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VORTEX TUBE REFRIGERATION SYSTEM

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VORTEX TUBE REFRIGERATION SYSTEM
THEORY
STEPS: πΆπ‘œπ‘šπ‘π‘Ÿπ‘’π‘’π‘ π‘’π‘‘ π‘Žπ‘–π‘Ÿ 𝑖𝑛 → π‘†π‘‘π‘Žπ‘‘π‘–π‘œπ‘›π‘Žπ‘Ÿπ‘¦ π‘”π‘’π‘›π‘’π‘Ÿπ‘Žπ‘‘π‘œπ‘Ÿ π‘π‘Ÿπ‘’π‘Žπ‘‘π‘’π‘  π‘Ž π‘£π‘œπ‘Ÿπ‘‘π‘’π‘₯(106 π‘Ÿπ‘π‘š) ↓
↓ π‘‡β„Žπ‘–π‘  π‘œπ‘’π‘‘π‘’π‘Ÿ π‘£π‘œπ‘Ÿπ‘‘π‘’π‘₯ π‘”π‘Žπ‘–π‘›π‘  β„Žπ‘’π‘Žπ‘‘ π‘“π‘Ÿπ‘œπ‘š π‘’π‘›π‘’π‘Ÿπ‘”π‘¦ π‘™π‘œπ‘ π‘‘ 𝑖𝑛 π‘–π‘›π‘›π‘’π‘Ÿπ‘’ π‘£π‘œπ‘Ÿπ‘‘π‘’π‘₯
π‘†π‘œπ‘šπ‘’ β„Žπ‘œπ‘‘ 𝑒π‘₯β„Žπ‘Žπ‘’π‘ π‘‘ π‘Žπ‘–π‘Ÿ 𝑖𝑠 𝑣𝑒𝑛𝑑𝑒𝑑 π‘‘β„Žπ‘Ÿπ‘œπ‘’π‘”β„Ž π‘Žπ‘› π‘Žπ‘‘π‘—π‘’π‘ π‘‘π‘Žπ‘π‘™π‘’ π‘£π‘Žπ‘™π‘£π‘’ ↓
↓ π‘‡β„Žπ‘–π‘  π‘–π‘›π‘›π‘’π‘Ÿ π‘£π‘œπ‘Ÿπ‘‘π‘’π‘₯ π‘™π‘œπ‘ π‘’π‘  π‘’π‘›π‘’π‘Ÿπ‘”π‘¦ ← π‘…π‘’π‘šπ‘Žπ‘–π‘›π‘–π‘›π‘” π‘Žπ‘–π‘Ÿ π‘“π‘™π‘œπ‘€π‘  π‘π‘Žπ‘π‘˜ π‘‘π‘œπ‘Žπ‘Ÿπ‘‘ π‘‘β„Žπ‘’ π‘”π‘’π‘›π‘’π‘Ÿπ‘Žπ‘‘π‘œπ‘Ÿ
π‘‡β„Žπ‘’ π‘π‘œπ‘œπ‘™π‘’π‘‘ π‘Žπ‘–π‘Ÿ π‘π‘Žπ‘ π‘ π‘’π‘  π‘‘β„Žπ‘Ÿπ‘œπ‘’π‘”β„Ž π‘‘β„Žπ‘’ π‘”π‘’π‘›π‘’π‘Ÿπ‘Žπ‘‘π‘œπ‘Ÿ → π‘†π‘’π‘π‘’π‘Ÿ π‘π‘œπ‘œπ‘™π‘’π‘‘ π‘Žπ‘–π‘Ÿ 𝑒π‘₯𝑖𝑑𝑠 π‘‘β„Žπ‘’ π‘£π‘œπ‘Ÿπ‘‘π‘’π‘₯ 𝑑𝑒𝑏𝑒
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: 100℉ (or 56℃) 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.
πΉπΌπΊπ‘ˆπ‘…πΈ: 𝑉𝑂𝑅𝑇𝐸𝑋 π‘‡π‘ˆπ΅πΈ
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.,
𝑇−
βƒ— βˆ™πœ”
βƒ—βƒ—βƒ— ×π‘ŸΜ…
𝑣
𝑐𝑝
= π‘π‘œπ‘›π‘ π‘‘
Where is the temperature at stagnation point of a fluid (stagnation temperature)
𝑣 is absolute gas velocity observed from fixed reference frame
πœ”
βƒ— is angular velocity of system
π‘ŸΜ… is radial position of rotating gas
𝑐𝑝 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.
πΉπΌπΊπ‘ˆπ‘…πΈ: π‘€π‘œπ‘Ÿπ‘’ π‘‘π‘’π‘‘π‘Žπ‘–π‘™π‘’π‘‘ π‘ π‘β„Žπ‘’π‘šπ‘Žπ‘‘
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:
βˆ†π‘‡π‘
(βˆ†π‘‡π‘ )π‘šπ‘Žπ‘₯
= 0.849 + 1.49π‘₯𝑐 − 4.505π‘₯𝑐2 + 2.427π‘₯𝑐3
βˆ†π‘‡
Where, (βˆ†π‘‡ ) 𝑐
𝑐 π‘šπ‘Žπ‘₯
a fraction that tells how much accurate our result is which is always < 1.
π‘₯𝑐 is cold flow fraction or cold mass ratio is the ratio of the mass flow rate at the cold outlet π‘šΜ‡ 𝑐
π‘šΜ‡
to that at the inlet π‘šπ‘–π‘›
Μ‡ , π‘₯𝑐 = π‘š Μ‡ 𝑐 .
𝑖𝑛
βˆ†π‘‡
And the optimized value of π‘₯𝑐 is 0.2 which gives (βˆ†π‘‡ ) 𝑐
𝑐 π‘šπ‘Žπ‘₯
≈ 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,
βˆ†π‘»π’„,𝒕𝒐𝒕 = π‘»π’Šπ’,𝒕𝒐𝒕 − 𝑻𝒐𝒖𝒕,𝒕𝒐𝒕
2. Temperature efficiency, which compares the actual temperature decrease with that in
the isentropic expansion process,
βˆ†π‘»π’„,𝒕𝒐𝒕
πœΌπ‘» =
𝜸−𝟏
𝑷𝒄,𝒕𝒐𝒕 𝜸
π‘»π’Šπ’,𝒕𝒐𝒕 [𝟏 − (𝑷
) ]
π’Šπ’,𝒕𝒐𝒕
Where, 𝑃𝑐,π‘‘π‘œπ‘‘ and 𝑃𝑖𝑛,π‘‘π‘œπ‘‘ are the stagnation pressure values at the cold outlet and the
inlet, respectively, and 𝛾 is the specific heat ratio of air.
3. Cooling capacity of the cold air,
𝑸̇ 𝒄 = 𝒙𝒄 π’ŽΜ‡π’„π’‘ βˆ†π‘»π’„,𝒕𝒐𝒕
Where, π‘šΜ‡ 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),
𝒙𝒄 𝒄𝒑 βˆ†π‘»π’„,𝒕𝒐𝒕
π‘ͺ𝑢𝑷𝑹 =
𝜸−𝟏
π‘·π’Šπ’,𝒕𝒐𝒕 𝜸
𝜸
− 𝟏]
𝜸 − 𝟏 π‘Ήπ‘»π’Šπ’,𝒕𝒐𝒕 [( 𝑷𝒄,𝒕𝒐𝒕 )
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
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