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	<title>Direct and indirect realism - Revision history</title>
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		<title>Prab: CSV import</title>
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		<summary type="html">&lt;p&gt;CSV import&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;[[Image:Naive realism.jpg|thumb]] [[Image:Café wall.svg|thumb]] [[Image:Double-alaskan-rainbow.jpg|thumb]] [[Image:Rep-perception.jpg|thumb]] &amp;#039;&amp;#039;&amp;#039;Boltzmann Constant&amp;#039;&amp;#039;&amp;#039;&lt;br /&gt;
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The &amp;#039;&amp;#039;&amp;#039;Boltzmann constant&amp;#039;&amp;#039;&amp;#039; (symbol: \(k_B\) or \(k\)) is a physical constant that relates the average kinetic energy of particles in a gas with the temperature of the gas. It is a fundamental constant in [[physics]] that plays a crucial role in the field of [[statistical mechanics]], linking the microcosmic and macrocosmic worlds. The Boltzmann constant is named after the Austrian physicist [[Ludwig Boltzmann]], who made significant contributions to the theory of [[statistical mechanics]] during the 19th century.&lt;br /&gt;
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==Definition==&lt;br /&gt;
The Boltzmann constant is defined as the ratio of the [[gas constant]] \(R\) to the [[Avogadro constant]] \(N_A\):&lt;br /&gt;
\[k = \frac{R}{N_A}\]&lt;br /&gt;
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This relationship provides a bridge between macroscopic and microscopic physical quantities, connecting temperature, a macroscopic property, with the energies of particles, which are microscopic properties.&lt;br /&gt;
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==Value==&lt;br /&gt;
As of the latest standards, the value of the Boltzmann constant is exactly 1.380649 × 10^-23 joules per kelvin (J/K), following the redefinition of the [[SI base units]] in 2019, where the kelvin is now defined in terms of the Boltzmann constant.&lt;br /&gt;
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==Applications==&lt;br /&gt;
The Boltzmann constant appears in several fundamental equations in physics and chemistry, including the [[Boltzmann distribution]], which predicts the distribution of energy levels among particles in a system. It also appears in the [[Stefan-Boltzmann law]], relating the total energy radiated per unit surface area of a black body to the fourth power of its temperature, and in the definition of [[entropy]] in statistical mechanics.&lt;br /&gt;
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==Direct and Indirect Realism==&lt;br /&gt;
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Direct and indirect realism are philosophical concepts concerning the nature of [[perception]]. These theories address the fundamental question of how we can know the world around us and the extent to which our perceptions reflect reality.&lt;br /&gt;
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===Direct Realism===&lt;br /&gt;
Direct realism, also known as naive realism or common sense realism, posits that the world is as we perceive it; that is, objects exist in the world independently of our perception and are directly perceived by us without any intermediary. According to this view, the properties we observe in objects, such as color, texture, and shape, are present in the objects themselves.&lt;br /&gt;
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===Indirect Realism===&lt;br /&gt;
Indirect realism, on the other hand, suggests that we do not perceive the external world directly. Instead, our perception of the world is mediated by sensory information that is processed by our brain, which then constructs a representation of the external world. According to this view, the objects we perceive are not the objects themselves but rather a representation or a mental image of those objects.&lt;br /&gt;
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==Comparison and Debate==&lt;br /&gt;
The debate between direct and indirect realism is central to the philosophy of perception. Direct realism argues for a straightforward relationship between perception and reality, while indirect realism suggests a more complex process involving mental representation. Philosophers and scientists have explored these concepts to understand the nature of perception, the accuracy of our sensory experiences, and the implications for our knowledge of the external world.&lt;br /&gt;
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[[Category:Physics]]&lt;br /&gt;
[[Category:Philosophy of Mind]]&lt;br /&gt;
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		<author><name>Prab</name></author>
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