Sensors Calibration
Electrochemical characterizations were performed for both salicylic acid and ethylene sensors. The salicylic acid sensor was made with a composite coating of copper metal-organic framework-carbon black-Nafion, while the ethylene sensor was fabricated with a composite copper complex (I)-single-walled carbon nanotube coating (details in Section S1 of the supporting information). First, differential pulse voltammetry (DPV) was performed in a 0.05M tris HCl buffer (pH = 7.1) to characterize the salicylic acid sensor. DPV test was performed in the voltage range from − 1.0V to 1.5V with a 0.01V step and scan rate of 10 mV/s. The magnitude and duration of the pulse (Epulse and tpulse) were 0.3V and 0.1s, respectively. The SA sensor was calibrated with 0.1 µM, 1 µM, 50 µM, 100 µM, 200 µM, 400 µM, 600 µM, 800 µM and 1000 µM of SA. The DPV response had two redox peaks, as shown in Fig. 2a. The current peak (ICuMOF) located at approximately − 0.2V was due to the reduction of Cu2+ in the CuMOF coating, whereas the peak (ISA) at 0.85V was attributed to SA oxidation. It is noteworthy to mention that with increasing concentrations of SA, the oxidation peak current at 0.85V increased. Simultaneously, the reduction peak current at -0.2V diminished owing to the increased reduction of Cu2+ ions. Because of the considerable separation of 1.05V between the Cu2+ and the SA peaks, the ratio of two peak currents (ISA/ ICuMOF) was used as the sensor response. Figures 2a and 2b show the DPV responses of the SA sensor and the corresponding calibration curve fitted with a power series, respectively.
Cyclic voltammetry (CV) was used to characterize the ethylene sensor. CV was performed from − 0.2V to 0.5V at a scan rate of 50mV/s and potential step (i.e., Estep) of 0.01V. The sensor was exposed to varying concentrations of gaseous ethylene, including 0.1 ppm, 1 ppm, 10 ppm, 30 ppm, 50 ppm, 75 ppm, and 115 ppm. The CV plots shown in Fig. 2c indicate that the redox peak occurred between 0.13V and 0.2V. Upon exposure to ethylene, copper complex (I) bound with ethylene to form a second complex, limiting its interactions with the single-walled carbon nanotubes. As a result, the conductivity of the single-walled carbon nanotubes decreased, and hence current decreased. With an increased concentration of ethylene, there was a proportional reduction in the peak current (Fig. 2c). The peak oxidation current values were plotted as a function of ethylene concentrations in the logarithm scale to generate the calibration curve shown in Fig. 2d. The peak current showed a linear relation to varying ethylene concentrations.
The temperature, humidity, pressure, and strain sensors were resistive by nature. This is attributed to resistance variations in response to temperature, humidity, pressure, or strain variations. The temperature sensor was fabricated with a Poly(3,4-ethylenedioxythiophene): poly(styrenesulfonate) (PEDOT:PSS) coating, the relative humidity sensor was composed of functionalized multiwalled carbon nanotube-hydroxyethyl cellulose coating, the pressure sensor had a porous polydimethylsiloxane- deep eutectic solvent-carbon black (PDMS:DES:CB) framework, and the strain sensor was made with reduced graphene oxide (rGO) (details in Section S1 of the supporting information). The sensors were calibrated at an operating frequency of 100 Hz. The temperature sensor was calibrated with temperature values ranging from 10°C to 90°C. As PEDOT:PSS has a negative temperature coefficient of resistance, its resistance decreases with increasing temperature [50]. The calibration curve of the temperature sensor showed a high degree of linearity with a Pearson coefficient of 0.9899 (Fig. 2e). Next, the humidity sensor was calibrated for relative humidity values ranging from 10–90%. With increasing relative humidity, the resistance also increased, as demonstrated in Fig. 2f. The resistance versus relative humidity measurements was fitted with a power series having r2 = 0.99383. Similarly, the pressure sensor was calibrated with various pressure values ranging from 0.1 kPa to 100 kPa. As the pressure increased, the resistance of the pressure sensor decreased (Fig. 2g), confirming the negative pressure coefficient of resistance of PDMS:DES:CB [51]. The strain sensor was calibrated for various angles of curvature, as shown in Fig. 2h. As the stem grows radially, the strain sensor encounters a proportional change in its resistance. The radial growth of the stem was mimicked by cylindrical blocks of various radii (and hence various angles of curvature), as was done in our preliminary results presented at the 2021 IEEE Sensors Conference [52]. The equation that relates the angle of curvature of the strain sensor and stem radius is given by:
$$\theta =\frac{360 S}{2\pi r}$$
1
Where s, r, and θ represent arc length, radius, and angle of curvature, respectively. Here, the arc length, s, is the same as the length of the sensor (2cm). Cylindrical blocks of various radii (r = 1.8cm, 1.43cm, 1.25cm, 1.09cm, 0.88cm, 0.72cm, 0.63cm, 0.54cm, 0.53cm, 0.45cm, and 0.4 cm) were printed using a stereolithography 3D printer (Form 3B, Formlabs, Somerville, MA). These r values cover the stems of small plants such as bell pepper (stem diameter = 0.6 cm), cucumber (stem diameter = 1.1 cm), squash (stem diameter = 1.3 cm), tomato (stem diameter = 1.34 cm), and maize (stem diameter = 2.8 cm). The strain sensor was mounted on the cylindrical blocks and the variation in sensor resistance was measured. The r values were substituted into Eq. (1) to get the angles of curvature ranging from 8.98° to 290° (Fig. 2h).
The gauge factor (GF =\(\frac{\frac{\varDelta R}{R}}{\epsilon }\)), defined as the ratio of relative change in sensor resistance to the mechanical strain, was found to be 842 under a bending strain of 1.4%. Eq. 2 shows the equation for the mechanical bending strain, ε
ε =\(\frac{t}{2{r}_{b}}\) (2)
where t is the combined thickness of the polyimide sheet and the overlaid sensing layers (= 127 µm) and rb is the bending radius of the sensor under the bending state. The bending radius, rb, was calculated following the method outlined in [53] as was also done in our prior work [52]. Figure S9a in the supporting information shows the gauge factor versus the bending strain plot. A motorized translation stage (MTS50-Z8, Thorlabs Inc., Newton, NJ, USA) was used to measure the bending radius, as illustrated in Figure S9b in the supporting information. The resolution, defined as the smallest detectable change in the angle of curvature in response to the radial growth in the stem, was calculated to be approximately 0.02°.
Sensitivity and LOD Analysis
The calibration curves for salicylic acid, humidity, pressure, and strain sensors were fitted with power series (\({y=ax}^{b}+c\) ). The sensitivity,\({S}_{y}{|}_{x}\), was calculated by the method described in [54].
$${S}_{y}{|}_{x} := \frac{dy}{dx} =ab{x}^{b-1}$$
3
Where x and y represent the target parameter (i.e., SA concentration/RH/pressure/angle of curvature depending on the sensor type) and sensor response, respectively, while a and b denote parameters of the fitted curve. Sensitivity values were calculated at both the lowest and highest x values. In contrast, ethylene and temperature sensors exhibited a linear response (Figs. 2d and 2e) and hence the slope (m) of the linear fit (\(y=mx+c)\) was used as a measure of sensitivity.
The limit of detection (LOD) for the physical sensors, i.e., temperature, humidity, pressure, and strain sensors, was calculated using the following formula:
$$LOD= \frac{3* std. dev.}{Sensitivity}$$
4
The LOD for chemical sensors, i.e, SA and ethylene sensors, was calculated using the following sets of equations [55]:
$$LOB=mean of signal \left(blank sample\right)+1.645 \left( std. dev. of blank sample\right)$$
5
$$yLOD=LOB+1.645 ( std. dev. of target at low concentration )$$
6
$$LOD=\frac{yLOD-intercept}{slope}$$
7
Tables I and II summarize the sensitivity, LOD, and resolution for all the sensors.
Table I
Performance metrics of non-linear sensors.
Sensor | Equation | Low Concentration Sensitivity | High Concentration Sensitivity | LOD | Resolution |
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Salicylic acid, SA | ISA/ICuMOF =\(0.0143{\left(SA\right)}^{0.3787}+0.8346\) | 0.002264 µM-1 (at 0.1 µM) | 7.409 X 10− 5 µM-1 (at 1000 µM) | 0.644 µM | 0.301 µM |
Humidity, RH | R = 0.0037\(({RH)}^{2.161}+1.411\) | 0.011589 kΩ/ (%RH) (at 10%RH) | 0.1485 kΩ/ (%RH) (at 90%RH) | 11.321%RH | 0.245%RH |
Pressure, P | R = -1.369\({P}^{0.1713}+10.44\) | 5.04 kΩ/ (kPa) (at 0.1 kPa) | 0.0164 kΩ/ (kPa) (at 100 kPa) | 0.3733 kPa | 0.11kPa |
Strain,\(\theta\) | R = 0.000248\({\theta }^{0.1442}+18260\) | 1.5935 X 10− 6 kΩ/° (Gauge factor = 100) | 1.006 X 10− 8 kΩ/° (Gauge factor = 900) | 9.3211° (0.1%) | 0.02° |
Table II
Performance metrics of linear sensors.
Sensor | Equation | Sensitivity | LOD | Resolution |
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Ethylene, ET | I =\(-17.073 \left(ET\right)+34.635\) | 17.073 µA/log(ppm) | 0.6089 ppm | 0.424 ppm |
Temperature, T | \(\frac{R}{Ro}=0.0098 \left(T\right)+1.17313\) | 0.0098/°C | 10.5478°C | 1.03°C |
Temperature and Humidity Corrections
In an agricultural field setting, temperature and humidity level change frequently. Hence, we characterized the performance of our sensors in response to varying temperature and humidity levels. All but the temperature sensor were tested and corrected for temperature variations because the temperature sensor was designed to respond to temperature variations. Likewise, all but the humidity sensor were tested and corrected for humidity variations. Figures 2i, j, k, l, and m show the calibration plots of the sensors under varying relative humidity levels. Likewise, Figs. 2n, o, p, q, and r show the responses of all but the temperature sensor under varying temperature conditions. The coefficient of variance between the calibration plots of each sensor was found to be less than 9%.
The correction factors for the intercept, slope, and exponent (for nonlinear curve fit) were calculated at different temperature and humidity levels using the following equations [55]. Room temperature (250C) and humidity (60%RH) were considered as references.
fintercept(temp ) = \(\frac{intercept\left(temp\right)}{intercept(25^\circ C)}\) fintercept(%RH) = \(\frac{intercept\left(\text{%}RH\right)}{intercept\left(\text{%}60\right)}\) (8)
fslope(temp) = \(\frac{slope\left(temp\right)}{slope(25^\circ C)}\) fslope(%RH) = \(\frac{slope\left(\%RH\right)}{slope\left(\text{%}60\right)}\) (9)
fexponent(temp) = \(\frac{exponent\left(temp\right)}{exponent(25^\circ C)}\) fexponent(%RH) = \(\frac{exponent\left(\text{%}RH\right)}{exponent\left(\text{%}60\right)}\) (10)
Repeatability, Reproducibility, Bending, and Hysteresis Studies
All six sensors were tested for repeatability, reproducibility, bending, and hysteresis, to confirm their feasibility of field deployment. Reproducibility was tested by repeating the calibration with four identical sensors from each category (Figs. 3a1-a6). The coefficient of variance for four repeated measurements was found to be less than 3%. The sensors also demonstrated repeatable characteristics under cyclic variations in SA (Fig. 3b1), ethylene (Fig. 3b2), temperature (Fig. 3b3), humidity (Fig. 3b4), pressure (Fig. 3b5), and strain (Fig. 3b6). For instance, the SA sensor was exposed to increasing, followed by decreasing concentrations of SA, and the cycle was repeated five times. The same SA concentration values (i.e., 0.1 µM, 1 µM, 50 µM, 100 µM, 200 µM, 400 µM, 600 µM, 800 µM, and 1000 µM) as shown in Fig. 2b were used for the repeatability test. A similar procedure was adopted for investigating the repeatable characteristics of other sensors. All the sensors demonstrated a coefficient of variance of less than 5%, which is reasonable for in-field operation. Figure S10 in the supporting information shows the dynamic response of all sensors over half cycle. The responses were measured with the custom-made data acquisition and processing module shown in Fig. 1d. All the sensors demonstrated a rapid response time of less than a minute.
The flexible substrate carrying the sensors was subjected to 30, 60, 90, and 100 cycles of bending at an angle of 45°, and the calibration curve of each sensor was repeated (Figs. 3c1-c5). It was observed that even after 100 cycles of bending, the coefficient of variance between the calibration curves remained less than 3%. The hysteresis between the 0th and 100th cycles of bending was calculated to be less than 3% for all but the SA sensor (Figure S11 in Supporting Information). A higher hysteresis for the SA sensor could be attributed to the crack formation in the carbon black coating after 100 cycles of bending [56], which resulted in a degradation in the sensor performance by 1.23%. Generally, 450 bending of the leaf surface may not occur in a live plant. Yet, if needed a separate correction factor can be introduced to account for such performance degradation under large bending angles, as is explained below. The response of the strain sensor was recorded for 1000 cycles of repeated bending, as shown in Fig. 3c6. Nevertheless, the hysterics was found to be less than 3% even after subjecting the strain sensor to 1000 cycles of bending (Figure S11 in Supporting Information).
A separate strain sensor can be integrated with the leaf patch and the hormone measurements (i.e., SA and ethylene levels) can be corrected by recalculating the slope, intercept, and exponent of the initial calibration graphs. The corrected intercept, slope, and exponent of the sensors were found using the values computed in Equations (8–10) [55]:
\(intercept\left(corr.\right)=\) fintercept(temp) fintercept(%RH) fintercept(bend) \(intercept\left(init.\right)\) (11)
\(slope\left(corr.\right)=\) fslope(temp) fslope(%RH) fslope(bend) \(slope\left(init.\right)\) (12)
\(exponent(corr.)=\) fexponent(temp) fexponent(%RH) fexponent(bend) \(exponent(init.)\) (13)
Drift Analysis
The sensors were characterized for drift by first measuring the sensor response every 20 minutes over an hour (Figs. 3d1-d6) and then every 4 hours over 12 hours (Figs. 3e1-e6). The mean coefficient of variance was < 2%, indicating the minimal drift displayed by the sensors.
Stability Analysis
The long-term stability of the six sensors was evaluated over a week. The sensor responses are demonstrated in Figs. 3f1-f6. The coefficient of variance in the sensor response was measured to be < 2% over 7 days, indicating an acceptable stable response for in-plant measurements.
Selectivity Analysis
The details of selectivity analysis are described in Section S4 and the results are plotted in Figure S12 of the supporting information. The salicylic acid and ethylene sensors showed high degree of selectivity to other interfering species.