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Matter

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Matter

In classical physics and general chemistry, matter is any substance that has mass and takes up space by having volume. All everyday objects that can be touched are ultimately composed of atoms, which are made up of interacting subatomic particles. In everyday as well as scientific usage, matter generally includes atoms and anything made up of them, and any particles (or combination of particles) that act as if they have both rest mass and volume. However it does not include massless particles such as photons, or other energy phenomena or waves such as light or heat. Matter exists in various states (also known as phases). These include classical everyday phases such as solid, liquid, and gas – for example water exists as ice, liquid water, and gaseous steam – but other states are possible, including plasma, Bose–Einstein condensates, fermionic condensates, and quark–gluon plasma. Usually atoms can be imagined as a nucleus of protons and neutrons, and a surrounding "cloud" of orbiting electrons which "take up space". However, this is only somewhat correct because subatomic particles and their properties are governed by their quantum nature, which means they do not act as everyday objects appear to act – they can act like waves as well as particles, and they do not have well-defined sizes or positions. In the Standard Model of particle physics, matter is not a fundamental concept because the elementary constituents of atoms are quantum entities which do not have an inherent "size" or "volume" in any everyday sense of the word. Due to the exclusion principle and other fundamental interactions, some "point particles" known as fermions (quarks, leptons), and many composites and atoms, are effectively forced to keep a distance from other particles under everyday conditions; this creates the property of matter which appears to us as matter taking up space. For much of the history of the natural sciences, people have contemplated the exact nature of matter. The idea that matter was built of discrete building blocks, the so-called particulate theory of matter, appeared in both ancient Greece and ancient India. Early philosophers who proposed the particulate theory of matter include the Indian philosopher Kaṇāda (c. 6th century BCE), and the pre-Socratic Greek philosophers Leucippus (c. 490 BCE) and Democritus (c. 470–380 BCE).

Tables

Quark properties[36] · Structure › Quarks
up-type quarks
up-type quarks
name
up-type quarks
up
up
name
up
symbol
u
spin
1⁄2
electric charge(e)
+2⁄3
mass(MeV/c2)
1.5 to 3.3
mass comparable to
~ 5 electrons
antiparticle
antiup
antiparticlesymbol
u
charm
charm
name
charm
symbol
c
spin
1⁄2
electric charge(e)
+2⁄3
mass(MeV/c2)
1160 to 1340
mass comparable to
~ 1 proton
antiparticle
anticharm
antiparticlesymbol
c
top
top
name
top
symbol
t
spin
1⁄2
electric charge(e)
+2⁄3
mass(MeV/c2)
169,100 to 173,300
mass comparable to
~ 180 protons or~1 tungsten atom
antiparticle
antitop
antiparticlesymbol
t
down-type quarks
down-type quarks
name
down-type quarks
down
down
name
down
symbol
d
spin
1⁄2
electric charge(e)
−1⁄3
mass(MeV/c2)
3.5 to 6.0
mass comparable to
~10 electrons
antiparticle
antidown
antiparticlesymbol
d
strange
strange
name
strange
symbol
s
spin
1⁄2
electric charge(e)
−1⁄3
mass(MeV/c2)
70 to 130
mass comparable to
~ 200 electrons
antiparticle
antistrange
antiparticlesymbol
s
bottom
bottom
name
bottom
symbol
b
spin
1⁄2
electric charge(e)
−1⁄3
mass(MeV/c2)
4130 to 4370
mass comparable to
~ 5 protons
antiparticle
antibottom
antiparticlesymbol
b
name
symbol
spin
electric charge(e)
mass(MeV/c2)
mass comparable to
antiparticle
antiparticlesymbol
up-type quarks
up
u
1⁄2
+2⁄3
1.5 to 3.3
~ 5 electrons
antiup
u
charm
c
1⁄2
+2⁄3
1160 to 1340
~ 1 proton
anticharm
c
top
t
1⁄2
+2⁄3
169,100 to 173,300
~ 180 protons or~1 tungsten atom
antitop
t
down-type quarks
down
d
1⁄2
−1⁄3
3.5 to 6.0
~10 electrons
antidown
d
strange
s
1⁄2
−1⁄3
70 to 130
~ 200 electrons
antistrange
s
bottom
b
1⁄2
−1⁄3
4130 to 4370
~ 5 protons
antibottom
b
Lepton properties · Structure › Leptons
charged leptons
charged leptons
name
charged leptons
electron
electron
name
electron
symbol
e−
spin
1⁄2
electric charge(e)
−1
mass(MeV/c2)
0.5110
mass comparable to
1 electron
antiparticle
antielectron
antiparticlesymbol
e+
muon
muon
name
muon
symbol
μ−
spin
1⁄2
electric charge(e)
−1
mass(MeV/c2)
105.7
mass comparable to
~ 200 electrons
antiparticle
antimuon
antiparticlesymbol
μ+
tau
tau
name
tau
symbol
τ−
spin
1⁄2
electric charge(e)
−1
mass(MeV/c2)
1,777
mass comparable to
~ 2 protons
antiparticle
antitau
antiparticlesymbol
τ+
neutrinos
neutrinos
name
neutrinos
electron neutrino
electron neutrino
name
electron neutrino
symbol
νe
spin
1⁄2
electric charge(e)
0
mass(MeV/c2)
< 0.000460
mass comparable to
< 1⁄1000 electron
antiparticle
electron antineutrino
antiparticlesymbol
νe
muon neutrino
muon neutrino
name
muon neutrino
symbol
νμ
spin
1⁄2
electric charge(e)
0
mass(MeV/c2)
< 0.19
mass comparable to
< 1⁄2 electron
antiparticle
muon antineutrino
antiparticlesymbol
νμ
tau neutrino
tau neutrino
name
tau neutrino
symbol
ντ
spin
1⁄2
electric charge(e)
0
mass(MeV/c2)
< 18.2
mass comparable to
< 40 electrons
antiparticle
tau antineutrino
antiparticlesymbol
ντ
name
symbol
spin
electric charge(e)
mass(MeV/c2)
mass comparable to
antiparticle
antiparticlesymbol
charged leptons
electron
e−
1⁄2
−1
0.5110
1 electron
antielectron
e+
muon
μ−
1⁄2
−1
105.7
~ 200 electrons
antimuon
μ+
tau
τ−
1⁄2
−1
1,777
~ 2 protons
antitau
τ+
neutrinos
electron neutrino
νe
1⁄2
0
< 0.000460
< 1⁄1000 electron
electron antineutrino
νe
muon neutrino
νμ
1⁄2
0
< 0.19
< 1⁄2 electron
muon antineutrino
νμ
tau neutrino
ντ
1⁄2
0
< 18.2
< 40 electrons
tau antineutrino
ντ

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