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mass transfer in multiphase systems - Greenleaf University

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MASS TRANSFER IN MULTIPHASE SYSTEMS: VOLATILE ORGANIC COMPOUND<br />

REMOVAL IN THREE-PHASE SYSTEMS<br />

This is because unit vector dot products: 1 and <br />

0 . Us<strong>in</strong>g the equations of cont<strong>in</strong>uity and<br />

i i i j<br />

equation of motion:<br />

v<br />

0<br />

(74)<br />

Dv<br />

2<br />

p v g<br />

(75)<br />

Dt<br />

With some rearrang<strong>in</strong>g, the follow<strong>in</strong>g is arrived at:<br />

<br />

g<br />

*<br />

Dv * * *2 * gD <br />

p v<br />

* 2 <br />

Dt Dv v g<br />

(76)<br />

The terms <strong>in</strong> brackets are reciprocals of the Reynolds (Re) number and Froude (Fr) number respectively.<br />

If <strong>in</strong> two different <strong>systems</strong> the scale factors are such that the Re and the Fr are the same, then both<br />

<strong>systems</strong> are described by identical dimensionless differential equations (Placeholder1). In addition, if the<br />

<strong>in</strong>itial and boundary conditions are the same, they are mathematically identical. Such <strong>systems</strong> are<br />

geometrically and dynamically similar and scale-up is easily done <strong>in</strong> that case.<br />

Another method used to elucidate dimensionless numbers. This is the Buck<strong>in</strong>gham Pi method of<br />

dimensional similarity. In the case of local liquid <strong>mass</strong> <strong>transfer</strong> as a function of its variables rose to<br />

different powers:<br />

k K v D d<br />

(77)<br />

L<br />

1<br />

<br />

AB<br />

Now by <strong>in</strong>sert<strong>in</strong>g the appropriate dimensions with<strong>in</strong> this assumed equation:<br />

<br />

2<br />

L L M M L<br />

<br />

K1 3 <br />

t t L Lt t <br />

<br />

L<br />

<br />

(78)<br />

There are three equations <strong>in</strong> L, M, and t respectively:<br />

1 3 2 <br />

(79)<br />

0 <br />

(80)<br />

1 <br />

(81)<br />

Elim<strong>in</strong>at<strong>in</strong>g some of the constant exponents and <strong>in</strong>sert<strong>in</strong>g back <strong>in</strong>to the orig<strong>in</strong>al equation for local <strong>mass</strong><br />

<strong>transfer</strong>:<br />

48

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