On anisotropic thermoelectric materials figure of merit increase

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On anisotropic thermoelectric materis-x figure of merit Increase

Luk~gen I.Rnotyjchuk and rllg J.

The

thermoelemernts

anisotropy

thormoelements of

based

homogeneous

in

and

haterogeneous

thormoelement

have

The

of

simplest

Lust.

on

media

thermopiles

using

materials

1[1

been this

known Seebeck

Some

patented kind

the

are

Seebeck as

effact

our

as in

classical

the

variants

particularly

thermoelements

coefficlent

well

in

the

called

circuit

of

such

USA

[2,3L

anisotropic

is

represented in figtl. The voltage produced by the thermoelement To+AT

TO a Fig.l.

Anisotropic

thermoelement

The top and bottom *Ldowe o4a. therxmetabttrLzd at dWfferent tempercature., as % reeuLt of anteotroptc thermal e. m.f., the thermoetement procjcea a vottLge between the Left and the right sLte.

is

determined according to the expression A

A

a

T

U2 vhere

a

A

compownmts, height

is A

of

peculiarity

the T is

the is

the

difference

temperature

b

of

thermoelectric

difference,

thermoelement.

The

dependence

of

a

and

power

I

are

anisotropic

the

tensor

length

and

thermoelement

produced

voltage

on

the

dimensions

and

geometrical dimensions ratio a/b. The

essentially

temperature which

are

greater

differences also

patented

are

voltages

at

develops

M31 The

scheme

the by of

some helix

such

thermoelements, thermoelement

Mat. Res. Soc. Symp. Proc. Vol. 234. @1991Materials Research Society

is

80

shown in fig.2- The thermoelement

developed voltage is a-n

AaAT U-

NH 2

b

a

on

It

It -d

Fig.2-

thermoelement

Helix

M IX - heeater;the surfaceby temeaos thermosttLc. The trenrm•oLement current externaa Le conveyed of conta.ctso vhtch

where

N

ate dIsptacod

is

the

on the hettx onds.

of

number

helix

turns.Efficiency

thermoelements at small temperature differences

Carnot efficiency, Tav

this

1

S-? where Tc is

of

is

Za

is

CA a)

Tz "

,

mean working temperature,

2

a

Za x

a

and

electrical The absence

X

attractive of

thermoelement The

are

the

values

effective

of

the

specific

and thermal conductivity. of

such

regulation

are

thermoelements of

voltage

by

evident:

choice

of

geometry and configuration.

main

determination

features

junctions,

of

problem the

of

suitable

anisotropic anisotropic

thermoelement material.

usage

is

Parameters

of

81

the known anisotropic thermoelectric materials are represented

in

the table. Parameters of anisotropic thermoelectric

Table

Temperature.

Material

IT E M F Electrical anisetropy,

conductivity,

materials

Thermal conductivity,

Z a'

K

-1

a 0,08

9,9.10

54

0,9.10 -4

Bi

350

Sb

300

2,6

2,9.10

Cd

300

3,2

1,4.10

Zn

300

1,74

1,8.10

CdSb

400

BiGGSbz

3W50

280 25

CrSi.

800

s0

300

26

4.10

0,11

6,2.10

300

55

490

9,6.10

300

130

4,0

3,8.10 -z 2,9.10

CrSi. MnSi

1

,7

To

4

BizTea

400

40

ZnSb

400

140

400

145

ZnI

5 C0dasSbio

5

-5

O•18

2,7.10

0,92

3,3,8.10

5

4.10 4 15.10

1,13

-7 -7

1,2.10-.e

-s

1,2.10 -a 3,3.1