A primary magnesium battery has been constructed using the maximum conductivity biopolymer electrolyte (40%CA:60% Mg(ClO 4 ) 2 ).. Magnesium metal in pellet form was taken as the.[r]
Trang 1Original Article
Characterization of biopolymer electrolytes based on cellulose acetate
M Mahalakshmia,b,c, S Selvanayagama, S Selvasekarapandianb,d,*, V Monihab,e,
R Manjuladevib,f, P Sangeethab
a PG & Research Dept of Physics, Govt Arts College, Melur, 625 106, India
b Material Research Center, Coimbatore, 641 045, India
c Department of Physics, Sri Meenakshi Govt Arts College for Women(A), Madurai, 625 002, India
d Department of Physics, Bharathiar University, Coimbatore, 641 046, India
e Centre for Research and PostGraduate Studies in Physics, Ayya Nadar Janaki Ammal College, Sivakasi, 625 124, India
f Department of Physics, SNS College of Engineering, Coimbatore, 641 107, India
a r t i c l e i n f o
Article history:
Received 27 January 2019
Received in revised form
14 April 2019
Accepted 21 April 2019
Available online 28 May 2019
Keywords:
Biopolymer electrolyte
Cellulose acetate
Magnesium perchlorate
ac impedance technique
Mgþion primary battery
a b s t r a c t Magnesium ion conducting biopolymer electrolytes have been prepared using cellulose acetate and different wt % of magnesium perchlorate with DMF as a solvent by the solution casting technique As-prepared membranes were subjected to different characterization techniques such as XRD, FTIR, DSC,
ac impedance analysis and transference number measurement The amorphous/crystalline nature of the prepared biopolymers was studied by using XRD FTIR study has revealed the formation of complexes between the cellulose acetate and the magnesium perchlorate Glass transition temperatures for the biopolymer electrolytes were found using a differential scanning calorimeter From the ac impedance analysis, the ionic conductivity was calculated The biopolymer membrane (40%CA: 60% Mg (ClO4)2) has shown the highest conductivity of 4.05 104S/cm at room temperature The ionic transference number
of Mg2þ was found as 0.31 by the Evan's method The electrochemical stability of 3.58 V has been observed for the 40%CA:60%Mg(ClO4)2biopolymer membrane by the linear sweep voltammetry study The Mgþ ion primary battery has been constructed using the highest ionic conducting biopolymer membrane The performance of the battery was studied and the open circuit voltage of the battery was found as 1.9 V
© 2019 The Authors Publishing services by Elsevier B.V on behalf of Vietnam National University, Hanoi This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/)
1 Introduction
Biopolymers are natural polymers from renewable resources,
produced by a living organism They contain monomeric units that
are covalently bonded to form a large structure[1] Biodegradable
polymers have been the center of enormous worldwide attention,
as a potential of white pollution[2] Biopolymer electrolytes (BPEs)
are low cost, environmentally green, and suitable to be used as a
host polymer compared to the synthetic polymer electrolytes[3]
for the momentous development of BPE in many electrochemical
devices, such as batteries, fuel cells, sensors, supercapacitors, and
display devices, etc.[4]
Solid Biopolymer Electrolytes (SBPEs) receive more attention due to its non-leakage, high ionic conductivity, long-term structural stability, good thermal, mechanical and electrical stability There are three types of biopolymers, namely polysaccharides, polyesters, and polyamides which are naturally produced by microorganisms
[5] Among the polysaccharide biopolymers, cellulose acetate (CA) has got many advantages, such as excellent transparency, low cost, non-toxic nature, biodegradability and biocompatibility[6] CA is a semi-crystalline biopolymer It is not soluble in water The chemical properties of CA are unique since it contains the carboxyl groups (C¼O) in its structure It has got a good film-forming property because of the intermolecular hydrogen bondings CAfilms are homogeneous and have high mechanical strength The above mentioned properties are essential for any ionic conducting membranes to construct the energy storage devices like a battery, and also various intensive electrochemical applications[7] Despite
* Corresponding author Material Research Center, Coimbatore, 641 045, India.
E-mail address: sekarapandian@rediffmail.com (S Selvasekarapandian).
Peer review under responsibility of Vietnam National University, Hanoi.
Contents lists available atScienceDirect Journal of Science: Advanced Materials and Devices
j o u r n a l h o m e p a g e : w w w e l s e v i e r c o m / l o c a t e / j s a m d
https://doi.org/10.1016/j.jsamd.2019.04.006
2468-2179/© 2019 The Authors Publishing services by Elsevier B.V on behalf of Vietnam National University, Hanoi This is an open access article under the CC BY license
Journal of Science: Advanced Materials and Devices 4 (2019) 276e284
Trang 2the advantages, it has a high crystalline nature which gives the
lowest ionic conductivity that limits the applications of this
poly-mer as electrolyte To overcome the drawbacks, CA has been doped
with different salts
Rani M et al have studied biopolymer electrolytes based on the
derivatives of cellulose from Kenaf Bastfiber[8] Abidin et al have
reported electrochemical studies on cellulose acetate-LiBOB
poly-mer gel electrolytes [9] Proton conducting solid bio-polymer
electrolytes based on carboxymethyl cellulose doped with oleic
acid has been studied by M N Chai and M IN Isa[10] Selvakumar
et al have carried out a research on biodegradable polymer CA
doped with lithium perchlorate (LiClO4) for supercapacitors [11]
Properties of CA membrane with lithium salt (LiTFSI) have been
studied by Ramesh et al.[12] The dielectric behavior of CA
com-plexes with ammonium tetrafluoroborate (NH4BF4)& polyethylene
glycol (PEG) has been reported by Harun et al.[13] S Monisha et al
has studied CA with ammonium salts (NH4SCN)& (NH4NO3) and
the energy storage lithium battery has been constructed using CA
with lithium nitrate (LiNO3)[14e16]
According to a survey, it is observed that the study of the
magnesium ion conducting electrolyte is scarce when compared to
Hþ/Naþ/Liþ[17] Magnesium metal has several advantages such as
low cost, high safety, low equivalence weight, and high reduction
potential when compared to lithium[18] Magnesium-based
bat-teries perform very closely to lithium-based ones Magnesium
batteries have turned up as an alternate for the next rank batteries
due to the intrinsic advantage of the Mg metal Magnesium battery
is an electro-deposited battery that works efficiently, without any
dendrite growth[19] Owing to the divalent property of Mg2þ, this
battery can provide a higher theoretical volumetric capacity
(3832 mAh∙cm3) than Li (2062 mAh∙cm3) So, Mg batteries are
spirited for energy storage devices[20]
The incorporation of Mg (ClO4)2enhances the ionic conductivity
of PVP to 1.1 104 S/cm at room temperature as reported by
Mangalam et al.[21] Kumar Y et al have reported a conductivity
value of 5.6 104S/cm for PEO when complexed with a
magne-sium salt[22] Manjuladevi et al studied a membrane, based on
PVA: PAN/MgCl2 for energy storage devices[23] Shanmugapriya
et al have studied the biopolymer I-carrageenan with magnesium
perchlorate and reported the conductivity value 2.18 103S/cm
[24] Shukur et al have studied the conductivity and dielectric
properties of potato starch doped with magnesium acetate[25]
Hambali et al have reported the plastic crystalline gel polymer
electrolytes based on poly (Vinylidene chloride-Co-Acrylonitrile)
doped with magnesium triflate (MgTf)[26]
Only a few works have reported on a biopolymer with
magne-sium salts To the best of our knowledge, there has been no work
based on cellulose acetate with magnesium salts
In this work magnesium ion conducting biopolymer electrolytes
were prepared using the cellulose acetate and magnesium
perchlorate with DMF as a solvent by the solution casting
tech-nique The prepared membranes were then characterized by
various techniques, namely XRD, FTIR, DSC, and ac impedance
analysis Furthermore, the ionic transference number has been
evaluated by the Evan's method and a primary magnesium battery
has been constructed using the highest conduction electrolyte
2 Materials and experimental methods
Polymer cellulose acetate (CA) from Sigma Aldrich with average
Mn ¼ 50,000 by GPC, p.code: 1001345528 and magnesium
perchlorate Mg(ClO4)2 of the molecular weight of 223.21 g/mol
from Himedia were used without any further purification to
pre-pare the biopolymer electrolytes Dimethylformamide (DMF) with
molecular weight 73.08 g/mol, density¼ 0.948e0.949 kg/m3from Merck specialties private Ltd., Mumbai, India was used as a solvent Different concentrations of CA and Mg(ClO4)2were separately added with DMF solvent at room temperature and stirred contin-uously with a magnetic stirrer for several hours to obtain clear solutions Then both the solutions were mixed together and stirred continuously for several hours to get a homogeneous solution Finally, the solutions were poured into polypropylene Petri dishes and allowed to dry at 60C for 2 days in a vacuum oven for the evaporation of the solvent It yielded a stable free-standingfilm of thicknesses ranging from 180 to 200mm Thefilms were stored in vacuum desiccators Pure CA, 60%CA:40%Mg(ClO4)2, 50%CA:50% Mg(ClO4)2, 40%CA:60%Mg(ClO4)2, and 30%CA:70%Mg(ClO4)2 films were prepared by this method Then, the samples were subjected to various characterization techniques
XRD patterns of polymer membranes were taken on the Philips X'pert PRO diffractometer, where x-rays of 1.5406Aowavelength generated by a Cu-Ka source was uitilized The diffraction peaks were recorded at a 2qangle varied from 10to 90 The biopolymer electrolytes were subjected to the FTIR study using the BRUCKER spectrophotometer in the wave number ranges from 400 to
4500 cm1with a resolution of 1 cm1 The DSC Q20V24.10 Build
122 TA instrument was used to conduct the DSC measurements to analyze the glass transition temperature of the sample The impedance measurements of the biopolymer electrolytes were made in the frequency range of 42 Hz to 1 MHz at room temper-ature using the HIOKI 3532-50LCR HiTESTER The transport number
of the Mg2þions for the highest conducting electrolyte was eval-uated using the Evan's and the Wagner's method The linear sweep voltammetry was used to evaluate the electrochemical stability of the highest conducting electrolytes A primary magnesium battery was constructed using the membrane with the highest ionic con-ductivity as the electrolyte, a magnesium metal plate as the anode and MnO2with graphite in the ratio of 3:1 in form of a pellet as the cathode
3 Results and discussion 3.1 XRD analysis
XRD measurements were performed on the biopolymer elec-trolytes to study their crystalline/amorphous nature.Fig 1shows the XRD patterns for the pure CA, 60%CA:40%Mg(ClO4)2, 50%
Fig 1 XRD patterns of pure CA, 60%CA:40%Mg(ClO 4 ) 2 , 50%CA:50%Mg(ClO 4 ) 2 , 40%
Trang 3CA:50%Mg(ClO4)2, 40%CA:60%Mg(ClO4)2, and 30%CA:70%Mg(ClO4)2
electrolytefilms The peaks are observed for pure CA at 2q¼ 9, 13,
18, 27, and 65which agree with the research already reported
[12,27] The intensity of the peaks decreases with the increase of
the Mg(ClO4)2concentration, which reveals that the doping salt
enhances the amorphous nature of the electrolytes This result was
interpreted by the Hodge et al.[28]criterion, which proves a
cor-relation between the intensity of peak and the degree of the
crys-tallinity XRD patterns confirm the absence of the peaks
corresponding to Mg(ClO4)2in the biopolymer electrolytes which
indicates the complete dissociation of the salt in the polymer
ma-trix The maximum amorphous nature is observed for the sample of
40%CA:60%Mg(ClO4)2 Furthermore, at the addition of 60% of
Mg(ClO4)2, the salt gets recrystallized, which reduces the
amor-phous nature of the polymer matrix
3.2 FTIR analysis
FTIR spectroscopy was used to prove the complex formation and
the interactions between the biopolymer CA and the Mg(ClO4)2salt
by means of the change in the vibrational modes of the electrolyte
under investigation.Fig 2shows the FTIR spectra for the pure CA
and the CA: Mg(ClO4)2complexes of various compositions in the
wavenumber range from 400 to 4000 cm1 The corresponding
vibration frequencies were assigned and are listed inTable 1
The band at about 3372 cm1is assigned to the OeH stretching
of the pure CA The peak observed at 1740 cm1is assigned to the
C¼O stretching in the aldehyde carbonyl group of CA[29] The
medium intensity peak 1374 cm1is attributed to the CeH bending
in the alkanes of the pure CA The absorption peak observed at
1221 cm1for pure CA is assigned to the CeO stretching of the ester
group The peak determined for pure the CA at 1034 cm1 is
assigned to the CeOeC stretching of a pyrose ring and the medium
intensity peak observed at 906 cm1 is assigned to the OeH
bending vibrational mode of the pure CA
The addition of 40, 50, 60, 70, wt % of Mg(ClO4)2to CA produces
changes in the intensity, the shape, and the position of the bands
This implies that the complex reaction occurred due to oxygen from
the ester group[30] The broad peak observed around 3372 cm1
and assigned to the stretching vibration of the hydroxyl groups of
the pure CA gets shifted and widened in the salt added systems
This reveals the coordination between the cations of the salt and the hydroxyl groups of CA The hydroxyl band is shifted towards the higher wavenumber in the salt compositions indicating the specific interaction between the salt and the polymer[31]
The band appeared around 1740 cm1 in the pure CA and assigned to C¼O stretching of CA is decreased in intensity due to the incorporation of Mg(ClO4)2 The decrease in the intensity of the peak indicates the formation of the ion-dipole C¼O Mg2 þcomplex
[32] The new peak appeared at 1646 cm1in the salte biopolymer spectra is assigned to the C¼O stretching in the carbonyl group due
to the interaction of the dopant and the polymer The peaks observed at 1374 cm1, 1221 cm1, and 1034 cm1are attributed to the CeH bending, the CeO stretching and the CeOeC stretching of pure CA, respectively Their intensity is decreased and the wave-number position is shifted towards the increasing value for various complexes of Mg(ClO4)2 This indicates the completed formation of complexes of the biopolymer with the salt at different concentra-tions The peak observed around 608 cm1in all doped samples are ascribed to the CeCl stretching peak, which confirms the presence
of the Clion in the CA-doped Mg(ClO4)2electrolytes[33]
Fig 3 illustrates the possible interaction between CA and Mg(ClO4)2 The interactions between the pure CA and Mg(ClO4)2via
a carboxyl group, i.e ClO4 , imply that the ions are mobile in the
system The high mobility of ions favors the highest ionic conduc-tivity This predicts that Mg(ClO4)2has the potential to function as the charge carrier in the system The weakly bounded Mg2þion can hop through the coordinating site of the C¼O host polymer and the conduction process takes place [34] These results explain the complex formation of the host polymer with the salt
3.3 Differential scanning calorimetry (DSC) study The thermal analysis using a differential scanning calorimeter (DSC) was executed to observe the change in the glass transition temperature of the biopolymer electrolyte (BPE) system Fig 4
shows the DSC thermograms of the pure CA, 60%CA:40% Mg(ClO4)2, 50%CA:50%Mg(ClO4)2, 40%CA:60%Mg(ClO4)2, and 30% CA:70%Mg(ClO4)2 The Tgvalue of the pure CA is 83.4C A similar Tg
value has been previously reported by Monisha et al The Tgvalue of the CA doped with Mg(ClO4)2at different concentrations is slightly shifted towards lower temperatures The Tg values obtained are 81.7C, 70.40 C, and 64.52 C for the complexes of 60%CA:40% Mg(ClO4)2, 50%CA:50%Mg(ClO4)2, and 40%CA:60%Mg(ClO4)2, respectively The decreasing Tgvalue is pointing out an effect of the Mg(ClO4)2on softening the complex formation due to the plasti-cizing effect of the magnesium salt on the biopolymer structure It
is useful for the magnesium ion to mobilize within the membrane
[35] The glass transition temperatures for the various components
of CA with Mg(ClO4)2are listed inTable 2 The further increase in the salt concentration for the 30% CA:70%Mg(ClO4)2electrolyte causes an increase in the value Tgto 72.35C This may occur due to the presence of the undissoci-ated salt in the polymer matrix[23] Similar results have been reported by Mangalam et al [21] for the composition 50% PVA:50%PVP with 25% Mg(ClO4)2, and Manjuladevi et al.[23]for the composition 92.5PVA:7.5PAN:0.5 mm% MgCl2system 3.4 Impedance analysis
The Cole-Cole plots for the pure CA and for CA: Mg(ClO4)2 polymer electrolytes with different dopant molar ratios at room temperature (303 K) in the equivalent circuit are shown inFig 5 The graph shows the semicircular portion of the high-frequency region It arises from a parallel combination of the bulk resistance
of the cell with a capacitor and shows the linear region with a slight
Fig 2 FTIR spectrum for pure CA, 60%CA:40%Mg(ClO 4 ) 2 , 50%CA:50%Mg(ClO 4 ) 2 , 40%
films.
M Mahalakshmi et al / Journal of Science: Advanced Materials and Devices 4 (2019) 276e284 278
Trang 4curvature that occurs in the low-frequency region due to the effect
of the blocking electrodes[36] A slight depression of the semicircle
is observed in the plot for all the compositions, indicating the
non-Debye nature of the electrolytes and the distribution of the
relax-ation times[37] The bulk resistance (Rb) of the polymer
electro-lytes has been calculated from the Cole-Cole plot using the
Boukamp software[38] The ionic conductivity (s) was calculated
using the equation:
where t and A are thickness and the area of the polymer
electro-lytes, respectively
The value of the ionic conductivity was calculated using Eq.(1)
for all compositions at room temperature and the results are listed
inTable 3 The highest ionic conductivity at room temperature was obtained as 4.05 104S/cm for the biopolymer electrolyte with
40%CA:60%Mg(ClO4)2ratio Generally, ionic conductivity is given by the equation
where‘n’ is the number of charge carriers, ‘e’ is the charge and ‘m’ is the mobility of the charge carriers When the numbers of charge carriers increased, the conductivity increases The ionic conduc-tivity of the pure CA is 3.1 109S/cm The addition of Mg(ClO4)2to
a polymer increases the number of charge carriers in such a way that the salt Mg(ClO4)2dissociates into Mg2þand ClO4ions, thereby producing more charge carriers When 60 wt % of Mg(ClO4)2 is added to the polymer, the maximum number of charge carriers is produced So, the conductivity reaches the maximum value of 4.05 104S cm1 It has been enhanced by an increase of the
Table 1
FTIR assignments of all prepared biopolymer electrolytes.
Wavenumbers (cm1)
Pure CA 60%CA:40%Mg(ClO 4 ) 2 50%CA:50%Mg(ClO 4 ) 2 40%CA:60%Mg(ClO 4 ) 2 30%CA:70%Mg(ClO 4 ) 2 Assignments
1034 1040 1042 1042 1042 CeOeC Stretching of pyrose ring
Fig 3 Possible interaction between CA and Mg(ClO 4 ) 2
Fig 4 (a) DSC thermogram and the glass transition temperature (T g ) for pure CA and 60%CA:40%Mg(ClO 4 ) 2 (b) DSC thermogram and the glass transition temperature (T g ) for 50%
Table 2 Glass transition temperature for various components of CA with Mg(ClO 4 ) 2
Sl No CA:Mg(ClO 4 ) 2 composition (%) Glass transition temperature ( o C)
Trang 5amorphous nature The segmental motion of the biopolymer is
raised by the magnitude of the amorphous phase and it leads to the
higherflexibility of the biopolymer chain
It is observed that the further addition of the Mg(ClO4)2salt over
40%CA:60%Mg(ClO4)2 decreases the conductivity, due to the
for-mation of more ion aggregates in the polymer network[39] From
theFig 5it is inferred that the diameter of the semicircle gradually
decreases with the addition of the dopant The semicircular portion
is a combination of the bulk resistance and the bulk capacitance
The random dipole orientation of the polar side groups present in
the polymer network decreases the diameter of the semicircular
portion at the higher frequency region, which indicates the
non-capacitive nature of the polymer electrolytes
3.5 Frequency-dependent conductivity
The frequency dependence of the conductivity as a function of
frequency for the pure CA and the CA with different composition
of Mg(ClO4)2at room temperature is shown in Fig 6 There is a
low-frequency dispersion region in the plot which is attributed as
due to the electrodeeelectrolyte space charge polarization effects
[40], whereas the frequency independent plateau region
corre-sponds to dc conductivity (sdc) of the composition of the polymer
electrolytes From the ac conductivity spectra, it is observed that
the conductivity increases with the increase in the salt
composi-tion, which is attributed to the increase in the number of charge
carriers The sdc values for all the electrolytes (pure CA, 60%
CA:40%Mg(ClO4)2, 50%CA:50%Mg(ClO4)2, 40%CA:60%Mg(ClO4)2,
and 30%CA:70%Mg(ClO4)2) were calculated by extrapolating the
plateau region to the logsaxis The conductivity values obtained
from the conduction spectra coincide with the bulk conductivity
values received from the Cole-Cole plot
3.6 Dielectric studies The ionic transport phenomenon is characterized by using the dielectric properties of the pure CA, 60%CA:40%Mg(ClO4)2, 50% CA:50%Mg(ClO4)2, 40%CA:60%Mg(ClO4)2, and 30%CA:70% Mg(ClO4)2 polymer electrolytes as the frequency-dependent parameters Fig 7reveals that the dielectric parameters ε0 and
ε00increase at low frequencies due to the formation of the space
charge region at the electrodeeelectrode interface which is known as the un 1 variation or the non-Debye type behavior,
where the space charge regions with respect to frequency are explained in terms of the ion diffusion[41] At low frequencies, the dielectric constant (ε0) and the dielectric loss (ε00) are very
high due to the interfacial polarization and the free charge motion within the material[42] At high frequencies, the mobile ions are not able to orient themselves in thefield direction due
to the rapid periodic reversal of the applied electricfield, which leads to the saturation or to a decrease in the dielectric constant
[43] The values of the dielectric parameter are found to be increased with the Mg(ClO4)2 salt content in the polymer electrolytes
Fig 5 (a) ColeeCole plot for pure CA with the corresponding equivalent circuit (b) ColeeCole plots for 60%CA:40%Mg(ClO 4 ) 2 , 50%CA:50%Mg(ClO 4 ) 2 , 40%CA:60%Mg(ClO 4 ) 2 , and 30% CA:70%Mg(ClO 4 ) 2 with the corresponding equivalent circuit.
Table 3
Ionic conductivity values of CA doped with Mg(ClO 4 ) 2
Sl No CA:Mg(ClO 4 ) 2 composition (%) Ionic conductivity S$cm 1
1 Pure CA 3.1 10 9
2 60:40 4.97 10 6
3 50:50 3.88 10 5
4 40:60 4.05 10 4
5 30:70 2.6 10 4
Fig 6 Frequency dependence conduction spectra for pure CA, 60%CA:40%Mg(ClO 4 ) 2 , 50%CA:50%Mg(ClO 4 ) 2 , 40%CA:60%Mg(ClO 4 ) 2 , and 30%CA:70%Mg(ClO 4 ) 2
M Mahalakshmi et al / Journal of Science: Advanced Materials and Devices 4 (2019) 276e284 280
Trang 63.7 Transport number measurement
3.7.1 Wagner's dc-polarization technique
This technique is one of the fundamental methods to measure
the transference number which is used to identify whether the
conductivity in the biopolymer electrolyte is due to the presence of
ions or electrons The transference number is calculated by the
formula,
where Iiis the initial and Ifthefinal current
In this technique, a dc-potential of 1.5 V was applied across the
cell of the SS/40%CA:60%Mg(ClO4)2/SS configuration for
polari-zation and the polaripolari-zation current was monitored as a function of
time The initial total current decreases with time and reaches a
constant value in the fully depleted situation due to the depletion
of the ionic species in the biopolymer electrolyte[44] The cell is
polarized at a steady state and the currentflows across the
elec-trolyte interface because of the ion migration The total
trans-ference number (tion) for the maximum conductivity biopolymer
40%CA:60%Mg(ClO4)2is calculated to be 0.98 using the Eq.(2), which is close to unity, meaning that only a negligible contribu-tion comes from the electrons Hence, it is evident that the charge transport is mainly due to the ions
3.7.2 Evan's polarization technique The Evan's polarization technique was used to calculate the transport number (tþ) of the Mg2þions in the solid biopolymer The combination of the ac and dc polarization methods was applied on the Mg/40%CA:60%Mg(ClO4)2/Mg cell The cell was polarized by applying a dc-voltage of 1.5 V Then the initial (Io) and thefinal current (Is) values were derived from the currentetime plot as shown inFig 8 The cell resistance was recorded before and after the polarization by using the impedance measurement, and a graph plotted for corresponding values is shown inFig 9
The transport number of Mg2þis calculated using the formula
tþ ¼ IsðDV RoIoÞ = IoðDV RsIsÞ (4)
Fig 7 (a) Plot of loguvs ε ’ for BPEs with different concentrations of Mg(ClO 4 ) 2 (b) Plot of loguvs ε ” for BPEs with different concentrations of Mg(ClO 4 ) 2
Fig 8 D.C polarization curve of SS/40%CA:60%Mg(ClO 4 ) 2 /SS cell and SS/40%CA:60% Fig 9 Cole-Cole plot before and after polarization of a typical symmetric Mg/40%
Trang 7where Ioand Isare the initial and thefinal current,DV is the applied
dc-voltage of 1.5 V, and Roand Rsare the cell resistance before and
after the polarization, respectively The value of the Mg2þ ion
transport number was calculated to be 0.31 for the highest
con-ductingfilm of the 40%CA:60%Mg(ClO4)2electrolyte
Shanmugap-riya et al have reported a value as 0.313 for the transport number of
the Mg2þ ions in their work for the carrageenan with the
0.6g Mg(ClO4)2electrolyte Similar results have been reported by
Mangalam et al for the composition of 50%PVA:50%PVP with 25%
Mg(ClO4)2 Manjuladevi et al have reported for the composition of
the 92.5PVA:7.5PAN:0.5 mm% MgCl2system a value of 0.38, and
Kumar et al have studied the PMMA-based GPE system with the
Mg(CF3SO3)2salt and reported a value of 0.33
3.8 Linear sweep voltammetry (LSV) The electrochemical stability of the highest conductivity polymer electrolyte 40%CA:60%Mg(ClO4)2was studied using the linear sweep voltammetry (LSV) with a two-electrode system The LSV was recorded for SS/40%CA: 60%Mg(ClO4)2/Mg at a scan rate of 5 mVs-1 The currentevoltage response curve is plotted in
Fig [10] The voltage at which the currentflows through the cell was taken as the anodic decomposition limit of the biopolymer electrolyte A sudden rise in the current is observed from the graph This shows the electrochemical stability window of 3.58 V This result reveals that the electrolyte could be used for its application in Mg ion batteries Osman et al have reported the stability window of 3.5 V for the SS/PVDF-HFP:20% Mg(CF3SO3)2/Mg and Manjuladevi et al also reported the sta-bility window of 3.66 V for the 92.5PVA:7.5PAN:0.3 mm% MgCl2
polymer electrolyte
3.9 Construction and performance of the Mg battery cell
A primary magnesium battery has been constructed using the maximum conductivity biopolymer electrolyte (40%CA:60% Mg(ClO4)2) Magnesium metal in pellet form was taken as the anode and MnO2mixed with graphite in form of a pellet acts as the cathode The highest conductivity BPE 40%CA:60%Mg(ClO4)2 has been sandwiched between the anode and the cathode in the bat-tery holder The schematic diagram of the fabricated batbat-tery is shown in Fig 11 a The initial open circuit voltage (OCV) was recorded as 2.12 V and the OCV was monitored with respect to time After 1 day the OCV was reduced slightly to 1.9 V, which remains at the same value for 7 subsequent days As it is shown inFig 11b, a small intermediate drop in battery voltage occurs after fabrication due to the cell formation reactions at the electrodes [45] The chemical reactions taking place in the battery cell are characterized
as the followings:
Fig 10 Linear sweep voltammetry of SS/40%CA:60%Mg(ClO 4 ) 2 /Mg cell recorded at a
scan rate of 5 mVs1at room temperature.
Fig 11 (a) Schematic diagram of battery configuration (b) Open circuit potential as a function of time for 40%CA:60%Mg(ClO 4 ) 2 biopolymer electrolyte (c) Discharge curves of cell using 100 KUfor 40%CA:60%Mg(ClO ) biopolymer electrolyte.
M Mahalakshmi et al / Journal of Science: Advanced Materials and Devices 4 (2019) 276e284 282
Trang 8At the anode
Mg þ 2ðOHÞ / MgðOHÞ2 þ 2e
At the cathode
2MnO2 þ H2O þ 2e / Mn2O3 þ 2OH
Over all reaction
Mg þ 2MnO2 þ H2O/ MgðOHÞ2 þ Mn2O
The Hydroxyl ions present in the Mge MnO2battery may be
generated from the occluded moisture/H2O present in the
biopolymer membrane The occluded water is a type of
non-essential water that is retained due to the physical force in
micro-scopic pores, spaced irregularly throughout the solid biopolymer
CA[26]
An external load of 100 kUwas connected to the circuit for the
measurement of the battery discharge characteristics at room
temperature The discharge behavior of the battery with respect to
time is shown inFig 11c The electrical potential of the battery
decreases initially due to the polarization effect at the
electrolyteeelectrode interface [46] The battery potential
dis-charged at a constant load of 100 kUwas found to remain constant
at 1.68 V, which was observed for 7 days The battery cell
param-eters are listed inTable 4
4 Conclusion
The discovery of a new solid biopolymer electrolyte CA doped
with a various concentrations of Mg(ClO4)2was prepared by the
solution casting technique using DMF as a solvent The XRD
pat-terns reveal that the inclusion of Mg(ClO4)2increases the
amor-phous nature of the biopolymer electrolyte FTIR analysis confirms
the formation of the complex between CA and the magnesium ions
The DSC studies indicate that the glass transition temperature
de-creases with the increase of Mg(ClO4)2 salt concentration Ionic
conductivity of 4.05 104S/cm has been obtained for the 40%
CA:60%Mg(ClO4)2membrane using the ac-impedance analysis at
room temperature The dielectric study predicts the non-Debye
nature of the electrolyte membranes Using the Evans method,
the ionic transference number for Mgþhas been estimated as 0.31
for the 40%CA:60%Mg(ClO4)2electrolyte The electrochemical
sta-bility window has been determined by LSV as 3.58 V which is
sufficient for electrochemical applications Optimized highest ionic
conductivity membrane 40%CA:60%Mg(ClO4)2 was used to
construct a primary magnesium battery, on which the Open Circuit
Voltage (OCV) has been found as 1.9 V
Declaration of interest statement
As corresponding author I S Selvasekarapandian hereby declare
that myself and on behalf of all other authors this manuscript has
not been published in any other journal, and is not being submitted
to any other journal We don't have conflict of interest
References
[1] D.T Hallinan, N.P Balsara, Polymer electrolytes, Annu Rev Mater Res 43 (1) (2013) 503e525
[2] A.L Azlan, M.I.N Isa, Proton conducting biopolymer electrolytes based on tapioca starch-NH 4 NO 3 , Solid State Sci Technol Lett 18 (1 & 2) (2012) 124e129
[3] S Chandra, S.A Hashmi, G Prasad, Studies on ammonium perchlorate doped polyethylene oxide polymer electrolyte, Solid State Ionics 40e41 (1990) 651e654
[4] S Ramesh, Chiam-Wen Liew, A.K Arof, Ion conducting corn starch biopolymer electrolytes doped with ionic liquid 1-butyl-3-methylimidazolium hexa-fluorophosphate, J Non-Cryst Solids 357 (2011) 3654e3660
[5] Florentina Adriana Cziple, J Anlonio, Veliz Marques, Biopolymers versus synthetic polymers, 2008, pp 1453e7397 UEM, ANUL XV NR.1, ISSN [6] A Daniel Cerqueira, J.M Artur Valente, R Guimes Filho, D Hugh Burrows, Synthesis and properties of polyaniline- cellulose acetate blends: the use of sugarcane 22 bagasse waste and the effect of the substitution degree, Car-bohydr Polym 78 (2009) 402e408
[7] W.L Chou, D.G Yu, M.C Yang, C.H Jou, Effect of molecular weight and con-centration of PEG additives on morphology and permeation performance of cellulose acetate hollow fibers, Separ Purif Technol 57 (2007) 209e219 [8] M Rani, S Rudhziah, A Ahmad, N Mohamed, Biopolymer electrolyte based on derivatives of cellulose from Kenaf Bast fiber, Polymers 6 (9) (2014) 2371e2385
[9] S.Z.Z Abidin, A.M.M Ali, O.H Hassan, M.Z.A Yahya, Electrochemical studies on cellulose acetate-LiBOB polymer gel electrolytes, Int J Electrochem Sci 8 (2013) 7320e7326
[10] M.N Chai, M.I.N Isa, Novel proton conducting solid bio-polymer electrolytes based on carboxymethyl cellulose doped with oleic acid and plasticized with glycerol, Sci Rep 6 (1) (2016)
[11] M Selvakumar, D.K Bhat, LiClO 4 doped cellulose acetate as a biodegradable polymer electrolyte for supercapacitors, J Appl Polym Sci 110 (1) (2008) 594e602
[12] S Ramesh, R Shanti, E Morris, Characterization of conducting cellulose ace-tate based polymer electrolytes doped with a “green” ionic mixture, Carbo-hydr Polym 91 (1) (2013) 14e21
[13] M.A Ramlli, M.I.N Isa, Structural and ionic transport properties of protonic conducting solid biopolymer electrolytes based on carboxymethyl cellulose doped with ammonium fluoride, J Phys Chem B 120 (44) (2016) 11567e11573
[14] S Monisha, S Selvasekarapandian, T Mathavan, A Milton Franklin Benial,
S Manoharan, S Karthikeyan, Preparation and characterization of biopolymer electrolyte based on cellulose acetate for potential applications in energy storage devices, J Mater Sci Mater Electron 27 (9) (2016) 9314e9324 [15] S Monisha, T Mathavan, S Selvasekarapandian, A Milton Franklin Benial,
G Aristatil, N Mani, D Vinoth pandi, Investigation of biopolymer electrolyte based on cellulose acetate-ammonium nitrate for potential use in electro-chemical devices, Carbohydr Polym 157 (2017) 38e47
[16] S Monisha, T Mathavan, S Selvasekarapandian, A.M.F Benial, M.P latha, Preparation and characterization of cellulose acetate and lithium nitrate for advanced electrochemical devices, Ionics 23 (10) (2016) 2697e2706 [17] J Song, E Sahadeo, M Noked, S.B Lee, Mapping the challenges of magnesium battery, J Phys Chem Lett 7 (2016) 1736e1749
[18] O Crowther, A.C West, Effect of electrolyte composition on lithium dendrite growth, J Electrochem Soc 155 (2008) A806eA811
[19] M Matsui, Study on electrochemically deposited Mg metal, J Power Sources
196 (2011) 7048e7055 [20] H.S Kim, T.S Arthur, G.D Allred, J Zajicek, J.G Newman, A.E Rodnyansky, A.G Oliver, W.C Boggess, J Muldoon, Structure and compatibility of a mag-nesium electrolyte with a sulphur cathode, Nat Commun 2 (2011) 427 [21] R Mangalam, M Thamilselvan, S Selvasekarapandian, S Jayakumar,
R Manjuladevi, Polyvinyl pyrrolidone/Mg(ClO 4 ) 2 solid polymer electrolyte: structural and electrical studies, Ionics 23 (10) (2016) 2837e2843 [22] Y Kumar, S.A Hashmi, G.P Pandey, Ionic liquid-mediated magnesium ion conduction in poly(ethylene oxide) based polymer electrolyte, Electrochim Acta 56 (11) (2011) 3864e3873
[23] R Manjuladevi, M Thamilselvan, S Selvasekarapandian, P Christopher Selvin,
R Mangalam, S Monisha, Preparation and characterization of blend polymer electrolyte film based on poly(vinyl alcohol)-poly(acrylonitrile)/MgCl 2 for energy storage devices, Ionics 24 (4) (2017) 1083e1095
[24] S Shanmuga Priya, M Karthika, S Selvasekarapandian, R Manjuladevi, Preparation and characterization of polymer electrolyte based on biopolymer I-Carrageenan with magnesium nitrate, Solid State Ionics 327 (2018) 136e149
[25] M.F Shukur, R Ithnin, M.F.Z Kadir, Ionic conductivity and dielectric proper-ties of potato starch-magnesium acetate biopolymer electrolytes: the effect of glycerol and 1-butyl-3-methylimidazolium chloride, Ionics 22 (7) (2016) 1113e1123
[26] D Hambali, N.H Zainol, L Othman, K.B Md Isa, Z Osman, Magnesium ion-conducting gel polymer electrolytes based on poly(vinylidene chloride-co-acrylonitrile) (PVdC-co-AN): a comparative study between magnesium tri-fluoromethane sulfonate (MgTf 2 ) and magnesium bis(tri-fluoromethanesulfonimide) (Mg(TFSI) 2 ), Ionics (2018) 15e18
Table 4
Cell parameters.
Specification of cell parameters Values of cell parameters
Cell area (cm 2 ) 1.13
Cell weight (g) 1.15
Effective cell diameter (cm) 1.2
Cell thickness (cm) 0.248
Open circuit voltage (V) 2.12
Cut off potential (h) 168
Current drawn (mA) 24
Trang 9[27] S Ramesh, R Shanti, E Morris, Plasticizing effect of
1-allyl-3-methylimidazolium chloride in cellulose acetate based polymer electrolytes,
Carbohydr Polym 87 (4) (2012) 2624e2629
[28] R.M Hodge, G.H Edward, G.P Simon, Water absorption and states of water
in semicrystalline poly(vinyl alcohol) films, Polymer 37 (8) (1996)
1371e1376
[29] M Ali, M Zafar, T Jamil, M.T.Z Butt, Influence of glycol additives on the
structure and performance of cellulose acetate/zinc oxide blend membranes,
Desalination 270 (1e3) (2011) 98e104
[30] D.K Pradhan, R.N.P Choundhary, B.K Samantaray, Studies of dielectric
relaxation and AC conductivity behavior of plasticized polymer
nano-composite electrolytes, Int J Electrochem Sci 3 (2008) 597e608
[31] E.M Abdelrazek, I.S Elashmawi, A El-khodary, A Yassin, Structural, optical,
thermal and electrical studies on PVA/PVP blends filled with lithium bromide,
Curr Appl Phys 10 (2) (2010) 607e613
[32] A.M Rocco, R.P Pereira, Solid electrolytes based on poly(ethylene oxide)/
poly(4-vinyl phenol-co-2-hydroxyethyl methacrylate) blends and LiClO 4 ,
Solid State Ionics 279 (2015) 78e89
[33] J.L Koenig, Spectroscopy of Polymers, second ed., Elsevier, Amsterdam, 1999
[34] M.J Reddy, P.P Chu, Ion-pair formation and its effect in PEO: Mg solid
poly-mer electrolyte system, J Power Sources 109 (2002) 340e346
[35] A.R Polu, R Kumar, Preparation and characterization of PVA based solid
polymer electrolytes for electrochemical cell applications, Chin J Polym Sci.
31 (4) (2013) 641e648
[36] G.K Prajapati, P.N Gupta, Comparative study of the electrical and dielectric
properties of PVAePEGeAl 2 O 3 eMI (M¼Na, K, Ag) complex polymer
electro-lytes, Phys B Condens Matter 406 (15e16) (2011)
[37] G.M Wu, S.J Lin, C.C Yang, Preparation and characterization of PVA/PAA mem-branes for solid polymer electrolytes, J Membr Sci 275 (1e2) (2006) 127e133 [38] B.A Boukamp, A nonlinear least squares fit procedure for analysis of immit-tance data of electrochemical systems, Solid State Ionics 20 (1986a) 31e44 [39] C.S Ramya, S Selvasekarapandian, T Savitha, G Hirankumar, R Baskaran, M.S Bhuvaneswari, P.C Angelo, Conductivity and thermal behavior of proton conducting polymer electrolyte based on poly (N-vinyl pyrrolidone), Eur Polym J 42 (10) (2006) 2672e2677
[40] S Ramesh, A Arof, Ionic conductivity studies of plasticized poly(vinyl chlo-ride) polymer electrolytes, Mater Sci Eng B 85 (1) (2001) 11e15 [41] R Baskaran, S Selvasekarapandian, N Kuwata, J Kawamura, T Hattori, Ac impedance, DSC and FT-IR investigations on (x) PVAce(1_x) PVdF blends with LiClO 4 , Mater Chem Phys 98 (2006) 55e61
[42] A Kyritsis, P Pissis, J Grammatikakis, Dielectric relaxation spectroscopy in poly (hydroxyethyl acrylates)/water hydrogels, J Polym Sci B Polym Phy 33 (12) (1995) 1737e1750
[43] K Adachi, O Urakawa, Dielectric study of concentration fluctuations in concentrated polymer solutions, J Non-Cryst Solids 307 (2002) 667e670 [44] S Shanmuga Priya, M Karthika, S Selvasekarapandian, R Manjuladevi,
S Monisha, Study of biopolymer I-carrageenan with magnesium perchlorate, Ionics (2018), https://doi.org/10.1007/s11581-018-2535-1
[45] G.P Pandey, R.C Agrawal, S.A Hashmi, Performance studies on composite gel polymer electrolytes for a rechargeable magnesium battery application,
J Phys Chem Solids 72 (12) (2011) 1408e1413 [46] C.V.S Reddy, A.K Sharma, V.N Rao, Conductivity and discharge characteristics
of polyblend (PVPþ PVAþ KIO 3 ) electrolyte, J Power Sources 114 (2) (2003) 338e345
M Mahalakshmi et al / Journal of Science: Advanced Materials and Devices 4 (2019) 276e284 284