Stirred Mill (Power, Heath)
Description
This article describes the Heath et al. (2017) method for estimating the power draw of a castellated rotor High Intensity Grinding stirred mill (HIGmill).[1]
Model theory
Heath et al. (2017) proposed the following relationship for the power draw, [math]\displaystyle{ P }[/math] (kW), of a HIGmill with castellated rotors:[1]
- [math]\displaystyle{ P = k_1 \cdot n_{\rm d} {d_{\rm r}}^{k_2} {v_t}^{k_3} ( p_{\rm s,g} + k_4 p_{\rm s,c}) }[/math]
where:
- [math]\displaystyle{ n_{\rm d} }[/math] is the number of submerged discs
- [math]\displaystyle{ d_{\rm r} }[/math] is the rotor tip diameter (m)
- [math]\displaystyle{ v_{\rm t} }[/math] is the rotor tip velocity (m/s)
- [math]\displaystyle{ p_{\rm s,g} }[/math] is the solids pressure due to gravity (N/m2)
- [math]\displaystyle{ p_{\rm s,c} }[/math] is the solids pressure due to centrifugal force (N/m2)
and [math]\displaystyle{ k_1-k_4 }[/math] have the values shown in Table 1.
Coefficients and exponents of the Heath et al. power equation.[1] Coefficient or exponent Value [math]\displaystyle{ k_1 }[/math] 0.000197 [math]\displaystyle{ k_2 }[/math] 1.3 [math]\displaystyle{ k_3 }[/math] 0.8 [math]\displaystyle{ k_4 }[/math] 0.15
The solids pressure due to centrifugal force, [math]\displaystyle{ \rho_{\rm s,c} }[/math] (N/m2), is:
- [math]\displaystyle{ p_{\rm s,c} = \frac{4}{3} \pi^2 \omega^2 \left (\rho_{\rm b} - \rho_{\rm s} \right ) \left ({r_{\rm rotor}}^2 - {r_{\rm shaft}}^2 \right ) }[/math]
where:
- [math]\displaystyle{ \omega }[/math] is the rotation rate of the rotor (rps)
- [math]\displaystyle{ \rho_{\rm b} }[/math] is the density of the grinding beads (t/m3)
- [math]\displaystyle{ \rho_{\rm s} }[/math] is the density of slurry (t/m3)
- [math]\displaystyle{ r_{\rm rotor} }[/math] is the rotor tip radius (m), i.e [math]\displaystyle{ 0.5d_{\rm r} }[/math]
- [math]\displaystyle{ r_{\rm shaft} }[/math] is the rotor shaft radius (m)
The solids pressure due to gravity, [math]\displaystyle{ \rho_{\rm s,g} }[/math] (N/m2), is:
- [math]\displaystyle{ p_{\rm s,g} = \begin{cases} 0.5 g h_{\rm b} \left (\rho_{\rm b} - \rho_{\rm s} \right ) \left ( 1 - \dfrac{U_{\rm slip}}{U_{\rm rise}} \right ) & U_{\rm slip} \lt U_{\rm rise}\\ 0 & U_{\rm slip} \geq U_{\rm rise}\\ \end{cases} }[/math]
where:
- [math]\displaystyle{ h_{\rm b} }[/math] is the height of the bead bed (m)
- [math]\displaystyle{ U_{\rm slip} }[/math] is is the slip velocity (m/s)
- [math]\displaystyle{ U_{\rm rise} }[/math] is the rise velocity (m/s)
- [math]\displaystyle{ g }[/math] is acceleration due to gravity (m/s2)
The rise velocity, [math]\displaystyle{ U_{\rm rise} }[/math] (m/s) is:
- [math]\displaystyle{ U_{\rm rise} = \dfrac{Q}{\pi \left ( \dfrac{d_{\rm ID}}{2} \right )^2 (1 - \phi_{\rm m})} }[/math]
where:
- [math]\displaystyle{ Q }[/math] is the volumetric flow rate of slurry feed to the mill (m3/s)
- [math]\displaystyle{ d_{\rm ID} }[/math] is the internal diameter of the mill (m)
- [math]\displaystyle{ \phi_{\rm m} }[/math] is the fraction of the charge volume (i.e. bead bed) occupied by beads (v/v)
The slip velocity, [math]\displaystyle{ U_{\rm slip} }[/math] (m/s) is:
- [math]\displaystyle{ U_{\rm slip} = \dfrac{U_{\rm s} \phi_{\rm m}}{1 - \phi_{\rm m}} }[/math]
The Stokes settling rate, [math]\displaystyle{ U_{\rm slip} }[/math] (m/s), is determined from:
- [math]\displaystyle{ U_{\rm s} = \dfrac{ {d_{\rm b}}^2 g (\rho_{\rm b} - \rho_{\rm s} ) (1 - \phi_{\rm m})^{4.65} }{18 \mu \left ( 1 + 0.15 \mathrm{Re}^{0.687} \right )} }[/math]
and
- [math]\displaystyle{ \mathrm{Re} = \dfrac{ d_{\rm b} \rho_{\rm s} U_{\rm s}}{\mu} }[/math]
where:
- [math]\displaystyle{ d_{\rm b} }[/math] is the bead diameter (m)
- [math]\displaystyle{ \mu }[/math] is the slurry viscosity (N.s/m2)
The Reynolds number, [math]\displaystyle{ \mathrm{Re} }[/math], requires the settling velocity, [math]\displaystyle{ U_{\rm s} }[/math], which itself requires the Reynolds number. Therefore an iterating numerical solution is necessary to resolve the slip velocity.
Additional notes
The Heath et al. (2017) publication appears to contain a printing error, where the value of coefficient [math]\displaystyle{ k_4 }[/math] is inadvertently referred to as [math]\displaystyle{ k_2 }[/math].[1]
Furthermore, the coefficient [math]\displaystyle{ k_1 }[/math] appears twice, in both the equations for [math]\displaystyle{ P }[/math] and [math]\displaystyle{ p_{\rm s,c} }[/math].[1] The [math]\displaystyle{ p_{\rm s,c} }[/math] term itself also appears in [math]\displaystyle{ P }[/math] and is adjusted by [math]\displaystyle{ k_4 }[/math], making the [math]\displaystyle{ k_1 }[/math] repetition unusual, and somewhat redundant. It is probable that the presence of [math]\displaystyle{ k_1 }[/math] in the equation for [math]\displaystyle{ p_{\rm s,c} }[/math] is also a printing error and should be omitted. This is supported by application of the power model to industrial HIGmill specifications, which produces an appropriate result only with the equations as presented above.
Excel
The Heath HIG stirred mill power model may be invoked from the Excel formula bar with the following function call:
=mdMillPower_Heath(Parameters as Range)
Invoking the function with no arguments will print Help text associated with the model, including a link to this page.
The Parameters array and model results are defined below in matrix notation, along with an example image showing the selection of the same arrays in the Excel interface:
where:
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SysCAD
The Heath power model is an optional calculation for stirred mill units. If selected, the input and display parameters below are shown.
