Difference between revisions of "Phantom cyclone"
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===Bond models=== |
===Bond models=== |
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+ | Fred Bond spends a lot of effort describing the shapes of particle size distribution curves in his Third Theory (Bond, 1952) and several earlier works. He sums up the intended shape of a size distribution for which is model is calibrated as: |
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− | Fred Bond |
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+ | ''Experience has shown that the average slope [...] of the size distribution percent passing [...] on a log-log plot of the percent passing against the sieve opening, is very close to <math>1 \over {\sqrt{2}}</math>'' <sup>[[Bibliography: Specific energy consumption models|Bond, 1952]]</sup> |
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+ | Bond also proposed this model of a particle size distribution: |
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+ | <math>Y = 80 \left( {{X}\over {P} } \right) ^ {1 \over {\sqrt{2}}}</math> |
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+ | where: |
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+ | ''Y'' is the percent passing a size ''X'' and ''P'' is the 80% passing size (all sizes in µm). |
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+ | Bond claims this model to be suitable for most of the crushing, rod milling and ball milling machines and applications that were surveyed by Bond and his colleagues in the 1940's and 1950's. |
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+ | ===SAG mills and HPGRs=== |
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+ | Autogenous and semi-autogenous grinding mills were not unknown during Bond's day, but they were relatively minor equipment that was used in a few boutique applications. The widespread adoption of SAG milling happened in the 1970's and 1980's, well after Bond's Third Theory was already established. High pressure grinding rolls (HPGR's) did not exist in a modern sense during Bond's day, and they were only adopted into the minerals industry from the very early part of the 21<sup>st</sup> century (although they existed earlier in the cement industry). |
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+ | The problem with SAG mills and HPGRs, from a modelling sense, is that their particle size distributions do not follow Bond's specification; both have more fines in their product stream than Bond's specification of an "average" size distribution. There are a variety of ways to describe this phenomenon; arguably the most common terms are the ''phantom cyclone effect'' in SAG milling and ''microcracking'' in HPGRs (which are treated as the same effect for power-modelling purposes). |
Revision as of 17:36, 14 April 2015
Phantom cyclone effect
SAG and AG mills produce more fines, as a proportion of the whole particle size distribution, than more classical comminution machines such as rod mills. This causes a problem for power-based models because only a single point (the 80% passing point) is used as a proxy to represent the whole particle size distribution, and the whole distribution is assumed to be "normal".
Bond models
Fred Bond spends a lot of effort describing the shapes of particle size distribution curves in his Third Theory (Bond, 1952) and several earlier works. He sums up the intended shape of a size distribution for which is model is calibrated as:
Experience has shown that the average slope [...] of the size distribution percent passing [...] on a log-log plot of the percent passing against the sieve opening, is very close to Bond, 1952
Bond also proposed this model of a particle size distribution:
where: Y is the percent passing a size X and P is the 80% passing size (all sizes in µm).
Bond claims this model to be suitable for most of the crushing, rod milling and ball milling machines and applications that were surveyed by Bond and his colleagues in the 1940's and 1950's.
SAG mills and HPGRs
Autogenous and semi-autogenous grinding mills were not unknown during Bond's day, but they were relatively minor equipment that was used in a few boutique applications. The widespread adoption of SAG milling happened in the 1970's and 1980's, well after Bond's Third Theory was already established. High pressure grinding rolls (HPGR's) did not exist in a modern sense during Bond's day, and they were only adopted into the minerals industry from the very early part of the 21st century (although they existed earlier in the cement industry).
The problem with SAG mills and HPGRs, from a modelling sense, is that their particle size distributions do not follow Bond's specification; both have more fines in their product stream than Bond's specification of an "average" size distribution. There are a variety of ways to describe this phenomenon; arguably the most common terms are the phantom cyclone effect in SAG milling and microcracking in HPGRs (which are treated as the same effect for power-modelling purposes).