“…Eventually the lowest power for each of the splitter become decreased too with reference to the highest power reading. Common problem with a liquid level sensor using other fiber based scheme such as the FBG and interferometer [2,5] is that the range of the liquid level is very limited to short range of a few centimeters. In contrast, the proposed sensor scheme can support greater range from short to very long up to a few meters.…”
Section: Results and Analysismentioning
confidence: 99%
“…The low insertion loss contributes to low overall loss for the total reflected power and hence maximizes the dynamic range of the sensor. The main advantage of this sensor scheme is that it could provide customization of liquid level measurement range up to hundred meters with simple configuration instead of the complicated point measurement scheme employed by MMI [9,[16][17][18], U-shaped [16,19,20,21] and POF [17,22,23,24] based sensors. Since our sensor is based on intensity measurement, it is suggested to have one of the multiple outputs acting as the reference signal using the ratio metric scheme.…”
Section: Results and Analysismentioning
confidence: 99%
“…Optical fiber sensors offer several advantages as compared to other technologies in terms of their relativelysmall size, lightweight, high survivability in extreme environments, inexistence of electrical signal at the sensor head, immunity from electromagnetic interference, having a remote distance between signal generation and detection, possibility of multiplexing as well as demonstrating high sensitivity. Therefore, several optical fiber liquid level sensors with differing approaches have been extensively developed and applied including liquid level sensor based on the fiber grating [1][2][3][4], fiber interferometry sensing [5][6][7], multimode interference (MMI) scheme [8][9][10] and fiber bend configuration [11,12].…”
A novel simple fiber sensor to sense liquid level is presented. The operation principle is based on the relative Fresnel reflective intensity. The sensor consists of a fiber splitter with the configuration of one input to multiple fiber outputs, i.e. 1×4, 1×8 and 1×12 arrangements that act as a discrete liquid level. A broadband source (BBS) is used as the light source supply. The total reflected power intensity is measured using a power meter. Experimental results show that the power intensity decreases as the level of liquid is increased. The sensor has a simple configuration, low cost, and it can be customized for a wide height measurement range spanning from a few centimeters up to a hundred meters.
“…Eventually the lowest power for each of the splitter become decreased too with reference to the highest power reading. Common problem with a liquid level sensor using other fiber based scheme such as the FBG and interferometer [2,5] is that the range of the liquid level is very limited to short range of a few centimeters. In contrast, the proposed sensor scheme can support greater range from short to very long up to a few meters.…”
Section: Results and Analysismentioning
confidence: 99%
“…The low insertion loss contributes to low overall loss for the total reflected power and hence maximizes the dynamic range of the sensor. The main advantage of this sensor scheme is that it could provide customization of liquid level measurement range up to hundred meters with simple configuration instead of the complicated point measurement scheme employed by MMI [9,[16][17][18], U-shaped [16,19,20,21] and POF [17,22,23,24] based sensors. Since our sensor is based on intensity measurement, it is suggested to have one of the multiple outputs acting as the reference signal using the ratio metric scheme.…”
Section: Results and Analysismentioning
confidence: 99%
“…Optical fiber sensors offer several advantages as compared to other technologies in terms of their relativelysmall size, lightweight, high survivability in extreme environments, inexistence of electrical signal at the sensor head, immunity from electromagnetic interference, having a remote distance between signal generation and detection, possibility of multiplexing as well as demonstrating high sensitivity. Therefore, several optical fiber liquid level sensors with differing approaches have been extensively developed and applied including liquid level sensor based on the fiber grating [1][2][3][4], fiber interferometry sensing [5][6][7], multimode interference (MMI) scheme [8][9][10] and fiber bend configuration [11,12].…”
A novel simple fiber sensor to sense liquid level is presented. The operation principle is based on the relative Fresnel reflective intensity. The sensor consists of a fiber splitter with the configuration of one input to multiple fiber outputs, i.e. 1×4, 1×8 and 1×12 arrangements that act as a discrete liquid level. A broadband source (BBS) is used as the light source supply. The total reflected power intensity is measured using a power meter. Experimental results show that the power intensity decreases as the level of liquid is increased. The sensor has a simple configuration, low cost, and it can be customized for a wide height measurement range spanning from a few centimeters up to a hundred meters.
“…The appearance of other lasing modes was evident as the temperature increased because of the modal competitions was similar for all the lasing modes involved. It is well recognized that fiber-optic interferometers exhibit a suitable sensitivity for refractive index and temperature variations [44]; however, the ring laser cavity represents an alternative method to extract phase information [1][2][3][4][5][6][7][8][9]. In analyzing peaks P2, P3, and P6, the following thermal-wavelength relations can be expected: 21.01 pm/°C (P2), 16.99 pm/°C (P3), and 16.97 pm/°C (P6), as well as adequate linear responses of 0.96306 (P2), 0.99507 (P3), and 0.9890 (P6).…”
Section: Temperature Analysismentioning
confidence: 99%
“…For several decades, the ability to generate tunable or switched multi-wavelength fiber lasers has been one of the focuses pursued by the fiber laser community. These lasers are associated with many reliable applications related to multi-wavelength spectra such as optical fiber sensors [1][2][3][4][5][6][7][8][9], spectroscopy systems [10], biomedical imaging [11], telecommunications [12], microwave photonics [13], and radio frequency optical domain systems [14]. These applications require achieving compact configuration, stable emission, narrow linewidth, and adequate spacing mode.…”
A tunable multi-wavelength fiber laser is proposed and demonstrated based on two main elements: an erbium-doped fiber ring cavity and compact intermodal fiber structure. The modal fiber interferometer is fabricated using the cost-effective arc splice technique between conventional single-mode fiber and microfiber. This optical fiber structure acts as a wavelength filter, operated in reflection mode. When the refractive index and temperature variations are applied over the fiber filter, the ring laser cavity provides several quad-wavelength laser spectra. The multi-wavelength spectra are tuned into the C-band with a resolution of 0.05 nm. In addition, the spectra are symmetric with minimal power difference between the lasing modes involved, and the average of the side mode suppression ratio is close to 37 dB. This laser offers low-cost implementation, low wavelength drift, and high power stability, as well as an effect of easy controllability regarding tuned multi-wavelength.
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