Chemical & Process Industry

CFD Flow and Thermal Analysis of a Heated Tubular Reactor with Static Mixer

2024 Europe CFD · Thermal Analysis
Industry
Chemical Processing
Services
CFD & Thermal Analysis
Software
Ansys Fluent
Scenarios
4 operating conditions

The Challenge

A chemical processing company required an in-depth understanding of the flow behaviour and heat transfer performance inside a compact tubular reactor. The reactor, measuring 240 mm in length with a 20 mm inner diameter, contains a helical static mixer screw and a centrally placed thermocouple. The screw induces a whirling flow path that promotes mixing of the process fluid as it travels through the heated tube.

The client needed to validate the internal flow patterns and velocities, and determine how effectively the reactor transfers heat from the externally heated wall to the fluid under different operating conditions. Four scenarios were defined, combining two volume flow rates (6 ml/min and 19 ml/min) with two fluid viscosity values (0.3 mPa·s and 1 mPa·s). Understanding the interplay between flow rate, viscosity and heat transfer is essential for optimising the reactor's performance and scale-up potential.

CFD streamlines coloured by temperature inside a tubular reactor with static mixer, showing progressive heating from inlet to outlet
CFD streamlines coloured by flow temperature inside the reactor. The fluid enters at 200 °C (blue-green) and heats up progressively as it spirals through the static mixer toward the outlet (red).

Our Approach

We built a full 3D conjugate heat transfer model of the reactor in Ansys Fluent, including both the fluid domain and the solid components: the Inconel 625 outer tube and the S316L stainless steel helical screw. A conjugate heat transfer approach was essential because the thermal interaction between the heated tube wall, the metallic screw and the flowing fluid determines the actual temperature distribution inside the reactor.

Temperature-dependent fluid properties

The process fluid exhibits strongly temperature-dependent thermal properties. Between 60 °C and 600 °C, the density drops from 1,002 kg/m3 to 504 kg/m3, while the heat capacity nearly doubles from 1,678 J/kg·K to 3,497 J/kg·K. The thermal conductivity decreases by more than half over the same range. Each property was implemented as a polynomial fit derived from measured data points, ensuring the simulation faithfully captures how the fluid's behaviour changes as it heats up along the reactor length.

Calibrating the heat input against measurements

The reactor is heated by a 2,300 W thermal radiator surrounding the tube. However, due to the low emissivity of Inconel 625 (below 0.1) and unknown heat losses to the environment, only a fraction of this power reaches the fluid. The client provided a measured fluid temperature of 510 °C at 200 mm from the inlet for the 6 ml/min case with a 200 °C inlet temperature. Using an energy balance, the actual heat absorbed by the fluid was estimated at approximately 73 W — just 3% of the radiator's rated power. We tuned the applied heat load on the tube wall to 96.6 W to match this measurement point, then applied the same heat load to all four scenarios for a consistent comparison.

Laminar steady-state solver

Given the very low flow rates and small tube diameter, the Reynolds numbers in all scenarios are well below the turbulent transition threshold. A steady-state laminar solver was therefore appropriate, avoiding unnecessary computational cost while maintaining accuracy. The polyhedral mesh was refined around the helical screw surfaces to capture the complex spiralling flow path and the thermal boundary layers on the screw and tube walls.

3D geometry of the tubular reactor with Inconel 625 outer tube and S316L helical static mixer screw visible inside
Reactor geometry showing the Inconel 625 outer tube and the internal S316L helical screw. Fluid enters at the top right and exits at the bottom left.
Polyhedral mesh of the helical static mixer screw inside the tubular reactor, showing refined surface elements
Polyhedral mesh of the helical screw. Surface refinement captures the complex geometry that drives the whirling flow pattern.

Results

The streamline visualisations confirmed that the helical screw successfully induces a well-defined whirling flow throughout the reactor, with no significant dead zones or flow stagnation regions. The spiralling motion brings the fluid into repeated contact with the heated tube wall, which is exactly the mixing behaviour the static mixer is designed to achieve.

Effect of flow rate on outlet temperature

As expected, the flow rate has a decisive impact on the outlet temperature. At the lower flow rate of 6 ml/min, the fluid has more residence time in the heated zone, reaching an average outlet temperature of approximately 531 °C — well above the 510 °C measured at the 200 mm position. At the higher flow rate of 19 ml/min, the shorter residence time limits heating to an average outlet temperature of about 323 °C. Despite this temperature difference, the total heat absorbed by the fluid is marginally higher at the higher flow rate (approximately 81 W versus 80 W), indicating slightly improved convective heat transfer at the increased velocity.

Effect of viscosity on heat transfer

One of the most significant findings was that fluid viscosity has virtually no effect on the heat transfer efficiency. The temperature profiles and absorbed heat values were nearly identical between the 0.3 mPa·s and 1 mPa·s cases at the same flow rate. Viscosity primarily affects the pressure drop across the reactor and therefore the pumping power required, but both values remain very small and negligible in the overall energy balance.

CFD temperature contour plot on a longitudinal cross-section through the heated tubular reactor, showing progressive temperature increase from 200 degrees at the inlet to over 530 degrees at the outlet
Temperature contour plot on a longitudinal section through the reactor at 6 ml/min. The progressive heat-up from 200 °C (inlet, right) to over 530 °C (outlet, left) is clearly visible.
CFD velocity contour plot showing the whirling laminar flow distribution created by the helical static mixer screw inside the reactor
Velocity contour plot on a longitudinal section, showing the characteristic spiralling flow induced by the static mixer.
CFD temperature contour plots at four cross-sections along the reactor length at 0 mm, 120 mm, 200 mm and 240 mm, showing radial temperature uniformity improving downstream
Temperature distribution at four cross-sections along the reactor (0, 120, 200 and 240 mm from the inlet). The temperature becomes increasingly uniform toward the outlet.
531 °C
Outlet temperature at 6 ml/min
323 °C
Outlet temperature at 19 ml/min
4
Operating scenarios evaluated
~0%
Effect of viscosity on heat transfer

The cross-sectional temperature plots at 0, 120, 200 and 240 mm from the reactor inlet revealed how the thermal field evolves along the reactor length. At the inlet, a strong radial temperature gradient exists between the hot tube wall and the cooler core flow. By the outlet, the static mixer has redistributed the heat across the cross-section, significantly reducing the radial non-uniformity. This confirms that the helical screw is effective at promoting radial heat transport, a critical factor for achieving consistent product quality in chemical processing applications.

Value Delivered

This CFD analysis provided the client with validated, quantitative insight into the reactor's thermal-hydraulic performance across the full operating envelope. The calibrated model, anchored to a physical temperature measurement, gives confidence that the predicted temperatures and flow patterns are representative of real-world conditions.

The key finding that viscosity does not influence heat transfer efficiency simplifies the client's process design: they can adjust fluid viscosity to suit other process requirements without impacting the reactor's thermal performance. The detailed streamline and contour visualisations provide a clear understanding of the mixing quality achieved by the helical screw, which is directly relevant for future design optimisation — for example, adjusting the screw pitch, reactor length or heating power for different target temperatures and throughputs.

By combining CFD flow simulation with conjugate heat transfer analysis, we delivered a comprehensive performance characterisation in a single simulation campaign — a far more efficient and informative approach than iterative physical prototyping and testing.

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