Laser ultrasonic excitation using graphene heat dissipation film for ultrasonic detection of seismic physical model

2.1. Characterization of graphene heat dissipation film

The GHDF has a thickness ranging from 17 µm to 200 µm. Scanning electron microscopy (SEM), x-ray diffraction (XRD, Bruker, D8 Advance) and ultraviolet-visible spectroscopy (UV-vis) are respectively used to characterize the structure and morphology of the GHDF. Fig. 1(a) shows the top-view SEM image of the film with a thickness of 50 µm. The film surfaces have smooth and uniform arrangement. Fig. 1(b) shows the cross section SEM image with film thickness of 50 µm. The multi-layer film structure can be clearly observed.The XRD analysis in Fig. 1(c) shows that the material has a strong characteristic diffraction peak at 2-theta of 26.44°, which corresponds to the (002) crystal plane of carbon. The UV-vis spectrum of GHDF is demonstrated in Fig. 1(d). The curve of the spectrum tends to rise first and then fall, and the material has strong absorption of visible light.

Fig. 1a) Top-view SEM image of the film with a thickness of 50 µm; b) Cross-section SEM image of the film with a thickness of 50 µm; c) XRD pattern of the GHDF; d) UV-vis absorption spectra of the GHDF

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2.2. Theoretical simulation

PA effect is actually the interaction between laser and material. The conversion of light energy into heat energy causes the increase of material temperature, which produces thermal expansion and finally results in acoustic waves. A two-dimensional axisymmetric model is developed to simulate the effects of laser and material parameters on PA signal, as shown in Fig. 2(a).

The laser parameters are referenced to the typical commercial laser used in the experiment, where the laser wavelength is 532 nm, pulse power ranges from 1 mW to 3 mW, laser spot radius is 0.1 mm, pulse duration is 8 ns. The simulated PA signal is shown in Fig. 2(b). Because the thermal diffusion has a delay after laser irradiation, there are several attenuated oscillations following the main signal peak. Similar waves can also be observed in measurements. Different laser powers are applied to excite the film and the results are shown in Fig. 2(c). When the laser power is set in the damage threshold range of the film, the signal amplitude increases with the laser power. However, when the laser power exceeds the damage threshold, the material may be gasified. Fig. 2(d) shows the excited signals with the films thickness ranging from 10 µm to 200 µm. When the film thickness is around 100 µm, the signal amplitude reaches the maximum.

Fig. 2a) The ultrasonic excitation in two-dimensional axisymmetric model: 1 – water area; 2 – GHDF; 3 – silica glass substrate; b) PA signal excited in simulation; c) PA signal excited by different laser powers; d) PA signal excited with different thicknesses of films

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3.1. PA signal of GHDF

The PA effect of the GHDF is demonstrated in the system of Fig. 3. A 532 nm pulsed laser is used as the excitation source: the pulse repetition frequency is 1 Hz, the single pulse power ranges from 1 mW to 6 mW, and the spot radius is 1 mm. The nanosecond laser is focused and irradiated on the graphene material through a series of mirrors. The film is attached onto the SPM surface and both of them are placed underwater for laser irradiation. A PZT with a central frequency of 1 MHz is used to receive the ultrasonic waves. An electric moving stage is used here for SPM scanning detection.

The thickness of the GHDF is 100 μm. Fig. 4(a) shows the signal amplitude change when the laser power increases from 1 mW to 3 mW. It can be seen that the signal pulse widths at different laser powers keep consistent. Fig. 4(b) shows the signal amplitude variation with the laser power increasing from 1 mW to 6 mW. The signal amplitude fluctuates from 4 mW to 6 mW, possibly because of the overloaded laser power reaching the damage threshold of GHDF.

Fig. 4(c) shows the ultrasonic signals with film thicknesses of 50 μm, 100 μm, and 200 μm. The maximum signal amplitude is obtained at the 100 µm thickness, which is consistent with the theoretical calculation. The above acoustic measurements prove the great PA effect of the GHDF, and thus provides a new approach for the subsequent laser ultrasonic detection of physical model.

Fig. 3Experimental set-up: 1 – 532 nm Nd: YAG laser; 2 – PC; 3 – data acquisition card; 4 – mirror set; 5 – PZT; 6 – water tank; 7 – electric moving stage

Fig. 4a) Ultrasonic signals with laser powers of 0.96 mW, 1.83 mW, and 2.92 mW; b) signal amplitudes with laser powers increasing from 1 mW to 6 mW; c) ultrasonic pulses with different material thickness, d) variation of signal amplitude with material thickness

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3.2. SPM detection

In order to verify the feasibility of GHDF in laser ultrasonic detection of SPM, a simple geological stepped structure is designed in Fig. 5(a). The height is 25 mm, 15 mm, 30 mm from left to right. The ultrasonic waves are effectively excited on surface 1, where the GHDF is attached. The time-domain echo signal of the model at point A is shown in Fig. 5(b), where the first peak signal is from surface 1 and the second peak signal around 53.7 µs is reflected from surface 2. Given the ultrasonic velocity of 2583.33 m/s in the model, the model height at point A can be calculated as 31.12 mm, which agrees well with the actual value.

Fig. 5a) SPM photographs with GHDF coating; b) time-domain echo signal at the point A of SPM

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