21-Mat-B1 Hydrometallurgy and Electrometallurgy · December 2013
Question 4 of 6: Stokes' Law: Equal-Settling-Velocity Particle Diameters
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. National Professional Examinations, December 2013 — 10-Met-B1, Mineral Processing. Three hours, closed book, approved Casio/Sharp calculator only. Six numbered Problems plus a two-mark Bonus Question; the rubric requires all problems except Problem 5, which is answered as any SIX of ten short sketch-and-describe topics. All ten topics of Problem 5 are answered below.
Note on the exam title
Nothing on the paper is a hydrometallurgy (leaching, solvent extraction, electrowinning) or electrometallurgy question; the syllabus actually examined is comminution and grinding-circuit mass balance, sampling theory, classification, gravity concentration and froth flotation — i.e. the physical/mechanical beneficiation stage that precedes hydro- or pyro-metallurgical extraction.
Reference texts. The answers below are keyed to the works normally recommended for this syllabus code:
B. A. Wills and J. A. Finch, Wills' Mineral Processing Technology, 8th ed. — comminution and Bond's law (Ch. 6), particle size analysis and sampling (Ch. 3–4), classification and hydrocyclones (Ch. 9), gravity concentration (Ch. 10), froth flotation (Ch. 12), dense-medium separation (Ch. 11).
P. M. Gy, Sampling of Particulate Materials: Theory and Practice — the Gy sampling-constant equation used in Question 1(e).
F. F. Aplan (ed.), SME Mineral Processing Handbook — flotation reagents (collectors, frothers, activators, depressants), flotation kinetics.
A. Taggart, Handbook of Mineral Dressing — classical terminology (probable error, imperfection, ratio of concentration, jigging, crusher types).
Given. Quartz: $d_q=30\ \mu\text{m}$, $\text{SG}_q=2.65$; Coal: $\text{SG}_c=1.4$; medium 1 = water ($\text{SG}=1.0$); medium 2 = air ($\text{SG}\approx0.0012$); both particles obey Stokes' law in each medium; same $g$, same $\mu$ within a given medium.
Find. The coal particle diameter $d_c$ that settles at the same velocity as the 30 µm quartz particle, first in water, then in air.
Approach. For two particles settling at the SAME velocity in the SAME medium, $g$ and $\mu$ (and $V$ itself) cancel between the two Stokes'-law expressions, leaving a simple ratio of $d^2(\text{SG}_{particle}-\text{SG}_{fluid})$ terms — the classical "equal-settling-ratio" concept used to size gravity/classification equipment for mixed-density feeds.
Part (a) — Settling in water. Equal velocity, same medium: $$d_q^2(\text{SG}_q-\text{SG}_w)=d_c^2(\text{SG}_c-\text{SG}_w)$$ $$d_c=d_q\sqrt{\dfrac{\text{SG}_q-\text{SG}_w}{\text{SG}_c-\text{SG}_w}}=30\sqrt{\dfrac{2.65-1.0}{1.4-1.0}}=30\sqrt{\dfrac{1.65}{0.40}}=30\sqrt{4.125}=30(2.031)$$ $$d_c=60.9\ \mu\text{m}$$ \(\boxed{d_c\approx60.9\ \mu\text{m (in water)}}\) — more than double the quartz diameter, because water's density (SG 1.0) subtracts a much larger FRACTION from coal's low density (1.4) than from quartz's (2.65), so the lighter coal particle must be substantially coarser to sink at the same rate.
Part (b) — Settling in air. Repeating with $\text{SG}_{air}\approx0.0012$ (negligible next to either solid, but carried through for completeness): $$d_c=30\sqrt{\dfrac{2.65-0.0012}{1.4-0.0012}}=30\sqrt{\dfrac{2.6488}{1.3988}}=30\sqrt{1.8935}=30(1.376)$$ $$d_c=41.3\ \mu\text{m}$$ \(\boxed{d_c\approx41.3\ \mu\text{m (in air)}}\) — a noticeably SMALLER equal-settling coal diameter than in water, because with the fluid density essentially negligible in both terms the ratio collapses toward $\sqrt{\text{SG}_q/\text{SG}_c}=\sqrt{2.65/1.4}=1.376$, whereas water's SG of 1.0 (comparable in size to both particle SGs) inflates the ratio by preferentially depressing the coal term.
Medium
Equal-settling coal diameter
(a) Water
60.9 µm
(b) Air
41.3 µm
Check: both results assume Stokes' (laminar, creeping-flow) drag applies to both particles in both media at these sizes — a reasonable assumption for tens-of-micron mineral/coal particles in water or air, since particle Reynolds numbers stay well below the Re ≈ 1 upper bound of the Stokes regime at these sizes and typical settling velocities.