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Article

Thermal hydraulic analysis of supercritical water reactor cooled by TiO2 nanofluid

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Pages 291-299 | Received 02 Oct 2018, Accepted 11 Jan 2019, Published online: 03 Feb 2019

Figures & data

Figure 1. Fuel bundle geometry [Citation9].

Figure 1. Fuel bundle geometry [Citation9].

Table 1. Major parameters of SCW-CANDU and channel reactor with supercritical pressure water [Citation10]

Table 2. Density-specific thermal conductivity of TiO2.

Figure 2. Pure water density at supercritical pressure 25 (MPa) compared with Ref. [Citation23].

Figure 2. Pure water density at supercritical pressure 25 (MPa) compared with Ref. [Citation23].

Figure 3. Pure water specific heat at supercritical pressure 25 (MPa) between current model and Ref. [Citation23].

Figure 3. Pure water specific heat at supercritical pressure 25 (MPa) between current model and Ref. [Citation23].

Figure 4. Pure water viscosity at supercritical pressure 25 (MPa) compared with Ref. [Citation23].

Figure 4. Pure water viscosity at supercritical pressure 25 (MPa) compared with Ref. [Citation23].

Figure 5. Coolant temperature distribution in axial direction compared with Ref. [Citation24] at ϕ 6%.

Figure 5. Coolant temperature distribution in axial direction compared with Ref. [Citation24] at ϕ 6%.

Figure 6. Coolant temperature distribution in axial direction compared with Ref. [Citation24] at ϕ 10%.

Figure 6. Coolant temperature distribution in axial direction compared with Ref. [Citation24] at ϕ 10%.

Table 3. Maximum coolant temperature difference between SCWR cooled with pure water and SCWR cooled with TiO2 -water nanofluid at P = 25 (MPa)

Figure 7. Coolant temperature at constant pressure 25 (MPa) different volume fractions of TiO2 particles.

Figure 7. Coolant temperature at constant pressure 25 (MPa) different volume fractions of TiO2 particles.

Table 4. Maximum coolant temperature difference between SCWR cooled with pure water and SCWR cooled with TiO2 -water nanofluid at P = 30 (MPa)

Figure 8. Coolant temperature at constant pressure 30 (MPa) different volume fractions of TiO2 particles.

Figure 8. Coolant temperature at constant pressure 30 (MPa) different volume fractions of TiO2 particles.

Table 5. Maximum coolant temperature difference between SCWR cooled with pure water and SCWR cooled with TiO2 -water nanofluid P = 35 (MPa)

Figure 9. Coolant temperature at constant pressure 35 (MPa) different volume fractions of TiO2 particles.

Figure 9. Coolant temperature at constant pressure 35 (MPa) different volume fractions of TiO2 particles.

Table 6. Maximum fuel temperature difference between SCWR cooled with pure water and SCWR cooled with TiO2-water nanofluid at P = 25 (MPa)

Figure 10. Fuel temperature at constant pressure 25 (MPa) different volume fractions of TiO2 particles.

Figure 10. Fuel temperature at constant pressure 25 (MPa) different volume fractions of TiO2 particles.

Figure 11. Fuel temperature at constant pressure 30 (MPa) different volume fractions of TiO2 particles.

Figure 11. Fuel temperature at constant pressure 30 (MPa) different volume fractions of TiO2 particles.

Table 7. Maximum fuel temperature difference between SCWR cooled with pure water and SCWR cooled with TiO2 -water nanofluid at P = 30 (MPa)

Figure 12. Fuel temperature at constant pressure 35 (MPa) different volume fractions of TiO2 particles.

Figure 12. Fuel temperature at constant pressure 35 (MPa) different volume fractions of TiO2 particles.

Table 8. Maximum fuel temperature difference between SCWR cooled with pure water and SCWR cooled with TiO2/water nanofluid at P =35 (MPa)

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