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Absorbance spectra of phenol red at different pH values. 

Absorbance spectra of phenol red at different pH values. 

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Context 1
... our disposable sensor, the spectrum of the outgoing light ( , ) and thus the response of the sensor R( , ) is determined by two phenomena: the photon diffusion process in the hybrid-material drop applied to the optical fiber tip and the absorption of the indicator. Both these processes are pH-dependent; indeed, the size of the hybrid drop depends on the pH level of the solution and so, varying the pH, different photon optical paths are possible. In order to characterize the sensing probe, measurements were performed at room temperature in standard pH buffers (Fisher Scientific) evaluating the response of the disposable sensor R( , ) . According to the schematic representation in Fig. 5, the sensitive tip of the POF was immersed in 20 ml of sample solution; measurements were taken at 5 min after changing the pH level, monitored with the reference pH meter, which has a measuring uncertainty of 0.05 units. The system response R( , ) was calculated acquiring a reference spectrum ( , ) at pH ref =10 and varying the pH of the solution from 9 to 4. To evaluate the temporal response of the probe to a rapid change in pH, the pH value of the solution has been staircase decreased from 8 to 5 with unitary steps of duration 10 s each. The same protocol has been applied for the reverse direction of the staircase, i.e. from 5 to 8. Also during these measurements the testing solution was continuously monitored with the reference pH meter. The temporal response has been investigated firstly visually inspecting the color changes and then acquiring continuously the spectrum ( , ) and calculating R( , ) as a function of time. The optical properties of the interrogation system have been determined according to the measurement procedures reported in section 4.1. Spectra ( ) , ( ) and their ratio are shown in Fig. 6 together with the emission spectrum of the halogen lamp WLS. Other distortions of the halogen lamp spectrum are due to the transmission properties of the optical components used in the interrogation setup. ( ) Figure 6b shows the ratio that, according to Eq. (5), is proportional to the spectral ( ) response of the interrogation system. The spectral region of interest in our application is 500-600 nm, i.e. green-yellow-red; since the response of the interrogation system is satisfactorily flat in this interval, as shown in Fig. 6b, the information of interest is not corrupted. The spectral properties of the sensing indicator have been measured according to the procedure reported in section 4.2. The absorbance spectra of phenol red at different pH values are shown in Fig. 7; the maximum of all the spectra is well visible at the wavelength of about 560 nm. According to literature (Wang, 2003), at this wavelength the phenol red molecules exhibit a very low absorption that can be significantly enhanced by increasing the pH of the solution. Note that the absorbance at 560 nm showed a sharp transaction when the pH of the solution changed from 5 to 8. As shown in Fig. 8, the point of inflection (sigmoidal fitting function Eq. (6) equal to 0.5) corresponds to the apparent pKa value of 7.9. This value is in good agreement with the pKa of phenol red in aqueous solution reported in literature (Budavari, 1989). The sensor characteristics have been measured according to the procedure reported in section 4.3. As shown in Fig. 9, a visual inspection of the probe at two different pH values of the solution underlines the swelling described in the previous sections. The spectra Δ ( , ) = ( , ) − , acquired at different values of pH are shown in Fig. 10. Observing Fig. 10, it is clear that the swelling/shrinking processes induce a change in the amplitude of the whole spectrum. As far as these phenomena are concerned, parameters A and S were considered to quantify the response of the sensor. In particular, as shown in Fig. 11, given a typical spectrum Δ ( ) , parameter A and S were calculated as follow: (i) the two maxima = ( , ) , = ( , ) and the minimum = ( , ) of Δ ( ) have been calculated using a standard Matlab © routine; (ii) the equation of the line joining M 1 and M 2 has been calculated as ( ) = ( − ) ; (iii) A has been defined as ( ) − and S as ( ) . As shown in Fig. 11, parameter S is correlated to the spectrum amplitude and thus to swelling/shrinking processes while A is strictly related to the absorption (at about λ = 560 nm) performed by the indicator. In Fig. 12, parameters A and S were calculated for each spectrum acquired and the normalized results are plotted against pH. Parameter A exhibits a sharp transaction changing the pH of the solution from 5 to 8. The experimental data was fitted by the Boltzmann (sigmoidal) function according to Eq. (6). The point of inflection (sigmoidal fitting function equal to 0.5) corresponds to the apparent pKa value = 6.8 . This value is lower than the measured value of pKa=7.9 of phenol red in aqueous solution (Fig. 8). However, the pKa value can be shifted to lower pH with increasing ionic strength as observed by Holobar et al. (Holobar, 1993), and this phenomenon could occur also in our hybrid matrix. An increase in the value of pH determines a higher swelling of the hybrid drop, as shown in Fig. 9, which leads to an increase in the distance between the optical fiber tip and the probe- liquid interface and a consequent decrease in the mean optical path of the photons through the probe. As a consequence, according to Eq. (3), also the sensor response diminished. Coherently, as shown in Fig. 12b, parameter S decreased linearly with the pH of the solution. The linear fit of the experimental data exhibits a slope of 0.17. The response time of the probe PEO8000-8:2-PR was measured. A trade-off between the response time and the indicator leaching together with the adhesion between the sensitive matrix and the POF is required. In fact, high molecular weight PEO improves the adhesion and diminishes the indicator leaching, but causes long response time of the sensor. In general there are two different time constant; in fact, when pH is changed from 10 to 3, the sensor was found to reach 90% of the regime signal intensity ( τ 90 ) between 1 and 2 seconds, while changing the pH from a low value to a high one resulted in longer response times that can be quantify in the order of some minutes, i.e. the kinetics depends on the direction of ...
Context 2
... change (the 90% of the regime signal intensity was not reached in the time scale of the experiment, i.e. 10 seconds per step). This agrees with other experimental observations reported in literature (Ismail, 2002; Badini, 1995). Empirical quantification of this sensor behavior is shown in Fig. 13. In Fig. 13, the parameter A (blue line) is represented as a function of time together with the value of the reference pH (dashed line). We think that the slow response time observed changing the pH from 5 to 8 is strictly associated with the swelling/shrinking kinetics of the sensitive drop. Finally, the kinetics of swelling/shrinking has shown to be dependent on the direction of the pH change. This complex mechanism meddles in the photons propagation in the sensitive drop and thus in the response of the probe. The mean lifetime of disposable sensors, checked in the continuous mode operation at a pH level in the middle of the range, is two days. The reusability, tested with a series of probes checked once a day at a pH level in the middle of the range and preserved dry, has a mean life of one month. Table 1 shows these and other analytical parameters of the sensor. We present a disposable sensor based on a low-cost plastic optical fiber that covers an important pH range for physiological applications, e.g. in medicine and biotechnology, with excellent sensitivity. Some other advantages of the proposed sensor are: simple realization process, small size, high resistance to aggressive environments and electrical isolation. The sensor characterization has been performed using a simple optical setup based on a single wavelength measurement. Nevertheless according to Lei (Lei, 2010), a ratiometric approach could improve the sensing overall performance. To this purpose, the isosbestic wavelength, i.e. 480 nm, highlighted in the spectra shown in Fig. 7, could be conveniently exploited. 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Citations

... The absorbance of phenol red solutions at 560 nm is an indicator of pH, as previously described [73][74][75]. Phenol red is a pH indicator changing color from yellow below pH 6.8 to bright pink above pH 8.2. ...
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... The absorbance of phenol red solutions at 560 nm is an indicator of pH, as previously described (Held, 2018;Paye et al., 2018;Rovati et al., 2012). To analyze the pH changes in A. baumannii cultures during bacterial growth, indicated strains were maintained overnight in LB broth at 37 °C under shaking conditions. ...
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... After 72 h, the pH of the central compartment of each chamber was measured for the pH group and control group. For the leakage group, the absorbance of each compartment was measured using an absorptiometer and the absorbance at a wavelength of 560 nm was recorded [27]. Based on the measured values, the amount of leakage was estimated by dividing the average of the absorbance of the left and right compartments by the absorbance of the central compartment. ...
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... As the measured liquid, buffer solutions with values 4.0, 5.0, 6.0, 7.0, 8.0, 9.0, and 10.0 were employed in the test. Figure 7a depicts the typical measured absorbance spectra of phenol red at different pH values [53], where two significant peaks appear at wavelengths 430 nm (peak 1) and 560 nm (peak 2). Between the peaks is an isosbestic point at a wavelength of about 470 nm. ...
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