• Aucun résultat trouvé

FEASIBILITY STUDY OF A 10-GWh TOROIDAL SUPERCONDUCTIVE MAGNETIC ENERGY STORAGE SYSTEM2. CONCEPTUAL DESIGN OF COIL SYSTEM

N/A
N/A
Protected

Academic year: 2021

Partager "FEASIBILITY STUDY OF A 10-GWh TOROIDAL SUPERCONDUCTIVE MAGNETIC ENERGY STORAGE SYSTEM2. CONCEPTUAL DESIGN OF COIL SYSTEM"

Copied!
5
0
0

Texte intégral

(1)

HAL Id: jpa-00223587

https://hal.archives-ouvertes.fr/jpa-00223587

Submitted on 1 Jan 1984

HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

FEASIBILITY STUDY OF A 10-GWh TOROIDAL SUPERCONDUCTIVE MAGNETIC ENERGY STORAGE SYSTEM2. CONCEPTUAL DESIGN OF

COIL SYSTEM

M. Shimizu, T. Yoshioka, Y. Morita, Y. Tanabe, T. Hamajima, N. Fujiwara, N. Miki, M. Yamaguchi, T. Horiuchi, N. Takeda, et al.

To cite this version:

M. Shimizu, T. Yoshioka, Y. Morita, Y. Tanabe, T. Hamajima, et al.. FEASIBILITY STUDY OF A

10-GWh TOROIDAL SUPERCONDUCTIVE MAGNETIC ENERGY STORAGE SYSTEM2. CON-

CEPTUAL DESIGN OF COIL SYSTEM. Journal de Physique Colloques, 1984, 45 (C1), pp.C1-587-

C1-590. �10.1051/jphyscol:19841118�. �jpa-00223587�

(2)

JOURNAL DE PHYSIQUE

Colloque C1, suppl6ment au no I , Tome 45, janvier 1984 page C1-587

F E A S I B I L I T Y STUDY OF A 10-GWh TOROIDAL SUPERCONDUCTIVE MAGNETIC ENERGY STORAGE SYSTEM

2 , CONCEPTUAL DESIGN OF C O I L SYSTEM

M. Shimizu, T . ~ o s h i o k a * , Y. ~ o r i t a * , Y. ~ a n a b e * , T, ~ a m a j imar*, N. ~ u j i w a r a * ' , N . Mikir*, M . yamaguchir*, T . ~ o r i u c h i * ~ , N. ~akeda***, H. Miyazakirrr and K . ~amemura***

!The Kansai EZectric Power Company, Inc., Japan

*

l'he I n s t i t u t e of Applied Ene~gy, Japan

i* Toshiba Corpora t i o n , Japan

***

T a i s e i Corpora t i o n , Japan

RBsume

-

On p r 6 s e n t e l e p l a n d ' u n systgme d e s t i n e 21 l ' a c c u m u l a t i o n d'une Bner- g i e de 10 GWh p a r aimant supraconducteur. On p r e f e r e a d o p t e r un arrangement d'aimant t o r o ' i d a l . Le p r i n c i p a l avantage de c e systeme r e s i d e dans l a f a i t que l a f u i t e du champ magnetique e s t t r e s f a i b l e , l a r e a l i s a t i o n e t l ' e n t r e t i e n p l u s s i m p l e s . En consdquence, l e s charges pour l e s i t e de c o n s t r u c t i o n s o n t r e d u i t e s

.

A b s t r a c t - A conceptual design of a 10 GWh superconductive magnetic energy s t o r a g e (SMES) f o r d i u r n a l energy s t o r a g e u s e i s p r e s e n t e d . A t o r o i d a l f i e l d c o i l arrangement i s p r e f e r a b l y adopted. The main advantage of t h i s d e s i g n i s t h a t t h e s t r a y magnetic f i e l d is i n h e r e n t l y q u i t e s m a l l a n d m a n u f a c t u r a b i l i t y a s w e l l a s m a i n t a i n a b i l i t y i s more f e a s i b l e . T h e r e f o r e , requirements f o r a c o n s t r u c t i o n s i t e a r e r a t h e r small.

1. INTRODUCTION

A superconductive magnetic energy s t o r a g e i s worthy of m e r i t f o r d i u r n a l energy s t o r a g e use p r i m a r i l y from t h e p o i n t of view of h i g h e r e f f i c i e n c y and f a s t

c o n t r o l l a b i l i t y . The p r e s e n t e d SMES i n t h i s paper h a s t h e c a p a b i l i t y o f 10 GWh of which 75% of s t o r e d energy i s d e l i v e r e d t o t h e power system d u r i n g 8 hours with a c o n s t a n t power. This SMES would be a b l e t o be i n s t a l l e d i n l i e u of pumped s t o r a g e power s t a t i o n s . The SMES which h a s t h e t o r o i d a l f i e l d c o i l arrangement i s chosen i n p r e f e r e n c e t o s o l e n o i d a l c o i l type. The major advantages of t h e t o r o i d a l c o i l system a r e i t s extremely low s t r a y f i e l d and e a s i n e s s of c o i l manufacturing and maintenance.

The 10 GWh SMES with t h e t o r o i d a l f i e l d c o i l composed of 500 c o i l s i s p l a c e d a t t h e 30 m depth of underground. Major r a d i u s and minor r a d i u s a r e 272 m and 14.8 m r e s p e c t i v e l y . C o i l c u r r e n t i s 100 kA and c o i l maximum f i e l d i s 9.4 T, t h e r e f o r e b o t h Nb3Sn and NbTi superconductors a r e e f f e c t i v e l y a p p l i e d t o t h e c o i l . The pool b o i l i n g c o o l i n g s a t i s f i e s t h e cryogenic s t a b i l i t y of t h e c o i l . The t o r o i d a l f i e l d c o i l r e c e i v e s two k i n d s of electro-magnetic f o r c e : t h e . c e n t e r i n g f o r c e of

2.5 x l o 7 kg a c o i l and t h e hoop f o r c e of 9.2 x 10' kg a c o i l . Only t h e former i s supported with rock mass while t h e l a t t e r with s t a i n l e s s s t e e l m a t e r i a l . The s t r a y f i e l d r e g i o n i s very s m a l l , f o r i n s t a n c e t h e boundary of 200 G and 20 G from t h e t o r u s c e n t e r i s 320 m and 380 m i n r a d i u s r e s p e c t i v e l y , each considered a s t h e allowable f i e l d f o r e l e c t r i c a l machine and c o n t r o l equipment.

For c o n s t a n t power supply, 12-pulse number c o n v e r t e r s a r e p u t t o u s e , which have advantages with r e s p e c t t o t h e r e a c t i v e power requirement and harmonic c o n t e n t of t h e l i n e c u r r e n t . I n a d d i t i o n , bypass s w i t c h e s a r e used i n o r d e r t o decrease t h e peak v a l u e of t h e r e a c t i v e power, r e s u l t i n g i n t h e 60% decrease.

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:19841118

(3)

JOURNAL DE PHYSIQUE

2. TOROIDAL COIL SYSTEM 2.1 Coil parameters

Toroidal coil parameters were studied to optimize the coil weight, volume and conductor length taking account of coil fabrication and maintenance under the condition of the stored energy of 10 GWH (3.6 x 1013 J)

.

Main results are as follows /I/: (1) aspect ratio (major radius/minor radius) is about 20, (2) the torus is placed at depth of 30 m under the ground in an open trench, (3) 500 toroidal coils are adequately chosen, (4) the rock mass supports only the centering force, a part of electro-magnetic forces, (5) the hoop forces are supported by the coil itself.

Toroidal system and coil parameters on the basis of above optimization are listed in Tables 1 and 2, respectively. The maximum field is 9.4 T, which can make the coil compact. Therefore, Nb3Sn superconductor with copper matrix is used above 8 T. NbTi with mixed matrix below 8 T is chosen in order to reduce AC loss in the conductor /2/. Both type conductors are designed to satisfy the cryogenic

stabilization at the rated current of 100 kA. The coils are immersed in 4.2 K liquid helium, because of its matured technology.

The Heat conduction through the structures supporting the centering force and gravitational force will be the major one in the total heat load, and will be estimated to be about 29 kW at 4.2 K when the liquid nitrogen shield is employed.

The helium reservoir might consist of non-metalic materials such as FRP, which has been extensively developed, and therefore the eddy current loss should be-reduced below 1 kW. The satellite cooling systems, connected each other through coolant bus line, can be adopted for cooling down each divided sector of the torus.

The stray field distribution on radial and axial plane is shown in Fig. 1. The maximum field on the ground is about 1 KG, but the field rapidly decreases with the distance from the coil. The control equipment should be located outside the radial distance of 380 m from the torus center, where the field is less than 20 G, and the field at 800 m is the same order as the terrestrial magnetism of 0.3 G. Therefore, such weak stray field suggests that the SMES site could be arbitrarily selecfed.

und

/ Coil

Torus center Radial distance R (m) Fig. 1 Stray field distribution

(4)

Table 1- 10-GWh SMES System Parameters

Stored enerq-i 3.6 x loL3 5

Energy exchanged 2.7 x lox3 J

Mexlmum c u r r e n t 100 kA

Minimum c u r r e n t 50 kA

Discharge duration time 8 boors

Discharge power 940 MW

M a x i r n m f i e l d 9.4 T

Hoop f o r c e pee c o d 9 x 10' kg£

Centering f o r c e p e r c o i l 2.5 x 10' kgf

lteat load p e r c o ~ l 57 W a t 4.2-K

Cryogenic c o o l a n t pool boxling a t 4.2*K

Maximum s t r a y Eield on the ground 800 Gauss Cox1 l o c a t i o n i n t h e -pen trench 30 m Cross s e c t i o n of t h e open trench 40 x 80 m Table 2. 10-GWh T o r o i d a l C o i l C h a r a c t e r i s t i c s

Major r a d i u s Minor r a d i u s Aspect r a t i o C o i l t h i c k n e s s Number of c o i l s Number of t u r n s p e r c o i l Weight of one c o i l Windrng p a t t e r n

500 240 3000 tons pancake

2.2 C o i l S t r u c t u r e

There a r e s e v e r a l concepts concerning t h e s u p p o r t system of t h e e l e c t r o m a g n e t i c f o r c e . The o p t i o n s c o n s i d e r e d a r e :

(1) t h e u s e of an open t r e n c h i n rock a s a c e n t r a l compressive s t r u c t u r e which s u p p o r t s o n l y t h e r a d i a l c e n t e r i n g f o r c e ,

(2) t h e use of a t u n n e l i n rock which s u p p o r t s both t h e r a d i a l c e n t e r i n g f o r c e and t h e hoop f o r c e .

The o p t i o n 1 i s s e l e c t e d i n t h i s design.

The s t r u c t u r e of t h e t o r o i d a l f i e l d c o i l i s shown i n Fig. 2. The number of t h e c o i l s amounts t o 500. The o u t e r diameter of t h e helium v e s s e l i s 33.6 m and i t s c r o s s s e c t i o n i s 2.16 m x 2.7 m. The thermal i n s u l a t o r of f i b e r g l a s s r e i n f o r c e d p l a s t i c s i s provided t o t r a n s m i t t h e c e n t e r i n g f o r c e from c o i l t o rock. Thermal s h i e l d p l a t e (77K) is i n s t a l l e d i n t h e i n s u l a t o r i n o r d e r t o reduce t h e h e a t l e a k t o helium v e s s e l . The l e n g t h of t h e thermal i n s u l a t o r f o r 300K-77K r e g i o n i s 2 m and t h a t f o r 77K-4K r e g i o n is 1 m. The p r e s s u r e on t h e rock due t o t h e c e n t e r i n g f o r c e i s 3 MPa.

The e l e c t r o m a g n e t i c hoop f o r c e Intercoil

i s supported by t h e s t a i n l e s s s t e e l reinforcement around t h e conductor and n o t t r a n s m i t t e d t o t h e rock. The average t e n s i l e s t r e s s of t h e reinforcement i s 470 MPa which is below t h e allow- a b l e s t r e s s f o r SS316LN a s t h e reinforcement m a t e r i a l .

Another f e a t u r e of t h e s t r u c t u r a l c o n f i g u r a t i o n i s t h e g r a v i t y s u p p o r t system. The s u p p o r t i s p l a c e d a t t h e bottom of c o i l and between c o i l s . The i n t e r c o i l s u p p o r t beams a r e provided a s t h e

s u p p o r t i n g s t r u c t u r e f o r an ~ o c k mass

earthquake. F i g . 2 C o i l s t r u c t u r e c o n f i g u r a t i o p

3. POWER CONVERSION SYSTEM

The power conversion system f o r t h e SMES i s s t u d i e d h e r e on t h e b a s i s o f : (1) con- n e c t i o n t o t h e power l i n e of AC 275 kV o r AC 500 kV, (2) c o n s t a n t power of 940 MW

(5)

CI-590 JOURNAL DE PHYSIQUE

d u r i n g c h a r g i n g and d i s c h a r g i n g t h e c o i l , ( 3 ) p r e f e r a b l e c h o i c e of t h y r i s t o r con- v e r t e r i n i t s economy and r e l i a b i l i t y a s t h e power conversion equipment, (4) con- s i d e r a t i o n of r e a c t i v e power compensator, harmonic f i l t e r and a u x i l i a r y power supply.

A schematic main c i r c u i t diagram of t h e SMES power system i s shown i n F i g . 3 . The u l t r a - h i g h v o l t a g e i s stepped down t o t h e manageable v o l t a g e of 66 k V i n t h e con- v e r t e r equipment through t r a n s f o r m e r s . The c o n v e r t e r , r e a c t i v e power compensator and harmonics f i l t e r a r e connected t o t h e 66 k V bus l i n e . The a u x i l i a r y power i s s u p p l i e d from t h i s l i n e .

The t h y r i s t o r conversion equipment i s composed of 1 2 b r i d g e s (1.9 k V

-

100 kA f o r 8 b r i d g e s and 0.95 k V

-

100 kA f o r 4 b r i d g e s ) connected i n s e r i e s , and o p e r a t e d a t 12 p u l s e number. The by-pass switch connected i n p a r a l l e l w i t h each p a i r b r i d g e

( c o n s i s t e d of two 6-pulse Gretz b r i d g e s , which a r e connected i n s e r i e s ) i s employed i n o r d e r t o reduce b o t h t h e r e a c t i v e power and t h e j o u l e l o s s generated by c i r c u l a t - i n g c u r r e n t . The c e n t e r t a p of t h e c o i l i s grounded i n o r d e r t o reduce t h e c o i l v o l t a g e t o t h e ground.

The c o i l v o l t a g e is mainly c o n t r o l l e d by two p a i r b r i d g e s of 1.9 k V , w h i l e t h e o t h e r p a i r b r i d g e s a r e o p e r a t e d a t a c o n s t a n t phase angle. The r e a c t i v e power com- p e n s a t o r i s i n s t a l l e d t a k i n g account of s u p p r e s s i n g t h e a p p a r e n t power f l u c t u a t i o n of 200 MVA on t h e power l i n e , which may b e caused by t h e above o p e r a t i o n mode.

The two t r a n s f o r m e r s w i t h t a p changers a r e connected between two 1 . 9 k V p a i r b r i d g e s and t h e 6.6 k V bus l i n e t o minimize t h e r e a c t i v e power.

CONCLUSION

A SMES employing a t o r o i d a l f i e l d c o i l arrangement h a s t h e p o t e n t i a l of p r o v i d i n g an e f f i c i e n t energy s t o r a g e f o r d i u r n a l energy s t o r a g e u s e , because of i t s advantage t h a t t h e s t r a y magnetic f i e l d i s q u i t e small and it i s more f e a s i b l e from t h e stand- p o i n t of b o t h m a n u f a c t u r a b i l i t y and m a i n t a i n a b i l i t y .

F i g . 3 Schematic main c i r c u i t diagram of t h e SMES power system REFERENCES

(1) M. Shimizu, e t . a l : i n t h e proceedings of t h i s conference.

( 2 ) H. T s u j i , e t a l : 9 t h Symposium on Engineering Problems of Fusion Research (1981, Chicagp) p2035.

Références

Documents relatifs

Assuming the correctness of QED calculations in electronic hydrogen atom, the problem can be solved by shifting by 5 standard deviations the value of the Ryd- berg constant, known

HOMER suggested that the best battery bank (consisting of Trojan T-105 batteries) should have 500 batteries. Based on the maximum power coming out of batteries we selected a

Spectra on isolated lanthanide amine-bis(phenolate) amido complexes are similar to those seen from small scale parallel reactions of metal amides and protonated ligands. Although

S’il s’agit de passer de l’orbite ext´ erieure ` a l’orbite int´ erieure, il suffit d’appliquer un d´ ecr´ ement de vitesse ∆v B au point B (i.e. d’utiliser des

Four low-amplitude modes were found in spectroscopy and one of them, with frequency 8.4079 d , was identified as ,m (3,2) Based on this mode identification, we finally deduced an

Preliminary evaluations of the effect of the power modulation on the BPA transmission system reveal that a sinusoidal power variation of the SMES unit causes the AC Intertie

Abstract - A toroidal coil system is probably preferable to a sole- noid coil system in terms of stray magnetic field, fabrication, maintenance, and repair.. Judging from

In section 4 we show that the problem is equivalent to a certain estimate for integral means of derivatives of conformal maps, and use this connection to prove (1.5) and to