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Rotary Drum Vacuum Filter (RDVF) Sizing & Cake Dewatering Calculator

Perform industrial solid-liquid separation modeling for continuous rotary drum vacuum filters. Calculate filtration rate, cake thickness, cycle time, drum speed, vacuum air requirements, and dry solids yield using Ruth and Darcy models.

1. Slurry & Filter Operating Parameters

wt%
Standard vacuum level: 50 - 70 kPa (15 - 21 inHg vacuum)
×10¹¹ m/kg ×10¹⁰ m⁻¹
% of drum
Standard submergence: 30% - 37.5%; high-submergence: up to 50%
D (m) W (m)
RPM
Cycle time $t_{cycle} = 60 / N$ seconds (typical 0.2 - 2.0 RPM)
✓ Diagnostic Summary Copied!

2. Filtration Yield & Dewatering Results

Total Drum Area ($A$)
18.85m²
Submerged Form Area
6.22m²
Cake Thickness ($L_{cake}$)
7.8mm
Cake Discharge Feasibility
Optimal (Knife Release)
Cycle Time ($t_{cycle}$)
80.0s
Cake Form Time ($t_{form}$)
26.4s
Dry Solids Yield
3.12tonne/h
Specific Solids Flux
165.5kg/m²·h
Filtrate Production ($Q_f$)
22.4m³/h
Vacuum Air Requirement
1,130Am³/h

First-Principles Mathematical Derivation of Rotary Drum Vacuum Filtration

Rotary drum vacuum filtration operates via unsteady-state cake deposition across continuously rotating, vacuum-manifolded sectors. Darcy's fundamental filtration law governs cake formation and hydraulic permeation.

1. Ruth Constant-Pressure Filtration Equation

Under a constant applied vacuum differential $\Delta P$, the instantaneous filtrate flux $d(V/A)/dt$ is impeded by cake resistance $R_c = \alpha \cdot c \cdot (V/A)$ and filter medium resistance $R_m$:

\frac{dt}{d(V/A)} = \frac{\mu \cdot \alpha \cdot c}{\Delta P} \left(\frac{V}{A}\right) + \frac{\mu \cdot R_m}{\Delta P}\n t_{form} = \frac{\mu \cdot \alpha \cdot c}{2 \Delta P} \left(\frac{V}{A}\right)^2 + \frac{\mu \cdot R_m}{\Delta P} \left(\frac{V}{A}\right)

Solving the quadratic for specific filtrate volume $(V/A)_{form}$ collected during the submerged period $t_{form} = \frac{60 \cdot \psi}{N}$ (seconds) establishes the cake mass deposited per cycle.

2. Cake Thickness & Solids Deposition

Dry solids mass deposited per square meter is $m_{dry} = c \cdot (V/A)_{form}$ ($kg/m^2$). The resulting wet cake thickness $L_{cake}$ depends on cake dry packing density $\rho_{dry}$ and porosity $\epsilon_{cake}$:

L_{cake} = \frac{m_{dry}}{\rho_{dry}} = \frac{c \cdot (V/A)_{form}}{\rho_{solid} (1 - \epsilon_{cake})}\quad [m]

3. Continuous Dry Solids Yield ($Y_{dry}$)

Total dry solids production rate ($kg/h$) accounts for total active drum area $A = \pi D W$ and rotational cycle frequency:

Y_{dry} = m_{dry} \cdot A \cdot \left( \frac{60 \cdot N}{60} \right) \cdot 60 = m_{dry} \cdot A \cdot N \cdot 60\quad [kg/h]

5 Fatal Traps & Engineering Pitfalls in RDVF Operation

1. Sub-Critical Cake Thickness & Scraper Smear Failure

Increasing drum speed (RPM) to chase higher throughput reduces submerged cake form time $t_{form}$. If cake thickness drops below $3\,\text{mm}$, the scraper knife cannot peel the cake; instead, it smears the slurry directly into cloth pores, causing total cloth blinding and cutting output by 90%.

2. Dewatering Cake Cracking & Vacuum Loss

Fine compressible slurries shrink during dry cycle vacuum dewatering, forming fissures that penetrate to the cloth. Air rushes into the cracked zones, dropping system vacuum across the entire drum manifold. Upstream sectors lose suction, discharging wet, sloppy cake into transport bins.

3. Trough Solids Stratification & Agitator Dead-Zones

Heavy mineral concentrates (iron ore, silica) settle rapidly in the slurry vat. Inadequate oscillating pendulum rake agitation allows coarse solids to form a hardened bed in the trough bottom. The drum begins scraping against settled solids, causing motor torque overload trips and ripped filter cloths.

4. Rotary Valve Bridge Seal Air Leakage

The internal rotary distributor valve separates vacuum form, wash, dry, and blow-off sectors using graphite/bronze wear bridge blocks. Operating without adequate lubricated seal flushing causes abrasive wear that allows atmospheric blow-off air to leak into the vacuum zones, destroying vacuum efficiency.

5. Filtrate Vacuum Receiver Barometric Leg Cavitation

If the filtrate receiver seal tank has an insufficient barometric drop leg height ($< 10.3\,\text{m}$ at sea level, or shorter at altitude), filtrate backs up into the vacuum pipework and floods the vacuum pump. Liquid slugging destroys liquid-ring vacuum pump impellers within seconds.

Frequently Asked Questions: Rotary Drum Vacuum Filtration

What is a Rotary Drum Vacuum Filter (RDVF) and how does it operate continuously? +
A Rotary Drum Vacuum Filter (RDVF) is a continuous solid-liquid separation machine widely used in chemical, mineral, pharmaceutical, and wastewater processing. A cloth-covered cylindrical drum rotates partially submerged (typically 30% to 37.5%) in a slurry trough. An internal automatic rotary valve applies vacuum to the submerged sectors, drawing liquid filtrate through the cloth while depositing solid particles as an expanding filter cake on the drum exterior. As the drum rotates out of the slurry, the cake undergoes washing and vacuum dewatering before being peeled off by a scraper knife, roll, or string discharge mechanism.
How does Ruth's filtration equation model parabolic cake growth? +
Filtration through a porous cake obeys Darcy's law integrated over time. Under constant vacuum differential ($\Delta P$), the filtrate volume per unit area ($V/A$) grows parabolically with time: $\frac{t}{V/A} = \frac{\mu \alpha c}{2 \Delta P} \left(\frac{V}{A}\right) + \frac{\mu R_m}{\Delta P}$, where $\mu$ is liquid dynamic viscosity, $\alpha$ is specific cake resistance ($m/kg$), $c$ is dry cake mass per unit volume of filtrate ($kg/m^3$), and $R_m$ is filter medium resistance ($m^{-1}$). In a continuous RDVF, form time is $t_{form} = \psi / N$, where $\psi$ is drum submergence fraction and $N$ is drum speed (RPM).
Why is minimum cake thickness critical for mechanical discharge? +
Each mechanical discharge method requires a minimum physical cake thickness to successfully release cake from the filter fabric. A standard scraper knife requires at least $3\text{--}5\,\text{mm}$ of cake thickness to peel cleanly without smearing; roll discharge requires $1\text{--}3\,\text{mm}$; string discharge requires $6\text{--}12\,\text{mm}$; and precoat systems can shave layers as thin as $0.05\text{--}0.2\,\text{mm}$. Running drum RPM too fast produces an ultra-thin cake that smears into cloth pores, causing blinding.
What causes cake cracking and vacuum loss in the dewatering zone? +
Compressible cakes composed of fine particles, gelatinous sludges, or pigments contract as pore liquid drains during the dry cycle. This shrinkage creates tensile stresses that tear vertical fissures and cracks through the cake. Once cracks propagate to the cloth, atmospheric air bypasses through the cracks into the vacuum chambers, collapsing drum vacuum levels from $60\,\text{kPa}$ down to $< 15\,\text{kPa}$ and leaving uncracked cake drenched with residual mother liquor.
How is vacuum pump airflow capacity sized for an RDVF system? +
Vacuum pump air displacement depends on air permeability through the dewatering cake and leakage through the rotary port valve. Industrial empirical sizing typically allocates $0.6\text{--}1.5\,\text{m}^3/\text{min}$ of actual air per square meter of total drum area ($2\text{--}5\,\text{CFM/ft}^2$) at operating vacuum (typically $50\text{--}70\,\text{kPa}$ vacuum or $15\text{--}20\,\text{inHg}$).

Frequently Asked Questions

What is a Rotary Drum Vacuum Filter (RDVF) and how does it operate continuously? +
How does Ruth's filtration equation model parabolic cake growth? +
Why is minimum cake thickness critical for mechanical discharge? +
What causes cake cracking and vacuum loss in the dewatering zone? +
How is vacuum pump airflow capacity sized for an RDVF system? +
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