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§4. A Proposal for Prevention of Current Imbalance by Peltier Current Lead

Yamaguchi, S., Shimada, R. (Tokyo Institute of Tech- nology)

In order to reduce heat flux to low temperature magnet system, Peltier current lead

(PCL)

was proposed by S.

Yamaguchi et al and the experiment had been performed

[1].

The experimental result proves the principle and saves the consumption of the electric energy. PCL is composed of the pair of p-type and n-type thermoelectric semiconductors, which work as a heat pump. Current imbalance is one of the serious problems in large-scale magnets, and the current- lead-resistance method was proposed by S . Yamaguchi et al [2] and the experiment had been done and proven its principle [3]. This method uses the resistance of the current lead strand to improve the current imbalance, and it is quite effective even in large magnets. In this report, we propose the combination of both two ideas. The schematic structure is shown in Fig. 1.

Semi- conductors

IITS

---.+

Normal conductors for cnrrent lead

Semi- conductors

superc:oingdu~c~U~'1:1g~~~~~-':s~u~p;er~c~0~n~dUCting

stralld'~ble strand cable

Superconducting Magnet

Fig. 1. Schematic structure of the proposed Peltier current lead to improve current imbalance.

Each strand of the magnet and current lead are connected to the semiconductor individually. The resistance of semiconductors is high as compared with the metals, therefore, the current imbalance is improved and the semiconductor works as a PCL to reduce the heat flux to the low temperature system [4]. The generalized Ohm's law is given by

E=l1J +agnrlT (1)

where E is electric field, J is current density, 11 is resistivity, a is thermopower and

T

is temperature.

Therefore, we should consider the thermoelectric effect, and the circuit equation of the two wire model magnet is given by

(2)

(3)

where 11 and 12 are the currents in the two wires (strands), L 1 and L2 are the self-inductance of the two wires, M is the mutual inductance, Rl and R2 are the resistance of the two semiconductors, a 1 and a2 are the thermoelectric power of two semiconductors,

~Tl

and

~T2

are the temperature differences of two semiconductors ends and Vex is the external source voltage.

The current ratio of 1\ and 12 is calculated from Eqs.

(2)

and

(3),

and is given by

r 11

=

{iR (VexO -

al~Tl)

+ (-M VexO +

~(VexO

-

al~Tl

+

2

Ma2~T2)w} l{iR(Vexo-a2~T2)

+ (-MVexO + Ll (VexO':'" a2

~

T2 ) + M al

~

T 1) w }

If the condition of

(5) (6)

(4)

is satisfied, the equation (4) will be an usual equation and is given by

II R +

iw(~-

M)

- =

12 R+iw(L

1

-M) (4')

This idea is valid both for the superconducting magnets and cables. and if we use HTS conductor, PCL is only method to reduc~ the heat leak to the low temperature system. In the next step, we hope to perfoITI1 the experiment.

Reference

1) SYamaguchi, et ai, Proc. 16

th

Int. Cryogenic Eng.

Conf.lInt. Cryogenic Mat. Conf. (ICEC 16IICMC) part-2, pp. 1159-1162,1997.

2) S. Yamaguchi et aI, Cryogenics, vol. 36, pp. 661-665, 1996.

3) S. Yamaguchi et ai, Cryogenics, vol. 38, pp. 875-880, 1998.

4) S. Yamaguchi et ai, Applied Superconducitvity Conf., LFD-07, Palm springs, Cal., USA, 1998.

225

Fig.  1.  Schematic  structure  of  the  proposed  Peltier  current  lead to improve current imbalance

参照

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