Blasting (KCO): Difference between revisions
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== Description == | == Description == | ||
This article describes the '''Kuznetsov–Cunningham–Ouchterlony''' (KCO) model (Ouchterlony, 2005) | This article describes the '''Kuznetsov–Cunningham–Ouchterlony''' (KCO) model (Ouchterlony, 2005) for predicting rock fragmentation by blasting.{{Ouchterlony (2005)}} | ||
== Model theory == | == Model theory == | ||
{{ | === Swebrec distribution === | ||
[[File:BlastingKCO4.png|thumb|425px|Figure 1. Schematic of blast design geometry (after Bergman, 2005).{{Bergman (2005)}}]] | |||
The KCO model links blasting conditions to the particle size distribution of fragmented rock via the three-parameter [[Distributions#Swebrec|Swebrec function]]: | |||
:<math>P_i = \dfrac{1}{1 + \left [ \dfrac{\ln \left ( \dfrac{x_{\rm max}}{d_i} \right )}{\ln \left ( \dfrac{x_{\rm max}}{x_{50}} \right )} \right ]^b }</math> | |||
where: | |||
* <math>i</math> is the index of the size interval, <math>i = \{1,2,\dots,p\}</math>, <math>p</math> is the number of size intervals | |||
* <math>P_i</math> is the cumulative fraction passing size interval <math>i</math> | |||
* <math>d_i</math> is the size of the square mesh interval that mass is retained on (mm) | |||
* <math>d_{i+1}<d_i<d_{i-1}</math>, i.e. descending size order from top size (<math>d_{1}</math>) to sub mesh (<math>d_{p}=0</math> mm) | |||
* <math>x_{\rm max}</math> is the maximum (top) size of the distribution, i.e. the maximum block size (mm) | |||
* <math>x_{50}</math> is the mean size (passing 50%) of the distribution (mm) | |||
* <math>b</math> is a curve-undulation exponent. | |||
Figure 1 outlines the primary blast design dimensions relevant to the KCO model. | |||
=== Maximum block size, ''x''<sub>max</sub> === | |||
The maximum block size is the smallest value of the ''in situ'' block size, the blast-hole burden, <math>B</math>, and the spacing, <math>S</math>, (m), i.e.: | |||
:<math>x_{\rm max} = \min \{ \textit{in}\text{ }\textit{situ}\text{ block size}, S, B \}</math> | |||
=== Mean size parameter, ''x''<sub>50</sub> === | |||
The mean size of the distribution, <math>x_{50}</math> (mm), is estimated by: | |||
:<math>x_{50} = \dfrac{g(n) \cdot A \cdot Q^{\frac{1}{6}} \cdot \left (\dfrac{115}{s_{\rm ANFO}} \right )^{\frac{19}{30}}}{q^{0.8}} \cdot 10</math> | |||
where: | |||
* <math>A</math> is the rock mass factor | |||
* <math>Q</math> is the charge weight per hole (kg) | |||
* <math>s_{\rm ANFO}</math> is the explosive’s weight strength relative to ANFO (%) | |||
* <math>q</math> is the specific charge (kg/m<sup>3</sup>) | |||
* <math>g(n) = 1</math> is assumed | |||
* The 10 factor converts Ouchterlony's ''centimetre'' units to ''millimetres''. | |||
The rock mass factor, <math>A</math> is: | |||
:<math>A = 0.06 (\mathit{RMD} + \mathit{RDI} + \mathit{HF})</math> | |||
The rock mass description,<math>\mathit{RMD}</math>, is: | |||
:<math>\mathit{RMD} = | |||
\begin{cases} | |||
10 & \text{Powdery/friable}\\ | |||
\mathit{JF} & \text{Vertical joints}\\ | |||
50 & \text{Massive}\\ | |||
\end{cases} | |||
</math> | |||
The joint factor, <math>\mathit{JF}</math>, | |||
:<math>\mathit{JF} = \mathit{JPS} + \mathit{JPA}</math> | |||
where the joint plane spacing, <math>\mathit{JF}</math>, is related to the aversge joint spacing, <math>S_{\rm J}</math> (m), by: | |||
:<math>\mathit{JPS} = | |||
\begin{cases} | |||
10 & S_{\rm J}<0.1\text{ m}\\ | |||
20 & 0.1\text{ m}<S_{\rm J}\leq\text{oversize }x_{\rm o}\\ | |||
50 & S_{\rm J}>\text{oversize }x_{\rm o}\\ | |||
\end{cases} | |||
</math> | |||
The joint plane angle, <math>\mathit{JPA}</math>, is: | |||
:<math>\mathit{JPA} = | |||
\begin{cases} | |||
20 & \text{Dip out of face}\\ | |||
30 & \text{Strike perpendicular to face}\\ | |||
40 & \text{Dip into face}\\ | |||
\end{cases} | |||
</math> | |||
The rock density influence, <math>\mathit{RDI}</math>, is: | |||
:<math>\mathit{RDI} = 0.025 \rho - 50</math> | |||
where <math>\rho</math> is the rock density (kg/m<sup>3</sup>). | |||
The hardness factor, <math>\mathit{HF}</math>, is: | |||
:<math>\mathit{HF} = | |||
\begin{cases} | |||
\dfrac{E}{3} & E<50\\ | |||
\dfrac{\sigma_{\rm c}}{5} & E \geq 50\\ | |||
\end{cases} | |||
</math> | |||
where <math>E</math> is Young's Modulus (GPa) and <math>\sigma_{\rm c}</math> is the compressive strength of the rock (MPa). | |||
=== Curve-undulation exponent, ''b'' === | |||
The curve-undulation exponent <math>b</math> is determined from: | |||
:<math>b = \left [ 2 \ln 2 \cdot \ln \left ( \dfrac{x_{\rm max}}{x_{50}} \right ) \right ] \cdot n</math> | |||
where: | |||
:<math>n = \left (2.2 - \dfrac{0.014 B}{\varnothing_{\rm h}} \right ) \cdot \left (1 - \dfrac{\mathit{SD}}{B} \right ) \cdot \sqrt{\dfrac{\left( 1 + \dfrac{S}{B} \right )}{2}} \cdot \left [ \dfrac{\left\vert L_{\rm b} - L_{\rm c}\right\vert}{L_{\rm tot}} + 1 \right ]^{0.1} \cdot \left ( \dfrac{L_{\rm tot}}{H} \right )</math> | |||
and: | |||
* <math>\varnothing_{\rm h}</math> is the drill-hole diameter (m) | |||
* <math>L_{\rm b}</math> is the length of bottom charge (m) | |||
* <math>L_{\rm c}</math> is the length of column charge (m) | |||
* <math>L_{\rm tot}</math> is the total charge length (m) | |||
* <math>H</math> is the bench height or hole depth (m) | |||
* <math>\mathit{SD}</math> is the standard deviation of drilling accuracy (m). | |||
== Excel == | == Excel == | ||
The | The KCO blasting model may be invoked from the Excel formula bar with the following function call: | ||
<syntaxhighlight lang="vb">=mdUnit_Blasting_KCO(Parameters as Range, Size as Range)</syntaxhighlight> | <syntaxhighlight lang="vb">=mdUnit_Blasting_KCO(Parameters as Range, Size as Range)</syntaxhighlight> | ||
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B\text{ (m)}\\ | B\text{ (m)}\\ | ||
S\text{ (m)}\\ | S\text{ (m)}\\ | ||
\ | \varnothing_{\rm h}\text{ (m)}\\ | ||
L_{\rm b}\text{ (m)}\\ | L_{\rm b}\text{ (m)}\\ | ||
L_{\rm c}\text{ (m)}\\ | L_{\rm c}\text{ (m)}\\ | ||
L_{\rm Tot}\text{ (m)}\\ | L_{\rm Tot}\text{ (m)}\\ | ||
\ | \mathit{SD}\text{ (m)}\\ | ||
Q\text{ (kg)}\\ | Q\text{ (kg)}\\ | ||
q\text{ (kg/m}^3\text{)}\\ | q\text{ (kg/m}^3\text{)}\\ | ||
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\sigma_{\rm c}\text{ (MPa)}\\ | \sigma_{\rm c}\text{ (MPa)}\\ | ||
E\text{ (GPa)}\\ | E\text{ (GPa)}\\ | ||
\text{ | \textit{In}\text{ }\textit{situ}\text{ block size (m)}\\ | ||
\ | \mathit{RMD}\\ | ||
\end{bmatrix},\;\;\;\;\;\; | \end{bmatrix},\;\;\;\;\;\; | ||
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d_{1}\text{ (mm)}\\ | d_{1}\text{ (mm)}\\ | ||
\vdots\\ | \vdots\\ | ||
d_p\text{ (mm)}\\ | |||
\end{bmatrix} | \end{bmatrix} | ||
</math> | </math> | ||
=== Results === | === Results === | ||
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\begin{bmatrix} | \begin{bmatrix} | ||
\ | \mathit{RMD}\\ | ||
\mathit{RDI}\\ | |||
x_{\rm | \mathit{HF}\\ | ||
x_{\rm max}\text{ (mm)}\\ | |||
n\\ | n\\ | ||
g( | g(n)\\ | ||
x_{50}\text{ (mm)}\\ | x_{50}\text{ (mm)}\\ | ||
b\\ | b\\ | ||
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\begin{array}{c} | \begin{array}{c} | ||
\begin{bmatrix} | \begin{bmatrix} | ||
\mathit{ | \mathit{P}_1\text{ (w/w)}\\ | ||
\vdots\\ | \vdots\\ | ||
\mathit{ | \mathit{P}_p\text{ (w/w)} | ||
\end{bmatrix} | \end{bmatrix} | ||
\\ | \\ | ||
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\end{bmatrix} | \end{bmatrix} | ||
</math> | </math> | ||
=== Example === | === Example === | ||
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| [[File:BlastingKCO3.png|left|frame|Figure 3. Example showing the selection of the '''Results''' (light blue frame) array in Excel.]] | | [[File:BlastingKCO3.png|left|frame|Figure 3. Example showing the selection of the '''Results''' (light blue frame) array in Excel.]] | ||
|} | |} | ||
== See also == | |||
* [[Distributions#Swebrec|Distributions (Swebrec)]] | |||
== References == | == References == | ||
[[Category:Excel]] | [[Category:Excel]] |
Latest revision as of 04:12, 27 May 2024
Description
This article describes the Kuznetsov–Cunningham–Ouchterlony (KCO) model (Ouchterlony, 2005) for predicting rock fragmentation by blasting.[1]
Model theory
Swebrec distribution
The KCO model links blasting conditions to the particle size distribution of fragmented rock via the three-parameter Swebrec function:
where:
- is the index of the size interval, , is the number of size intervals
- is the cumulative fraction passing size interval
- is the size of the square mesh interval that mass is retained on (mm)
- , i.e. descending size order from top size () to sub mesh ( mm)
- is the maximum (top) size of the distribution, i.e. the maximum block size (mm)
- is the mean size (passing 50%) of the distribution (mm)
- is a curve-undulation exponent.
Figure 1 outlines the primary blast design dimensions relevant to the KCO model.
Maximum block size, xmax
The maximum block size is the smallest value of the in situ block size, the blast-hole burden, , and the spacing, , (m), i.e.:
Mean size parameter, x50
The mean size of the distribution, (mm), is estimated by:
where:
- is the rock mass factor
- is the charge weight per hole (kg)
- is the explosive’s weight strength relative to ANFO (%)
- is the specific charge (kg/m3)
- is assumed
- The 10 factor converts Ouchterlony's centimetre units to millimetres.
The rock mass factor, is:
The rock mass description,, is:
The joint factor, ,
where the joint plane spacing, , is related to the aversge joint spacing, (m), by:
The joint plane angle, , is:
The rock density influence, , is:
where is the rock density (kg/m3).
The hardness factor, , is:
where is Young's Modulus (GPa) and is the compressive strength of the rock (MPa).
Curve-undulation exponent, b
The curve-undulation exponent is determined from:
where:
and:
- is the drill-hole diameter (m)
- is the length of bottom charge (m)
- is the length of column charge (m)
- is the total charge length (m)
- is the bench height or hole depth (m)
- is the standard deviation of drilling accuracy (m).
Excel
The KCO blasting model may be invoked from the Excel formula bar with the following function call:
=mdUnit_Blasting_KCO(Parameters as Range, Size as Range)
Invoking the function with no arguments will print Help text associated with the model, including a link to this page.
Inputs
The required inputs are defined below in matrix notation with elements corresponding to cells in Excel row () x column () format:
Results
The results are displayed in Excel as an array corresponding to the matrix notation below:
Example
The images below show the selection of input arrays and output results in the Excel interface.