Section 3.7.1.4: Flash Calculations with Fixed Relative Volatility

If the phase equilibrium properties of a mixture can be represented adequately by fixed relative volatilities, see notes here, then the equations describing a vapour-liquid `flash' system become particularly convenient to handle.

The situation is as illustrated in the diagram.



Specified Component Recovery

The simplest type of problem is when the recovery rj of one species j (usually in the vapour product) is given in terms of the ratio of:

flow of component in vapour : flow of same component in feed

If we write:

rj = vj / fj

Then we can calculate the ratio of vapour to liquid flows of the component:

sj = vj / lj

Using the component material balance equation:

fj = vj + lj

which with a bit of algebra gives:

sj = rj / (1 - rj)

From the definition of relative volatility and `K value':


\begin{displaymath}\alpha_{i,r} = \frac{K_i(T,P)}{ K_r(T,P)} = \frac{y_i/x_i}{y_r/x_r}
\end{displaymath}

If the total flow of e.g. the vapour stream is V then:

vi = V yi

So:

\begin{displaymath}\frac{v_i}{v_r} = \frac{V y_i}{V y_r} = \frac{v_i}{v_r}
\end{displaymath}

Hence, using this and the corresponding relationship for the liquid stream we can write:


\begin{displaymath}\alpha_{i,r} = \frac{v_i/l_i}{v_r/l_r}
\end{displaymath}

Problem 1

Show that for a two component flash this problem can be defined as follows:

In order to do this:


Specified Vapour Fraction

Let the total fraction of the feed which is vaporised be specified, i.e.:

Vs = V / F

In this case it is not possible to arrange the equations for direct solution. However, if the reference component recovery is assumed (or `torn') then the above procedure, and program, can be used to determine all component flows, and hence to calculate V/F, for the assumed rj

rj is then adjusted iteratively until the equations are satisfied, i.e. until:

\begin{displaymath}\phi = V_s - V/F = 0 \end{displaymath}

Problem 2

For the same two component mixture as above:


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