Atomization and Sprays, 29(1):59–78 (2019)
X-RAY PHASE CONTRAST IMAGING OF
CAVITATION AND DISCHARGED LIQUID
JET IN NOZZLES WITH VARIOUS SIZES
Rubby Prasetya,
1,*
Akira Sou,
1
Seoksu Moon,
2,*
Raditya Hendra Pratama,
3
Yoshitaka Wada,
4
&
Hideaki Yokohata
4
1
Graduate School of Maritime Sciences, Kobe University, Japan
2
Department of Mechanical Engineering, Inha University, Republic of Korea
3
Research Institute for Energy Conservation, National Institute of Advanced
Industrial Science and Technology, Japan
4
Powertrain Engineering Analysis Group, Mazda Motor Corporation, Japan
*Address all correspondence to: Rubby Prasetya, Graduate School of Maritime Sciences,
Kobe University, Japan; Tel.: +81 784 316 200; Fax: +81 784 316 355,
E-mail: 142w601w@stu.kobe-u.ac.jp;
or Seoksu Moon, Department of Mechanical Engineering, Inha University, Republic of
Korea; Tel.: +82 328 607 378, E-mail: ss.moon@inha.ac.kr
Original Manuscript Submitted: 12/19/2018; Final Draft Received: 4/17/2019
Visualization of internal cavitation flow in the nozzle is sometimes carried out with enlarged, trans-
parent nozzles, in order to capture the images of cavitation bubbles with relatively high spatial
resolution. However, it is unclear whether knowledge obtained from large-scale nozzles can be ap-
plied to nozzles with much smaller sizes, which provides a great impetus to study the nozzle size
effects on in-nozzle cavitation and discharged liquid jet characteristics. In this study, visualization
of cavitation in nozzles with various sizes was conducted to clarify the effects of nozzle size on cav-
itation. The visualization was carried out using x-ray phase contrast imaging (XPCI) to clearly
observe individual cavitation bubbles. Furthermore, to investigate the effects of cavitation in nozzles
with various sizes on the wavy interface structure of a discharged liquid jet, the discharged liquid
jets were also visualized. Rectangular plain-orifice nozzles with a length-to-width ratio of 4 were
used in the study. The width of the nozzles varies from 2.0, 1.0, and 0.50, to 0.25 mm. As a result
of the study, we clarified the fact that a cavitation cloud is made of a number of deformed bubbles,
while a sheet cavitation consists of a single cavitation film. In-nozzle cavitation bubbles follow the
similarity law; that is, the diameter of incipient cavitation bubbles changes along with the change in
nozzle size. Additionally, the wavy structure of the discharged liquid jet is finer at the super cavita-
tion regime, although the finer structure is suppressed as nozzle size decreases, due to the relatively
stronger surface tension force acting on the interface of the wavy liquid jet discharged from smaller
nozzles.
KEY WORDS: plain-orifice nozzle, in-nozzle cavitation, liquid jet, size effect, x-ray phase
contrast imaging
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