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		<title>BridgetteGrazian at 10:18, 17 September 2025</title>
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		<updated>2025-09-17T10:18:55Z</updated>

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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 10:18, 17 September 2025&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l1&quot;&gt;Line 1:&lt;/td&gt;
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&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;br&amp;gt;If any kitchen &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;software might &lt;/del&gt;be considered addictive, it is a pair of &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;excessive&lt;/del&gt;-quality kitchen shears. 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All Misen Knife &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;products include &lt;/del&gt;a lifetime guarantee &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;towards &lt;/del&gt;defects. For all &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;products&lt;/del&gt;, we &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;are going to change &lt;/del&gt;any defective knives. Learn &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;more &lt;/del&gt;about our &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;warranty policy &lt;/del&gt;here and what&amp;#039;s &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;covered&lt;/del&gt;.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;Viscosity is a measure of a fluid&amp;#039;s &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;charge&lt;/del&gt;-dependent resistance to a change in &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;form &lt;/del&gt;or to motion of its neighboring portions relative to each other. For liquids, it corresponds to the informal &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;concept &lt;/del&gt;of thickness; for &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;example&lt;/del&gt;, syrup has &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;a higher &lt;/del&gt;viscosity than water. Viscosity is defined scientifically as a &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;drive &lt;/del&gt;multiplied by a time divided by an &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;area&lt;/del&gt;. Thus its SI models are newton-seconds per metre squared, or pascal-seconds. Viscosity quantifies the &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;inner &lt;/del&gt;frictional &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;drive &lt;/del&gt;between adjoining layers of fluid &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;which &lt;/del&gt;are in relative &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;movement&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;For instance&lt;/del&gt;, when a viscous fluid is &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;compelled through &lt;/del&gt;a tube, it flows more shortly close to the tube&amp;#039;s &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;center &lt;/del&gt;line than near its &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;partitions&lt;/del&gt;. Experiments &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;show &lt;/del&gt;that some stress (&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;resembling &lt;/del&gt;a &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;pressure difference &lt;/del&gt;between the two ends of the tube) is &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;needed &lt;/del&gt;to &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;sustain &lt;/del&gt;the &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;stream&lt;/del&gt;. It is because a &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;drive &lt;/del&gt;is required to beat the friction between the layers of the fluid &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;that &lt;/del&gt;are in relative &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;movement&lt;/del&gt;. For a tube with a &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;continuing fee &lt;/del&gt;of &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;move&lt;/del&gt;, the &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;strength &lt;/del&gt;of the compensating &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;drive &lt;/del&gt;is proportional to the fluid&amp;#039;s viscosity.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;On the whole&lt;/del&gt;, viscosity &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;will depend &lt;/del&gt;on a fluid&amp;#039;s state, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;reminiscent of &lt;/del&gt;its temperature, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;strain&lt;/del&gt;, and &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;charge &lt;/del&gt;of deformation. 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Viscum also referred to a viscous glue derived from mistletoe berries. In &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;supplies &lt;/del&gt;science and engineering, there is &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;commonly &lt;/del&gt;interest in understanding the forces or stresses involved &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;in &lt;/del&gt;the deformation of a &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;material&lt;/del&gt;.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;For instance&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; [https://omnideck.org/index.php/Scrap_Metal_Processing_Equipment Wood Ranger Power Shears website] &lt;/del&gt;if the &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;fabric were &lt;/del&gt;a simple spring, the &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;reply could &lt;/del&gt;be given by Hooke&amp;#039;s &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;regulation&lt;/del&gt;, which says that the &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;pressure skilled &lt;/del&gt;by a spring is proportional to the distance displaced from equilibrium. Stresses which &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;may &lt;/del&gt;be attributed to the deformation of a material from some rest state are &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;known as &lt;/del&gt;elastic stresses. In &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;different &lt;/del&gt;materials, stresses are &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;current &lt;/del&gt;which &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;might &lt;/del&gt;be attributed to the deformation &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;price &lt;/del&gt;over time. These are &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;known as &lt;/del&gt;viscous stresses. &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;For example&lt;/del&gt;, in a fluid &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;such as &lt;/del&gt;water the stresses which arise from shearing the fluid don&amp;#039;t &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;depend &lt;/del&gt;on the space the fluid has been sheared; &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;fairly&lt;/del&gt;, they depend &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;on &lt;/del&gt;how &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;quickly &lt;/del&gt;the shearing &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;happens&lt;/del&gt;. Viscosity is the &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;fabric &lt;/del&gt;property which relates the viscous stresses in a fabric to the &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;speed &lt;/del&gt;of change of a deformation (the &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;strain charge&lt;/del&gt;). 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An &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;external force &lt;/del&gt;is &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;due to this fact &lt;/del&gt;required so as to &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;keep &lt;/del&gt;the &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;top &lt;/del&gt;plate &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;moving &lt;/del&gt;at constant &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;speed&lt;/del&gt;. The proportionality issue is the dynamic viscosity of the fluid, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;often &lt;/del&gt;merely referred to &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;as &lt;/del&gt;the viscosity. It &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;is &lt;/del&gt;denoted by the Greek letter mu (μ). This expression is referred to as Newton&amp;#039;s law of viscosity. It &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;is &lt;/del&gt;a &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;special &lt;/del&gt;case of the &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;general &lt;/del&gt;definition of viscosity (see &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;under&lt;/del&gt;), which can be expressed in coordinate-free &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;type&lt;/del&gt;. In fluid dynamics, it is sometimes &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;more appropriate &lt;/del&gt;to work &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;when it comes to &lt;/del&gt;kinematic viscosity (&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;typically additionally known &lt;/del&gt;as the momentum diffusivity), defined as the ratio of the dynamic viscosity (μ) over the density of the fluid (ρ). 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In &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;materials &lt;/ins&gt;science and engineering, there is &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;often &lt;/ins&gt;interest in understanding the forces or stresses involved &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;within &lt;/ins&gt;the deformation of a &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;fabric&lt;/ins&gt;.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;As an illustration&lt;/ins&gt;, if the &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;material had been &lt;/ins&gt;a simple spring, the &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;answer can &lt;/ins&gt;be given by Hooke&amp;#039;s &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;legislation&lt;/ins&gt;, which says that the &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;drive experienced &lt;/ins&gt;by a spring is proportional to the distance displaced from equilibrium. Stresses which &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;will &lt;/ins&gt;be attributed to the deformation of a material from some rest state are &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;called &lt;/ins&gt;elastic stresses. In &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;other &lt;/ins&gt;materials, stresses are &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;present &lt;/ins&gt;which &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;may &lt;/ins&gt;be attributed to the deformation &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;charge &lt;/ins&gt;over time. 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Viscosity is the &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;material &lt;/ins&gt;property which relates the viscous stresses in a fabric to the &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;rate &lt;/ins&gt;of change of a deformation (the &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;pressure rate&lt;/ins&gt;). Although it applies to &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;general &lt;/ins&gt;flows, it is &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;easy &lt;/ins&gt;to visualize and &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;define &lt;/ins&gt;in a easy shearing &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;flow&lt;/ins&gt;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;akin to &lt;/ins&gt;a planar Couette &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;circulation&lt;/ins&gt;. 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An &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;exterior pressure &lt;/ins&gt;is &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;subsequently &lt;/ins&gt;required so as to &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;maintain &lt;/ins&gt;the &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;highest &lt;/ins&gt;plate &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;shifting &lt;/ins&gt;at constant &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;velocity&lt;/ins&gt;. The proportionality issue is the dynamic viscosity of the fluid, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;usually &lt;/ins&gt;merely referred to &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;because &lt;/ins&gt;the viscosity. It&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;#039;s &lt;/ins&gt;denoted by the Greek letter mu (μ). This expression is referred to as Newton&amp;#039;s law of viscosity. It&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;#039;s &lt;/ins&gt;a &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;particular &lt;/ins&gt;case of the &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;overall &lt;/ins&gt;definition of viscosity (see &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;beneath&lt;/ins&gt;), which can be expressed in coordinate-free &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;form&lt;/ins&gt;. In fluid dynamics, it is sometimes &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;extra applicable &lt;/ins&gt;to work &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;by way of &lt;/ins&gt;kinematic viscosity (&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;generally also referred to &lt;/ins&gt;as the momentum diffusivity), defined as the ratio of the dynamic viscosity (μ) over the density of the fluid (ρ). In very normal terms, the viscous stresses in a fluid are defined as these resulting from the relative velocity of &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;various &lt;/ins&gt;fluid particles.&amp;lt;br&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>BridgetteGrazian</name></author>
	</entry>
	<entry>
		<id>https://wiki.timero.com.br/index.php?title=Premium_Kitchen_Shears_For_Effortless_Cutting&amp;diff=199654&amp;oldid=prev</id>
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The word &amp;quot;viscosity&amp;quot; is derived from the Latin viscum (&amp;quot;mistletoe&amp;quot;). Viscum also referred to a viscous glue derived from mistletoe berries. In supplies science and engineering, there is commonly interest in understanding the forces or stresses involved in the deformation of a material.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;For instance,  [https://omnideck.org/index.php/Scrap_Metal_Processing_Equipment Wood Ranger Power Shears website] if the fabric were a simple spring, the reply could be given by Hooke&amp;#039;s regulation, which says that the pressure skilled by a spring is proportional to the distance displaced from equilibrium. Stresses which may be attributed to the deformation of a material from some rest state are known as elastic stresses. In different materials, stresses are current which might be attributed to the deformation price over time. These are known as viscous stresses. For example, in a fluid such as water the stresses which arise from shearing the fluid don&amp;#039;t depend on the space the fluid has been sheared; fairly, they depend on how quickly the shearing happens. Viscosity is the fabric property which relates the viscous stresses in a fabric to the speed of change of a deformation (the strain charge). Although it applies to normal flows, it is straightforward to visualize and outline in a easy shearing movement, reminiscent of a planar Couette move. Each layer of fluid moves quicker than the one simply below it, and friction between them provides rise to a [http://wiki.die-karte-bitte.de/index.php/Benutzer_Diskussion:NFQSang1732 Wood Ranger Power Shears website] resisting their relative movement.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;Specifically, the fluid applies on the top plate a force in the path reverse to its motion, and an equal but reverse drive on the underside plate. An external force is due to this fact required so as to keep the top plate moving at constant speed. The proportionality issue is the dynamic viscosity of the fluid, often merely referred to as the viscosity. It is denoted by the Greek letter mu (μ). This expression is referred to as Newton&amp;#039;s law of viscosity. It is a special case of the general definition of viscosity (see under), which can be expressed in coordinate-free type. In fluid dynamics, it is sometimes more appropriate to work when it comes to kinematic viscosity (typically additionally known as the momentum diffusivity), defined as the ratio of the dynamic viscosity (μ) over the density of the fluid (ρ). In very normal terms, the viscous stresses in a fluid are defined as these resulting from the relative velocity of different fluid particles.&amp;lt;br&amp;gt;&lt;/div&gt;</summary>
		<author><name>RhysSowers8</name></author>
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