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Energy storage: EDLC & Pseudo –
Capacitors
Doron Aurbach Department of chemistry, Bar Ilan University
Ramat-Gan 52900 Israel Email: [email protected]
Energy is found everywhere
we just need to harvest and store it
We lack good storage technologies
We want to move ASAP to sustainable energy
Supercapacitors can be used for load leveling applications
overview Material design Aqueous SC High voltage SC PsC Summery
Spe
cifi
c Po
wer
(W
kg-1
)
Specific energy (Whkg-1)
Comm. Li-ion 5V. Li-ion
Primary Li
Ni/MH 1h
1 min 1 s
105
104
103
10
102
1 10 10-1 10-2 102 103 1
Ni/Cd
Lead acid
capacitor
Suprecapacitors (EDLC) fill the Energy Vs. Power gap between batteries and capacitors
Batteries are evaluated in terms of energy
and power densities
A typical Ragone plot, of common Faradaic electrochemical energy storage
cells (time constants in red)
Spe
cifi
c Po
wer
(W
kg-1
)
Comm. Li-ion 5V. Li-ion
Primary Li
Ni/MH 1h
1 min 1 s
105
104
103
10
102
1 10 10-1 10-2 102 103 1
Ni/Cd
ECs (2008)
Lead acid
overview Material design Aqueous SC High voltage SC PsC Summery
What is Capacitor?
• A capacitor (originally known as condenser) is a passive two-
terminal electrical component used to store energy in an
electric field.
• When there is a potential difference across the conductors, a
static electric field develops across the dielectric, causing
positive charge to collect on one plate and negative charge to
accumulate on the other plate. Energy is formed in terms of
electrostatic field.
overview Material design Aqueous SC High voltage SC PsC Summery
What is Supercapacitor? Supercapacitor (SC) also known as electric double-layer capacitor (EDLC)
or Ultracapacitor, is electrochemical capacitor. The capacitance value of an
electrochemical capacitor is determined by two storage principles, which both
contribute indivisibly to the total capacitance:
• Double layer capacitor – Electrostatic storage achieved by separation of charge in
a Helmholtz double layer at the interface between the surface of a
conductive electrode and an electrolyte. The separation of charge is of the order of
a few angstrom (0.3–0.8 nm), much smaller than in a conventional capacitor
than in a conventional capacitor.
• Pseudocapacitor - Faradaic electrochemical storage with electron charge
transfer, achieved by redox interaction, intercalation or electrosorption.
overview Material design Aqueous SC High voltage SC PsC Summery
Up to 109 V/m potential fall exist
on charged interfaces Electrical Double Layer (EDL)
+
+
+
-
+
-
-
+
-
OHP
-
-
-
-
-
-
-
-
Counter ion
Co-ions
+
-
Water molecule
+
Outer Helmholtz
plane
overview Material design Aqueous SC High voltage SC PsC Summery
The difference between
More power is required for short time interval in 200m race
Constant but less power required for long time in 20km race
overview Material design Aqueous SC High voltage SC PsC Summery
A = Surface area (very high in Activated
carbon).
d = Dielectric thickness, single solvent
molecule.
εr = limited by the solvent properties.
Possible electrolytes:
1. Aqueous electrolyte, high rates small ions high
ionic conductivity, limited voltage.
2. Organic electrolyte, moderate conductivity and
capacity up to 3V.
3. Ionic liquids- Low conductivity, lower capacity,
high voltage, safe.
dC
rA
0
www.youtube.com/watch?v=FJZKm5khaAA
Charged species can be stored
electrostaticly by the EDL
overview Material design Aqueous SC High voltage SC PsC Summery
M. Biswal, A. Banerjee, M. Deo, S. Ogale, Energy & Environmental Science 2013, 6, 1249-1259.
From dead
leaves till
energy storage
devices
overview Material design Aqueous SC High voltage SC PsC Summery
High capacitance graphene SC
P. A. Basnayaka, M. K. Ram, E. K. Stefanakos, A. Kumar, Electrochimica Acta 2013, 92, 376-382
overview Material design Aqueous SC High voltage SC PsC Summery
Increasing the
electrochemical window using
neutral electrolyte solutions
Q. Gao, L. Demarconnay, E. Raymundo-Pinero, F. Beguin, Energy & Environmental Science 2012, 5, 9611-9617.
overview Material design Aqueous SC High voltage SC PsC Summery
Electrodeposition
of Mn-Mo oxide
film on CNT/ITO
M. Nakayama, K. Okamura, L. Athouël, O. Crosnier, T. Brousse, ECS Transactions 2012, 41, 53-64.
overview Material design Aqueous SC High voltage SC PsC Summery
General features:
• Highly disordered
• Electrically conductive
• High surface area (up
to ~3000m2/g)
Activated carbon (AC)
Activated carbons possess unique
physicochemical properties:
M M M
M M M M
M
M M M
M M M M
M
Carbon
precursor
Carbon
material
Carbonization
under inert
atmosphere
Oxidizing
agent
Activated
carbon Carbon
precursor
Polymerization
overview Material design Aqueous SC High voltage SC PsC Summery
-100
-50
0
50
100
E (volts) vs S.C.E
C (
F/g
r)
0
50
100
150
200
250
300
350
400
0 0.2 0.4 0.6 0.8 1 1.2
Relative pressure (p/p0)
vo
lum
e a
dso
rb
ed
(m
l/g
r)
cc/g
Relative Pressure
0
50
100
150
200
250
300
0 0.2 0.4 0.6 0.8 1 1.2
Relative pressure (p/p0)
vo
lum
e a
dso
rb
ed
(m
l/g
r)
Relative Pressure
cc/g
-200
-150
-100
-50
0
50
100
150
-0.6 -0.4 -0.2 0 0.2 0.4 0.6
E (volts) Vs S.C.E C
(F
/gr)
CO 2+
C C
CO2
O
CO+
C
Activation
M. Noked, E. Avraham, A. Soffer, D. Aurbach, The Journal of Physical Chemistry C 2009, 113, 21319-21327.
overview Material design Aqueous SC High voltage SC PsC Summery
Using CNTs as a conductive additive and as a
reinforcing agent in novel electrodes
Rolling up a graphene sheet to form a tube. Properties: • Very strong and flexible molecular material due to the C-C covalent bonding and seamless hexagonal network architecture. •Thermal conductivity ~ 3000 W/m.K in the axial direction •Electric conductivity six orders of magnitude higher than copper
CNTs grow methods: a) Arc-discharge b) Laser ablation c) Catalytic chemical vapor deposition (CCVD)
b a
overview Material design Aqueous SC High voltage SC PsC Summery