final report on the multiport dryer - Argonne National Laboratory
final report on the multiport dryer - Argonne National Laboratory
final report on the multiport dryer - Argonne National Laboratory
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22Average C<strong>on</strong>densing Heat Transfer Coefficient (W/m 2 K)2500020000150001000050000System Pressure = 170 kPa - 620 kPaQuality = 0.10 - 0.8020 25 30 35 40 45 50Mass Flux (kg/m 2 s)Fig. 8. Average c<strong>on</strong>densing heat transfer coefficients as functi<strong>on</strong> of mass fluxPressure Effect. In Fig. 9, <strong>the</strong> average c<strong>on</strong>densing heat transfer coefficient for each test isplotted as a functi<strong>on</strong> of <strong>the</strong> system pressure. It can be seen that <strong>the</strong> c<strong>on</strong>densing heat transfercoefficient is also approximately independent of system pressure over <strong>the</strong> experimental range of170-620 kPa (25-90 psi).Quality Effect. Figure 10, which is a plot of <strong>the</strong> local c<strong>on</strong>densing heat transfer coefficientsas a functi<strong>on</strong> of quality in a representative <strong>multiport</strong> channel, shows that <strong>the</strong> heat transfercoefficient is approximately c<strong>on</strong>stant as quality changes over <strong>the</strong> experimental range of 0.8-0.1.This trend was also observed previously in ANL c<strong>on</strong>densing tests with refrigerants at low flowrates. Although <strong>the</strong> heat transfer coefficient gradually reduces with <strong>the</strong> decrease of <strong>the</strong> qualityfrom 0.80 to 0.10, <strong>the</strong> reducti<strong>on</strong> is not large. In fact, <strong>the</strong> results of wall-temperaturemeasurements dem<strong>on</strong>strate that very good uniformity of cylinder wall temperature distributi<strong>on</strong>can be achieved with <strong>multiport</strong> cylinder <strong>dryer</strong> technology (see Fig. 11). Thus our experimentaldata would suggest that at low steam flow rates <strong>the</strong>re will not be a tendency for a wet streak todevelop in <strong>the</strong> sheet at <strong>on</strong>e end of <strong>the</strong> <strong>dryer</strong> cylinder.Pressure Gradient. Figure 12 shows <strong>the</strong> two-phase pressure gradient as a functi<strong>on</strong> of massflux. The test secti<strong>on</strong> pressure gradient is shown to be relatively low, primarily because of <strong>the</strong>low mass flow range of operati<strong>on</strong> in <strong>multiport</strong> cylinder <strong>dryer</strong>s. This means that for a 10-m (32.8-ft)-wide <strong>dryer</strong> shell and a mass flux of 50 kg m 2 s (36,867 lb ft 2 hr ), <strong>the</strong> total pressure dropwould be ≈15 kPa (2.2 psi). This is less than <strong>the</strong> maximum acceptable value of 27.6 kPa (4.0psi) for cylinder <strong>dryer</strong>s. These low pressure-gradient values translate into almost negligiblechange in saturati<strong>on</strong> temperature al<strong>on</strong>g <strong>the</strong> channels of <strong>multiport</strong> cylinder <strong>dryer</strong>s. (Note that <strong>the</strong>data scatter in Fig. 12 is a quality effect that is not taken into account in <strong>the</strong> figure.)