A cross section through a high pressure aero-engine compressor. Reprinted with permission from Owen et al., Aerospace 5(1), 32, 2018. Copyright 2018 Author(s), licensed under a Creative Commons Attribution (CC BY) license.

A cross section through a high pressure aero-engine compressor. Reprinted with permission from Owen et al., Aerospace 5(1), 32, 2018. Copyright 2018 Author(s), licensed under a Creative Commons Attribution (CC BY) license.

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Future gas turbine engines require improved understanding of the heat transfer between compressor discs and air in compressor cavities under transient operating conditions. Calculation of transient heat fluxes from temperature measurements on compressor discs is a typical ill-posed inverse problem where small uncertainties of measurements can lead...

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... added compression will decrease the height of blades in high-pressure compressors and will require much smaller tip clearances to maintain high efficiency and reliability. Figure 1 shows the structure of a typical aero-engine high pressure compressor. The tip clearance is governed by the relative expansion of the casing and the rotor. ...
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... and fast predictive methods are important for engine clearance decisions using combined thermo-mechanical models across the full operating flight envelope. Under cruise conditions, the shroud is hotter than the throughflow (see Fig. 1 Physics of Fluids ARTICLE scitation.org/journal/phf and shroud. However, at other points in the flight cycle, the shroud can become colder than the cob, and this suppresses buoyancy effects; here, stratified flow may form with heat transfer governed by conduction rather than convection. This large reduction of heat transfer, which ...
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... University of Sussex. The transient behavior of temperature was discussed, but the heat fluxes were not calculated. Though research on transient heat transfer on compressor disks is limited, there are a broad range of experimental, theoretical, and computational studies on steady-state heat transfer in different compressor cavities. As shown in Fig. 1, there are axial gaps between adjacent disk cobs and these are referred to as open cavities. In some compressors, the axial gaps do not exist, leaving closed spaces between the shroud, the two adjacent disk and a hub. These configurations, often found in industrial compressors, are referred to as closed cavities. This section focuses ...
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... disks were gradually cooled to a virtually isothermal condition. Figure 10(c) shows the history of the non-dimensional parameters Re / ; bDT, and Gr and v: as the transient progressed, bDT decreased and Re / was kept constant, leading to a decrease in Gr and an increase in v. Figure 11 shows the transient temperature and the variation of non-dimensional parameters for the other three Re / (cases A, C, and D). The temperature distributions for case A (Re / ¼ 7 Â 10 5 ) were similar to those for case B. However, at Re / > 2:1 Â 10 6 (cases C and D), the disks were remained heated at the end of the transient. ...
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... disks were gradually cooled to a virtually isothermal condition. Figure 10(c) shows the history of the non-dimensional parameters Re / ; bDT, and Gr and v: as the transient progressed, bDT decreased and Re / was kept constant, leading to a decrease in Gr and an increase in v. Figure 11 shows the transient temperature and the variation of non-dimensional parameters for the other three Re / (cases A, C, and D). The temperature distributions for case A (Re / ¼ 7 Â 10 5 ) were similar to those for case B. However, at Re / > 2:1 Â 10 6 (cases C and D), the disks were remained heated at the end of the transient. ...
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... radial location x à where / ¼ 0 indicates the radius where the disk temperature is equal to the core temperature. Figure 12(a) shows that at Fo < 0:022; x à decreases as Fo increases, leading to a decrease in h x à (the disk temperature at x à ) and, hence, the core temperature. As Fo approaches 0.16, the heat flux gradually decreases to virtually zero, which implies that the flow becomes stratified. ...
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... Fo approaches 0.16, the heat flux gradually decreases to virtually zero, which implies that the flow becomes stratified. Figure 13(b) shows the radial distributions of the heat fluxes and their 95% confidence intervals at different Fo numbers for case B. At Fo ¼ 0, the steady-state disk heat flux reaches zero at x à ¼ 0:7, which is consistent with experiments in Ref. 4. At Fo ¼ 0.02, the radial location is close to x a , showing a dramatic decrease in the core temperature. Though the disk temperature at x b decreases dramatically, the disk heat flux / b at Fo ¼ 0.02 remains at a value of 4. This implies a constant temperature difference between the core and the disk at x ¼ x b , which suggests that the response speed of the core is similar to that of the outer part of the disk and much faster than that of the inner part. ...
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... fluxes are positive at all radii when Fo > 0:04, which suggests that the core temperature becomes lower than the temperature of the disk. Figure 13 also presents the calculated heat flux distributions for cases A, C, and D. The fluxes / b at Fo ¼ 0 stay almost constant from case A to case C and decrease at case D, owing to the increase in the compressibility parameter v 0 (see Table II). The calculated heat fluxes for cases A and C show similar behavior to that for case B: the flow gradually moves away from the buoyancy-induced regime and becomes stratified. ...

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... Notably, Bohn et al. were pioneers in this field 19,20 , contributing significantly to the design and development of testing rigs to advance understanding in the domain. In response to these findings, considerable progress has been made in analytical modeling for sealed cavities, including the development of fast Bayesian models [21][22][23] and theoretical models for estimating heat transfer based on flat plate correlations 24,25 . These models reveal that the Nusselt number is strongly influenced by the radial distribution of disk temperature and compressibility effects 26,27 . ...
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