This protocol describes the design and manufacture of a water bridge and its activation as a water fiber. The experiment demonstrates that capillary resonances of the water fiber modulate its optical transmission.
In this report, an optical fiber of which the core is made solely of water, while the cladding is air, is designed and manufactured. In contrast with solid-cladding devices, capillary oscillations are not restricted, allowing the fiber walls to move and vibrate. The fiber is constructed by a high direct current (DC) voltage of several thousand volts (kV) between two water reservoirs that creates a floating water thread, known as a water bridge. Through the choice of micropipettes, it is possible to control the maximal diameter and length of the fiber. Optical fiber couplers, at both sides of the bridge, activate it as an optical waveguide, allowing researchers to monitor the water fiber capillary body waves through transmission modulation and, therefore, deducing changes in surface tension.
Co-confining two important wave types, capillary and electromagnetic, opens a new path of research in the interactions between light and liquid-wall devices. Water-walled microdevices are a million times softer than their solid counterparts, accordingly improving the response to minute forces.
Since the breakthrough of optical fibers in communication, awarded with a Nobel prize in 20091, a series of fiber-based applications grew alongside. Nowadays, fibers are a necessity in laser surgeries2, as well as in coherent X-ray generation3,4, guided-sound5 and supercontinuum6. Naturally, the research on fiber optics expanded from utilizing solids into exploiting liquids for optical wave guiding, where liquid-filled microchannels and laminar flow combine the transportation properties of a liquid with the advantages of optical interrogation7,8,9. However, these devices clamp the liquid between solids and, therefore, forbid it to express its own wave character, known as capillary wave.
Capillary waves, similar to those seen when throwing a stone into a pond, are an important wave in nature. However, due to the obstacles of controlling a liquid without dampening its surface through channels or solids, they are hardly utilized for detection or application. In contrast, the device presented in this protocol has no solid boundaries; it is surrounded by and flows in air, allowing, therefore, capillary waves to develop, propagate, and interact with light.
To fabricate a water fiber, it is necessary to go back to a technique known as the floating water bridge, first reported in 189310, where two beakers filled with distilled water and connected to a high-voltage source will form a fluidic, water thread-like connection between them11. Water bridges can reach up to a length of 3 cm12 or be as thin as 20 nm13. As for the physical origin, it has been shown that surface tensions, as well as dielectric forces, are both responsible for carrying the bridge's weight14,15,16. To activate the water bridge as a water fiber, we couple light in with an adiabatically tapered silica fiber17,18 and out with a silica fiber lens19. Such a device can host acoustical, capillary, and optical waves, making it advantageous for multi-wave detectors and lab-on-chip20,21,22 applications.
CAUTION: This experiment involves high voltage. It is the reader's responsibility to verify with the safety authorities that their experiment follows regulations before turning on the high voltage.
NOTE: Any kind of polar liquid can be utilized to produce liquid fibers, such as ethanol, methanol, acetone, or water. The polarity of the liquid dictates the stability and diameter of the created fiber23,24. For best results, use deionized water with 18 MΩ resistance. Before choosing optical components, such as optical fibers and light sources, consult the literature to ensure a low absorption in the water/liquid fiber at the desired optical wavelength. The protocol can be paused at any given moment before filling the water reservoir (step 4.5).
1. Preparation of Water Reservoirs and Experimental Station
2. Choosing the Micropipettes and Voltage
3. Preparation of the Optical Couplers
NOTE: For the best transmission result, use a single-mode tapered fiber to launch laser light into the water fiber and a highly multimode reflowed fiber lens as the output coupler (core > 100 µm). However, for easy operation, use a low multimode fiber as the output coupler (for example, a 1550-nm single-mode fiber for a 780-nm wavelength).
4. Assembling
5. Running the Experiment
The coupling efficiency from a water fiber to a highly multimode fiber can be as high as 54%25,26. The coupling efficiency to a single-mode fiber is up to 12%25,26. Water fibers can be as thin as 1.6 µm in diameter and can have a length of 46 µm (Figure 3)25,26, or they can be up to 1.064 mm in length with a diameter of 41 µm (Figure 3)25,26. The transmission spectrogram reveals capillary oscillation of the water fiber, similar to that of a guitar string (Figure 4)25,26. The capillary quality factors were estimated to be as high as 14 for long fibers25,26. Considering the theory on water bridges, it is possible to estimate the ratio between the surface tension and the dielectric force25,26.
Figure 1: Schematics of the set-up. (a) This illustration shows the water fiber experimental set-up. (b) This sketch shows the water reservoir, the electrical connector, and the pipette clamp. (c) This panel shows the water-walled waveguide softness compared with common solids. This figure is reproduced in part from Douvidzon et al.25,26. Please click here to view a larger version of this figure.
Figure 2: Set-up photos. (a) This panel shows the PMMA-water reservoir on a 5-DOF mount. with the PMMA-pipette clamp, the micropipette, the optical fiber, and the electric connector. (b) This panel shows that a fluidic contact between the micropipettes is created. (c) This panel shows that the distance between the micropipettes is increased to establish a water fiber. Please click here to view a larger version of this figure.
Figure 3: Water fiber characterization. (a) This panel shows a water fiber longer than 1 mm. The next two panels show (b) a micron-scale-thin water fiber, (c) the surface scattering due to capillary waves at the water fiber liquid-phase boundary. (d) This panel shows light propagation through the water fiber volume confirmed by a fluorescent dye measurement. This figure is reproduced from Douvidzon et al.25,26. Please click here to view a larger version of this figure.
Figure 4: Experimentally measuring the water fiber "guitar-string" modes. (a) This panel shows a time trace measurement. (b) A fluctuation spectrum reveals a fundamental mode and, at integer multiplications, its three overtones (dash lines). (c) This panel shows a fluctuation spectrogram of a 0.94-mm-long fiber with changing voltage and, correspondingly, changing the fiber diameter, with voltage first constant, then increased, and finally, decreased. The color code describes the transmission. (d) This panel shows the fundamental frequency of the fiber as a function of the fiber diameter (circles) together with a theoretical prediction (dashed line). Horizontal and vertical error bars represent the uncertainty of eight consecutive, 250-ms-apart measurements of the central frequency and its corresponding fiber diameter. For all panels, the fiber length is 0.94 mm and the oscillation is optically interrogated with a photodetector. The diameter is measured via microscope. This figure is reproduced from Douvidzon et al.25,26. Please click here to view a larger version of this figure.
Water fiber | Pipette’s internal diameter | ||||
Length [µm] | Radius [µm] | Potential [V] | Taper side [µm] | Lens side [µm] | |
Fig. 1b | 830 | 51 | 6000 | 850 | 850 |
Fig. 2a | 1064 | 20.5 | 6000 | 850 | 850 |
Fig. 2b | 46 | 1.6 – 0.8 | 1500 | 150 | 850 |
Fig. 2c | 820 | 32.5 | 5000 | 850 | 850 |
Fig. 2d | 110 | 4.75 | 3000 | 150 | 150 |
Fig. 3 | 940 | 20 – 90 | 3000 – 8000 | 850 | 850 |
Fig. 4 | 24 – 73 | 2.7 – 3 | 2500 | 150 | 850 |
Table 1: Water fiber length and radius. This table shows the water fiber length and radius with respect to the electric potential and the pipette diameter. This table is reproduced from Douvidzon, et al.25.
To conclude, the major advantage and uniqueness of this technique is creating a fiber which hosts three different kinds of waves: capillary, acoustic, and optical. All three waves oscillate in different regimes, opening the possibility for multi-wave detectors. As an example, airborne nanoparticles affect the surface tension of liquids. Already at the current stage, it is possible to monitor changes in the surface tension through variations in the capillary eigenfrequency. Additionally, water-walled devices are a million times softer than their solid counterparts, improving the sensibility of sensors accordingly.
Based on experience with this set-up, we noticed a high dependency on the signal-to-noise ratio and the quality of the optical couplers. Therefore, it is recommended to pay close attention to the fabrication of the optical couplers. Consider an aquarium set-up to ensure a dust-free environment for the tapering station and the water fiber set-up. Also, the execution of the experiment involves a risk of breaking or damaging the tapered fiber coupler mechanically or through an electric arc. In that case, the optical transmission can drop and become noisy to such an extent that the capillary modes of the fiber are no longer visible in the spectrogram.
If capillary waves are not visible in the transmission measurements, remanufacture the couplers. Additionally, the water fiber and the optical fiber couplers do not attract each other. Adjusting the set-up for optimal transmission may require putting the water fiber a bit askew, to mechanically press the tapered fiber coupler inside the water fiber.
Another obstacle in this set-up to be aware of is the crucial electrical resistivity of the water. Even small amounts of ions in the liquid will cause the bridge to collapse. If the water fiber is shorter and less stable than expected, a contamination of the water might be the cause. Replace the water with 18 MΩ clean room water. Additionally, the high voltage attracts charged air particles in the surrounding of the water fiber, which dissolve and contribute to the instability. In this case, a closed chamber will help improve the water fiber longevity.
An outstanding aspect of this set-up is that any polar liquid can be utilized to create a liquid fiber, although deionized water is known for creating the longest, as well as, time-wise, the most stable water fibers. It is interesting to consider other liquids for different applications. Switching the water to a liquid or a mix of polar liquids with fitting viscosity, surface tension, or optical properties allows researchers to trim the fiber exactly to their demands.
The authors have nothing to disclose.
This research was supported by the Israeli Ministry of Science, Technology & Space; ICore: the Israeli Excellence center 'Circle of Light' grant no. 1802/12, and by the Israeli Science Foundation grant no. 2013/15. The authors thank Karen Adie Tankus (KAT) for the helpful editing.
Deioniyzed Water | 18MOhm resistance | ||
Micropipettes, Borosilicate Glass, round, inner diameter 850 micron | Produstrial.com | #133260 | |
Micropipettes, Borosilicate Glass, round, inner diameter 150 micron | Produstrial.com | #133258 | |
High voltage, low current source, 3kV with 5 mA. | Bertan | Model 215 | |
High voltage, low current source, 8 kV with 0.25 mA. | Home build | ||
Optical fiber | Corning | HI 780 C | 5 meter |
Optical fiber | Thorlabs | FTO 30 | 5 meter |
Optical fiber | Thorlabs | FTO 30 | 5 meter |
Fiber coupled laser | FIS | SMF 28E | |
Photoreceiver | New Port/ New Focus | 1801-FS | with fiber connection |
Oscilloscope | Agilent Technologies | DSO-X 3034A | |
2 Degree of freedom tilt stagestage | New Port/ New Focus | M-562F-TILT | |
3Degree of freedom linear micro translation stage | New Port/ New Focus | M-562F-XYZ | |
A set of magnets | |||
Objective 5X | Mitutoyo | MY5X-802 | |
Objective 20 x | Mitutoyo | MY20X-804 | |
Zoom | Navitar | 12x Zoom | |
Microscope tube | Navitar | 1-6015 standard tube | |
Isopropanol | Sigma Aldrich | 67-63-0 | Spec Grad |
2 x Bare Fiber holder | Thorlabs | T711-250 | |
2 x Translational Stage | Thorlabs | DT12 | |
Block of PMMA for fabricating the water reservoir and pipette holder | 150 x 60 x 10 mm | ||
PTFE-Tape | Gufero | 240453 | |
Fiber coupled, cw Laser Light Source | New Port/ New Focus | TLB-6712 | 765-781 nm |