Misplaced Pages

Laws of science: Difference between revisions

Article snapshot taken from Wikipedia with creative commons attribution-sharealike license. Give it a read and then ask your questions in the chat. We can research this topic together.
Browse history interactively← Previous editNext edit →Content deleted Content addedVisualWikitext
Revision as of 00:32, 16 December 2005 editFalcorian (talk | contribs)Autopatrolled, Extended confirmed users, Pending changes reviewers, Rollbackers10,010 edits Assisted clean up. Einstein --> Einstein. Also minor fixes.← Previous edit Revision as of 01:40, 29 December 2005 edit undoSadi Carnot (talk | contribs)8,673 editsm added the 3 thermo lawsNext edit →
Line 80: Line 80:
:*: <math> j^{\star} = \sigma T^4</math> :*: <math> j^{\star} = \sigma T^4</math>
''']''' ''']'''
:* ]
:* ]
:* ]
:* ] - sometimes called the ''Fourth Law of Thermodynamics'' :* ] - sometimes called the ''Fourth Law of Thermodynamics''
:*: <math> \mathbf{J}_{u} = L_{uu}\, \nabla(1/T) - L_{ur}\, \nabla(m/T) \!</math>; and :*: <math> \mathbf{J}_{u} = L_{uu}\, \nabla(1/T) - L_{ur}\, \nabla(m/T) \!</math>; and

Revision as of 01:40, 29 December 2005

This is a list of physical laws discovered by science. Bolded items are categories for the entries indented underneath instead of individual laws.

Einstein

Special Relativity
General Relativity

Newton

F = | q 1 q 2 | 4 π ϵ 0 r 2 {\displaystyle F={\frac {\left|q_{1}q_{2}\right|}{4\pi \epsilon _{0}r^{2}}}}
V = I R {\displaystyle V=IR}
Name Partial Differential form
Gauss's law : D = ρ {\displaystyle \nabla \cdot \mathbf {D} =\rho }
Gauss's law for magnetism: B = 0 {\displaystyle \nabla \cdot \mathbf {B} =0}
Faraday's law of induction: × E = B t {\displaystyle \nabla \times \mathbf {E} =-{\frac {\partial \mathbf {B} }{\partial t}}}
Ampere's law + Maxwell's extension: × H = J + D t {\displaystyle \nabla \times \mathbf {H} =\mathbf {J} +{\frac {\partial \mathbf {D} }{\partial t}}}
p + μ ( 2 u + 1 3 ( u ) ) + ρ u = ρ ( u t + u u ) {\displaystyle -\nabla p+\mu \left(\nabla ^{2}\mathbf {u} +{1 \over 3}\nabla (\nabla \cdot \mathbf {u} )\right)+\rho \mathbf {u} =\rho \left({\partial \mathbf {u} \over \partial t}+\mathbf {u} \cdot \nabla \mathbf {u} \right)}
Φ V = π r 4 8 η p l {\displaystyle \Phi _{V}={\pi r^{4} \over 8\eta }{\triangle p^{\star } \over l}}

Radiation laws

Thermodynamics

Quantum Mechanics

It is thought that the successful integration of Einstein's field equations with the uncertainty principle and Schrodinger equation, something no one has achieved so far with a testable theory, will lead to a theory of quantum gravity, the most basic physical law sought after today.

See also

Category: