• Aucun résultat trouvé

KPY 12 - A PRESSURE TRANSDUCER SUITABLE FOR LOW TEMPERATURE USE

N/A
N/A
Protected

Academic year: 2021

Partager "KPY 12 - A PRESSURE TRANSDUCER SUITABLE FOR LOW TEMPERATURE USE"

Copied!
5
0
0

Texte intégral

(1)

HAL Id: jpa-00223607

https://hal.archives-ouvertes.fr/jpa-00223607

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.

KPY 12 - A PRESSURE TRANSDUCER SUITABLE FOR LOW TEMPERATURE USE

F. Breimesser, L. Intichar, M. Poppinger, C. Schnapper

To cite this version:

F. Breimesser, L. Intichar, M. Poppinger, C. Schnapper. KPY 12 - A PRESSURE TRANSDUCER

SUITABLE FOR LOW TEMPERATURE USE. Journal de Physique Colloques, 1984, 45 (C1), pp.C1-

671-C1-674. �10.1051/jphyscol:19841136�. �jpa-00223607�

(2)

KPY 1 2

-

A PRESSURE TRANSDUCER S U I T A B L E FOR LOW TEMPERATURE USE

F . Breimesser, L . Intichar, M . Poppinger and C . Schnapper

Siemens AG, Research Laboratories, Paul Gossen S t r . 100, 0-8520 ErZangen, F.R.G.

R6sum6: Le capteur de pression K P Y 12 commercialis6 par Siemens permet de mesurer des diff6rence.s de pression jusqul$ 2 bars dans la plage de temp6rature de 243 K 5 298 K.

A des tempbratures tr&s basses atteiqnant 4 K , la lin6arit6 est conservge et la sensibilith sSaccroZt de 100 % environ. Le capteur a kt6 utilis6 avec succes 2 basse temp6rature dans une installation d'essai fonctionnant 2 3000 tr/min.

Abstract: The commercially available Siemens pressure sensor K P Y 12 in silicon planar technology measures differential pressures up to 2 bar in the temperature range from 243 K to 398 K . However, at temperatures down to 4 K the specified linearity is also preserved, and the sensi- tivity increases by about 100 %. The sensor has been successfully em- ployed at low temperatures in a test rig rotating at 3000 rpm.

Description of the K P Y 12

The pressure deflects a silicon plate, setting up strains in silicon resistors located on top of the plate. The strains are converted into an electrical signal by the piezoresistive effect.

As is usual with strain gages, four resistors are arranged in a Wheat- stone bridge. The pressure load causes a decrease in the resistance of two resistors and an lncrease in the resistance of the other two resistors. The chip of the K P Y 12 is shown in Figure 1 . It is mounted in a TO-8-like encapsulation (Figure 2 ) . The specifications of the KPY 12 are summarized in Table 1 .

Table 1 :

Specifications of K P Y I 2- pressure transducer

Operating temperature -30 to 125 " C

Bridge resistance s 7

kR

Full scale output 1 0 +

-

3 mV/V bar

Zero balance

- +

5 mV/V

~ i n e a r i t ~ l )

+

0.5 % FS Thermal sensitivity shift 1 0.2 typ- %/K Thermal zero shift - + 0.02 % / K FS Hysteresis < 0.5 % FS

Response time

<

1 ms

Weight % 2.7 9

1) maximum deviation from best straight line fit vs full scale output.

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:19841136

(3)

JOURNAL DE PHYSIQUE

F i q . 1 :

P r e s s u r e s e n s o r c h i p - s i z e 4 x 4 m m 2

F i g . 2 : K P Y I 2 s e n s o r

Low t e m p e r a t u r e e x p e r i m e n t s

The b r i d g e v o l t a g e , U , a n d t h e s u p p l y c u r r e n t , I s , of s e v e r a l

s e n s o r s w e r e m e a s u r e d a s a f u n c t i o n of p r e s s u r e , p , a n d t e m p e r a t u r e , T . The s u p p l y v o l t a g e was U = 5 V .

F i g . 3 shows some t r a n s d u c e r c h a r a c t e r i s t i c s o f o n e s e n - s o r . A t a l l t e m p e r a t u r e s , t h e l i n e a r i t y i s a s good a s s p e - c i f i e d a t room t e m p e r a t u r e . The s e n s i t i v i t y s = ( U - U o ) / p i n c r e a s e s w i t h d e c r e a s i n g t e m - p e r a t u r e .

F i g . 3 :

T y p i c a l o u t p u t v o l t a g e v e r s u s p r e s s u r e f o r a K P Y 1 2 s e n s q r a t d i f f e r - e n t t e m p e r a t u r e s

(4)

The o f f s e t v o l t a g e , U , i s s e n s o r - s p e c i f i c a n d d e p e n d s s l i g h t l y o n t e m p e r a t u r e . I n F i g .

8 ,

t h e n o r m a l i z e d s e n s i t i v i t y s ( T ) / s ( T = 2 9 3 K ) and t h e o f f s e t v o l t a g e U

o ( T ) o f a s e n s o r a r e p l o t t e d a g a i n s t t e m p e r a t u r e .

Due t o t h e s p e c i f i e d t o l e r a n c e s t h e i n d i v i d u a l s e n s o r h a s t o b e c a l i - b r a t e d f o r a p r e c i s e p r e s s u r e m e a s u r e m e n t . I n a d d i t i o n , t h e o p e r a t i n g t e m p e r a t u r e m u s t b e known. F o r r e d u c e d p r e c i s i o n r e q u i r e m e n t s i n t e r - p o l a t i o n b a s e d on t h r e e r e f e r e n c e m e a s u r e m e n t s a t 4 K, 77 K a n d room t e m p e r a t u r e may b e s u f f i c i e n t .

A t t e m p e r a t u r e s b e l o w 90 K a n d a b o v e 220 K t h e t e m p e r a t u r e c a n b e d e t e r m i n e d f r o m t h e b r i d g e r e s i s t a n c e Rb5 = U s / I s . I t i s a l m o s t i n d e - p e n d e n t o f p r e s s u r e ( d ( L \ R / R ) / d p h 6 . 1 0 - b a r - 1 ) b u t i t d e p e n d s o n t e m p e r a t u r e . F i g - 5 s h o w s t h e r a t i o R b r ( T ) / R b r ( T = 293 against t e m p e r a t u r e . The t e m p e r a t u r e d e p e n d e n c e was a l m o s t i d e n t i c a l f o r t h e s e n s o r s i n v e s t i g a t e d .

t e m p e r a t u r e

F i g . 4 :

N o r m a l i z e d s e n s i t i v i t y a n d o f f s e t v o l t a g e a g a i n s t t e m p e r a t u r e

t e m p e r a t u r e

F i g . 5 :

N o r m a l i z e d b r i d q e r e s i s t a n c e a g a i n s t t e m p e r a t u r e

(5)

JOURNAL DE PHYSIQUE

A p p l i c a t i o n

F o r t e s t i n g a c o o l i n g s y s t e m , t h e p r e s s u r e o f c o l d h e l i u m g a s h a s t o b e m e a s u r e d d i r e c t l y i n a c o n t a i n e r r o t a t i n g a t 3 0 0 0 r p m . T h e s e n s o r K P Y 1 2 w a s c h o s e n , b e c a u s e i t i s s m a l l , h i g h - v a c u u m t i q h t , w i t h s t a n d s h i g h m e c h a n i c a l l o a d s a n d h a s l i t t l e t h e r m a l l o a d ( t y p i c a l l y 5 mW a t U = 5 V ) . F o r m o r e t h a n o n e y e a r t h e s e n s o r h a s w o r k e d r e l i a b l y a n d w ? t h o u t p r o b l e m s .

S e n s o r s o f t h i s t y p e o f f e r t h e p o s s i b i l i t y o f m e a s u r i n g n o t o n l y t h e p r e s s u r e , b u t a l s o d e r i v e d q u a n t i t i e s , e . g . f l o w r a t e s ( b y m e a s u r i n g o r i f i c e s ) o r l i q u i d l e v e l s a t c r y o g e n i c t e m p e r a t u r e s .

A c k n o w l e d g e m e n t

T h e a u t h o r s w o u l d l i k e t o e x p r e s s t h e i r g r a t i t u d e t o Mrs. R u p p e r t ,

Mr. S u n k e a n d M r . S t u e v e f o r c a r r y i n g o u t t h e m e a s u r e m e n t s .

R e f e r e n c e s

/ I / B r e i m e s s e r , F . , P o p p i n g e r , M . , S c h w a i e r , A . , " P i e z o r e s i s t i v e p r e s s u r e s e n s o r w i t h s i l i c o n d i a p h r a g m " , S i e m e n s F o r s c h , u . E n t w i c k 1 . - B e r . V o l . 1 0 ( 1 9 8 1 ) No. 2 , p p 72-77

/ 2 / I n t i c h a r , L . , S c h n a p p e r , C . ; " E x p e r i m e n t a l s i m u l a t i o n o f a h e l i u m c o o l i n g s y s t e m f o r a s u p e r c o n d u c t i n q g e n e r a t o r " ; 8 t h I n t . C o n f . o n M a g n e t T e c h n o l o g y , MT-8, p a p e r 2 P 4 - 0 2 , G r e n o b l e , 5 - 9 S e p t . 1 9 8 3

Références

Documents relatifs

Propagation of Lamb waves in an immersed periodically grooved plate: Experimental detection of the scattered converted

The vibroacoustic behavior of a rectangular plate is then analyzed as a function of the excitation pressure field (either a purely turbulent excitation or a purely acoustic excitation

Silver iodide has been the object of a great number of investigations, but there is some disagreement in the literature regarding the phase diagram as well as on the

SiNWs exhibit a diameter around 100 nm (not shown here) and a length that can reach at least 10 µm. Since spacing between teeth does not exceed 10 µm, SiNWs can insure

In order to be able to analyse in TEM-STEM the crystallochemistry of recombining defects in p-type polysilicon (L = 100 pm), we have developed the scanning transmission

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des

The growth rate (G) of the epi-layers were measured by a profilometer and the wafer temperature was measured by a thin thermocouple attached to a test wafer

On the origin of the electrical activity in silicon grain boundaries..