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HYDROSTATIC PLUMBING LLC

a fluid cannot remain at rest under the presence of a shear stress . However · the fluid would move in the direction of the resulting force. Thus · the pressure on a fluid at rest is isotropic · i.e. · a force applied to a fluid in a pipe is transmitted · via the fluid · to the other end of the pipe. This principle was first formulated · in a slightly extended form · by Blaise Pascal · and is now called Pascal's law . &#91 · citation needed &#93 · Formulation [ edit ] In a fluid at rest · D u D t = &#x2212 · &#x2207 · [ p &#x2212 · &#x03B6 · ( &#x2207 · &#x22C5 · u ) ] + &#x2207 · { &#x03BC

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a fluid cannot remain at rest under the presence of a shear stress . However
the fluid would move in the direction of the resulting force. Thus
the pressure on a fluid at rest is isotropic
i.e.
a force applied to a fluid in a pipe is transmitted
via the fluid
to the other end of the pipe. This principle was first formulated
in a slightly extended form
by Blaise Pascal
and is now called Pascal's law . &#91
citation needed &#93
Formulation [ edit ] In a fluid at rest
D u D t = &#x2212
&#x2207
[ p &#x2212
&#x03B6
( &#x2207
&#x22C5
u ) ] + &#x2207
{ &#x03BC

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1 Medicine 3.2 Atmospheric pressure 4 Buoyancy Toggle Buoyancy subsection 4.1 Hydrostatic force on submerged surfaces 5 See also 6 References Toggle the table of contents Hydrostatic pressure 29 languages Asturianu Azərbaycanca Bosanski Català Čeština Deutsch Ελληνικά Esperanto Español Euskara Suomi Magyar Հայերեն Italiano 日本語 Қазақша 한국어 Latviešu Bahasa Melayu Nederlands Polski Русский Simple English Slovenčina Slovenščina Српски / srpski Українська Tiếng Việt 中文 Edit links Article Talk English

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