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Unknown macro: {latex}

\large
$$
\left( {\Delta h_

Unknown macro: {FCM}

A_

Unknown macro: {float}

\rho g} \right)L_

Unknown macro: {float;lever;arm}

= \left( {\rho g\Delta h_

Unknown macro: {stock}

A_

Unknown macro: {orifice}

} \right)L_

Unknown macro: {valve;lever;arm}

$$

where

Unknown macro: {latex}

$\Delta h_

Unknown macro: {FCM}

$

is the change in depth of the liquid level in the constant head tank and

Unknown macro: {latex}

$A_

Unknown macro: {float}

$

is the cross sectional area of the cylindrical float. Thus

Unknown macro: {latex}

$\Delta h_

Unknown macro: {FCM}

A_

Unknown macro: {float}

$

is the submerged volume of the float that when multiplied by the density,

Unknown macro: {latex}

$\rho$

and by acceleration due to gravity is equal to the total buoyant force acting on the float. The lever arm for the float has a length

Unknown macro: {latex}

$L_

Unknown macro: {float;lever;arm}

$

. The moment acting to open the valve is provided by the pressure of liquid from the stock tank,

Unknown macro: {latex}

$\rho g\Delta h_

Unknown macro: {stock}

$

, acting over the area of the valve opening

Unknown macro: {latex}

$A_

Unknown macro: {orifice}

$

. The lever arm for the opening moment is

Unknown macro: {latex}

$A_

Unknown macro: {orifice}

$

Unknown macro: {latex}

The derivative of the function $f$ at the point $x_0$ is
\begin

Unknown macro: {equation}

f'(x_0) =
\lim_

Unknown macro: {x rightarrow x_0}

\frac

Unknown macro: {f(x) - f(x_0)}
Unknown macro: {x - x_0}

\end

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