15
RGO-CoO-Ni(OHh as an electrode material of supercapacitor P.Y. Chan and S.R. Majid* Centre for lonics University of I -lalaya, Department of Physics, Faculty cf Science, University of Malaya, 50603 Kuala Lumpur, Malaysia. Corresponding author": Tel: +60379674146/4238 E-mail address:[email protected] Abstract A composite film containing reduced graphene oxide (RGO), CoO and Ni(OHJ2 has been prepared from CO(N03)2.6H 2 0 and 1 Ji(N03h6H 2 0 with its Co:Ni ratio of2:1 using simple electrodeposition technique. The effect of scan rate on the electrode film is highlighted. Changes in cyclic voltammetry (CV) curves and thus morphologies of the electrode film after CV test are identified. The electrode film exhibits specific capacitance of 558 F g-l at 5 mV s- I in 1M KOH. However, the cycling STabilityof the electrode film over 1000 cycles is low and need to be improved further. The morphology of the electrode film is demonstrated using field emission scanning electron rmcrosope (FESEM). Keywords: reduced graphene oxide, CoO, Ni(OHL cyclic voltarnrnetry 1.0 Introduction Electrochemical capacitor (EC), also called supercapacitor is well known for i.s high power capability and long cycle life as an energy storage device [1]. It can be used complementary with battery to achieve better performance for a device. In general, there are tv '0 basic types of supercapacitor: one is electrochemical double layer capacitor (EDLC) that utilizes the high surface area of carbon materials t) store charge based on electrostatic reaction another one is the pseudocapacitor that relies 01< .he capacitance contributed by the redox reactions offered by the transition metal oxides and conducting polymers. EDLC has low energy density due to the charge storage is actually simply based on adsorption/desorption process. Pseudocapacitor always can achieve higher specific capacitance due to the storage mechanism that is not limited to p. _ sical interactions but determined by the ele-ctron transfer processes occured at interface of electrode/electrolyte. An electrode is where the reactions occurred and used to store charge I: order to produce high performance of supercapacitor, it is very important to synthesize the electrode material with suitable microstruct .re tnat can offer a good pathway for electror .fc... nsfers inside electrode and insertion/deins ertion processes of electrolyte ions on ele trode surface. Transition metal oxides/ ydroxices (e.g. U02, Mn02. CoO, Ni(OHh NiO. Z 0) are studied widely due to their multiple oxida !O" states that offer redox reactions and hig t! eoretical specifi capacitance [2-7]. Ho 'e er. cue to the poor conductivity nature, there is only part of the active materials taking part in tne electron transportations. Many works ha e oeen carried out underway to investigate the p .eparation metho: s in order to enhance the e' -c:rcchemical

RGO-CoO-Ni(OHh as an electrode material of supercapacitoreprints.um.edu.my/13883/1/0001.pdf · RGO-CoO-Ni(OHh as an electrode material ofsupercapacitor P.Y. Chan and S.R. Majid* Centre

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Page 1: RGO-CoO-Ni(OHh as an electrode material of supercapacitoreprints.um.edu.my/13883/1/0001.pdf · RGO-CoO-Ni(OHh as an electrode material ofsupercapacitor P.Y. Chan and S.R. Majid* Centre

RGO-CoO-Ni(OHh as an electrode material of supercapacitor

P.Y. Chan and S.R. Majid*

Centre for lonics University of I-lalaya, Department of Physics, Faculty cf Science,University of Malaya, 50603 Kuala Lumpur, Malaysia.

Corresponding author": Tel: +60379674146/4238E-mail address:[email protected]

Abstract

A composite film containing reduced graphene oxide (RGO), CoO and Ni(OHJ2 has beenprepared from CO(N03)2.6H20 and 1 Ji(N03h6H20 with its Co:Ni ratio of2:1 using simpleelectrodeposition technique. The effect of scan rate on the electrode film is highlighted.Changes in cyclic voltammetry (CV) curves and thus morphologies of the electrode film afterCV test are identified. The electrode film exhibits specific capacitance of 558 F g-l at 5 mV s-I in 1M KOH. However, the cycling STabilityof the electrode film over 1000 cycles is lowand need to be improved further. The morphology of the electrode film is demonstrated usingfield emission scanning electron rmcrosope (FESEM).

Keywords: reduced graphene oxide, CoO, Ni(OHL cyclic voltarnrnetry

1.0 Introduction

Electrochemical capacitor (EC), also called supercapacitor is well known for i.s high powercapability and long cycle life as an energy storage device [1]. It can be used complementarywith battery to achieve better performance for a device. In general, there are tv '0 basic typesof supercapacitor: one is electrochemical double layer capacitor (EDLC) that utilizes the highsurface area of carbon materials t ) store charge based on electrostatic reaction another one isthe pseudocapacitor that relies 01< .he capacitance contributed by the redox reactions offeredby the transition metal oxides and conducting polymers. EDLC has low energy density due tothe charge storage is actually simply based on adsorption/desorption process.Pseudocapacitor always can achieve higher specific capacitance due to the storagemechanism that is not limited to p. _sical interactions but determined by the ele-ctron transferprocesses occured at interface of electrode/electrolyte. An electrode is where the reactionsoccurred and used to store charge I:order to produce high performance of supercapacitor, itis very important to synthesize the electrode material with suitable microstruct .re tnat canoffer a good pathway for electror .fc...nsfers inside electrode and insertion/deins ertionprocesses of electrolyte ions on ele trode surface.

Transition metal oxides/ ydroxices (e.g. U02, Mn02. CoO, Ni(OHh NiO. Z 0) are studiedwidely due to their multiple oxida !O" states that offer redox reactions and hig t! eoreticalspecifi capacitance [2-7]. Ho 'e er. cue to the poor conductivity nature, there is only part ofthe active materials taking part in tne electron transportations. Many works ha e oeen carriedout underway to investigate the p .eparation metho: s in order to enhance the e' -c:rc chemical

Page 2: RGO-CoO-Ni(OHh as an electrode material of supercapacitoreprints.um.edu.my/13883/1/0001.pdf · RGO-CoO-Ni(OHh as an electrode material ofsupercapacitor P.Y. Chan and S.R. Majid* Centre

utilization of transition metal oxide/hydroxide. The combination of two metaloxideslhydroxides or so called b~:-~~rymetal oxides/hydroxides based electrode is believed tobehave better than one metal oxide based electrode. Ni(OH)2 is well known for its lOW costand very flexible in forming desirable morphology based on different preparation methods [8-11]. O~1the other hand, cobalt based oxides such as CoO and C0304 are attractive electrodecandidates due to their high elecL oactivity and good electrochemical performances [12-14].

There are some reports about the electrochemical performances of the Ni(OH): based or Cobased oxides electrodes [8-14]. There are also studies regarding to the combination of thesetwo materials using different preparation methods [15, 16]. Herein, we report 6 simpleelectrodeposition technique to fabricate the composite directly on a stainless steel. It is knownthat the performance of the electrode material strongly depends on the particle properties forexample crystallinity, structure and particle size. All this determines by the syr -::"eticmethodapplied. Electrodeposition technic .ie offers certain advantages for the fabrication of electrodefilm, for example thin film with specific structure and chemical properties can be prepared.The physical properties can be controlled by means of electrodeposition variables such as theelectrolyte composition, electrolyte concentration, applied potential, applied current densityand electrodepositicn duration. Besides. by deposited transition metal oxi .eo:" electronicallyconductive substrate such as stainiess steel allow us to study the fundamental electrochemicalbehaviour of the film formed. In 0:':: work, we applied chronopotentiometry method for theelectrodeposition of the composite \Vi:J:-~reduced graphene oxide. The morphology andelectrochemical performance of .,:_,;;electrode film produced were examined.

2.0 Methodology

2.1.Materials

Sulfuric acid (H2SO,,), phosphoric acid (H3P04), hydrogen peroxide 30% (H202), hydrogenchloride (HCl) (Friendemann Schm.dt). graphite flakes (Nippon Graphite Industries, Ltd),potassium permanganate (KMnO_) (::Jendosen), L-ascorbic acid (UNILAB), nickel (II) nitratehexahydrate (Ni(N03)2.6H20) (Lnilab), cobalt (II) nitrate hexahydrate (COC\i03)2.6H20)(Sigma Aldrich) and sodium acetate ~CH3COONa) (Univar) were used as rcce.ved.

2.2 Preparation and characterizations of RGO-CoO-Ni(OHh based electrode film

Chronopotentiometry deposition technique was applied in this study. The current densityused for deposition was -2mA err -2. RGO was prepared firstly as shown in our previous study[17]. RGO was mixed with 8mmo Co"N03h.6H20, 4mmol Ni(N03h.6H20 and 0 ~MCH3COONa. This solution was sf Tee without heat overnight and being serve (is electrolytefor electrodeposition, Since the )').e_.nal was not fixed in this technique, two-electrodeconfiguration was used at where (iX:::) cm2 s ainless steel and carbon rod acting as workingand counter electrode respectively .fter electrodeposition for 10 minutes, the uc~)ositedstainless steel was rinsed with dis:' .ed water and heated at 100°C for 3 hours. I'ae depositedfilm was [hen ready for character., ~-..2:1S.

Page 3: RGO-CoO-Ni(OHh as an electrode material of supercapacitoreprints.um.edu.my/13883/1/0001.pdf · RGO-CoO-Ni(OHh as an electrode material ofsupercapacitor P.Y. Chan and S.R. Majid* Centre

The weights of bare and deposirec' stainless steel: were measured using a h~gr.)[ec_sionmicrobalance (Mettler Toledo M-:~5~.The weight ofthe composite film was estimated bysuotracting the weight of the bare stainless steel by the weight of the deposited stainicss steel.

All eiectrochemical _neasurements were carried out in a three-electrode setup in IV KOH atroom temperature: deposited stainless steel served as the working electrode. 8. )i<ni'2umelectrode and an Ag/AgCl electrode served as counter and reference electrode respectively.AUT50029 was used to measure the electrochemica.l. performances: cyclic voltammetry (CV),galva:.lostatic charge-discharge (CD) and frequency response analysis (FRA). CV tests wereperformed between -0.2 aad 0.4 V (vs. ,\g/AgCl) a: different scan rates of \:. :0, 15 and 20mV S-l . CD rneas rements were cC!:le in the potentia: range of 0.0 to 0.4 V 90: d:ffe::-~ntcurrentdensities of 1,5, 10, 15 and 20 A g'. FRA was carried out in the frequency range from 100kHz to 0.1 Hz. The specific capac;t::mce can be obtained from CV curve and c. lcu.ated

according to equation below:

Cs. = (II dV) I (v.m.V) ----- (1)

at where I = response current density. v=scan rate, m = weight of the composite film and V =

potential.

The morphology and microstructure of the electrode film were studied using Je 1JSM-7600Ffield emission scanning electron rr icroscopy (FESEMI and Jeol JE~-21 OOFtransmissionelectron microscopy (TEM) respectively. The elements presented in the composite film wereinvestigated using energy-disper:ive X-ray spectroscopy (EDX). The nature of the compositefilm was analyzed using D8-adv2..Ec::Xvray diffrac.ion XRD Bruker AXS with cu;~c!

rr:onochromatized radiation al 40k' and 40mA a: ambient temperature.

3.0 Results and Discussions:

3.1 x- ray diffraction (XRD) and 2nergy-dispers've X-ray spectroscopy (EDX)

(b)(a)

::~::-

45-2fl 0

65 5 15 25 35 45211 v

55 65 75

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(c)

5 15 25 35 45 55 65 75

Figure 1: XRD pattern of (a) as-prepared electrode film (powder), (b) electrode :lLTIS onstainless steel after different scar, rates and (c) bare stainless steel

Fig. 1(a) shows the XRD patterns ofthe as-prepared electrode film scrapping cf frcm thestainless steel. No obvious peaks were found indicating the structure forrnec is' ~":1orphous innature. However, there were structural changes detected after the cyclic voltamrnetry testsimplying that the irreversibity 0:tne electrode films.

Fig. 1(b) displays the XRD patterr s )1' e.ectrode films after experienced different scan rates.As shown, the electrode film ex2-:.:[)~~eClno diffraction peaks at 1 mV sol showinz .vell. ~depositing film on the stainless stFe CL where the diffraction peaks of stainless s1.:;;:;.S were notdetected, Two obvious sharp peaks, :\.\'0 broad humps and one small hump were recognisedfor electrode film experienced 5 n 'V S·l. By comparing to Fig, (c), the sharp pe aks <an beattributed to the stainless steel, \,,:! ..:: is exposed after reactions. The broad :1U lC~S ?t at

-r' 1,)0 d 7"0 b '1-, c.ri" (001) '006) 1 f N'(OH\ -. Q' -~h 11arou~.Q - an ~_) can e attnt -..~ - .0 ana I, panes 0 u- _ 1 /2 "L< ..J. _ e smahump at aro and 740 can be assig ...ed to (31 : ) planes of CoO. In fact, CoO has. c;ffractionpeak located around 44" belonge. to \200) plane (JCPDS 75-0393), However, . may

overlapp d by the intense peak of stainless steel. Tl.e electrode films that underwent higherscan rates (10, 15 and 20.L1V S-l)~~::,oexhibited same peaks and humps with :,'\ r,~~.ntensitycompared to 5 mV s' indicating rv comoositions of electrode films remained .'1--:: ::.ame. Thedifference of intensity of the peak _a r relate 1:0 the amount of electroactive S:t;:;3 .sed duringreactions. At higher scan rate, there .5: less electroactive sited involved in reactions. Theappe: ranee of the diffraction pezxs efte reactions can be caused by the imba ,-r:Oo oetweenoxidaiion/redcction processes d '"', .g reactions that lead to changes in amou,u .~':"'c'"'.oxspecies in elect~ode ~llm.

The composition has ~een verifier1 :'15: 19 e~1ergy dispersive X-ray spectrosco'J_ ,":'!::X) asshown ~r Fig. 2.

Page 5: RGO-CoO-Ni(OHh as an electrode material of supercapacitoreprints.um.edu.my/13883/1/0001.pdf · RGO-CoO-Ni(OHh as an electrode material ofsupercapacitor P.Y. Chan and S.R. Majid* Centre

j 2 .. SN Salle ....14 c:t!l. CUr:sar: 0.000

e 10 12 16IreV

•• tlij'

Fig. 2 cisplays the elements present nside tne electrcoe film after 5 mV S-I. Tl.ere are Co, Ni,C and K which is consistent to the Yz<_Dand TElv, .attice fringes results. The appearance of Kon the electrode film indicates tha: he there is SOJ.le insertions of electrolyte ions curing the

cyclic voltammetry test.

The elecrrochemical performance. c,~'~GO-CoO-, ii(c)H)2 composite electrode :::::1",1 be testedusing cyclic voltammetry (CV), gs.l\ ancstatic charge-discharge (CD) and frequency responseanalysis (F~<\') it: three-electrode cr ..figuration.

Page 6: RGO-CoO-Ni(OHh as an electrode material of supercapacitoreprints.um.edu.my/13883/1/0001.pdf · RGO-CoO-Ni(OHh as an electrode material ofsupercapacitor P.Y. Chan and S.R. Majid* Centre

moo .--- .:a) I-lmV!s (b)~. -SmV!sI

.... -rooo.-v: -lOmV!s~ o:.: "( coco -lSmV!s== ~ -20mV!s~-;

t: ~- - 0G ....'C bJJ~ ~= ,::._000~ .....S(5 -~oooZ

-6000-0.1 ° 0.2 004

Potential applied, Y ,-

600 ( )0.6

• \ /

•500 0.5

....btJ • •r... 400 I 2:°04r.Sv I >-:: t ";:co::..... 300 :;::0.:'-'C I ~co:: I~ -0v 200 A.o.:!vt.='0"Q. 100 0.1ell

0 00 5 10 15 20 0

Scan rate, mV S·l

120

100,QQ"

~er~ 80-,...~(,.I

~ 60:::.,..._0._,... -10~'!:r:.G

10

00 100 ~OO 600 800 1000 1'200

Cycles

(d)

-lA1g

-5A1g

-lOA/g

-15A/g

-20Alg

500 1000Time, t.s

1500 2000

Page 7: RGO-CoO-Ni(OHh as an electrode material of supercapacitoreprints.um.edu.my/13883/1/0001.pdf · RGO-CoO-Ni(OHh as an electrode material ofsupercapacitor P.Y. Chan and S.R. Majid* Centre

-1000 ~i

-lstcycle e' I, ) i 1-1 (f)

3000.t. -1000thcyclezc: 12d.- 2000"e '".... - 10a: ~ ~;... ... 1000 -t

:: b N 8C~- '

,~ et, 0N -< 6- .~.'.': ..... -1000::a -I

2: .zooo ~

-3000-0.2 0 o.~ 0.-1 5 10 15

Cycles 7.'1£1

1.5 (h)

1

q

N •0.5

o 0.5 1 15

7,' .0 enFigure 3: RCNIGmins (a) normalized CV curves with different scan rates, (CJ) scec.ficcapacitance vs scan rate, (c) galvar.cstatic charge-disc1,arge curves at different c::.rrent density,(d) cr.oacitance retention test, (e) CV curves oefore and after 1000 cycles, (i,g) ~.yquist plot

of electrode film before e.ectrochemical test and (1:) equivalent circuit for electroce film.

Cyclic voltammetry (CV) is a versati.e e1eclroanal~'Tical technique used to srucv .hee.ectrcchemical reactions. It can ):; used to deter:-:jr:.e the redox potentials a:1C identify theredox species Fig. 3(a) SFlOWS the : :';:C! of scan rate or. the CV curves of tne electrode filmin l M KOH. The scan rates are 1,.5. ~O,15 and 20 mV S·I. For more clarity, peak currentswc::e normalized wit]; scar rate 2 4 ~ • esented in Pig. 3(a). Generally a pai: o: ) 't;, oefinedredo, peaks can ,..Ie or serx ed in a C 1 :;l...•• es wi.l ~- - .2 V ':00.4 V. The r .become broader with nigl.er scar, lc,t;. Besides, ,he »cidation and red ictioi ~- ~ "'lift ton:.ort poslfve 2nc. E:...::-e :,,'::Jallve .': l;; •. :al fc..,peC! \ e.~ when the scan rate ;D.,..;_.~.~::':::. The1 ' d ., ,.. hCL<;f,g"'S !!e ox poten::a. ana pc:' ..' _ 1T=J. ...ens t •• ::,~.'cate t e reaox pea •. : '. -. scan rated:"~,eI'de-1 2.I1dthe e ....:;t~OE L:!n:: ·~.c::, s.cm ' .E. e. .ctrode rIm mLy ex ~ ~ (_ chemicalc!--.ST'.2e\\lhich is du." t) h_; inser! .. 1 ~ ct oly :0 '_ .nside the f ,r_1. ~ht r ::>gy afterel c ... :"rL ~.L::icalI :!st 1'".8.S b~e~ cal. . '-'_ ut l~ g f1 ......sSlon scan "t'!C ~la.cL.) .:> _ ••••• J.1 - -'0 ~.- •

(F..:= ~ 1). D~.Lf: 1 •-. !:. . the ~.. _:-':- C , ca:r_oc' ~ '?,:{S at s. cmid 0 2V '......)...': nroscope'V ca~ be. ,'. There

Page 8: RGO-CoO-Ni(OHh as an electrode material of supercapacitoreprints.um.edu.my/13883/1/0001.pdf · RGO-CoO-Ni(OHh as an electrode material ofsupercapacitor P.Y. Chan and S.R. Majid* Centre

is cn.y one set of reccx peaks beL1,~ ::.::::ectea. This is CLe to the reason tha. -::f_potentials for both reccx couples . :(~:: JSe to eacr _:)-:uer.

S ( \' -I,can rate. v m i s -)

552-;-74

15'}(i~v

-.-41325

Table 1: Specific capacitances corresponding to different scan rates.

Specific capacitance has been calcu.ated by integrating area under the discharging .urve(Table 1) and the trend is snown ir, Fig. 3[':;), The 0, timum specific capacitance is achieved at5 ~ v sol and it is found to drop g!.'K~.A&li.) with ~-:_igbrscan rate, Since the reaction .sdiffusion controlled, the decreasing Trend of capacitance shows {hat the electrouctive sites ofelectrode film cannot be fully utilisec at higher rr2SS transport rate, The d'.a;_'~-I.' schargebehaviour is measu-ed by chronopo.enticmetry a~ (l;-;--:'-c:~entcurrent densities . ." le.15':lY'f1" ......0 /\ 0-1 and 4"'1""e · ..'esult _'I~ S'}I'\ ' ", ; ... r:-;a ""'(c .....-,...), CD Cllrve~ ro. eal the ,..,.~ " r· pacitivec.u_~.f__ _n_ '=' CJ_ ~ ~~1 _cS ,_, _S l'~ ,',c~ ~_~ "ty _J J" .___ .::, '- 1 -" :-':,_~ -~-" -,. 1 -

behaviour of the electrode film,

The cvcle stabilitv l'~ 9r--O--'''c~~-j'm"" -t"-, t P"l'?' ~1"'+"'" ---. ~+l"rml'nA thl f> D"u';Ctl'co'j q~JI --"-ll'O-rl of an.l..l..~'-'~, _'-'-' J. 1. __ '" ..... _. __ L_-"'.J... _.1t._,,-' .(..;..1. u ......_......"'..\.,... ~ ,~.....Io".-_ ......... , ... _._- _t --_ .-':1. --

e:ec~;c_)(ie fu"ld demols-~;:-atc-:dby::::: c,:c v;:;ltarrJne:c C\7) over 1000 cycles_ C ..' i_'_e""_od isused to per:orm cyc_e smbility test :'n ,his s-:udy be::::<".Lsewe are interesled Q!,. ~ '::: _::t'.2.ngesinrea~tions of the electrode Slm af,e, :;x_perienceci lO:clg cycling, The capacita~-:__~::s&~~:::revery 25cy::::le~a:-ecC'Jculated ane: t:1e rete:Ll,))} )erce:1tag-t , I -::;,_pacitancecomparee:_ _~.:;'.'-:!ialc."·......r ...·t~I·C ;n e~-l'm"""""';,:,u~'-"'"'no ""a1-'t:'+ \"'-'''-C"",, "'_"~-~r+~ -''" +G,-, 'esu't l'SS~O"'~ l'r TC'1"~~ ! r /\. ~ sl..own::!_:c.l,;._.:l ~ > 1::> ::'l C_._ ,1" '" r" ~_,Cl _ r.:; .t:.~ _v., l._d. __ 1 U V'/.l.-,- -'-11"_1:). __ '/ r~:::; ~l ,

t11r r'- -a~(o~ per~c.,., .' 0-" ~. -r ",p"rl " ~"'11~ 1h; ,;th' "'" ,';ng cycle n"n'b'~r' T': ," (' ..t.. r>v~leLC. ~ .... Llo..,..ltwi 1_ Lv.l.! ...a:;:>",", ~ U:::, Lt.:. ::,.!.("' ..... ~.J<J " ...... 1..&. '-" ,_. .... ..;IJ._ l..1;. .;._ '-'_ {~ ... : ... -'",.',-' ':1 vJ """

a~1G~ creaseG r&pidly after that. ~-_~.~~suggesTs thc.~' ,e ,;yding stability of.::; ::-.eG_::-odefilmis low, The CV curves Jc~o:'ea!1c. ftel:he tests ?r::- d~splayed in Fig, 3(e), r[ "l~ ::\n"-?ction ofthe curve from the ir:itie.l CV cmy:; s:-'ter : 000 CYC.eS :.::obviou~, 'Ite redQ). _';X::_JS ve~ed~sappea::-ed indicating the degraa-"..ior. of the e:e ~l '12 j,;:: ::lm. The degracah)' ~~-r '~c2_usedby Ca) th~ change :n ac!iv ~lasse5 Ln:rr,t indt:ceu :;) -::ledif feLce ~n vo L!:1-,. ~-_e~lS~!ybe~\'eer~ oxid:zed a::d red !.l.cedrcJc.' spec:cs whic::'_82.s to the poor elect:-o _ :-a::_51:onation,a:-c._ Cb partial i~so utwn ofe-,-ect'old:~ f~L after 1,)Lg. ycling [20J. "e;sicies. ':-:;ersiblech:;;mically change of eleclrode £i _ ,~ durLg cycliiJ.~ ,:':' cess rna) a so caus,~ ,"'-';;:;'<"adationof

T:_ \.n(lru:{}et1ta~be __a\.0Jr oftD" ,-','0> '''"rod.; .11m n;;i~ ;::-enexamined using":: ! ;r1.':;y

Rtsp ,~se l\nalysis (FH.A~ Fig. ~ ~'- ',_d(g e.' ;;b;~s .le ~vquist plm o~ th -._'),;e filrr.p-=rto:met at the freqt,enc:v range 8-'C.1 _2 to 0.1.\ _ z' _ 1M KOE and the ec. .!v:..:eilt circuitused 0 [;t t e data ~ssho' :1 in Fig, ~ 1'" ·~he. ') '::,',:pot consists of a hih-.'- . "e.--:~;:;yin! r \' frequ~:1C_

Page 9: RGO-CoO-Ni(OHh as an electrode material of supercapacitoreprints.um.edu.my/13883/1/0001.pdf · RGO-CoO-Ni(OHh as an electrode material ofsupercapacitor P.Y. Chan and S.R. Majid* Centre

\ .. .:::nt series

res.s.a lee. which is tne combina, cr f e.ectrolyte resistance, resistance 0:;".::.. .: r:~.t 'ode film, ." ~'l p' ~ana tr,e contact resistance ot inter :,',;' at eiecrrooe __..n/sram.ess steer. Ig.:' ',,_ 1' . .)\\/S us to

ha Ie L de.aii .ook on tne depress';" se.nic.rcle. By evaluating the diameter 0_' ._',,: :;;;'~·:[].icircle,(he cr.arze transfe ....resistance car <,.~. "c),l-cl (~68ml_'~ T"'"'e visual observaricr ro," _, .hat tne_. '_''::;~' c... c_ ,'-' .. ! .a __ ~ .~!.' . _' \.J • ! -/ - ," . a. "i .-'~ .j , - .-.~ ."

e teet c ce film has 9. small charge' :' •. ,_t~resistance. r:~1is is co.zributed by '.-: :.:: =~JLO:Ogy

0:' elec trode EL-r:.formed that allcv s .:e ease penet:zr:o_: of electrolyte ions 8':~,~.;".ectrontransportation. Lower free. uency ::: '::;"~),'" basically !e~e!':--ed1:0 the- ste.ight line .- ':; ..1::

deptes::;ed semici::-cie, in:ii2a'leS t1:.t: ....i:',:usior. eOEn: io~ 0fthe charges.

The be:'avi:::;ur 0: the elecT:-ode fil,~'L::"'.~he electrcl 'te 'v\ (is si!!1plifieci and ex'")L ::If''C. usingR2:1C..CS circuit, Fig. 3~h), Highe" r'-;Gle:1cy ~egl0r. :2.l"...show us the equivaler' sc"<':'s

re~l' ~+l>Y' ca. l'nd'I'c~Yed as n J'n +he r'): .,._ "cs;a'es t'no.v",";s a const~nt Dhase el"-Y"=,'(" (""DE 1'):, S. __ l v a.l -,,-, l ~l:=,,_'-- . .o,-, _ ,. ~~'-' • C!.. ~C",' .• l ,~, ,

used :0 repiace tr.o.e capacidve eie:,' ...cr:..s Que to the .1oll-Ideal behaviou:-s of ~2'P:~i'Lor duri:lgrrpac:~r_'o-n"pnt re....:·e~~r~l'S ~l-.edo" b":... I-V:=;'V' £8rIT!eri ---. t ,0. a'le~trode +]l~-n ....u '"'.-r.'-_ ~ -l'e c)"her"" _" •• ~ .• ~ " .J_ ",¥_ ... .o. U J. -J _. • ~ V.L _ .... '-. '-' •• --:, .. ,(l,.~ '- - -, --

l""\r''''~ +).-,-, ....=-1·8 anJ...._1,.,~-~""'-"Sl'~rl'vee)--'!'"'l-" i'~1naV"r-''''le \1. "+', r-u1=' 1 ''IT;l·r •....., l'~ t'nc:.. ··C:.~l· -" -"<.:1•• " ••~ l._C_~ ".~l"' •• C:S. -Jed ':;_. _,_l:" l.a.1 1 ,'_,. '---'_~ v,'.o. ,'-".0. :, ,'. ,,', _.: ... "-

encm.:~lte_..edduri:r:g (,large trans!",:' 'Jl'.J2eSSeS (Rp/. '~PE2 is used te descr~ _'C ,;' -::ffusionp:-oc:es::; aLlce c212:-ges, !n ,senera., ::-~£ eaL be ~Ldur:eQ by diffusiof\-liP-lite:-- ~-' ..:'l' 'e>n,gec.;(2,,;~i2;factoro::, C::) scaEograp:-· > ~".Y':;~og~llei:.~':.~...d :>.uggish ::roc~sses £C. e ,~""':') e

Fun":e"-!Ilore, we l-:.Z.Ve carr;ed au: (; ''::..C voltamm~:r) +ests for RGO-CoO a:1C r )-Ni(OH)2b'y c,pp yi::lg t:-le S31Y!~ eke rodep,~ ~ijc~'! [.no mea~lre;:-~:e!lt conditions, The C .J ~~~,: "'S obtained

are shown in Fig, 4.

5000

.;, 3000:'"i:.~.:--;: ~ 1000~-I

:: 5c ...._ I:>t!

~ ~ -1000._~~§.z. -3000 -RGO-Ni(OH)2

- RGO-CoO-Ni(OH)2

-5000-0.2 o U,2 004

Pot('ntial applied. Y Y

F' .- cl' t (C - R{~' '0 ROO '(0' U' 'r. C ......19u:-e;.: L lC' 01.<..E.lc ry ." .:ves .to: '-' - .....0, -'. DJ2 ~ l "- c,- 0,--'-

1'\'(0 ')2 at : v,' S' • j r(Or~

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0. <ssigned to_ ::;.;;)ec::vely.

CoO -- O:-f ~ CoOOE 7 e'

As seer." the conversion afNi(II) ".J ~v(~E) occurs -ign: before oxygen evo ..·]~:,::,.-:. _:.ereduction peak o:':'Ni(IlI) to ~i(II; .s sman compared '~Joxidation peaks of vi ..'::_-:'~Ti(III).This S:-:O'HS the irreversibility of ~',\ i.,) anc carr causes .ne degradation of e :;:_.~:::::,_:~filmduring iong cycling, The CV curve .J '~~C0-CoO- -i:OH)2 presents the recoxnc ,e atials inberween tnt two potentials of CO··"l. <: redox species The current density ~<.- eas :~ afterthese '~1"('" recox (.''''e·......ies mixed -r" '!:~ ~ ':".,... J\." Q"'Y' C.C+,~F t"'" specific .apacitar '.C{;: ... "" individual_H..:S'" vvvo 1.1. ... "-"'i-' vL'.__ 1-1 C 'u6 .... --v •• r'l.:S ".\._.J" .v_..• 0,-"' 1"'-' .v ....c; "~L •• _ v L.u "'"

RGO-CoO and RGO-Ni(OH)2 a:_': :-:, ';:;::comparee tc ~~GO-(Ni-Co)OH, wh. c, ~~~' ..97 F g']

32 FESEM study

The I0:TI2.l:lOn C)1' RGO-CoO-N:( ,-,r- ;: composite ~1~T<IS exp.ained as follow c '.:':. .ry, theelectro reductior of nitrate ion ~- 'C 'C''''- ·I-._Tr, _ 'V-I~;C'" -, ..ther reo' ""f' to "-T? r '" " ,,- 0p-10H'~'_v-:" '- I,_, 1 J ':J__,.t_c:~· ....._~~' L_ ,,-.~....~ ~'\"'__'2 'I _..._!.__ ..._l! .... "'ll ~ ~L-»..v·_ .J._"_ Ct.... _ ...... j~ .....1_ ... _"",,,,""'\..:' •

Treese !i.ydroxide ions attract Ni a:-,i "..:. ::;,,::i}.1S 21:.'i ~c.T~:~iCOH)2 2.nd COt,O,t-.J·;22c8crdingly.Th::: e: ectrochemi ca_ reac:ions Ca., :::e :.c0se~lted 2.: _c _!OWiLg [23 ~:

Cc~---20H'-J>. Co(OE):

Lie CJ~:nposite ti~m fo:'m.ed is an.:,,;.;,:ed at }ODoC .'0:- 3 ~ours which ::::onver;:<:·~.:(:.._\)(OH)2 toCeO tUi retain the }..~(,.::::::-:'2. ~n 0:':,:£ 10 ~xamine :h~ rr~orphology formed. 5-: .. ~r.:.:ssiorrsca:-h--:~ngelectro£. m' cr scopy (FS S_~:--/.i)hES beer :L-ried out and the imagc:~: ': ..':i.'~~_edarcS._C';,1: in following.

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Figure S, (a, b) 'Y::::.:L: (\, e;:,t ! •

v. : 20 ::1I I c..

F:g.5(~..-o;: ~\I~ L

t .~~~~. he electrode _n : the s I...__-

, ., ._L ~ _ .......... ~

en . any·c

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f:1V s r : Tr,e particies are bidderd~~~'l~.,:;deeper in:o th,·,:\e-::t-1L:.c

reaclS'~C"1; J '~l' g - I r, -I -,--f.- c' r" . ~;'C1,·-f~'-H __ _ _ J ,:::;. • "_~ • ~'-' ,-1- -,_

cor.r.ection s. d relanor. betweer,

~:':_g.)~& 'I, the c....trl).,_.,e:..:ze cf 1 '~:-:25 _~_g. The

': ~S.:-.rate (1

:e pc.. ceres can be ~"YI_ /_~

L . -:-_J ••1 T s- ),::1":;(:;,([0., .:-

_1) seen at

__" Le :19,-"~ -~< • ..:- es <t.:: bi.._:'::>l OUT 0:

.g.ie. ~TG.g_:_ :-~: ~ "::-1 (x..OC.:C) (Fig. :r ~~_( 0~r:~"':1~ " )": e l:arr- cles \vere fc

~ " T i~ incicates th?-,(Fi ....( ,'~lO- ) + ,.-.0' .....-

t:

rr.icrcscopy (':EM) has beer; carrinEg . .;;

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Figure 6: TENl ~:d~<:,~,;o: a~ _s-'=. -, 'l, __J Id <10 r~ \ - . j . \ 1" r-_.. ....~ y -' ~ () ......_ ~. ~C j -' __

~v ..::nagc ., 'cparESE,

./.....'-~.. 0 ~,:; ..1.. ... "_1 . is cle.~. .TO;,- .!:. croS::'UCI~~\',,', consiste;» 'C\:',.: Fig. 6 a.o). From

, .OLS aner Cy c .. c 'ottamme:is J:

''';:,. =- ron F~gC '7 _/ r we:'" 'ou d a C c ,.:1 be

l' _c .•."':-·1, -::In

tr.e _~ er hand, n 2'-'1. - a.tice S.t

Besi ',:s, the presence .~ ,-_ i(OC "rr_:1 \,\-:1:C: S

,,J

C , Si ) 1

11\

ue. TCDO-~ OSlLe

1 oroho 02. C:_ ,_,.I .,~heT. calJ 5 - ~- ofue t

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Q_lC to tIle chemical; ::.•8. 'ge C';'

hCO' -', I·-~:--, '-.' ectrolvte ;r ~, c'· ·,.n t~,Co...... -_ '" ,..,.... ' __ \, _ iI., .. .o._ ..... v ....~ ..._...., \_;

., co .r

<>,_ .U-_' __ :,1

Co _"~"1L.__

~',~~ . ~ !_~:; :~0~~-

, • r ~::. sfer:.t - ~ '_e :'2 "'I~ .t .::

1.

2.hP~. ·C:t"C(iS. 1999: S;J:;(tg::Sc',zz' Jli, J., -, T:c.~-::a(0iO';)::l1cH.d:;~r n 0C.C S[ utic J~

3.4,_1: o. 57··6-t<' o. S.-~.2 c!~"'/20

- :V

v ....,. \

4,

E

de rieniots c, ~

,I r-a cf A':J ,':~ E ecrrc.c.

.I~I .. ~,e;: "'c, ;:)cne

;_o "-'11 I':Vt:"tL"

.' (Jf: el.. ,0'::

. ) ..le.,J ....

-::_·tio!-(_oJ, Ni. 0)-enrxanhe' .rnesed some~ ,e.ully- a-Io

'11rr l.as'J:

<ted :::f-lerr; entsurs of theactions

"0Cce films

late

.. __lTO ~g.fl

, /)/09; -:::11

.ertc .. t..' t, 1S74.

;- of f/n02·tY,2006 .

, -n

'lOr .

one I res