Figures & data
Figure 2. Typical RDE flow field in a two-dimensional simulation a-fresh propellants; b-reaction products; c-reaction products from the previous cycle.
![Figure 2. Typical RDE flow field in a two-dimensional simulation a-fresh propellants; b-reaction products; c-reaction products from the previous cycle.](/cms/asset/89053a7a-e841-4247-8e03-5f34ca7a1cbb/tctm_a_1758346_f0002_oc.jpg)
Figure 5. Profiles of the flow field calculated by the one-step kinetic model (a) pressure; (b) temperature; (c) expansion slope; (d) Mach number.
![Figure 5. Profiles of the flow field calculated by the one-step kinetic model (a) pressure; (b) temperature; (c) expansion slope; (d) Mach number.](/cms/asset/24280e37-d437-45da-8019-46198c3d9715/tctm_a_1758346_f0005_oc.jpg)
Figure 7. Normalised velocity of detonation (colour and line labels) under the variation of the pre-detonation state, where
denotes
(a) with a constant temperature of 450 K; (b) with constant pressure 2 atm.
![Figure 7. Normalised velocity of detonation Dex/Dnon−ex (colour and line labels) under the variation of the pre-detonation state, where Σ denotes (dσ/dx)/σ0 (a) with a constant temperature of 450 K; (b) with constant pressure 2 atm.](/cms/asset/e93e60a6-e1d4-4103-8b0f-092b2923faaf/tctm_a_1758346_f0007_oc.jpg)
Figure 8. Comparison of the reaction rate when the pre-detonation temperature changes at 2 atm (a) reaction rate (b) extra work in reaction process in front of sonic point (In the p-v diagram, the extra work can be defined as the area between the leading shock process line and reaction-expansion process line shown in Fig. ).
![Figure 8. Comparison of the reaction rate when the pre-detonation temperature changes at 2 atm (a) reaction rate (b) extra work in reaction process in front of sonic point (In the p-v diagram, the extra work can be defined as the area between the leading shock process line and reaction-expansion process line shown in Fig. 6).](/cms/asset/029c4240-604d-4de4-ae77-12accb360f9c/tctm_a_1758346_f0008_oc.jpg)
Figure 9. Profiles of the flow field calculated by two-step kinetics model with pre-detonation (a) pressure; (b) temperature; (c) expansion slope; (d) Mach number.
![Figure 9. Profiles of the flow field calculated by two-step kinetics model with pre-detonation (a) pressure; (b) temperature; (c) expansion slope; (d) Mach number.](/cms/asset/790de56c-54b2-40af-846b-74b62e780b0d/tctm_a_1758346_f0009_oc.jpg)
Figure 10. Normalised velocity of detonation and equilibrium reaction progress parameter (colour and line labels) under the pre-detonation state variation, where denotes
(a) the normalised deficit of velocities
with a constant temperature of 450 K; (b) normalised deficit of velocities
with constant pressure of 2 atm; (c) equilibrium reaction progress parameter
with a constant temperature of 450 K; (d) equilibrium reaction progress parameter
with a constant pressure of 2 atm.
![Figure 10. Normalised velocity of detonation and equilibrium reaction progress parameter (colour and line labels) under the pre-detonation state variation, where Σ denotes (dσ/dx)/σ0 (a) the normalised deficit of velocities Dex/Dnon−ex with a constant temperature of 450 K; (b) normalised deficit of velocities Dex/Dnon−ex with constant pressure of 2 atm; (c) equilibrium reaction progress parameter λ with a constant temperature of 450 K; (d) equilibrium reaction progress parameter λ with a constant pressure of 2 atm.](/cms/asset/98397117-98d6-466e-bfe3-7559b4f0b6bf/tctm_a_1758346_f0010_oc.jpg)