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This article summarizes equations in the theory of fluid mechanics. Q.

F

b

=

f

V

i
m
m

g

=

F

g

{\displaystyle \mathbf {F} _{\mathrm {b} }=-\rho _{f}V_{\mathrm {imm} }\mathbf {g} =-\mathbf {F} _{\mathrm {g} }\,\!}

Apparent weight

W

a
p
p

=

W

F

b

{\displaystyle \mathbf {W} _{\mathrm {app} }=\mathbf {W} -\mathbf {F} _{\mathrm {b} }\,\!}

u

t

+

(

u

(

u

)

)

+

Visit This Link p
=
0

{\displaystyle {\frac {\partial \rho {\mathbf {u} }}{\partial t}}+\nabla \cdot \left(\mathbf {u} \otimes \left(\rho \mathbf {u} \right)\right)+\nabla p=0\,\!}

E

t

+

(

u

(

E
+
p

)

)

=
0

{\displaystyle {\frac {\partial E}{\partial t}}+\nabla \cdot \left(\mathbf {u} \left(E+p\right)\right)=0\,\!}

E
=

(

U
+

1
2

u

2

)

click to read

{\displaystyle E=\rho \left(U+{\frac {1}{2}}\mathbf {u} ^{2}\right)\,\!}

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