Analysis of Disruption of Airflow and Particle Distribution by Surgical Personnel and Lighting Fixture in Operating Rooms
Abstract
1. Introduction
1.1. Air Cleanliness
1.2. Air Distribution Systems of the Operating Room
- Laminar air flow (LAF);
- Turbulent mixed flow;
- Temperature-controlled airflow (TCAF).
1.2.1. Laminar Airflow
1.2.2. Turbulent Mixed Airflow
1.2.3. Temperature-Controlled Airflow
2. Methodology
2.1. CFD Modelling
2.1.1. Computational Domain and Modelling Assumptions
2.1.2. CFD Parameters
- Turbulence model: Realisable k–ε model with enhanced wall treatment.
- Discretisation schemes: Second-order upwind for momentum, energy, turbulence quantities; SIMPLE algorithm for pressure-velocity coupling.
- Gradient calculation: Least-squares cell-based.
- Gravity: −9.81 m·s−2 along the z axis.
- Meshing: Tetrahedron, refined at surfaces inside the LAF volume.
- ○
- Supply diffusers: Constant velocity inlet.
- ○
- Return diffusers: Outflow or pressure outlet boundary.
- ○
- Walls and equipment: No-slip adiabatic or prescribed heat flux (for heated components).
2.1.3. Grid Independence Study
2.1.4. Modelling of Equipment and Occupants
2.1.5. Modelling of Gaseous Contaminants
2.1.6. Modelling of Particle Tracking
2.1.7. Boundary Conditions
- Inlet air velocity, temperature, and pressure, which were varied across simulation cases to study airflow sensitivity.
- Outlet boundaries were defined using a pressure outlet condition.
- Thermal and metabolic heat loads applied to human and equipment surfaces were specified based on empirical values, as detailed in Table 3.
2.2. Field Measurement
3. Results and Discussion
3.1. Effect of Position of Surgical Lamp on Flow Distribution
3.2. Shape of Surgical Lamp on Flow Distribution
- A classic closed-shape lamp, and
- A semi-open shape featuring ventilation gaps between its structural elements.
- Figure 15 demonstrates that the airflow is markedly reduced beneath the closed lamp, leading to stagnation zones.
- Figure 16, on the other hand, shows that the semi-open lamp allows airflow to maintain its uniformity, with minimal distortion observed below the fixture.
3.3. Comparison of the Results with Literature
3.4. Modelling of Particle Tracking
3.5. Experimental Results
On-Site Measurement
3.6. Modelling of Contaminant Concentration Using Species Transport
- ➢
- Mass fraction of carbon dioxide in the air within the model,
- ➢
- The exhalation velocity of human beings lies in the range of 0.6–1.4 m/s. So, on average, 1 m/s is taken.
4. Conclusions
- Position 1: One lamp positioned above the patient’s bed and the other laterally above the surgical staff.
- Position 2: Both lamps placed directly above the patient, over the head and abdominal region.
Author Contributions
Funding
Data Availability Statement
Conflicts of Interest
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ISO CLASS | 0.1 μm | 0.2 μm | 0.3 μm | 0.5 μm | 1.0 μm | 5.0 μm |
---|---|---|---|---|---|---|
1 | 10 | 2 | - | - | - | - |
2 | 100 | 24 | 10 | 4 | - | - |
3 | 1000 | 237 | 102 | 35 | 8 | - |
4 | 10,000 | 2370 | 1020 | 352 | 83 | - |
5 | 100,000 | 23,700 | 10,200 | 3520 | 832 | 29 |
6 | 1,000,000 | 237,000 | 102,000 | 35,200 | 8320 | 293 |
7 | - | - | - | 352,000 | 83,200 | 2930 |
8 | - | - | - | 3,520,000 | 832,000 | 29,300 |
9 | - | - | - | 35,200,000 | 8,320,000 | 293,000 |
No. | Set | Nodes | Elements |
---|---|---|---|
1 | A | 92,776 | 488,978 |
2 | B | 91,138 | 479,564 |
3 | C | 89,395 | 470,395 |
4 | D | 87,291 | 465,236 |
Items | Dimensions | Heat Dissipation |
---|---|---|
Operating table | 1.9 × 0.6 × 0.85 m | None |
Surgical lights (1) | 0.5 m in diameter | 150 W each |
Surgical staff (2) | 0.3 × 0.25 × 1.7 m high | 100 W each |
Anaesthesia machine | 0.5 × 0.3 × 1.2 m high | 200 W |
Patient | 0.3 × 0.25 × 1.7 m high | 46 W |
Back table | 0.5 × 0.3 × 1.1 m high | None |
No. | Instrument Used | Specifications | |
---|---|---|---|
1 | Vane anemometer Testo-400 | measuring range +0.3 to +35 m/s, (−20 to +70 °C) | |
2 | Testo-480 | Accuracy (Temp) | ±0.2 °C (with high-precision probe) |
Accuracy (Humidity) | ±1.0% RH | ||
CO2 Measurement Range | 0 to 10,000 ppm | ||
Flow Velocity | 0 to 100 m/s (with pitot tube/anemometer probe) | ||
3 | IAQ Probe | Temperature—NTC | |
Measuring range—0 to +50 °C | |||
Accuracy—±0.5 °C | |||
Resolution—0.1 °C | |||
Humidity—Capacitive | |||
Measuring range | |||
0 to +100% RH | |||
Accuracy | |||
±(1.8% RH + 0.7% of mv) | |||
Resolution | |||
0.1% RH | |||
Absolute Pressure | |||
Measuring range | |||
+700 to +1100 hPa | |||
Accuracy ±3.0 hPa | |||
Resolution | |||
0.1 hPa | |||
Ambient CO2 | |||
Measuring range | |||
0 to +10,000 ppm | |||
Accuracy | |||
±(75 ppm + 3% of mv) | |||
±(150 ppm + 5% of mv) | |||
0 to +5000 ppm | |||
5001 to +10,000 ppm | |||
Resolution 1 ppm | |||
4 | Black globe thermometer | Thermocouple type K | |
Measuring range: 0 to +120 °C | |||
5 | Mini Laser Aerosol Spectrometer (Mini-LAS) 11-R | Count range: | |
1 to 2,000,000 particles/L | |||
Particle mass: | |||
From 0.1 μg/m3 to 100 mg/m3 | |||
Size channels: 31 channels |
Time Stamp | Runtime (s) | hPa Abs | hPa Diff | Velocity | Temp (°C) | RH (%) | hPa Abs | CO2 (ppm) | g/m3 |
---|---|---|---|---|---|---|---|---|---|
19:55:11 | 0 | 1005.7 | −0.006 | 1.0 | 22.9 | 80.5 | 1005.3 | 770 | 16.5 |
19:55:21 | 10 | 1005.7 | −0.006 | 1.0 | 23.0 | 80.8 | 1005.3 | 774 | 16.6 |
19:55:31 | 20 | 1005.7 | −0.006 | 1.0 | 23.0 | 80.4 | 1005.3 | 778 | 16.5 |
19:55:41 | 30 | 1005.7 | −0.006 | 1.0 | 23.0 | 80.5 | 1005.3 | 792 | 16.6 |
19:55:51 | 40 | 1005.7 | −0.006 | 1.0 | 23.0 | 80.1 | 1005.3 | 798 | 16.5 |
19:56:01 | 50 | 1005.7 | −0.006 | 1.0 | 23.0 | 80.1 | 1005.3 | 791 | 16.5 |
19:56:11 | 60 | 1005.7 | −0.006 | 1.0 | 23.0 | 80.2 | 1005.3 | 781 | 16.5 |
19:56:21 | 70 | 1005.7 | −0.006 | 1.0 | 23.1 | 80.1 | 1005.3 | 783 | 16.6 |
19:56:31 | 80 | 1005.8 | −0.006 | 1.0 | 23.1 | 80.2 | 1005.3 | 786 | 16.6 |
19:56:41 | 90 | 1005.8 | −0.006 | 1.0 | 23.1 | 80.4 | 1005.3 | 792 | 16.6 |
19:56:51 | 100 | 1005.8 | −0.006 | 1.0 | 23.1 | 80.2 | 1005.3 | 785 | 16.6 |
Time Stamp | Runtime (s) | hPa Abs | hPa Diff | Velocity | Temp (°C) | RH (%) | hPa Abs | CO2 (ppm) | g/m3 |
---|---|---|---|---|---|---|---|---|---|
20:10:23 | −1 | 1006.0 | −0.005 | 0.9 | 23.4 | 78.1 | 1005.5 | 755 | 16.5 |
20:10:33 | 9 | 1006.0 | −0.005 | 0.9 | 23.3 | 78.4 | 1005.5 | 756 | 16.5 |
20:10:43 | 19 | 1006.0 | −0.005 | 0.9 | 23.4 | 78.8 | 1005.6 | 765 | 16.6 |
20:10:53 | 29 | 1006.0 | −0.005 | 0.9 | 23.5 | 78.4 | 1005.6 | 761 | 16.6 |
20:11:03 | 39 | 1006.0 | −0.005 | 0.9 | 23.5 | 78.3 | 1005.6 | 770 | 16.5 |
20:11:13 | 49 | 1006.0 | −0.005 | 0.9 | 23.5 | 78.2 | 1005.5 | 773 | 16.5 |
20:11:23 | 59 | 1006.0 | −0.005 | 0.9 | 23.5 | 78.4 | 1005.6 | 770 | 16.6 |
20:11:33 | 69 | 1006.0 | −0.005 | 0.9 | 23.5 | 78.4 | 1005.5 | 770 | 16.6 |
20:11:43 | 79 | 1006.0 | −0.005 | 0.9 | 23.5 | 78.3 | 1005.6 | 770 | 16.6 |
20:11:53 | 89 | 1006.0 | −0.005 | 0.9 | 23.5 | 78.2 | 1005.6 | 774 | 16.6 |
20:12:03 | 99 | 1006.0 | −0.005 | 0.9 | 23.5 | 78.1 | 1005.6 | 768 | 16.6 |
0.25 µm | 0.28 µm | 0.30 µm | 0.35 µm | 0.40 µm | 0.45 µm | 0.50 µm |
---|---|---|---|---|---|---|
200 | 100 | 200 | 50 | 50 | 0 | 0 |
100 | 200 | 0 | 50 | 0 | 50 | 0 |
200 | 0 | 150 | 0 | 0 | 0 | 50 |
150 | 0 | 50 | 0 | 0 | 0 | 100 |
150 | 150 | 200 | 100 | 50 | 0 | 0 |
250 | 200 | 0 | 0 | 100 | 0 | 0 |
250 | 300 | 300 | 150 | 50 | 100 | 0 |
200 | 0 | 100 | 50 | 0 | 0 | 0 |
150 | 50 | 250 | 250 | 50 | 0 | 0 |
50 | 0 | 0 | 100 | 0 | 0 | 0 |
0.25 µm | 0.28 µm | 0.30 µm | 0.35 µm | 0.40 µm | 0.45 µm | 0.50 µm |
---|---|---|---|---|---|---|
700 | 150 | 300 | 100 | 0 | 0 | 0 |
150 | 200 | 100 | 0 | 0 | 0 | 0 |
200 | 150 | 100 | 150 | 0 | 0 | 0 |
250 | 150 | 250 | 250 | 50 | 0 | 0 |
200 | 150 | 200 | 200 | 50 | 0 | 0 |
200 | 150 | 150 | 50 | 0 | 0 | 0 |
150 | 150 | 100 | 150 | 0 | 50 | 0 |
200 | 200 | 100 | 0 | 0 | 50 | 0 |
350 | 150 | 200 | 200 | 50 | 0 | 100 |
250 | 150 | 200 | 50 | 0 | 50 | 0 |
0.25 µm | 0.28 µm | 0.30 µm | 0.35 µm | 0.40 µm | 0.45 µm | 0.50 µm |
---|---|---|---|---|---|---|
2850 | 1550 | 950 | 1000 | 350 | 100 | 50 |
2000 | 1650 | 1550 | 1500 | 100 | 50 | 50 |
2000 | 1850 | 1600 | 1150 | 250 | 300 | 100 |
2050 | 1450 | 1200 | 1050 | 300 | 50 | 50 |
2750 | 1950 | 1800 | 1200 | 400 | 150 | 150 |
2050 | 1500 | 1450 | 1000 | 300 | 50 | 150 |
1750 | 1350 | 950 | 1200 | 200 | 100 | 0 |
2050 | 1550 | 2000 | 1250 | 150 | 200 | 250 |
1650 | 1050 | 1450 | 1200 | 350 | 300 | 50 |
2150 | 1400 | 950 | 1100 | 500 | 100 | 100 |
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Valsala Krishnankutty, V.; Muraleedharan, C.; Palatel, A. Analysis of Disruption of Airflow and Particle Distribution by Surgical Personnel and Lighting Fixture in Operating Rooms. Fluids 2025, 10, 225. https://doi.org/10.3390/fluids10090225
Valsala Krishnankutty V, Muraleedharan C, Palatel A. Analysis of Disruption of Airflow and Particle Distribution by Surgical Personnel and Lighting Fixture in Operating Rooms. Fluids. 2025; 10(9):225. https://doi.org/10.3390/fluids10090225
Chicago/Turabian StyleValsala Krishnankutty, Vikas, Chandrasekharan Muraleedharan, and Arun Palatel. 2025. "Analysis of Disruption of Airflow and Particle Distribution by Surgical Personnel and Lighting Fixture in Operating Rooms" Fluids 10, no. 9: 225. https://doi.org/10.3390/fluids10090225
APA StyleValsala Krishnankutty, V., Muraleedharan, C., & Palatel, A. (2025). Analysis of Disruption of Airflow and Particle Distribution by Surgical Personnel and Lighting Fixture in Operating Rooms. Fluids, 10(9), 225. https://doi.org/10.3390/fluids10090225