A Multipollutant Smoke Emissions Sensing and Sampling Instrument Package for Unmanned Aircraft Systems: Development and Testing

Abstract

Poor air quality arising from prescribed and wildfire smoke emissions poses threats to human health and therefore must be taken into account for the planning and implementation of prescribed burns for reducing contemporary fuel loading and other management goals. To better understand how smoke properties vary as a function of fuel beds and environmental conditions, we developed and tested a compact portable instrument package that integrates direct air sampling with air quality and meteorology sensing, suitable for in situ data collection within burn units and as a payload on multi-rotor small unmanned aircraft systems (sUASs). Co-located sensors collect carbon dioxide, carbon monoxide, and particulate matter data at a sampling rate of ~0.5 Hz with a microcontroller-based system that includes independent data logging, power systems, radio telemetry, and global positioning system data. Sensor data facilitates precise remote canister collection of air samples suitable for laboratory analysis of volatile organic compounds (VOCs) and other major and trace gases. Instrument package specifications are compatible with common protocols for ground-based and airborne measurements. We present and discuss design specifications for the system and preliminary data collected in controlled burns at Tall Timbers Research Station, FL, USA and Sycan Marsh Preserve, OR, USA.

1. Introduction

Smoke from wildfires and prescribed fires degrades regional air quality and has consequences for human health [1], radiation budgets [2,3,4], and vegetation management activities used to reduce fire hazard and risk [5,6]. In recent decades, the impacts of smoke have piqued interest because of escalating wildfire activity due to climate warming and drought [7], and the widespread use of prescribed burning to reduce hazardous fuels. Emissions inventories estimate smoke production by pairing fuel consumption with emission factors—multiplication factors that convert the amount of fuel mass combustion to the amount of emissions released into the atmosphere [8,9]. Emissions factors for many gases and particulate matter (PM) remain uncertain and depend greatly on combustion processes that arise from the characteristics of fuel beds and weather conditions prior to and during burning [8,10]. Accurate emissions estimates from wildland fires are needed for reducing uncertainties in atmospheric chemical transport models and for improving predictions of fire effects on air quality [11,12].

Characterization and quantification of smoke emissions is difficult and complex due to the innate hazards associated with collecting measurements and samples in and near open burning areas, and also because smoke is highly dynamic in space and time. Laboratory burning is often favored due to safety and the practical convenience associated with combusting fuel and collecting smoke near precision instrumentation. However, laboratory conditions rarely reflect the range of environmental and fuel conditions present in the natural environment where wildland fires occur [9,13]. Field data collection is needed to overcome this limitation, and smoke emissions have a long history of being monitored with human-piloted aircraft and satellites [14,15]. Recent development of compact, lightweight instrumentation has expanded low altitude and mobile ground measurements of combustion emissions [13,16] and air quality [17]. Mobile aerial platforms including aerostats [13,18,19] and rotary- and fixed-wing small unmanned aircraft systems (sUASs) [16,20] have come into favor for smoke measurement because they can maneuver into shifting smoke plumes and near combusting fuels while investigators maintain a safe distance from fire and airborne operations.

To better understand how smoke emissions vary with fuel beds and environmental conditions, we developed and tested a compact portable instrument package that integrates whole air sampling with air quality and meteorology sensing, suitable for ground and aerial emissions monitoring applications within and adjacent to burn units and as a mobile payload on multi-rotor sUASs. The sensing system monitors carbon monoxide (CO), carbon dioxide (CO₂), and particulate matter (PM) concentrations and fire weather conditions, and is suitable for characterizing spatial and temporal patterns of modified combustion efficiency and carbon fluxes in prescribed and wildfire smoke. The smoke sampling system enables the remote collection of air samples suitable for laboratory analysis of VOCs and other gases. We discuss the specifications and performance of the system and present data collected in a calibration experiment, and on controlled burns at Tall Timbers Research Station, FL, USA and Sycan Marsh Preserve, OR, USA.

2. Materials and Methods

A lightweight compact instrument package capable of collecting air samples and measuring CO, CO₂, and PM concentrations and fire weather conditions (i.e., temperature, relative humidity) was developed to characterize smoke plumes. This instrument package is suitable for airborne deployment on sUASs and stationary ground-based monitoring, and matches the desired specifications for the Fire and Smoke Model Evaluation Experiment (FASMEE)—Smoke and Emissions priority area [12,21]. The instrument package consists of two parts: (1) A measurement device (~625 g) consisting of a sampling module that includes a solenoid valve system for collecting air samples and a sensing module for characterizing atmospheric gas concentrations and meteorological conditions in real-time, and (2) a radio-operated remote-control device (~145 g) for initiating air sample collection and displaying time-series data from the sensing module. The sampling module permits air to flow on-demand into one or several evacuated 1000-mL volume SilcoCan canisters (RESTEK, Bellefonte, PA, USA) that are returned to the lab for specialized analysis capable of enumerating of up to 100 VOCs and other trace gases. In this configuration, a power supply operates the solenoid valves, allowing for up to eight sampling ports (i.e., valves) to be accommodated. The sensing module includes regulated air flow across CO and CO₂ sensors using custom inline flow caps designed to draw the sample over the diffusion medium with a ~0.5 L/min micropump (Figure 1). A custom low-volume flow cap was designed and 3D printed for the CO sensor and a commercial flow cap was purchased for the CO₂ sensor. The PM sensor was mounted in an external cutout in the enclosure and contains a built-in fan to control air flow. The measurement device is housed in a rectangular, weather resistant box (24.8 × 19.7 × 7.1 cm). Both devices can be powered using a 5 to 18 V supply and can operate for several hours using a standard 9 V battery. Teensy 3.6 and 3.2 microcontrollers (PJRC, Sherwood, OR, USA) control signal processing for the measurement and remote control devices, respectively.

2.1. Instrument Components

2.1.1. Teensy 3.6/3.2 Microcontroller Units

Payload device executions were carried out using the Teensy 3.6 microcontroller (PJRC, Sherwood, OR, USA), a 32-bit 180 MHz advanced reduced instruction set computer machine processor with 62 input/output pins and 13-bit analog read resolution. The Teensy 3.6 features a built-in Secure Digital Input/Output port used for saving data to a micro Secure Digital (i.e., microSD) card and a built-in real-time clock (RTC) provides timekeeping. The remote-control device used the smaller Teensy 3.2 (PJRC, Sherwood, OR, USA) with a slower rated speed (72 MHz) and fewer digital pins. The Arduino Integrated Development Environment, an open-source software, was used to program both microcontrollers in a C-based language.

2.1.2. K-30 Carbon Dioxide Sensor

Carbon dioxide measurements were obtained using the K-30 CO₂ sensor (Senseair, Delsbo, Sweden). The K-30 is a non-dispersive infrared (NDIR) sensor that outputs CO₂ concentrations from 0 to 10,000 ppm with an accuracy of ± 30 ppm, or ± 3%, up to 5000 ppm and a diffusion time (T_1/e) of ~20 s. Additional specifications are shown in Supplementary Table S1.

2.1.3. DGS-CO 968-034 Carbon Monoxide Sensor

Carbon monoxide measurements were obtained using the DGS-CO 968-034 CO Sensor (Spec Sensors LLC, Newark, CA, USA). The DGS-CO 968-034 is a digital electrochemical gas sensor that outputs carbon monoxide concentrations from 0 to 1000 ppm with 0.1 ppm resolution and an accuracy of ± 15%. The chemical sensor has a manufacturer stated time response (T₉₀) of 30 s. The CO sensor exhibits low cross-sensitivity to other combustion gases with a <1 ppm response in CO at concentrations of 5000 ppm CO₂, 3000 ppm CH₄, 10 ppm NO₂, 25 ppm H₂S, 500 ppm n-Heptane, and 200 ppm Toluene, and a 17 ppm response in CO at 100 ppm H. Additional specifications are shown in Supplementary Table S1.

2.1.4. PMS5003 Particulate Matter Sensor

Particulate matter measurements were obtained using the PMS5003 sensor (Plantower, Beijing, China). The PMS5003 is a compact laser scattering sensor that outputs mass concentrations (µg m⁻³) for PM_1.0, PM_2.5, and PM₁₀ at a 1 µg m⁻³ resolution with a minimum particle diameter of 0.3 µm and includes the number of particles per unit volume for various particle size ranging between 0.3 µm and 10.0 µm. Mass concentration data is output in standard particle and atmospheric environment units, and we report data in atmospheric environment units. Additional specifications are shown in Supplementary Table S1.

2.1.5. Global Positioning System (GPS)

Time and position data were obtained using an Adafruit Ultimate GPS breakout board (Adafruit Industries, New York, NY, USA). The position is output with a 3 m accuracy and includes time and date at a capture rate up to 10 Hz.

2.1.6. BME 280 Humidity Sensor

Relative humidity, ambient temperature, and barometric pressure were obtained using the BME 280 (Bosch Sensortec, Reutlingen/Kusterdingen, Germany). The BME 280 sensor has an accuracy tolerance of ±3.0%. The BME280 was placed inside of the instrument housing for internal temperature readings and was used for investigating the temperature dependence of the CO and CO₂ sensors (see Section 2.2).

2.1.7. SHT-15 Temperature Sensor

Ambient temperature and relative humidity were obtained using the SHT-15 sensor (Sensirion, Staefa ZH, Switzerland). The SHT-15 is a complementary metal-oxide semiconductor digital sensor with an accuracy of ± 0.3 °C for temperature and ± 2.0% relative humidity. Measurements were used to evaluate environmental conditions outside of the instrument housing.

2.1.8. MPL3115A2 Pressure Sensor

Absolute pressure was measured using the MPL3115A2 sensor (NXP Semiconductors, The Netherlands). The MPL3115A2 sensor is a piezoresistive sensor with a 1.5 Pa pressure resolution, is internally temperature compensated, and was adjusted to sea level pressure using the US Standard Atmosphere 1976 protocol [22].

2.1.9. Micropump

We used a 0.5 L min⁻¹ flowrate diaphragm pump (Thomas by Gardner Denver, Sheboygan, WI, USA) to control the flow through the chemical sensors. The pump runs on a 5 V direct current from the printed circuit board and operated continuously while measurements were being collected. Air is drawn from outside the instrument housing and pushed across the CO and CO₂ sensors to ensure that both sensors measure the same air sample.

2.1.10. XBee Pro S3B Radio Module

Two-way communication between the payload and the remote control device was facilitated with 900 MHz XBee radio modules (Digi International, Hopkins, MN, USA). These modules can communicate with a data-transfer rate of 10 to 200 kb s⁻¹ over a 6.5 to 15.5 km line-of-sight distance.

2.1.11. Adafruit Featherwing Touch Screen

Data transmitted between the measurement and remote controller devices were displayed on a 8.9 cm touch screen with a 480 × 320 pixel resolution (Adafruit Industries, New York, NY, USA). A graphical user interface permits sending instructions to initiate air sample collection to the measurement device and also displays real-time CO, CO₂, PM_1.0, PM_2.5, and PM₁₀ concentration data as time-series. Data display can be used to determine when conditions are appropriate for collecting air samples, such as when the instrument package is within the target smoke plume. The screen also displays the temperature, pressure, relative humidity, date, and time readings from the measurement device.

2.2. Instrument Performance Experiments

We investigated the CO and CO₂ sensor performance and developed span and offset calibration correction factors by constructing three complete sensing instruments and testing them on a calibration system where standard gas concentrations were systematically varied using a computerized gas mixer and delivered via in line plumbing to each measurement device instrument (Figure 2). Each instrument was tested individually on the calibration system using the same experimental procedure. Data for each sensing instrument reflected observations collected during a single calibration experiment and were evaluated separately to judge consistency in sensor performance and together to evaluate the efficacy of using a global calibration model across multiple instruments. The experimental procedure consisted of diluting concentrated standard gas (1800 ppm CO: 22.5% CO₂) with zero air using a gas mixer (Environics, Inc., Tolland, CT, USA) capable of dilution ratios spanning 1:20 to 1:2000 at flow rates ranging from 2 to 20 L min⁻¹ with the concentration and flow accuracy reported to be ±1%. The gas mixer was programmed to alternate gas concentrations between five minute periods of “background” gas (i.e., 3.2 ppm CO and 400 ppm CO₂) and seven minute periods of progressively higher concentrations reflecting the following target CO and CO₂ concentrations: 8/1000, 16/2000, 24/3000, and 32/4000 ppm, respectively. Output concentrations from the mixer did not exactly match target concentrations owing to the high concentration of our standard and the dilution ratios/flow rates offered by the mixer. Sensing instruments collected data at 0.5 Hz. CO and CO₂ sensor output was compared against two industry standard analyzers: a LI-7000 (LI-COR, Lincoln, NE, USA) for CO₂ and a CO Analyzer Model 8830 (TeleDyne Monitor Labs, Englewood, CO, USA) for CO. The PM sensor has been evaluated in other studies (e.g., [23,24,25,26]) and further evaluation of the Plantower PMS5003 PM sensor was not completed as part of the present study.

Span and offset calibration correction factors were computed by fitting linear regression calibration models, and calibrated signal concentrations and model uncertainty were estimated using inverse regression [27]. Models took the form, y = mx + b, where y is the sensor response, x is the input concentration generated by the gas mixer, m is the model slope (i.e., span), and b is the model intercept (i.e., offset). Calibration model data had a sample size of n = 5 for each sensing instrument and were prepared by computing the mean input concentration supplied by the gas mixer and mean sensor response concentration from a 2-minute subset of the time series that corresponded with each concentration level. Global models were fit by combining data across all instrument calibration experiments and concentrations (n = 15).

To examine variation in the sensor accuracy, precision, and response time among instruments, we applied instrument specific and global calibration models to raw CO and CO₂ data and computed descriptive statistics using one two-minute subset of data at each concentration level (n = 60 samples per concentration level at 0.5 Hz over 2 minutes). Sensor accuracy was assessed by investigating absolute and relative percent error rates, and sensor precision was judged using standard deviation. Absolute error was computed as the difference between sensor and mixer (i.e., true) concentrations, and the relative percent error was computed as the absolute error divided by the mixer concentration times 100%. T₉₀ response time, the time required for a sensor exposed to the background concentration to achieve 90% of the applied concentration, was computed for each sensor and target concentration level. Sensor temperature sensitivity was investigated by cooling the measurement device to ambient outdoor temperature (~10 °C), then transferring the device to a drying oven and warming the device over 15 min to 40 °C. Background gas concentrations were held constant by enclosing the measurement instrument in a sealed plastic bag. The CO sensor provided internal temperature compensation and was not examined further.

2.3. Field Testing

The sampling and sensing modules were tested separately in experimental prescribed fires at Tall Timbers Research Station, FL, USA and Sycan Marsh Preserve, OR, USA, respectively. Only one instrument was available for sampling in each field campaign.

2.3.1. Tall Timbers Research Station, FL, USA

The sampling module was deployed to collect smoke samples from experimental prescribed fires near the Tall Timbers Research Station north of Tallahassee, FL, USA (30°39′19″N 84°13′33″W). On April 18, 2018, a 2-ha burn was conducted at the Pebble Hill site and on April 20, 2018, a 40-ha burn was conducted at the Scrub Course site. Vegetation at the Pebble Hill site is dominated by longleaf pine-wiregrass (Pinus palustris-Aristida beyrichiana) savanna with sparse understory fuels due to frequent (every ~2 to 3 years) prescribed burns. The Scrub Course site includes additional overstory of turkey oak (Quercus laevis), mockernut (Carya tomentosa), and pignut hickory (Carya glabra), which are being reduced by intentional frequent prescribed fires to restore the landscape to a historic longleaf pine-wiregrass ecosystem. To collect samples, the sampling device and up to three evacuated 1000 mL volume SilcoCan sample canisters were mounted on a custom aluminum rack under a DJI Matrice 600 Pro hexacopter sUAS that measured 52.5 × 48.0 × 64.0 cm with a weight of 10 kg (including batteries) and a recommended payload capacity of 5.5 kg (Supplementary Figure S1). As configured, the payload weight was 2.6 kg (including 1 sample canister weighing 0.9 kg) and the sUAS endurance was ~20 minutes. Additional canisters were added depending on the sampling mission objectives; however, the UAS payload capacity and canister weight currently limit our ability to lift more than 4 canisters at a time. The sUAS and its payload were manually piloted into the smoke plume at 25 m above ground-level. CO₂ and PM data transmitted from a preliminary version of the sensing module provided confirmation that the payload was in the smoke plume. Samples were collected by remotely triggering the solenoid valve system with the remote-control device, allowing smoke to flow into the evacuated canister for 10 s. After sampling, canisters were capped and shipped to the Organic Analysis Lab (https://www.dri.edu/oal-lab) of the Desert Research Institute, Reno, NV, USA and processed for VOC content.

Stainless steel SilcoCan canisters of a 1000 mL capacity were cleaned prior to sampling by repeated evacuation and pressurization with humidified ultra-high purity (UHP) nitrogen (Airgas, Sparks, NV, USA) following the U.S. Environmental Protection Agency (EPA) protocol [28,29]. Eight cycles of evacuation to ~25 in Hg vacuum followed by pressurization to ~15 psig were performed to clean the canisters. One canister per lot was filled with humidified UHP nitrogen and analyzed by gas chromatograph with mass spectrometric and flame ionization detectors (GC-MS/FID), as described below. The canisters were considered clean if the target compound concentrations were less than 0.05 ppbv.

Canister samples were analyzed for 74 VOC species using GC-MS/FID according to the EPA Method TO-15 [30]. The GC-MS/FID includes a Lotus Consulting Ultra-Trace Toxics sample preconcentration system built into a Varian 3800 gas chromatograph coupled to a Saturn 2000 ion trap mass spectrometer (Varian, Inc. Walnut Creek, CA, USA). The Lotus preconcentration system consists of three traps. Mid- and heavier weight hydrocarbons are trapped on the front trap consisting of 1/8” nickel tubing packed with multiple adsorbents. Trapping is performed at 55 °C and eluting is performed at 200 °C. The rear traps consist of two traps: Empty 0.040” ID nickel tubing for trapping light hydrocarbons and a cryo-focusing trap for mid and higher weight hydrocarbons isolated in the front trap. The cryo-focusing trap is built from 6′ x 1/8” nickel tubing filled with glass beads. Trapping of both rear traps occurs at −180 °C and eluting at 200 °C. Light hydrocarbons are deposited to a Varian CP-Sil5 column (15 m × 0.32 mm × 1 μm) plumbed to a column-switching valve in the GC oven, then to a Chrompack Al2O3/KCl column (25 m × 0.53 mm × 10 μm) leading to the FID for quantitation of light hydrocarbons. The mid-range and heavier hydrocarbons cryo-focused in the rear trap are deposited to a J&W DB-1 column (60 m × 0.32 mm × 1 μm) connected to the MS. The GC initial temperature was 5 °C and was held for approximately 9.5 min, then increased at 3 °C min⁻¹ to 200 °C for a total run time of 80 min.

The GC-MS/FID response for individual VOCs was calibrated with a compressed gas mixture (Apel-Riemer, Environmental, Inc., Miami, FL, USA) containing 74 hydrocarbons ranging in size from ethane to n-undecane at 0.2 to 10 ppbv concentrations. Replicate analyses were performed at least for one in every 10 injections. The minimum detection limit (MDL) was approximately 0.01 ppbv. The replicate precision of the GC-MS/FID method was ~8% for all analyzed compounds.

2.3.2. Sycan Marsh Preserve, OR, USA

The sensing module was deployed to monitor CO, CO₂, and PM concentrations and meteorological conditions (i.e., temperature, relative humidity) in an experimental prescribed fire at Sycan Marsh Preserve (The Nature Conservancy) in Oregon’s Upper Klamath Basin (42°48′32.4″ N 121°07′01.1″ W) north-west of Lakeview, OR, USA. On October 24, 2018, a prescribed burn was conducted at Brattain Ridge, a site occupied by ponderosa pine (Pinus ponderosa) and western juniper (Juniperus occidentalis) with a sagebrush (Artemisia tridentata)/bitterbrush (Purshia tridentata) shrub understory and a surface fuelbed of needle litter and senesced annual grasses. The sensing device was hung at 8-m height from a ponderosa pine branch (using a pole pruner) to monitor the full temporal profile of gas concentrations and temperature and relative humidity conditions as a head fire passed under the sensing device (Supplementary Figure S1). The sUAS was not used for sampling because battery replacement would have interrupted the sampling of the time series. The device was calibrated in the laboratory prior to deployment in the field and CO₂ data exhibited minor signs of noise (varying ±40 ppm at ambient concentrations). This noise was later resolved in laboratory testing (prior to the calibration experiments) by adding shielding to the K-30 sensor. Data were collected at ~0.5 Hz and boxcar smoothing was applied to reduce sensor noise (i.e., each data point was replaced by the mean of m number of adjacent points (m = 60/2)). The modified combustion efficiency (MCE) was computed using the smoothed data as the ratio of the excess CO₂ concentration to the sum of excess CO and CO₂ concentrations (MCE = ΔCO₂/(ΔCO + ΔCO₂)).

All data processing and statistical analysis was conducted in the R software program using the following r-packages: Base [31], EnvStats [27], lubridate [32], tibbletime [33], and tidyverse [34].

3. Results and Discussion

3.1. Gas Sensor Performance

CO calibration models for individual sensors exhibited high correlation coefficients (r² = 0.99), indicating strong statistical relationships between sensor readings and calibration gas concentrations. A global calibration model using data from all sensors resulted in a poorer fit (r² = 0.94,

Table 1. Individual and global regression calibration model results for Spec Sensors DGS-CO 968-034 carbon monoxide (CO) sensors.

	Coefficient	SE	t	p	r2
Instrument 1
Intercept	10.975	0.19	58.326	<0.001	0.999
Raw CO (ppm)	1.516	0.01	166.347	<0.001
Instrument 2
Intercept	7.633	0.35	21.8	<0.001	0.999
Raw CO (ppm)	1.492	0.02	87.968	<0.001
Instrument 3
Intercept	17.773	0.15	118.261	<0.001	0.999
Raw CO (ppm)	1.483	0.01	203.794	<0.001
Global (All Instruments)
Intercept	12.123	2.14	5.655	<0.001	0.941
Raw CO (ppm)	1.497	0.1	14.42	<0.001

) and greater absolute and relative error rates than individually calibrated sensors.

Span coefficients for CO ranged from 1.48 ± 0.01 SE to 1.52 ± 0.01 SE with a global model span coefficient of 1.50 ± 0.10 SE, where tolerances are denoting standard errors (SE). Offsets ranged from 7.63 ± 0.35 SE to 17.77 ± 0.15 SE ppm with a global offset of 12.12 ± 2.14 SE ppm. Absolute error across individually calibrated sensors ranged from 0.02 ± 0.38 SD ppm at 16 ppm to 0.13 ± 0.33 ppm at 3.2 ppm with an overall absolute error of 0.01 ± 0.45 SD ppm, where tolerances are denoting standard deviations (SD). Standard deviation ranged from 0.33 ppm at 3.2 ppm to 0.50 ppm at 32 ppm for all sensors calibrated individually (Figure 3). Percent relative error across individually calibrated sensors ranged from 1.5 ± 0.4 SD% at 32 ppm to 9.7 ± 4.9 SD% at 3.2 ppm with an overall rate of 4.0 ± 4.0 SD% (Figure 3). In all cases, the relative error rates for Spec Sensors DGS-CO 968-034 CO sensor performed better than the manufacturer stated measurement error rate of ±15%. The Monitor Labs Inc. CO Analyzer Model 8830 exhibited improved accuracy over our low-cost CO sensors under calibration, with relative error rates ranging from 1.0 ± 0.7 SD% at 32 ppm to 8.3 ± 5.8 SD% at 3.2 ppm with an overall error rate of 2.9 ± 3.9 SD%. The relative difference between the calibrated CO Analyzer Model 8830 and the DGS-CO 968-034 CO sensors was 3.3 ± 4.4 SD%. Both absolute and relative error rates for the DGS-CO 968-034 CO sensor were greater than those of the Citicell electrolytic CO sensor used by Ward et al. [35,36], but similar, if not slightly better, than those of the EC4-500-CO sensor. It is important to note that the range of concentrations in our calibration was smaller than those used in calibrating the EC4-500-CO [16]. Using the global calibration model, the mean absolute error was approximately double and the SD was ~10 times greater than that found in individual sensor calibrations and ranged from 0.05 ± 2.81 SD ppm at 16 ppm to 0.26 ± 2.66 ppm at 24 ppm with an overall absolute error of 0.03 ± 2.80 SD ppm. The relative error was substantially higher using the global calibration model, ranging from 7.3 ± 3.9 SD% at 32 ppm to 80.0 ± 38.0% at 3.2 ppm with an overall absolute error of 27.9 ± 33.1 SD% (Figure 3). Overall, the Spec DGS-CO 968-034 sensor performed well when calibrated individually, but variation between sensors resulted in high absolute and relative error rates, suggesting that the use of a global calibration model is inappropriate for this sensor.

CO₂ calibration models exhibited high correlation coefficients for both individual and global models (r² = 0.99,

Table 2. Individual and global regression calibration model results for Senseair K-30 carbon dioxide (CO₂) sensors.

	Coefficient	SE	t	p	r2
Instrument 1
Intercept	144.389	23.6	6.107	0.009	0.999
Raw CO2 (ppm)	0.698	0.01	76.202	<0.001
Instrument 2
Intercept	143.947	27.2	5.298	0.013	0.999
Raw CO2 (ppm)	0.71	0.01	67.442	<0.001
Instrument 3
Intercept	157.002	18.8	8.348	0.004	0.999
Raw CO2 (ppm)	0.695	0.01	95.309	<0.001
Global (All Instruments)
Intercept	148.439	13.4	11.099	<0.001	0.999
Raw CO2 (ppm)	0.701	0.01	135.259	<0.001

), and equivalent absolute and relative error rates, suggesting that individual and global calibration models are appropriate for use with the Senseair K-30 CO₂ sensor. Span coefficients ranged from 0.695 ± 0.007 SE to 0.710 ± 0.011 SE with a global model span coefficient of 0.701 ± 0.005 SE. Offsets ranged from 143.947 ± 27.171 SE to 157.002 ± 18.807 SE ppm with a global offset of 148.439 ± 13.374 SE ppm. Absolute error across individually calibrated sensors ranged from 18.1 ± 5.5 SD ppm at 2000 ppm to 36.9 ± 3.7 ppm at 400 ppm with an overall absolute error of 0.01 ± 30.9 SD ppm. Standard deviation ranged from 1.9 ppm at 1000 ppm to 8.7 ppm at 3000 ppm for all sensors calibrated individually (Figure 3). Absolute error rates using the global calibration model were nearly identical; SD was nominally greater, ranging from 18.1 ± 18.1 SD ppm at 2000 ppm to 36.8 ± 9.6 ppm at 400 ppm with an overall absolute error of 0.01 ± 36.7 SD ppm. Relative error across individually calibrated sensors ranged from 0.9 ± 0.3 SD% at 2000 ppm to 9.1 ± 0.9 SD% at 400 ppm with an overall rate of 2.8 ± 3.2 SD% (Figure 3). Similarly, relative error when using the global calibration model ranged from 0.9 ± 0.9 SD% at 2000 ppm to 9.1 ± 2.4% at 400 ppm with an overall absolute error of 2.8 ± 3.4 SD% (Figure 3). Overall concentrations, and absolute and relative percent error rates for the Senseair K-30 CO₂ sensor were within manufacturer stated measurement error rates; however, error rates at our lowest concentration (400 ppm) were greater than the manufacturer stated error rate (± 30 ppm or ± 3% of the measured value, whichever is greater). For comparison, the Li-COR LI-7000 exhibited favorable relative error rates ranging from 0.1 ± 0.1 SD% at 3000 ppm to 2.6 ± 0.4 SD% at 400 ppm with an overall error rate of 1.0 ± 0.9 SD%. The relative difference between the calibrated LI-7000 and K-30 CO₂ sensors was 3.7 ± 4.6 SD%. Absolute and relative error rates for the K-30 sensor were greater than those found for the DX6220 CO₂ sensor [16] and the Valtronics (model 2015 BMC) CO₂ sensor employed by Ward et al. [35,36]. Similar to the findings by Yasuda et al. [37], no temperature dependence of the offset was observed for the CO₂ sensor at ambient concentrations and for a temperature range of 10 to 40 °C.

Response time was evaluated as the time required for each sensor to shift from background to 90% of the applied concentration (T₉₀). CO sensor T₉₀ increased asymptotically with the concentration change and ranged from 32.3 ± 4.5 SD seconds with a concentration increase from 3.2 to 8 ppm and 107.0 ± 4.4 SD seconds with a concentration increase from 3.2 to 32 ppm (Figure 4), substantially slower than the T₉₀ reported by the manufacturer and that reported for a EC4-500-CO sensor [16] and a Citicell electrolytic CO sensor [35,36]. The CO₂ sensor T₉₀ response time also increased asymptotically and ranged from 41.0 ± 1.7 SD seconds when the concentration increased from 400 to 1000 ppm and 95.0 ± 2.6 SD seconds when the concentration increased from 400 to 4000 ppm (Figure 4). T₉₀ for the K-30 CO₂ sensor was slower than the 20 s diffusion time reported by the manufacturer, but slightly faster than the response observed by Yasuda et al. [37]. In comparison to other NDIR sensors, the response time of the K-30 was slower than the Valtronics (model 2015 BMC) sensor [35,36] and the DX6220 CO₂ sensor [16]. A slow sensor response may complicate sensor use for the identification of peak gas concentrations and to fully describe the temporal variation in gas concentrations, but are not expected to hinder estimates of total CO and CO₂ fluxes in the smoke plume [16].

3.2. Smoke Emissions Sampling

The performance of our smoke sampling module was demonstrated onboard an sUAS at Tall Timbers Research Station, FL. We collected five canister samples for VOC determination by remotely triggering the valve system at the 50–100 m range; two under prefire ambient conditions and three from the smoke plume during active burning. Regional burning outside of our study area may have contributed to trace VOC concentrations in samples. Prefire ambient samples contained total VOC concentrations of 0.8 and 1.8 ppbv, whereas samples collected during active burning contained 7.3 to 24.3 ppbv (Figure 5). The seven most abundant VOCs observed in ambient samples were iso-pentane, benzene, 1-butene + isobutene, isoprene, α-pinene, n-decane, and n-octane. Samples collected from the smoke plume included a total of 42 VOCs. Six VOCs (i.e., iso-pentane, benzene, 1-butene + isobutene, 1,3-butadiene, toluene, and styrene) accounted for ~71% and 15 VOCs accounting for ~90% of total VOCs by ppbv observed during active burning (Figure 5, Supplementary Table S2). Figure 5 presents the top 10 most abundant individual VOCs measured in the ambient air and in the fire smoke plumes. Emission factors were not determined because canister sample concentrations were too low for additional laboratory analysis of total carbon content.

Comparing the C4–C10 VOCs in the fire plumes with those reported in the literature, we found that the top 10 VOCs in our research were observed and reported in other studies [13,38,39,40,41]. Dreessen et al. [40] studied emissions transported from a Canadian wildfire that occurred in June 2015. Even though the plume was aged and diluted, high concentrations of isoprene, benzene, and xylenes were observed. Similar to our results, α-pinene, benzene, toluene, 1-butene, isoprene, 1,3-butadiene, and m+p-xylenes were in the top 10 VOCs (>C4) in a fresh Canadian boreal forest fire plume [41]. Simpson et al. [41] reported 0.99 ± 032 ppbv of benzene and 0.37 ± 0.14 ppbv of toluene; these values are a factor of 1.2 to 3.5 lower than our levels (Figure 5). This is most likely due to different meteorological conditions and variation in the dilution of fire emissions during the sampling in fire plumes. In general, the VOC results presented here show good agreement with the literature.

3.3. Smoke Emissions Sensing

The performance of our smoke sensing module was demonstrated in a near-ground (8-m height above ground) deployment of the instrument at Sycan Marsh Preserve, OR, USA. Prior to the burn, CO and CO₂ sensors were calibrated in the laboratory over a concentration range spanning 3 to 48 ppm for CO and 400 to 6000 ppm for CO₂. Calibrated CO concentrations in the smoke plume ranged from an ambient minimum of −1 to a peak of 197 ppm (Figure 6); boxcar smoothing constrained the CO concentration range from −1 to a maximum of 180 ppm. Calibrated CO₂ concentrations ranged from an ambient minimum of 440 ppm to a maximum of 6326 ppm (Figure 6) and boxcar smoothing constrained the CO₂ concentration range from 418 ppm to a peak of 4336 ppm. The ranges of the CO₂ and CO concentrations observed at Sycan Marsh Preserve indicate that future deployments will require calibration of the CO sensor over a greater concentration range while the CO₂ sensor’s calibration range was appropriate for the application. MCE estimates the efficiency of fuel combustion with smoldering combustion recognized as occurring below a threshold of 0.85 to 0.90 and flaming combustion occurring above this level. Computed using the boxcar smoothed data, the MCE measured in Sycan Marsh Preserve, OR ranged from 0.84 to 1.00 (Figure 6) and generally matches findings from studies that observed flaming combustion in senescent grass and pine litter fuel types [8,13].

PM_2.5 mass concentration measurements using the Plantower PMS5003 sensor ranged from 0.0 to 1717 µg m⁻³ and from 0.8 to 1599 µg m⁻³ after boxcar smoothing (Figure 6). As expected, levels observed directly in the smoke plume here were greater than other studies that used the sensor to investigate regional smoke impacts on ambient air conditions during the fire season [24,26]. Recent evaluations of the Plantower PMS series (i.e., PMS1003/3003/5003/7003) sensors primarily investigated the sensor at PM_2.5 concentrations up to 150 µg m^-3 and found strong correlation with reference monitors [23,24,25], but one study found correlations were degraded during the wildfire season [24]. Multiple authors noted that raw sensor readings may overestimate PM mass concentrations [23,24,25] and attributed some overestimation to an increased sampling frequency over reference monitors that permitted greater detection of temporal variation and short lived events [25,26]. Authors also observed a nonlinear response at high concentrations (pronounced above 125 µg m⁻³, [23]) and a high correlation with relative humidity [23,25]. Percent error after calibration ranged from 21% to 201% in one study and varied depending on the type of reference monitor used for calibration [23]. PM_2.5 mass concentrations observed in our study were very high in comparison with other studies and exceeded the manufacturer’s suggested maximum concentration (i.e., 1000 µg m⁻³). Therefore, we urge caution in interpreting PM_2.5 mass concentrations observed directly in smoke plumes using uncalibrated Plantower PMS5003 sensors but highlight the potential utility of investigating temporal trends using the sensor. Further exploration of sensor calibration and environmental correction are necessary to ascertain the sensor’s measurement limits in smoke plumes.

Air temperature and relative humidity are essential parameters for predicting fuel flammability and fire behavior, and are routinely collected and used in fire behavior, fire monitoring, and fire modeling studies. Data collected during the experimental burn illustrate the dynamic range of environmental conditions observed with the passage of a flaming front. At 8 m height, the temperature ranged from 11.5 to 50.5 °C and the relative humidity ranged from 8.6% to 43.6% (Figure 7). Further work is necessary to compare the temperature and humidity sensors used in our sensing instrument with industry standards in fire weather forecasting (i.e., Remote Automated Weather Stations (RAWS)) and to better understand how gas and particulate sensors perform across such a large range of environmental conditions at short time scales.

4. Conclusions

We developed a compact lightweight atmospheric sensing and sampling instrument package to measure and monitor smoke emissions from wild and prescribed fires, and tested it in aerial and ground-based deployment during two experimental burns. The instrument effectively collected canister samples from a fire plume onboard an sUAS at distances of 50 to 100 m from the operator. Laboratory analysis of sample canisters estimated concentrations of 42 VOCs in the smoke plume and can be used in future experiments to identify emissions factors related to these and other VOCs. The sensing instrument module performed well in calibration experiments and in a near-ground field deployment above a flaming front. The instrument is well suited for characterizing gas and meteorological conditions within and adjacent to experimental burn plumes, and can be used to trigger the smoke sampling module under user-specified combustion conditions (e.g., [13]). As outfitted with a weatherproof enclosure and a high-capacity battery, the instrument package is capable of measurements over extended periods on the order of days to weeks.

The integration of air sampling with air quality and meteorological sensing is promising for the development of a methodology for investigating gas and PM fluxes and estimating emissions factors from measurements in wildland fire smoke plumes. Continued evaluation of sensor performance is necessary to minimize measurement uncertainty in the field, where gas concentrations and environmental conditions may vary widely over short time scales. Calibration of the CO and CO₂ sensors prior to each sampling campaign is necessary to ensure accurate measurements. Enclosing the sensors in a closed, pump driven system was useful for facilitating the calibration procedure and for preventing variation in airflow across the sensor’s diffusion/electrochemical sampling medium. As with other gas sensors used to monitor wildland fire emissions, response time delays may inhibit the sensors’ ability to capture the true dynamics of the smoke plume.

We did not directly investigate the influence of the sUAS on gas, PM, and meteorological measurements and recent work shows mixed results depending on the parameter being measured. As one would intuitively expect, rotor wash has been found to exert substantial influence on measurements of wind velocity within close distances to rotors (e.g., [42,43]); however, little impact has been noted for other meteorological measurements (e.g., temperature, relative humidity, pressure) [44]. For gas and particulate measurements, rotors are hypothesized to increase the mixing of air roughly equivalent in size to the rotor’s zone of influence, likely increasing the scale of inference of a given sample or measurement to represent a voxel of air roughly equivalent to that size. As long as sensors are placed away or sheltered from high-velocity air currents that could cause mechanical interference with their function, rotor wash is not expected to interfere with PM and gas measurements. Still, further research in necessary to confirm when and to what extent rotor wash influences air quality and emissions measurements.

Further development of the instrument package could include enhancements that broaden the measurement range of the sampling and sensing modules, improve field calibration procedures, prolong measurement times, and deliver real-time data to a cloud-based repository. The use of a pump system to fill sample canisters would boost the sample volume and broaden the suite of laboratory analyses conducted on each sample (e.g., [45]). Additional sensors, such as for methane (CH₄) and nitrous oxides (NO, NO₂) concentrations, would improve carbon emissions quantification and enhance the understanding surrounding the role that nitrogen species play in atmospheric chemistry, especially in ozone (O₃) production. The instrument package could be adapted for long-term and remote monitoring applications with the incorporation of a long-term power supply and an automated or streamlined calibration methodology. Real-time data transmission and networking would improve data delivery and could provide air quality monitoring and smoke emissions data to air resource and fire managers on actionable time horizons. General improvements, such as reducing the overall instrument size and 3D printing a custom housing, are currently underway.