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Revision as of 00:32, 16 December 2005 edit Falcorian (talk | contribs )Autopatrolled , Extended confirmed users , Pending changes reviewers , Rollbackers 10,010 edits Assisted clean up. Einstein --> Einstein . Also minor fixes.← Previous edit
Revision as of 01:40, 29 December 2005 edit undo Sadi Carnot (talk | contribs )8,673 editsm added the 3 thermo lawsNext edit →
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:*: <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 :
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