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Author’s note: This article consolidates publicly‑available data, standard test methods and practical calculations for engineers dealing with bulk‑solid handling. All numbers are order‑of‑magnitude values; actual figures depend on particle size distribution, moisture content and compaction level.
When a powder is stored, conveyed or discharged, air must move through the inter‑particle voids. The ease of that movement is described by permeability (k) – a material‑specific property that directly influences pressure drop, silo vent sizing, fluidised‑bed stability and the speed at which trapped air is expelled (deaeration rate).
Low‑permeability powders can cause pulsating flow, silo arching, or incomplete filling, while highly permeable powders may fluidise unintentionally, leading to dust emissions. Understanding and quantifying these properties is therefore essential for reliable plant design.
\( \displaystyle \Delta P = \frac{\mu \, L \, v}{k} \)
\( \displaystyle k = \frac{\varepsilon^{3}}{F\,(1-\varepsilon)^{2}} \; \frac{d_{p}^{2}}{180} \)
This semi‑empirical relation lets you estimate k from basic particle data when laboratory measurements are unavailable.
\( \displaystyle v_{a} = \frac{k \, \Delta P}{\mu \, L} \)
The time to deaerate a layer of thickness L is roughly t = L / vₐ.
(v_{a}) stands for the average air‑release velocity through the powder bed.
| Symbol | Meaning | Units |
|---|---|---|
| (v_{a}) | Average linear speed of the air that escapes from the pores of the consolidated powder. It tells you how fast the trapped air moves upward (or downward) per unit cross‑section of the bed. | meters per second (m s⁻¹) |
In practice, (v_{a}) is the effective superficial velocity of the gas that is driven by the pressure difference (\Delta P) across the powder layer of thickness (L).
The result (v_{a}) tells you how quickly the air will be expelled.
Often you care about the time needed to deaerate a given thickness. That is simply
[ t_{\text{deaeration}} = \frac{L}{v_{a}} ]
where (t) is in seconds if you keep (L) in metres and (v_{a}) in m s⁻¹.
[ v_{a}= \frac{1.3\times10^{-6}\times 2000}{1.85\times10^{-5}\times0.5} \approx 0.028;\text{m s}^{-1} ]
[ t = \frac{0.5}{0.028}\approx 18;\text{s} ]
So the air will leave the 0.5 m flour bed in roughly 18 seconds under those conditions.
Bottom line: (v_{a}) is the air‑release speed that results from the interplay of permeability, pressure drop, air viscosity, and bed thickness. Knowing it lets you size vents, choose fans, and predict how long a batch will need to “settle out” its trapped air before processing.
| Factor | Effect on k | Typical Range |
|---|---|---|
| Particle size (dₚ) | k ∝ dₚ² (larger particles → higher k) | 10 µm – 5 mm |
| Particle shape | Irregular shapes increase tortuosity → lower k | F ≈ 1–3 |
| Size distribution | Broad distributions can pack tighter → lower k | – |
| Bulk density / Compaction % | Higher compaction → lower porosity → lower k | 10 % – 50 % |
| Moisture / Cohesion | Capillary bridges reduce pore connectivity → lower k | – |
| Temperature | Viscosity μ decreases with T → apparent k rises | – |
Permeability is “a measure of how easily a powder is crossed by an air flow” – a definition repeated across industry resources.
| Method | Standard / Reference | Typical Sample Size | What It Gives |
|---|---|---|---|
| Steady‑state pressure‑drop cell | ASTM D8327‑24 (Freeman FT4) | 100 g – 500 g | Direct k (m²) at chosen consolidation |
| Gas pycnometer + Kozeny‑Carman | NIST‑recommended | 10 g | True density → porosity → estimated k |
| Dynamic flow tester (GranuPack) | Research papers (ScienceDirect) | 200 g | k vs. packing fraction, useful for process‑condition mapping |
| Air‑permeability probe (single‑point) | IEC 60404‑9 | Small plug | Quick screening, less precise |
Note : orders of magnitude only, of course variying depending on the actual specification of materials
| Material | Compaction % | Porosity ε | True ρ (kg m⁻³) | Bulk ρ (kg m⁻³) | Permeability k (×10⁻⁶ m²) | De‑aeration vₐ (×10⁻³ m s⁻¹) |
|---|---|---|---|---|---|---|
| Alumina – sandy | 17 | 0.62 | 3950 | 3270 | 0.42 | 19 |
| Barytes | 43 | 0.48 | 4500 | 2340 | 0.48 | 3.9 |
| Ordinary Portland Cement | 40 | 0.55 | 3150 | 1418 | 0.71 | 3 |
| Coal – granular (as‑supplied) | 14 | 0.70 | 1400 | 980 | 42 | 24 |
| Coal – degraded | 36 | 0.58 | 1400 | 620 | 1 | 2.9 |
| Coal – pulverised | 31 | 0.61 | 1400 | 730 | 0.53 | 4.3 |
| Copper concentrate | 30 | 0.57 | 3500 | 1505 | 0.33 | 9.8 |
| Fly ash – fine | 49 | 0.45 | 2300 | 1265 | 0.6 | 2 |
| Iron powder | 34 | 0.52 | 7800 | 4050 | 0.34 | 7 |
| Magnesium sulphate | 29 | 0.68 | 1700 | 550 | 6.3 | 17 |
| Polyethylene – pellets | 5 | 0.92 | 950 | 86 | 420 | 60 |
| Potassium chloride | 16 | 0.63 | 1910 | 714 | 11 | 26 |
| PVC – powder | 22 | 0.59 | 1400 | 574 | 1.2 | 8 |
| Silica sand | 12 | 0.66 | 2650 | 1760 | 3.9 | 34 |
| Wheat flour | 37 | 0.51 | 1500 | 735 | 1.3 | 6.2 |
| Zircon sand | 15 | 0.60 | 4700 | 1.3 | 10 |
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Given:
$$\Delta P = \frac{1.85\times10^{-5}\times 2 \times 0.2}{0.71\times10^{-6}} \approx 5.2\times10^{3}\,\text{Pa}\;(5.2\text{ kPa})$$
Interpretation: a vent rated for ≈ 6 kPa will comfortably handle the required airflow.
Assume a 0.5 m thick flour layer, ΔP = 2 kPa.
$$v_a = \frac{k\,\Delta P}{\mu L} = \frac{1.3\times10^{-6}\times 2000}{1.85\times10^{-5}\times0.5} \approx 0.028\;\text{m s}^{-1}$$
Time to purge the layer:
$$t = \frac{L}{v_a}= \frac{0.5}{0.028}\approx 18\;\text{s}$$
Only a few seconds of venting clear most trapped air – valuable for rapid batch changes.
Target mass flow = 5 kg s⁻¹, bulk density ≈ 800 kg m⁻³ (degraded coal).
Volumetric flow:
$$Q = \frac{\dot{m}}{\rho_b}= \frac{5}{800}=6.25\times10^{-3}\,\text{m}^3\!\!/\text{s}$$
Keeping pressure drop ≤ 10 kPa and using Darcy’s law, an iterative solution gives a pipe diameter of ≈ 80 mm.