Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

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1 Effects of Discharge Rates on the Capacity Fade of Li-ion Cells Department of Chemical Engineering University of South Carolina Effects of Discharge Rates on the Capacity Fade of Li-ion Cells Gang Ning, Bala S. Haran, B. N. Popov

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells. Gang Ning, Bala S. Haran, B. N. Popov. Objectives. To determine the capacity fade of Li-ion cells cycled under different discharge rates To break down total capacity fade of Li-ion cells into separate parts - PowerPoint PPT Presentation

Transcript of Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Page 1: Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

Effects of Discharge Rates on the

Capacity Fade of Li-ion Cells

Gang Ning, Bala S. Haran, B. N. Popov

Page 2: Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

Objectives

To determine the capacity fade of Li-ion cells cycled under

different discharge rates

To break down total capacity fade of Li-ion cells into

separate parts

To analyze the mechanism of the capacity fade

To provide experimental data for the capacity fade model

under high discharge rate

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

Background

Capacity fade is a key factor in determining the life of the battery in a

specific application.

Generally there are two ways to analyze this phenomenon:

calendar/shelf life study ( under no applied current)

cycling study (under a specific charge&discharge protocol)

Many papers regarding charge protocols and the capacity fade can be

found in current literature. Performance of Li-ion cells cycled at higher

discharge rate is scarcely reported.

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

Capacity fade as a function of cycle No.

0 30 60 90 120 150 180 210 240 270 300

Cycle No.

0.00

0.02

0.04

0.06

0.08

0.10

0.12

0.14

0.16

0.18

Cap

acit

y Fa

de P

erce

ntag

e

1C Discharge Rate

2C Discharge Rate

3C Discharge Rate

16.9%

13.2%

9.5%

CC+CV charge: (1.0A+4.2

V+50 mV)

Discharge Rates: 1C, 2C,

3C

Frequency: once/50 cycles

Capacity Measurement

Rate: 0.7 A

Temperature: 25 0C

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

Discharge Profile of fresh Li-ion cell and cells cycled after 300 times

0.1 0.3 0.5 0.7 0.9 1.1 1.3

Discharge Capacity (Ah)

2.5

2.7

2.9

3.1

3.3

3.5

3.7

3.9

4.1Vo

ltage

(V)

Initial Discharge

3C Discharge

2C Discharge

1C Discharge

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

Rate capability study

0.00 0.42 0.84 1.26 1.68 2.10 2.52 2.94 3.36 3.78 4.20

Discharge Current (A)

0.5

0.6

0.7

0.8

0.9

1.0

1.1

1.2

1.3

1.4

Dis

char

ge C

apac

ity (A

h)

Battery_Fresh

Battery_1C

Battery_2C

Battery_3C

Cells were fully charged with

CC-CV protocol and

discharged subsequently

with C/10, C/4, C/2, 1C, 2C

and 3C rates

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

DC resistance Rdc as a function of depth of discharge (DOD)

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0

Depth of Discharge (DOD)

240

250

260

270

280

290

300

310

320

330

DC re

sist

ance

(m

)

3C 300 Cycles

1C 300 Cycles

2C 30 Cycles

Initially

Internal DC resistance of

the whole-cell was

determined by

intermittently interrupting

the discharge current in the

process of discharge

Rdc = (Discharge Voltage –

Open Circuit Voltage (0.1

second after the pulse rest))/

Discharge Current (1A)

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

Impedance Spectra of fresh cell and cells cycled up to 300 cycles

0.24 0.26 0.28 0.30 0.32 0.34 0.36 0.38

Z Re ( )

0.00

0.01

0.02

0.03

0.04

0.05

0.06

0.07

0.08

Z Im

(

)

Fresh

1C Discharge

2C Discharge

3C Discharge

SOC: 0%

(a)

0.25 0.26 0.27 0.28 0.29 0.30 0.31

Z Re (

0.000

0.005

0.010

0.015

0.020

0.025

0.030

Z Im

(

SOC: 100%Fresh

1C Discharge

2C Discharge

3C Discharge

(b)

(a) 0% SOC (b) 100% SOC

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

Half Cell Study (T-cells)

Carbon Half-cell LiCoO2 Half-cell

0 20000 40000 60000 80000 100000 120000 140000

Time (s)

1.0

1.7

2.3

3.0

3.7

4.3

5.0

Vol

tage

(V

)-2.0E-004

-1.0E-004

0.0E+000

1.0E-004

2.0E-004

Cur

rent

(A

)

Current

Voltage

Delithiation

Lithiation

0 20000 40000 60000 80000 100000 120000 140000

Time (s)

0.0

0.2

0.4

0.6

0.8

1.0

1.2

1.4

1.6

1.8

2.0

2.2

Vol

tage

(V)

-2.0E-004

-1.0E-004

0.0E+000

1.0E-004

2.0E-004

Cur

rent

(A)

Current

Voltage

Lithiation Delithiation

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

Half-cell analysis of capacity fade (in percentage) of negative Carbon electrode and positive LiCoO2 electrode

Capacity Fade (in

percentage)Fresh

1C 300 Cycles

2C 300 Cycles

3C 300 Cycles

Carbon 0.00% 2.77% 8.30% 10.59%

LiCoO2 0.00% 3.98% 4.38% 5.18%

The percentage

loss of capacity

is calculated

based on the

capacity of

fresh electrode

material.

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

Breakdown of the total capacity fade of the whole lithium-ion battery

Q: total capacity loss of

the whole lithium-ion

cell

Q1: capacity correction

due to rate capability

Q2: capacity fade due to

the loss of secondary

material (Carbon or

LiCoO2)

Q3:capacity fade due to

the loss of primary

material (Li+)

Cell cycled at 1C rate

Cell cycled at 2C rate

Cell cycled at 3C rate

Total capacity fade of Li-ion

Battery9.5% 13.2% 16.9%

Q1 3.5% 2.9% 2.8%

Q2 (Carbon)NA 8.4% 10.6%

Q2 (LiCoO2) 3.8% NA NA

Q3 2.3% 2.0% 3.4%

Q:=Q1 + Q2 +Q3

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

0 2000 4000 6000 8000 10000 12000 14000 16000

Z Re (

0

1000

2000

3000

4000

5000

6000

7000

8000

9000

10000

11000

Z Im

(

)

1.154 V

1.730 V

0.992 V

0.913 V

1 mHz

(a)

0 125 250 375 500 625 750 875 1000

Z Re (

0

100

200

300

400

500

600

700

800

900

1000

Z Im

(

)

1.154 V

1.730 V

0.992 V

0.913 V(b)

Typical Nyquist plots of Carbon half-cell obtained at 25 0C (a)

potential ranging from 0.913 to 1.730 V vs. Li+/Li

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

Typical Nyquist plots of Carbon half-cell obtained at 25 0C (b)

potential ranging from 0.126 to 0.773 V vs. Li+/Li

0 100 200 300 400 500 600 700

Z Re ( )

0

50

100

150

200

250

Z Im

(

)

0.126 V

0.406 V

0.258 V0.587 V

0.773 V 1 mHz

(c)

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

Equivalent circuit of the EIS spectra

Relect Rf Rct Re Zw Cint

Qf Qct Qe

Re: resistance of bulk material

Zw: Resistance of Warburg

Diffusion

Cint:intercalation capacitance

Q: constant phase elements

Relect: resistance of electrolyte

Rf: resistance of surface film

Rct: resistance of charge transfer

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

Data Fitting

0.0 187.5 375.0 562.5 750.0 937.5 1125.0 1312.5 1500.0

Z Re ()

0.0

187.5

375.0

562.5

750.0

937.5

1125.0

1312.5

1500.0

Z im

(

)

plot by fitting

plot by experiment

0.001 Hz

0.0001 Hz

Rf : 6.87

Re : 110

Rct :=40.37

Cint := 1.5 F

Log(D) := -9.7

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

10% SOC 20% SOC

State of Charge

0.0

1.0

2.0

3.0

4.0

5.0

6.0

7.0

Rf

()

2C

1C

3C

1C

2C

3C

10% SOC 20% SOC

State of Charge

0

20

40

60

80

100

120

140

R e

(

)

1C

2C

3C

1C

2C

3C

10% SOC 20% SOC

State of Charge

0

10

20

30

40

50

60

70

80

90

R c

t (

)

3C

2C

1C 1C

2C

3C

Parameter comparisons

Rf Re

Rct

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

SEM images of the electrode surface

• SEM (X1000/30 m)

of Carbon materials

cycled at different

discharge rates.

• (A) : Carbon cycled

at 1C

• (B) : Carbon cycled at

2C discharge rate

• (C)+(D) : Carbon

cycled at 3C

discharge rate

A B

DC

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

Mechanism of Property Changes

Carbon Particles

Initial SEI film

Binder particles

Current collector

2Li+ + 2e- + 2(CH2O) CO (EC) → CH2 (OCO2Li) CH2OCO2Li ↓+ CH2CH2 ↑

2Li+ + 2e- + (CH2O) CO (EC) → Li2CO3 ↓ + C2H4 ↑

Li+ + e- + CH3OCH2CH3 (DMC) → CH3 OCO2Li ↓ + CH3•

Thicker SEI film

Page 19: Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

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Effects of Discharge Rates on the Capacity Fade of Li-ion Cells

Department of Chemical Engineering

University of South Carolina

ConclusionThe negative Carbon electrode deteriorates much faster than the positive

LiCoO2 electrode when the Li-ion cell was cycled under higher CC

discharge rate.

Increase of the internal impedance, (predominantly resulting from the

thicker SEI film of carbon) is the primary cause of the capacity fade of

the whole Li-ion battery.

High internal temperature due to high discharge rates probably leads to

the cracks of initial SEI film and more electrolyte will take part in the side

reactions. As a consequence, the products of those side reactions will

make the SEI film become thicker and thicker.