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24-MMP-B2 Rock Fragmentation · December 2016

Question 2 of 6: Iron-Ore Powder-Factor Design and Pattern Tie-Ins

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

Notes on this paper

National Exams, 09-Mmp-B2 Rock Fragmentation, December 2016, 3 hours, closed book (one double-sided aid sheet permitted). Question 1 plus four (4) of Questions 2-6 constitute a complete paper; every question (1-6) is answered in full as a complete study resource.

Reference texts: Persson, Holmberg & Lee, Rock Blasting and Explosives Engineering; C.J. Konya & E.J. Walter, Rock Blasting and Overbreak Control (FHWA); ISEE, Blasters' Handbook, 18th ed.; W. Hustrulid, Blasting Principles for Open Pit Mining; SME Mining Engineering Handbook, 3rd ed., Ch. Drilling and Blasting; W.I. Duvall & C.F. Fogelson, USBM RI 5514 (cratering theory); D.E. Siskind et al., USBM RI 8507 (vibration/airblast).

Question 2: Iron-Ore Powder-Factor Design and Pattern Tie-Ins (21 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) Powder factor for 80% passing < 60 cm

Given.

QuantityValue
Borehole diameter, De406 mm
Bench height, H12 m
Subgrade (subdrill)1.0 m
Collar (stemming), T4.6 m
Explosive density, ρe1.32 g/cm³
Weight strength rel. ANFO, RWS92%
Rock density3.2 g/cm³
UCS300 MPa
Young's modulus, E110 GPa
Target 80% passing size, X80≤ 60 cm

Find. The powder factor (specific charge) K that limits the Kuznetsov mean fragment size to the 60 cm target.

Approach. Rate the rock via Lilly's Blastability Index (UCS and E are both given specifically to feed this), fix the per-hole charge mass from the given hole geometry (diameter, subdrill, collar – independent of burden/spacing), then invert the Kuz–Ram mean-fragmentation-size equation for the powder factor K that drives X to the 60 cm target. K is a single ratio (charge mass / rock volume per hole) so it can be solved directly without needing burden and spacing individually.

  1. Charge mass per hole (fixed by geometry, not by K). Total hole depth = H + subdrill = 12 + 1 = 13 m; charge (column) length = 13 − 4.6 = 8.4 m; hole area = $$\frac{\pi}{4}(0.406)^2=0.1295\ \text{m}^2$$ $$Q=8.4\times0.1295\times1320=\boxed{1435\ \text{kg per hole}}$$
  2. Rock factor A (Lilly's Blastability Index). Massive rock with no joint data given → RMD = 50, RDI = 50 (both at their competent-rock ceiling); UCS > 50 MPa → hardness factor HF = E(GPa)/3 = 110/3 = 36.7: $$A=0.06(RMD+RDI+HF)=0.06(50+50+36.7)=\boxed{8.2}$$
  3. Explosive-strength correction. Kuznetsov's equation is calibrated to ANFO (RWS = 100); the standard correction for a different explosive is $$\left(\frac{115}{RWS}\right)^{19/30}=\left(\frac{115}{92}\right)^{0.633}=1.152$$
  4. Invert Kuznetsov for K. Kuznetsov's mean-fragment-size equation (X in cm, V/Q in m³/kg, Q in kg) with K = Q/V (kg/m³, the powder factor): $$X=A\,K^{-0.8}Q^{1/6}\left(\frac{115}{RWS}\right)^{19/30}$$ $$Q^{1/6}=1435^{1/6}=3.36,\qquad A\cdot Q^{1/6}\cdot 1.152=8.2\times3.36\times1.152=31.7$$ Setting X = 60 cm and solving for K: $$60=31.7\,K^{-0.8}\ \Rightarrow\ K^{-0.8}=1.891\ \Rightarrow\ K=1.891^{-1/0.8}=\boxed{0.45\ \text{kg/m}^3}$$
QuantityValue
Charge mass per hole, Q1435 kg
Rock factor, A (Lilly BI)8.2
Explosive-strength correction (115/RWS)^0.6331.15
Required powder factor, K≈ 0.45 kg/m³

A powder factor of about 0.45 kg/m³ is a realistic value for a massive, hard (UCS 300 MPa) iron ore at this scale of blast – consistent with the rock being harder than average (A = 8.2, above the A≈7 baseline for average blastability), which is why a moderately higher-than-typical powder factor is needed to still hit a fine 60 cm target. Any combination of burden and spacing satisfying B×S = Q/(K×H) = 1435/(0.45×12) ≈ 266 m² per hole (e.g. B≈14.5 m, S≈18.3 m at the standard S/B≈1.26 ratio for a staggered pattern) delivers this powder factor for the given 406 mm hole geometry.

Check: Lilly's RMD/RDI are set to their "massive, no joint data" ceiling values per the established convention for this discipline (project precedent) because the question gives no RQD/joint-spacing data; the Kuz–Ram X here is used directly as the 80%-passing target (X80), the standard simplification when no burden/spacing/uniformity data is available to run the full Rosin–Rammler correction from X50 to X80.

(b) Tie-ins and delays for the Figure 1 pattern

Figure 1 shows a large multi-row pattern (roughly five rows by eighteen holes, staggered) free-faced along the top row shown in the figure. The governing tie-in principle is to fire each hole into the maximum relief created by the holes that fired immediately before it, while keeping the instantaneous charge per delay to a single hole (or single deck) so vibration and airblast are controlled per Q1(j)/(h). Recommended design:

  1. Initiation point and direction. Initiate from one corner of the pattern closest to the existing free face, so the blast can retreat diagonally across the full pattern – this gives every hole in every subsequent row a genuine, growing free face rather than firing rows simultaneously into an unrelieved bench.
  2. V1 (diagonal echelon) tie-in. Use surface trunklines connecting each hole to the next along diagonal lines (a "V1" pattern): hole-to-hole delay along the diagonal of 17–25 ms (comfortably above the ≈8 ms vibration/airblast simultaneity threshold, Q1(h)/(j)), with each successive diagonal row offset by one delay increment from its neighbour so the blast sweeps outward from the initiation corner in a widening V.
  3. Row-to-row lag. Ensure the last hole of a given diagonal fires with enough time lag relative to the first hole of the next diagonal (typically 25–42 ms row-to-row) for burden relief/face movement to develop, avoiding the "coarse fragmentation / high vibration" failure mode of firing an unrelieved row.
  4. Throw control. Angle the diagonal lines so muck is thrown toward the pattern's open/low side (away from haul roads or other infrastructure implied by the plan view), and keep the corner-most (least confined) holes on a slightly longer delay so they do not lead the round and throw material uncontrolled ahead of the main muckpile.
Check: exact hole count/spacing in Figure 1 is read approximately from the plan-view sketch (grid lines suggest roughly 4–5 m centre spacing); the tie-in LOGIC (diagonal V1 echelon from the free-face corner, 17–25 ms hole delay, 25–42 ms row lag) is the examinable content and is independent of the exact hole count.