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Figure 2
Time dependence of the X-ray intensities at 2θ = 0.8° for pure water droplets in mist using a flow cell with (above) and without (below) Kapton windows. When the power to the ultrasonic oscillators (US) was on, a significant jump was observed when using the flow cell without Kapton windows (below). |


journal menu![[Figure 2]](cj6005fig2.jpg)



