Table 1 Selected electrocaloric effects at phase transitions near and away from room temperature.

From: Giant room temperature electrocaloric effect in a layered hybrid perovskite ferroelectric: [(CH3)2CHCH2NH3]2PbCl4

EC material

TC (K)

ΔS (J/kg/K)

Q (kJ/kg)

ΔT (K)

ΔE (kV/cm)

ΔSE (J cm/kg/K/kV)

ΔTE (mK cm/kV)

Ref.

KH2PO4

123

3.5

0.4

1.0

10

0.35

100

14

BaTiO3

397

2.1

0.8

0.87

4

0.525

220

15

PbZr0.95Ti0.05O3

499

8.0

4

12

480

0.017

25

9

Pb0.8Ba0.2ZrO3

290

46.9

14

45.3

598

0.0782

76

36

Hf0.5Zr0.5O2

448

10.9

4.9

10.8

3260

0.003

3

47

SrBi2Ta2O9

565

2.4

1.4

4.9

600

0.004

8

35

CuInP2S6

315

5.8

1.8

3.3

142

0.041

23

37

0.87PMN-0.13PT

343

0.6

0.2

0.6

24

0.025

25

48

BNBT/BCZT bilayer

370

26.1

0.6

23

620

0.042

37

49

P(VDF-TrFE)

353

60

21

12.5

2090

0.0287

6

10

NaKC4H4O6·4H2O

265–298

0.003

1.2

25

50

TGS

323

0.11

1.6

68

16

NH4HSO4

271

0.1

0.03

0.025

1.5

0.067

17

51

(iBA)2PbCl4

302

25.64

7.7

11.06

29.7

0.86

370

Herein

  1. Isothermal entropy change |ΔS|, adiabatic temperature change |ΔT|, and isothermal heat |Q|, at starting temperature T, due to changes of electric field |ΔE|. For all entries, Q = TΔS.
  2. PMN PbMg1/3Nb2/3O3, PT PbTiO3, P(VDF–TrFE) poly(vinylidene fluoride-trifluoroethylene) 55/45 mol%, TGS (NH2CH2COOH)3H2SO4, BNBT (Bi0.5Na0.5)TiO3–BaTiO3, BCZT Ba(Zr0.2Ti0.8)O3–(Ba0.7Ca0.3)TiO3.