Home » First Law of Thermodynamics

First Law of Thermodynamics

1850
  • Julius Robert von Mayer
  • James Prescott Joule
  • Hermann von Helmholtz
  • Rudolf Clausius
Laboratory experiment demonstrating the First Law of Thermodynamics with a heat engine setup.

The First Law is a statement of the conservation of energy. It posits that the change in a closed system’s internal energy (\(\Delta U\)) is equal to the heat supplied to the system (\(Q\)) minus the work done by the system on its surroundings (\(W\)). The governing equation is \(\Delta U = Q – W\). This law links heat, work, and internal energy, establishing heat as a form of energy transfer.

The First Law of Thermodynamics generalized the principle of conservation of energy, which was previously known in mechanics, to include heat. Its formulation was a major step in physics, as it definitively refuted the prevailing caloric theory, which considered heat a weightless fluid. Experiments by James Joule in the 1840s, which demonstrated the mechanical equivalent of heat, were crucial in establishing that heat and work are mutually convertible.

The law introduces internal energy (\(U\)) as a state function, meaning its value depends only on the current state of the system, not on how it got there. In contrast, heat (\(Q\)) and work (\(W\)) are path-dependent process quantities. The law’s differential form is \(dU = \delta Q – \delta W\). For a cyclic process, where the system returns to its initial state, the change in internal energy is zero (\(\Delta U = 0\)), so the net heat supplied equals the net work done. This principle is the basis for all heat engines. The law also implies the impossibility of a perpetual motion machine of the first kind—a machine that produces work without any energy input.

UNESCO Nomenclature: 2212
– Thermodynamics, statistical physics, and condensed matter

Type

Abstract System

Disruption

Revolutionary

Usage

Widespread Use

Precursors

  • Sadi Carnot’s analysis of heat engines and thermodynamic cycles
  • James Joule’s experiments on the mechanical equivalent of heat
  • rejection of the caloric theory of heat
  • principle of conservation of energy in mechanics as formulated by Leibniz and others

Applications

  • heat engines (internal combustion, steam turbines)
  • refrigerators, air conditioners, and heat pumps
  • chemical reaction analysis (enthalpy calculations)
  • power plant design and efficiency analysis
  • nutritional calorimetry for calculating food energy (calories)

Patents:

NA

Potential Innovations Ideas

Professionals (100% free) Membership Required

You must be a Professionals (100% free) member to access this content.

Join Now

Already a member? Log in here
Related to: first law, conservation of energy, internal energy, heat, work, thermodynamics, enthalpy, closed system, state function, perpetual motion.

Leave a Reply

Your email address will not be published. Required fields are marked *

AVAILABLE FOR NEW CHALLENGES
Mechanical Engineer, Project, Process Engineering or R&D Manager
Effective product development

Available for a new challenge on short notice.
Contact me on LinkedIn
Plastic metal electronics integration, Design-to-cost, GMP, Ergonomics, Medium to high-volume devices & consumables, Lean Manufacturing, Regulated industries, CE & FDA, CAD, Solidworks, Lean Sigma Black Belt, medical ISO 13485

We are looking for a new sponsor

 

Your company or institution is into technique, science or research ?
> send us a message <

Receive all new articles
Free, no spam, email not distributed nor resold

or you can get your full membership -for free- to access all restricted content >here<

Historical Context

(if date is unknown or not relevant, e.g. "fluid mechanics", a rounded estimation of its notable emergence is provided)

Related Invention, Innovation & Technical Principles

Scroll to Top

You May Also Like