
The law of conservation of energy states that energy cannot be created or destroyed, only transformed from one form to another.In the mid-19th century, several scientists independently concluded that heat is not a mysterious fluid but a form of particle motion. Julius Mayer, observing the color of sailors' blood, noticed a connection between the body's work and heat. James Joule, through precise experiments, measured how much heat mechanical work produces. Hermann von Helmholtz formalized it into a coherent theory. The law of conservation of energy states: in an isolated system, total energy — the sum of kinetic, potential, thermal, and other forms — is constant. It's like a family budget: income and expenses can change form, but the total amount in the account is preserved if no external source intervenes.
The idea of the indestructibility of 'vis viva' (mv²) goes back to Leibniz in the 17th century. However, until the mid-19th century, heat was considered a special substance — caloric. Physician Julius Mayer in 1842 was the first to formulate the mechanical equivalent of heat, observing people in the tropics. James Joule in 1843–1847 experimentally proved the conversion of mechanical work into heat. Hermann von Helmholtz in 1847 gave a mathematical formulation for all types of energy. Emmy Noether in 1918 revealed the deep connection between symmetries and conservation laws. Albert Einstein extended the law to the relativistic domain, including mass-energy equivalence (E=mc²).
The law is applied in all branches of physics and engineering: from calculating planetary trajectories to designing heat engines and nuclear reactors. Its boundaries are indicated by general relativity, where gravitational field energy is non-local, and quantum mechanics, where energy fluctuations are possible on short intervals (uncertainty principle). However, in the macroscopic world and in closed systems it is absolute.
Without this law, power plants would not work: the chemical energy of coal turns into heat, then into electricity. In every battery and solar panel, its action is present.
Thanks to this law, we know exactly: the flap of a butterfly's wing does not disappear without a trace, but dissipates in the chaos of thermal motion of air.
| \Phi | variable | Flux (e.g., particle or energy flux) — flux varies |
| E | variable | Energy — energy joule |
| \Phi_0 | variable | Normalization constant (flux at E = E_0) — flux constant varies |
| E_0 | variable | Reference energy — energy joule |
| \gamma | variable | Spectral index (power-law exponent) — spectral index |
| ρ_1 | variable | Energy density of fluid 1 — energy density joule per cubic metre |
| ρ_2 | variable | Energy density of fluid 2 — energy density joule per cubic metre |
| p_1 | variable | Pressure of fluid 1 — pressure pascal |
| p_2 | variable | Pressure of fluid 2 — pressure pascal |
| H | variable | Hubble parameter — hubble parameter per second |
| Q | variable | Energy transfer rate between fluids — energy transfer rate joule per cubic metre per second |
| ˙ | operator | Derivative with respect to cosmic time — time derivative |
| σ | variable | Cross section — cross section metre squared |
| E | variable | Energy of the incident particle — energy joule |
| α | variable | Power-law exponent — dimensionless exponent |
| ∝ | operator | Proportional to, up to a constant factor — proportionality |











