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Randall is incorrect in stating "Quarks only", since {{w|gluon}}s (the particle that carries the color force) are themselves colored. However, the colors of gluons are much more complicated, with a total of eight distinct superpositions of every possible color-anticolor pair. The fact that gluons are subject to the force they mediate also means that the strong force has a defined radius of effect, unlike the electromagnetic force, whose gauge bosons (the photon) are uncharged.
 
Randall is incorrect in stating "Quarks only", since {{w|gluon}}s (the particle that carries the color force) are themselves colored. However, the colors of gluons are much more complicated, with a total of eight distinct superpositions of every possible color-anticolor pair. The fact that gluons are subject to the force they mediate also means that the strong force has a defined radius of effect, unlike the electromagnetic force, whose gauge bosons (the photon) are uncharged.
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This is the last entry currently used to describe particles by particle physicists.
 
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| Mood
 
| Mood
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| Proof
 
| Proof
 
| [0,200]
 
| [0,200]
| This refers to {{w|alcohol proof}}, which is the measure of the amount of ethanol in a beverage by volume. In the United States, 100 proof correspond to 50% alcohol, so the proof of a beverage is two times the percentage of ethanol, so the maximum value is at most 200.
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| This refers to {{w|alcohol proof}}, which is the measure of the amount of ethanol in a beverage by volume. In the United States, 100 proof correspond to 50% alcohol, so the proof of a beverage is two times the percentage of ethanol, so the maximum value is 200.
 
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| Heat
 
| Heat
 
| No jalapeño icons - 3 jalapeño icons, increasing
 
| No jalapeño icons - 3 jalapeño icons, increasing
 
| Spicy dishes are sometimes measured by the intensity of the spicy flavor, usually ranging from values like "mild" to "hot". The gray jalapeño likely represents negligible or no spicy taste in the food. However, as an objective scale it is largely meaningless, since there is no reliable consistency in how these ratings are applied - what may be considered a 3-chilli dish in one establishment may only be a 1-chilli dish in another (as restaurants rarely if ever intend their dishes to be rated on the {{w|Scoville scale}}). The scale being unlimited may be a reference to the practice of some restaurants where a fourth or fifth chilli may be added to exaggerate the heat of their dishes.
 
| Spicy dishes are sometimes measured by the intensity of the spicy flavor, usually ranging from values like "mild" to "hot". The gray jalapeño likely represents negligible or no spicy taste in the food. However, as an objective scale it is largely meaningless, since there is no reliable consistency in how these ratings are applied - what may be considered a 3-chilli dish in one establishment may only be a 1-chilli dish in another (as restaurants rarely if ever intend their dishes to be rated on the {{w|Scoville scale}}). The scale being unlimited may be a reference to the practice of some restaurants where a fourth or fifth chilli may be added to exaggerate the heat of their dishes.
 
This measure of heat is unrelated to the particle's {{w|Thermodynamics|thermodynamic}} momentum.
 
 
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| Street value
 
| Street value
 
| [0,∞) in $
 
| [0,∞) in $
| The value of a good or service (particles are usually not services{{fact}}) in non-retail, non-wholesale transactions between individuals.
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| The value of an illegal good or a legal/controlled good when bought or sold by illegal means usually by or to the end user.
 
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| Entropy
 
| Entropy
 
| ''This already has like 20 different confusing meanings, so it probably means something here, too.''
 
| ''This already has like 20 different confusing meanings, so it probably means something here, too.''
| The term "entropy", which {{w|History of entropy|began}} as a {{w|Entropy (classical thermodynamics)|thermodynamic measure}}, has since been adopted {{w|Entropy in thermodynamics and information theory|by analogy}} into {{w|Entropy (disambiguation)|multiple seemingly unrelated domains}} including, for example, information theory. The table allows that the term "entropy" must mean something in the context of particle physics, but isn't certain whether it's the classical, Gibbs' modern {{w|Entropy (statistical thermodynamics)|statistical mechanics}}, Von Neumann's {{w|Von Neumann entropy|quantum entropy}}, or some other meaning.
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| The term "entropy", which {{w|History of entropy|began}} as a {{w|Entropy (classical thermodynamics)|thermodynamic measure}}, has since been adopted {{w|Entropy in thermodynamics and information theory|by analogy}} into {{w|Entropy (disambiguation)|multiple seemingly unrelated domains}}. The table doesn't seem to know what domain it is in, but (possibly in a desperate attempt to hide this) deems it safe to assume the unknown domain uses the term "entropy" for ''something''! Entropy is often described as a measure of disorder or chaos so this may be another reference to the D&D alignment axis above.
 
 
In classical thermodynamics, entropy is a macroscopic property describing the disorder or randomness of a system with many particles. However, in statistical mechanics and quantum mechanics, the concept of entropy can also be applied to single particles under certain conditions. If the particle's position is not precisely known and can be described by a probability distribution, this contributes to entropy. Similarly, if the particle's momentum is uncertain and described probabilistically, this also contributes to entropy. A single quantum particle in a pure state (e.g., an electron in a specific atomic orbital) has zero entropy. This is because there is no uncertainty about the state of the system. If the single particle's state is described by a density matrix representing a mixed state (a probabilistic mixture of several possible states), the Von Neumann entropy can quantify the degree of uncertainty or mixedness of the state.
 
 
 
Imagine two identical balloons filled with the same gas and heated from two opposite sides with identical heat sources, creating symmetric temperature gradients in both; because the distribution of temperatures is the same, the Gibbs statistical thermodynamic entropy 𝑆 of the gas molecule particles in each balloon will be the same. In contrast, if one balloon is heated by a low-power heat source and another by an otherwise identical high-power heat source, the balloon next to the high-power heat source will have a steeper temperature gradient, increasing the number of [https://www.sciencedirect.com/topics/mathematics/accessible-microstates accessible] {{w|Microstate|microstates}}, so the Gibbs entropy 𝑆<sub>low power</sub> < 𝑆<sub>high power</sub>. Now consider electrons in two atoms excited by absorbing identical photons to a mixed state; if the mixed states have the same probabilities for different energy levels, their Von Neumann quantum entropy 𝑆 values will be the same. Conversely, if one atom has electrons excited to a {{w|Purity_(quantum_mechanics)|pure state}} and another to a mixed state by photons of different energies, the mixed state will have higher entropy due to greater uncertainty, i.e., 𝑆<sub>pure</sub> = 0 and 0 < 𝑆<sub>mixed</sub> ≤ ln(2).
 
 
 
Please see also [[2318: Dynamic Entropy]].
 
 
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==Transcript==
 
==Transcript==
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{{incomplete transcript|Do NOT delete this tag too soon. Is table alone the best solution? Layout is still not standard.}}
 
:<big>Particle Properties in Physics</big>
 
:<big>Particle Properties in Physics</big>
 
{| class=wikitable
 
{| class=wikitable

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