Loveday/Barratt SAG model

History

Brian Loveday (1978) published a scale-up procedure for autogenous pilot plant power draw to industrial sized machines that used an empirical power number to encompass all the motion effects of a mill charge. Derek Barratt (2002) derived a set of power numbers for industrial machines for use in Loveday's base formula, where a power number for a particular mill filling and speed are read from a chart and then charge density, including the ball load, are fed into Loveday's formula to predict SAG mill power draw.

The power numbers that Barratt published are based on mills with 'typical' cone-ends (probably 15° to 25°). A flat-ended (shell-supported) mill is expected to have 5% less power draw.

Model Form

Loveday's equation is:

$P=P_N D^{2.5} L \rho_{charge}$

Where:

• P is the power evolved at the mill shell, kW
• P_N is the empirical power number read from the chart below
• D is the mill diameter inside the effective liner thickness, m
• L is the mill effective grinding length (or 'belly length'), m
• ρ_charge is the density of the mill charge, including balls, rocks and slurry, t/m³

The formula for ρ_charge is as follows:

$\rho_{charge} = \left[\tfrac{J_{balls}}{J_{total}} \rho_{balls} + \tfrac{J_{ore}}{J_{total}} \rho_{ore} \right] \times \left( 1- J_{voids} \right) + J_{voids} \rho_{pulp}$

Where:

• J_total is the fractional mill volumetric filling (eg. 0.30 for 30%)
• J_balls is the fractional volumetric filling of balls (eg. 0.10 for 10%)
• J_ore is the fractional volumetric filling of coarse ore (eg. J_total - J_balls)
• J_voids is the fractional volumetric void space between rocks and balls (use 0.4)
• ρ_balls is the density of the grinding balls, t/m³
• ρ_ore is the density of the ore, t/m³
• ρ_pulp is the density of the pulp, excluding rocks and balls, t/m³

Power Number Nomograph

source: Barratt & Sherman (2002)