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22-Agric-A6 Physical Properties of Biological Materials and Food Products · May 2017

Question 7 of 9: Particle-Size Averages from a Screen Analysis, and the Sphericity of a Cube

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format. 04-Agric-A6 Physical Properties of Biological Materials and Food Products, National Exams May 2017 — a three-hour closed-book exam (approved calculator permitted; one aid sheet, both sides). Nine questions are set and candidates answer any five, each worth 20 marks, for a 100-mark paper. All nine are worked here so the set is a complete study resource.

Reference texts. M.A. Rao, S.S.H. Rizvi, A.K. Datta and J. Ahmed, Engineering Properties of Foods, 4th ed. (rheology of fluid and semisolid foods, particle size, surface/interfacial properties); N.N. Mohsenin, Physical Properties of Plant and Animal Materials, 2nd ed. (thermal properties, calorimetry, texture and rheological testing); R.P. Singh and D.R. Heldman, Introduction to Food Engineering, 5th ed. (thermal-property measurement, freezing-point depression, particle size); J.F. Steffe, Rheological Methods in Food Process Engineering, 2nd ed. (viscometry, viscoelasticity, the Kelvin-Voigt/Maxwell models, time-dependent flow behaviour); R.L. Earle, Unit Operations in Food Processing, 2nd ed. (particle-size averages, specific surface from sieve/count data).

Question 7: Particle-Size Averages from a Screen Analysis, and the Sphericity of a Cube (20 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

(a) Given. The particle-count size distribution \((D_{pi},N_i)\) tabulated above; five size classes from 0.2 to 0.6 cm.

Find. The length mean diameter \(\bar D_L\), surface mean diameter \(\bar D_S\), and volume-surface (Sauter) mean diameter \(\bar D_{vs}\).

Approach. Each mean diameter is a different moment ratio of the same count distribution: the length mean is the first moment, the surface mean is the square root of the second moment, and the volume-surface mean is the ratio of the third to the second moment.

Worked size analysis
\(D_{pi}\), cm\(N_i\)\(N_iD_{pi}\)\(N_iD_{pi}^2\)\(N_iD_{pi}^3\)
0.230.600.1200.024
0.3123.601.0800.324
0.4208.003.2001.280
0.584.002.0001.000
0.621.200.7200.432
Σ4517.407.123.06
  1. Length mean diameter. $$\bar D_L = \frac{\sum N_iD_{pi}}{\sum N_i} = \frac{17.40}{45} = \boxed{0.3867\ \text{cm}}.$$
  2. Surface mean diameter. $$\bar D_S = \left(\frac{\sum N_iD_{pi}^2}{\sum N_i}\right)^{1/2} = \left(\frac{7.12}{45}\right)^{1/2} = \boxed{0.3978\ \text{cm}}.$$
  3. Volume-surface (Sauter) mean diameter. $$\bar D_{vs} = \frac{\sum N_iD_{pi}^3}{\sum N_iD_{pi}^2} = \frac{3.06}{7.12} = \boxed{0.4298\ \text{cm}}.$$ Each mean is built from a progressively higher moment of the distribution, so \(\bar D_L < \bar D_S < \bar D_{vs}\) here, exactly as expected — the Sauter mean weights the larger (0.4–0.6 cm) particles most heavily because it is dominated by the volume/surface ratio those particles contribute.
Final results — part (a)
QuantityValue
Length mean diameter, \(\bar D_L\)0.3867 cm
Surface mean diameter, \(\bar D_S\)0.3978 cm
Volume-surface (Sauter) mean diameter, \(\bar D_{vs}\)0.4298 cm

(b) Given. A cube of side length \(W\). Find. Its sphericity \(\phi\) (ratio of the surface area of a volume-equivalent sphere to the cube's own surface area). Approach. Find the diameter \(D_p\) of a sphere with the same volume as the cube, then compare surface areas.

  1. Equivalent sphere diameter. Equating volumes, $$\frac{\pi}{6}D_p^3 = W^3 \;\Rightarrow\; D_p = W\left(\frac{6}{\pi}\right)^{1/3}.$$
  2. Form the sphericity ratio. Sphericity is the equivalent sphere's surface area divided by the actual (cube) surface area: $$\phi = \frac{\pi D_p^2}{6W^2} = \frac{\pi\, W^2(6/\pi)^{2/3}}{6W^2} = \left(\frac{\pi}{6}\right)^{1/3} = \boxed{0.806}.$$ The cube's side length \(W\) cancels completely — sphericity is a pure shape factor, independent of size, exactly as it must be to compare particles of different sizes on their shape alone.
Final results — part (b)
QuantityValue
Sphericity of a cube, \(\phi\)0.806 (independent of \(W\))