VORTEX TUBE REFRIGERATION SYSTEM THEORY STEPS: πΆπππππππ ππ πππ ππ → ππ‘ππ‘ππππππ¦ πππππππ‘ππ πππππ‘ππ π π£πππ‘ππ₯(106 πππ) ↓ ↓ πβππ ππ’π‘ππ π£πππ‘ππ₯ πππππ βπππ‘ ππππ ππππππ¦ πππ π‘ ππ ππππππ π£πππ‘ππ₯ ππππ βππ‘ ππ₯βππ’π π‘ πππ ππ π£πππ‘ππ π‘βπππ’πβ ππ ππππ’π π‘ππππ π£πππ£π ↓ ↓ πβππ πππππ π£πππ‘ππ₯ πππ ππ ππππππ¦ ← π ππππππππ πππ ππππ€π ππππ π‘ππππ π‘βπ πππππππ‘ππ πβπ ππππππ πππ πππ π ππ π‘βπππ’πβ π‘βπ πππππππ‘ππ → ππ’πππ ππππππ πππ ππ₯ππ‘π π‘βπ π£πππ‘ππ₯ π‘π’ππ Vortex tube is a simpler (no moving parts) and non-conventional mechanical device that produce cooling (separates hotter and cold streams) when compressed air source is readily available. TEMPERATURE DROP: 100β (or 56β) below the inlet air temperature. The compressed air is entered into a swirl chamber which cools the air (adiabatic expansion of the gas) and the lost heat is transferred into kinetic energy and the chamber which is designed to swirl the air and produce vortex at high speed which facilitates the tangential entry into hot side. Some of the hot gas leaves the hot outlet and the rest of the gas turns towards the cold outlet which have low velocity because it lost heat at the outlet and that means low kinetic energy and the enthalpy becomes low. The low enthalpy cools the air and leave the colder outlet. πΉπΌπΊππ πΈ: πππ ππΈπ πππ΅πΈ If you observe the above figure at the end of the tube conical nozzle is placed to facilitate the outer shell of the vortex air escapes and the remaining air turn back to colder side. To study the vortex tube refrigeration, a long debate is going on between empirical approach and the approach relies on observations and experimental data. If we take empirical approach, “The vortex tube effect” is completely explained by Euler turbine equation that is., π− β βπ βββ ×πΜ π£ ππ = ππππ π‘ Where is the temperature at stagnation point of a fluid (stagnation temperature) π£ is absolute gas velocity observed from fixed reference frame π β is angular velocity of system πΜ is radial position of rotating gas ππ is isobaric heat capacity of working fluid Actually, the turbine equation more focuses on power output and not on turbine cooling which is of very few applications and due to complexity of the vortex flow, it only shows the aspects of the effect but not operating principle. On the other hand, the design based on experimental data. When it comes to experimental data many factors taken into account like geometrical shape of the vortex tube, turbulence, acoustic phenomena, pressure fields and air velocities. These all parameters are taken into account to optimize inlet, outlet components and the main tube variations. It will be more convincing to explain the operating principle clearly by validating via experimental studies available in the literature. πΉπΌπΊππ πΈ: ππππ πππ‘πππππ π πβππππ‘ To validate our result there are so many researches are done, and one of famous one is Stephen et al. (1983) expressed his result as: βππ (βππ )πππ₯ = 0.849 + 1.49π₯π − 4.505π₯π2 + 2.427π₯π3 βπ Where, (βπ ) π π πππ₯ a fraction that tells how much accurate our result is which is always < 1. π₯π is cold flow fraction or cold mass ratio is the ratio of the mass flow rate at the cold outlet πΜ π πΜ to that at the inlet πππ Μ , π₯π = π Μ π . ππ βπ And the optimized value of π₯π is 0.2 which gives (βπ ) π π πππ₯ ≈ 1. Some of the theoretical formulas usually encountered in refrigeration analysis in vortex tube: 1. The difference between the total temperatures at the inlet and cold outlet, βπ»π,πππ = π»ππ,πππ − π»πππ,πππ 2. Temperature efficiency, which compares the actual temperature decrease with that in the isentropic expansion process, βπ»π,πππ πΌπ» = πΈ−π π·π,πππ πΈ π»ππ,πππ [π − (π· ) ] ππ,πππ Where, ππ,π‘ππ‘ and πππ,π‘ππ‘ are the stagnation pressure values at the cold outlet and the inlet, respectively, and πΎ is the specific heat ratio of air. 3. Cooling capacity of the cold air, πΈΜ π = ππ πΜππ βπ»π,πππ Where, πΜ is the inlet (supplied) mass flow rate of air, and is the specific heat at constant pressure. 4. Coefficient of performance of the vortex tube as a refrigerator, (Eiamsa-ard and Promvonge, 2008), ππ ππ βπ»π,πππ πͺπΆπ·πΉ = πΈ−π π·ππ,πππ πΈ πΈ − π] πΈ − π πΉπ»ππ,πππ [( π·π,πππ ) References: https://www.vortec.com/vortex-tubes-video https://www.sciencedirect.com/science/article/abs/pii/S0140700719303792 https://www.sciencedirect.com/science/article/abs/pii/S0140700710002057 https://www.sciencedirect.com/science/article/pii/S2214157X19305404 Image sources: https://www.youtube.com/watch?v=Q_y2FvH2DHE https://en.wikipedia.org/wiki/File:Ranque-Hilsch_Vortex_Tube.svg https://www.sciencedirect.com/science/article/abs/pii/S0140700719303792