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)
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.
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 =
$$\frac{\pi}{4}(0.406)^2=0.1295\ \text{m}^2$$
$$Q=8.4\times0.1295\times1320=\boxed{1435\ \text{kg per hole}}$$
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:
$$A=0.06(RMD+RDI+HF)=0.06(50+50+36.7)=\boxed{8.2}$$
Explosive-strength correction. Kuznetsov's equation is calibrated to
ANFO (RWS = 100); the standard correction for a different explosive is
$$\left(\frac{115}{RWS}\right)^{19/30}=\left(\frac{115}{92}\right)^{0.633}=1.152$$
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:
$$60=31.7\,K^{-0.8}\ \Rightarrow\ K^{-0.8}=1.891\ \Rightarrow\
K=1.891^{-1/0.8}=\boxed{0.45\ \text{kg/m}^3}$$
Quantity
Value
Charge mass per hole, Q
1435 kg
Rock factor, A (Lilly BI)
8.2
Explosive-strength correction (115/RWS)^0.633
1.15
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:
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.
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.
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.
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.