Abstract
A simple optical fiber sensing system of alcohol concentration in liquors has been studied. In this sensor head, a mixture polymer of novolac resin and polyvinylidenefluoride (PVDF) with a ratio of 9β:β1 was coated as a sensitive cladding layer on the plastic fiber core made of polystyrene-(PS-)coated polycarbonate (PC). Using this sensor head and a green LED light source, it was confirmed that alcohol concentration in several kinds of liquors from beer to whisky can easily be measured with a fast response time less than 1 minute.
1. Introduction
In every-day life, brewers supply several liquors (alcoholic drinks) such as beer, brandy, wine, and whisky, and people are fond of them. However, in brewery, it takes many times to check the alcohol concentration in product liquors, for example, using a distillation method [1] and gas or liquid chromatography [2]. Therefore, development of a simple and quick detection system of alcohol concentration in liquors is strongly required.
From the above view point, we have studied an optical measurement system of alcohol concentration in liquors using a plastic optical fiber (POF) because the POF has many advantages such as low cost, easiness in handling, and immunity from electrical interface [3β6]. This paper reports on its configuration and basic sensing properties of alcohol concentration in some alcoholic drinks.
2. Sensor Head Structure and Its Sensing Principle
A certain kind of polymers such as novolac swells when it is exposed to vapor-phase alcohol [7] or alcohol solutions. This effect produces a change in refractive index of that film. Figure 1 shows a change in the refractive index of novolac resin when exposed to ethanol, determined using an Abbe refractometer. As can be seen from this figure, after being exposed to the ethanolβ(EtOH), the refractive index in the novolac film decreased remarkably from to 1.46. In opposition, when is ethanol exhausted from the film, its refractive index returned to the initial value. This reversible property is more suitable to construct an optical sensor.
Using this property in the novolac film, we fabricated the POF-type sensor head. Figure 2 shows schematics of the sensor head structure and operation models with and without alcohol, respectively. In this POF sensor, the marketed polycarbonate (PC) fiber with a refractive index of was used after removing the cladding layer. The polystyrene (PS) layer with a refractive index of was coated on the PC fiber surface because the PC surface was broken by the solvent for novolac solution. Referring to the preliminary experiment [7], the novolac/iron complex (novolac/Feβ:βSO) was found to be superior to novolac resin only. Therefore, we used it as an alcohol sensitive material.
| (a) Without alcohol: (leaky-POF structure) |
| (b) With alcohol: (guided-POF structure) |
In Figure 2(a), the sensor head operates as a leaky POF (i.e., ), and the intensity of output light passing through it is very weak. In this case, by using a ray tracing method, the calculated total output light intensity is given by where P(ΞΈ) is the optical power for a ray with an angle , is the critical angle at the input side of the POF, is the power reflection coefficient, and is the reflection number in the sensor head.
On the other hand, when exposed to alcohol, the cladding layer swells, and its refractive index begins to decrease, becoming lower than that of the fiber core (i.e., ). Then, as shown in Figure 2 (b), the sensor head changes to a guided POF, and the output light intensity increases remarkably. In this case, the total output light intensity of the sensor head is given by where is the critical angle of the sensor head. The value of describes the relative change in the output light intensity depending on the alcohol.
As is evident from (1) and (2), for enabling this sensor to respond to alcohol at a low concentration, the difference between the initial refractive index of the cladding and that of core is required to be decreased so that switching from the leaky to the waveguide modes becomes easy. Hence, we have mixed low-refractive-index polyvinylidenefluoride (PVDF; ) with novolac resin so that the refractive index of the cladding polymer approaches that of the PC (polycarbonate) core. The mixed film of novolac/Fe:SO and PVDF with a ratio of 3 to 1 was coated on the above PS-coated-PC fiber (PS/PC) with a core diameter of 0.8βmm, by means of a dip coating.
Next, we consider the effect of the intermediate protective PS layer. In terms of a ray-tracing technique based on the Snellβs law where is the refractive index of PS. If the refractive index of the PC core layer, , is smaller than that of the intermediate PS layer, (i.e., ), the total reflection of light from the core at the cladding interface (on the core side) is determined from the refractive index of the PC core layer, , and that of the cladding layer, , regardless of the presence or absence of the intermediate PS layer. Therefore, the intermediate PS layer does not affect the total reflection.
3. Experimental Setup
Figure 3 shows the experimental setup. The POF-type sensor head was set in the small chamber and was connected to the normal POFs on its input and output side. A green LED light with a wavelength of about 530βnm was guided through the input-side POF, and the transmitted light intensity was measured at the end of output-side POF using a photodiode. The output electrical signal was fed to a digital voltmeter and a computer for data processing. As sensing samples, ethanol solutions diluted by water and several kinds of marketed liquor were used.
4. Experimental Results
First, the sensor response for 100% ethanol was checked. Its result is shown in Figure 4. From this figure, it is found that the transmitted light intensity passing through the sensor head (output light intensity) increased remarkably as soon as ethanol was injected and then reached a stable value after about 1βmin. In addition, this system showed good reproducibility. On the other hand, when the ethanol solution was ejected, the spiky signal suddenly appeared and then the output intensity began to decrease slowly. These phenomena are due to residual alcohol droplets attached on the sensor head surface. In fact, after sending dry air to the sensor head by using a blower, the output intensity returned to the initial value. So, next, the change in output light intensity against various ethanol solutions was measured. The result is shown in Figure 5.
From this figure, it is found that the output light intensity increases with fast response time less than 0.5βmin. Thus, the presented POF sensor operated as a quick and good ethanol-concentration sensor over the range of about 20βv/v% to 100βv/v%. However, it did not operate for the low-ethanol-concentration region below 10βv/v%. So, further improvement was needed to obtain higher sensitivity.
5. Fabrication of Taper-Type POF Sensor Head
As shown in Figure 2, lower modes in this POF-type sensor head mainly contribute to the sensitivity. Therefore, to improve sensitivity, it is better to use a sensor head with a small core diameter. So we tried to fabricate a taper-type POF sensor head by means of a solution etching. The PC fiber with a core diameter of 0.8βmm and a length of 50βmm was etched by immersing in 1,4-dioxane for about 1 hour at room temperature and then the PS layer and the novolac/Feβ:βSO +βPVDF sensitive cladding layer were dip-coated on it in turn, as shown in the illustrated sensor head structure in Figure 6.
6. Measurement of Alcohol Concentration in Liquors
The change in output light intensity against a various ethanol concentration was measured using the new taper-type POF sensor head. Its result is shown in Figure 7. As is clear from this figure, it became possible to measure a low concentration of ethanol solution below 5βv/v%. In addition, if we compare these data with the results obtained using non tapered sensors as shown in Figure 5, we can observe that the change in the intensity of the transmitted light with the concentration of each component becomes so large that the sensitivity is improved by at least a factor of three. This result shows that this sensor can be used for detecting alcohol concentration of several real liquors.
In addition, the result in Figure 8 shows that this sensor does not receive any influence from water. The change in the light intensity with temperature is shown in Figure 9. The light intensity has a negligible dependence on temperature. These properties are also very suitable for a real application. Through these experiments, a calibration curve against ethanol concentration could be obtained as shown in Figure 10. In addition, the response does not depend on the concentrations of sugar and salt or acid and alkali, which are potentially contained in alcoholic beverages. This is because novolac resin in the cladding polymer does not exhibit swelling due to these components.
So, next, we tried to measure the alcohol concentration in real liquors such as beer, βUmeβ brandy, red wine, white wine, and whisky, which were on the market. The result is shown in Figure 11. The data for white wine is not shown in Figure 11 because it almost overlapped the one of red wine. As can be seen from this figure, alcohol concentration in real liquors can be measured without receiving any influence of color substance and bubble in liquors.
Using the value of the output light intensity at about 1 minute after and the obtained calibration curve in Figure 10, the main result in this paper could easily be obtained as shown in Figure 12. This figure shows that the measured alcohol concentration fitted well to the one described on the label of real liquor bottle with an accuracy of βv/v%. Namely, usefulness of the presented POF-type alcohol concentration sensor was demonstrated.
7. Conclusions
A novel and very simple POF-type sensor for detecting alcohol concentration in liquors, which is based on the POF structure change in sensor head from leaky-type to guided-one, has been studied experimentally. Using this sensor head with a small core diameter of about 0.25βmm, optical detection of the alcohol concentration in real liquors, for example, from beer (5βv/v%) to whisky (40βv/v%) could easily be obtained with a fast response time less than 1βmin. Therefore, this sensor will be available for use in any brewery. In addition, the sensitive cladding polymer used here also responds to methanol in vapor phase and solution. Therefore, the presented POF-type alcohol sensor may be used for monitoring leakage of methanol in methanol battery system. Such a study is underway in our laboratory and its result will be reported in the near future.