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the coking properties of coal at elevated pressures. - Argonne ...

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The absolute bubble velocity is given by<br />

The bubble diameter, db,.<strong>at</strong> <strong>the</strong> top <strong>of</strong> <strong>the</strong> bed was found by assuming an initial di-<br />

ameter equal to <strong>the</strong> spacing <strong>of</strong> <strong>the</strong> he<strong>at</strong> exchanger tubes, and growth according <strong>the</strong><br />

correl<strong>at</strong>ion <strong>of</strong> Mori and Wen (16). This result; with <strong>the</strong> assumed velocity distri-<br />

bution; Equ<strong>at</strong>ions 2, 8, and 9; and <strong>the</strong> appropri<strong>at</strong>e experimental d<strong>at</strong>a; provide <strong>the</strong><br />

inform<strong>at</strong>ion required to calcul<strong>at</strong>e <strong>the</strong> initial entrainment by Equ<strong>at</strong>ion 1. No assump-<br />

tion has been made regarding <strong>the</strong> source <strong>of</strong> <strong>the</strong> particles, i.e., whe<strong>the</strong>r <strong>the</strong>y orig-<br />

in<strong>at</strong>e in <strong>the</strong> wake or <strong>the</strong> cap <strong>of</strong> a bubble.<br />

Calcul<strong>at</strong>ion <strong>of</strong> Particle Density<br />

The equ<strong>at</strong>ion <strong>of</strong> motion <strong>of</strong> <strong>the</strong> particles is<br />

Subject to <strong>the</strong> initial conditions<br />

v = v <strong>at</strong>Z=O 11)<br />

s si<br />

The toral particle density pr<strong>of</strong>ile along <strong>the</strong> freeboard is obtained by summing<br />

up all <strong>the</strong> contributions from ascending and descending particles.<br />

(all particle sizes)<br />

(all initial velocities)<br />

The calcul<strong>at</strong>ion must be repe<strong>at</strong>ed 6000 times if <strong>the</strong> particle size range is div-<br />

ided into 60 intervals and <strong>the</strong> initial velocity distribution into 100 intervals.<br />

The Simplified Model<br />

In order to save computer time <strong>the</strong> model was simplified by neglecting <strong>the</strong><br />

transient term for small particles and <strong>the</strong> drag force term for large particles.<br />

equ<strong>at</strong>ions to be solved are <strong>the</strong>n:<br />

for small particles (u<br />

for large particles (u > u ),<br />

t- g<br />

which gives for ascending particles<br />

v S =<br />

J.’ si - 2gz (PS - Pg)<br />

246<br />

< ug), vs = ug - u t<br />

PS<br />

The

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