Fluid Mechanics
Pressure head in Bernoulli's equation is:
An ideal fluid flows in the pipe as shown in the figure. The pressure in the fluid at the bottom $${p}_{2}$$ is the same as it is at the top $${p}_{1}$$. If the velocity of the top $${ v }_{ 1 }=m/s$$. Then the ratio of areas $${A}_{1}$$. $${A}_{2}$$ is
$${ P }_{ 1 }+\dfrac { 1 }{ 2 } { \rho V }_{ 1 }^{ 2 }+0={ P }_{ 2 }+\dfrac { 1 }{ 2 } { \rho V }_{ 2 }^{ 2 }-\rho g\left( 3 \right) $$
$$\Rightarrow \frac { 4 }{ 2 } +30=\dfrac { 1 }{ 2 } { V }_{ 2 }^{ 2 }$$
$$\Rightarrow { V }_{ 2 }=8m/s$$
Now according to torrlcellis theorem
$${ A }_{ 1 }{ V }_{ 1 }={ A }_{ 2 }{ V }_{ 2 }$$
$$\dfrac { { A }_{ 1 } }{ { A }_{ 2 } } =\dfrac { 8 }{ 2 } =4:1$$
Pressure head in Bernoulli's equation is:
Bernoulli's equation is conservation of:
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