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Discharge coefficient of the collector in Eq. (2).
The discharge coefficient also depended on turbulence in the flow.
The discharge coefficient is taken to be a varying parameter.
A new equation for the discharge coefficient is presented.
The experimental solar chimney discharge coefficient, Cd, was 0.52.
The discharge coefficient decreased about 2% with flow pulsation.
The simulated discharge coefficient values were compared with the calculated discharge coefficient values by the ISO empirical correlation.
For smaller sash opening angles the value of discharge coefficient was approaching unity and the discharge coefficient decreased with increase in the sash opening angle.
The discharge coefficient is a function of the pintle stroke, whereas the upstream and downstream pressures have rare influence on the discharge coefficient.
The effusion hole hole spacing has an effect on the discharge coefficient and the discharge coefficient commonly decreased with the increment of effusion hole hole spacing.
The real flow effects are included by means of an experimentally determined discharge coefficient.
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