1969
DOI: 10.1243/pime_conf_1969_184_205_02
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Paper 33: Liquid Phase Movement in the Last Stages of Large Condensing Steam Turbines

Abstract: This paper deals with the generation and the movement of the liquid phase in the last stages of large condensing steam turbines. Considering thermodynamic instability, the primary droplet size resulting from spontaneous condensation is dependent on radial position, the flow, and inlet parameters. The analysis of the liquid phase transport to the blade surface is given, and the stability and disintegration of the liquid films on the blade surface is discussed.

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Cited by 7 publications
(4 citation statements)
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“…The simulation results of droplet movement and deposition in the ordinary blade were converted into a fitting equation and curve, which depicts a good agreement with the experimental data of Valha [14], shown in previous works [10]. This accordance verified the reliability of DPM in simulating droplet deposition.…”
Section: Ordinary Stationary Bladessupporting
confidence: 85%
“…The simulation results of droplet movement and deposition in the ordinary blade were converted into a fitting equation and curve, which depicts a good agreement with the experimental data of Valha [14], shown in previous works [10]. This accordance verified the reliability of DPM in simulating droplet deposition.…”
Section: Ordinary Stationary Bladessupporting
confidence: 85%
“…Figure 5 shows the percentage of deposition of secondary water droplets got by the numerical simulation in this paper and the experimental data by J. Valha [11]. From the figure, it can be seen that the trend of two is the same.…”
Section: Calculation Of Water Droplets Depositionmentioning
confidence: 85%
“…This behaviour is consistent with that described in Young et al 16 , and Valha. 21 It can also be seen from Figure 6 that the deposition rate of the secondary droplets on the downstream blade surface is dependent on the axial distance between two blade rows. A small distance usually leads to a large deposition rate on the downstream blade surface.…”
Section: Calculation Results and Analysismentioning
confidence: 86%
“…Then the maximum diameter of the secondary droplets d max at the trailing edge of a blade can be calculated by equation (10). In actuality, the diameter of the secondary droplets is in the form of a normal distribution, 21 so the mean diameter of the secondary droplets is defined as half of d max , that is d ¼ d max /2. After the average diameter of the secondary droplets is determined, their trajectories can be obtained by solving equation (3).…”
Section: Wetness Losses Calculationmentioning
confidence: 99%