Abstract
We carried out natural convection heat transfer experiments around upper domes varying truncation angles (θ = 90°, 70°, 50°, and 30°) over a wide range of Rayleigh number (RaDb = gβΔTDb3/αν, 2.63 × 109 ≤ RaDb ≤ 1.08 × 1013). The shape of a dome is close to the hemisphere as θ is 90° and to flat plate as θ is 0°. To achieve high RaDb condition, mass transfer experiments using H2SO4–CuSO4 copper electroplating system were employed. Mass transfer rates were measured by electric current, and flows were observed by the Particle Image Velocimetry (PIV). The measured average Nusselt number (NuDb = hmDb/k) increased as RaDb increased and as the θ decreased. The enhancement was more significant at lower RaDb values, which is attributed to variations in the location of flow transition to turbulence and separation. At a relatively low RaDb (1.08 × 1010), flow remains attached but undergoes an early transition to turbulence when the θ is small. Meanwhile, when the θ becomes large, flow separation occurs without prior transition. As RaDb increases, however, flow separation occurs irrespective of the θ. NuDb of dome with θ = 30° had 35 % higher than the dome with θ = 90° at RaDb = 1.08 × 1010 until 18 % higher at RaDb = 1.08 × 1013. The NuDb correlation for an upper dome was developed. This work contributes not only to a deeper phenomenological understanding of natural convection heat transfer around upper domes but to the application to passive cooling of SMR outer containments.
| Original language | English |
|---|---|
| Article number | 111548 |
| Journal | Experimental Thermal and Fluid Science |
| Volume | 169 |
| DOIs | |
| Publication status | Published - Dec 2025 |
Bibliographical note
Publisher Copyright:© 2025 Elsevier Inc.
Keywords
- Dome shape
- High Rayleigh number
- Natural convection
- Truncation angle
- Upper dome
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