RESEARCH ARTICLE
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Synthesis of Novel CuO–Gelatin Nanofluids Using
Ultrasonic Technique
Mathana Gopal Arunachalam,* Padmavathi Paulraj, Irudaya Sahaya Lancy Sreedharan,
Krishna Kumar Pandey, Poongodi Jawaharlal, and James C.
Nanofluid molecular properties, such as acoustical properties, vary widely in
system parameters and are influenced by liquid cohesive characteristics.
Gelatin is a natural polymer made from the partial hydrolysis of collagen,
which allows the triple helix to unfold and split, resulting in a polydisperse
mixture of proteins in solution. The use of ultrasonic technology to create
nanoparticles from biopolymer base fluids is a novel method of nanofluid
synthesis. The focus of this research is to measure the ultrasonic velocity and
density of synthesized nanoparticles using gelatin as the base fluid at various
weight percentages. The study have synthesized the Copper oxide (CuO)
nanofluid by transforming an unstable Cu(OH)
2
to CuO as a precursor in
aqueous gelatin by ultrasonication process. To characterize the prepared
nanoparticles, the XRD and FESEM methods are used. The results of
ultrasonic velocity, density, and viscosity measurements are discussed after
ultrasonication. Experimental data and a theoretical approach to nanofluids
are used to study the stability of nanofluids. The outcomes of ultrasonic
spectroscopy and other investigations are very similar.
1. Introduction
The conventional working fluid which is used in various heat
exchangers such as water, oil, ethylene glycol plays an impor-
tant role in many engineering applications for heating and cool-
ing processes. To increase the heat transfer efficiency several
methods can be adopted such as utilization of extended surfaces,
M. G. Arunachalam, P. Paulraj, I. S. L. Sreedharan, J. C.
PG & Research Department of Physics
Scott Christian College
Nagercoil, Tamil Nadu 629003, India
E-mail: matgop04@gmail.com
K. K. Pandey
Acoustics Research Laboratory
Department of Physics
School of Basic Sciences and Research
Sharda University
Greater Noida, Uttar Pradesh 201310, India
P. Jawaharlal
Department of Physics
Kamaraj College
Thoothukudi, Tamil Nadu 628003, India
The ORCID identification number(s) for the author(s) of this article
can be found under https://doi.org/10.1002/masy.202200007
DOI: 10.1002/masy.202200007
applying vibration to the heat transfer sur-
faces, and improving the thermal conduc-
tivity of the working fluids.
The term nanofluid was first used by Choi
[1]
at Argonne National Laboratory in the USA.
At present the development takes place in
the field of nanoscience, the nanofluid are
very useful as working fluid due to more
heat transfer enhancement. The application
of nanofluid has a strong potential for en-
hancing the heat transfer in any type of heat
exchanger.
[2,3]
The important requirements considered
while preparation of nanofluid is even sus-
pension, no chemical changes, and low
agglomeration and stable suspension. By
using any nanomaterial or oxides with
basefluid the nanofluid can prepare by
the single-step method or two stepmethod
(dispersionmethod).
[4–10]
2. Results and Discussions
Peaks at 2 values corresponding to the lattice planes of CuO
nanoparticles were obtained. CuO nanoparticles with a mon-
oclinic structure and a crystalline size of 55.53 nm were pro-
duced as confirmed by JCPDS card no. 77–1898. XRD patterns
of nanoparticles reveal an excellent crystalline structure among
the peaks in their particle size range shown in Figure 1. Images
of dry CuO nanoparticles were taken with a FESEM. Highly ag-
glomerated particles in the micrometer range are observed under
atmospheric conditions, with the bulk of nanoparticles appearing
spherical in shape. As a result, the results revealed that the CuO
nanoparticles are both spherical in shape shown in Figure 2.
[11–13]
Ultrasonic velocity of CuO–Gelatin increased as the tempera-
ture increased from 308 to 333K. The ultrasonic velocity of CuO–
Gelatin increases with weight percentage increases. This results
in CuO–Gelatin molecular interactions with a maximum range
of 1577 m s
−1
, as shown in Figure 3. In Figure 4, the relative den-
sity decreases with increase in temperature of all weight percent-
ages with uniform behavior. Similarly Auerbach surface tension
also shows the same at decreases in parameters at 323 K for all
wt% shown in Figure 5. Where the viscosity can also be seen to
show the uniform behavior of the CuO–Gelatin while increas-
ing the weight percentage, the viscosity also decreases while in-
creasing the temperature shows the extensive polymer behavior
in Figure 6.
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