such as the use of a pump. Iron exposed to the earth’s...
Isothermal Processes01:21

Isothermal Processes

A thermodynamic process that occurs at constant temperature is called an isothermal process. Heat slowly flows into the system or out of the system to maintain thermal equilibrium. Processes involving phase changes like water evaporation into steam or freezing water into ice at a constant temperature are examples of Isothermal Processes.
An ideal gas can also undergo isothermal expansion or compression.
For example, consider 1 mole of an ideal gas inside an isolated cylinder at initial volume V...
Reversible and Irreversible Processes01:14

Reversible and Irreversible Processes

The thermodynamic processes can be classified into reversible and irreversible processes. The processes that can be restored to their initial state are called reversible processes. It is only possible if the process is in quasi-static equilibrium, i.e., it takes place in infinitesimally small steps, and the system remains at equilibrium However, these are ideal processes and do not occur naturally. An ideal system undergoing a reversible process is always in thermodynamic equilibrium within...
Thermodynamic Processes01:25

Thermodynamic Processes

A thermodynamic process is a path through a sequence of states that takes a system from an initial state to a final state. In a cyclic process, the system returns to its initial state, so the changes in state properties and state functions (ΔT, Δp, ΔV, ΔU, ΔH) over one complete cycle are zero. However, heat and work transfers can still occur during the cycle, and the net heat and net work over the cycle need not be zero.A reversible process occurs when the system is infinitesimally close to...
Calculation of First-Law Quantities II01:24

Calculation of First-Law Quantities II

The first law of thermodynamics establishes that the change in internal energy of a system is given by ΔU = q + w, where q is the heat exchanged, and w is the work performed. For a perfect gas, both internal energy (U) and enthalpy (H) depend solely on temperature. Consequently, for any change of state, whether reversible or irreversible, the internal energy change is determined by integrating the heat capacity at constant volume, and the enthalpy change by integrating the heat capacity at...

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Related Experiment Video

Updated: Jul 11, 2026

Characterization of Thermal Transport in One-dimensional Solid Materials
05:20

Characterization of Thermal Transport in One-dimensional Solid Materials

Published on: January 26, 2014

Quasiparticles in a thermal process.

Ferenc Márkus1, Katalin Gambár

  • 1Institute of Physics, Budapest University of Technology and Economics, Budafoki út 8, H-1521 Budapest, Hungary. markus@phy.bme.hu

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|August 11, 2005
PubMed
Summary
This summary is machine-generated.

This study introduces a new scalar field to unify Fourier heat conduction and wave-like heat propagation. It enables calculating an effective mass for thermal processes and expressing dissipative action units using universal constants.

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Last Updated: Jul 11, 2026

Characterization of Thermal Transport in One-dimensional Solid Materials
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Published on: January 26, 2014

Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry
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Area of Science:

  • Thermodynamics
  • Theoretical Physics
  • Continuum Mechanics

Background:

  • Traditional heat conduction models (Fourier's law) describe diffusive heat transfer.
  • Wave-like heat propagation models consider ballistic transport, particularly at micro/nano scales.
  • A unified framework for these phenomena is lacking.

Purpose of the Study:

  • To introduce a novel abstract scalar field as a dynamical generalization of temperature.
  • To formulate a covariant field equation connecting Fourier heat conduction and wave-like heat propagation.
  • To explore the physical implications of this new field, including effective mass and dissipative action.

Main Methods:

  • Postulation of an abstract scalar field.
  • Derivation of a covariant field equation governing the scalar field.
  • Calculation of an effective mass associated with the thermal process.
  • Expression of the unit of dissipative action in terms of fundamental constants.

Main Results:

  • A theoretical framework is established to bridge diffusive and wave-like heat transport.
  • The concept of an effective mass for thermal processes is introduced and calculable.
  • A new expression for the unit of dissipative action is derived using universal constants.

Conclusions:

  • The proposed scalar field offers a unified dynamical perspective on heat transfer.
  • The framework provides insights into the effective mass and dissipative properties of thermal phenomena.
  • This work contributes to a deeper understanding of heat propagation across different regimes.