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DETERMINATION OF PHOTO ACOUSTIC SPECTRA OF DYES-I CONGO RED
R. Mathur, G. Pandey
To cite this version:
R. Mathur, G. Pandey. DETERMINATION OF PHOTO ACOUSTIC SPECTRA OF DYES-I CONGO RED. Journal de Physique Colloques, 1983, 44 (C6), pp.C6-171-C6-175.
�10.1051/jphyscol:1983626�. �jpa-00223185�
JOURNAL DE PHYSIQUE
Colloque C6, suppIbment au nulO, Tome 44, octobre 1983 page C6- 171
DETERMINATION OF PHOTO ACOUSTIC SPECTRA OF DYES-I CONGO RED
R.N. Mathur and G . C . Pandey
University Service and Instrumentation Centre, JawaharZaZ Nehru University, New DeZhi 110067, India
msUME
Gn prgsente l e s spectres photo acoustiques du Rouge Congo qui e s t un materiau opaque. On canpare l e s spectres PA du solide, l e s spectres de transmission d'une solution dilu&, l e spectre PA du colorant dGpos6 sur un papier f i l t r e .
ABSTRACT
Photo acoustic (PA) spectra of one of the optically opaque material
-
dye Congc-Red has been reported. The PA spectra of solid dye have been compared with the transmission spectrum of the diluate aquous solution of the dye as well a s the PA spectrum of the air dried aquous solution of the dye on a f i l t e r paper.
PA spectroscopy i s one of t h e v e r y s t r o n g a n a l y t i c a l t o o l f o r i n v e s t i g a t i o n o f m a t e r i a l s n o t amenable t o
a n a l y s i s by t h e c o n v e n t i o n a l s p e c t r o s c o p y ( 1 ) S a t u r a t i o n e f f e c t s observed i n s u c h studies,however l i m i t i t s u t i l i t y i n t h e i n v e s t i g a t i o n of h i g h l y s b s e r b i n g compounds l i k e o r g a n i c dyes and semi-conductors(2).
L i n and ~ u d e k / 3 / have shown t h a t sample p r e p a r a t i o n t e c h n i q u e s c a n overcome t h e P.A. s a t u r a t i o n problem.
They developed t h r e e s e p a r a t e methods f o r d e t e r m i n a t i o n of P.A Spectrum of h i g h l y a b s o r b i n g compounds. These a r e :
( i ) D e p o s i t i o n of a t h i n l a y e r of t h e sample onto a q u a r t z p l a t e e i t h e r by vacuum d e p o s i t i o n o r by smearing w i t h a s u i t a b l e a p p l i c a t o r .
( i i ) Nolecular d i s p e r s i o n of t h e sample over t h e s u r f a c e of a non a b s o r b i n g medium such a s barium s u l p h a t e , magnesium oxide, n e u t r a l a l u n i n a and s i l i c a g e l , ( i i i ) The sample i s coground with a non a b s o r b i n g
s u b s t r a t e i n a v i b r a t i n g mill(mechanica1 d i s p e r s i o n technique) and t h e mixture used a s t h e sample
L i n and ~ u d e k / 3 / have s u c c e s s f u l l y used above methods f o r d e t e r m i n a t i o n of P A s p e c t r a of t e t r a phenyl- porphin a t d i f f e r e n t concentrations. However, t h e presence of d i l u e n t o r t h e s u b s t r a t e w i t h t h e sample may r e s u l t i n d e v i a t i o n s and d i s t o r t i o n s of t h e a c t u a l spectrum.
A n a t t e m p t w a s , t h e r e f o r e , made t o o b t a i n PA S p e c t r a of one of t h e h i g h l y a b s o r b i n g compolmds-Congo-Red i n s o l i d s t a t e ( w i t h o u t any s u b s t r a t e ) and i s r e p o r t e d i n t h e p r e s e n t paper.
Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:1983626
JOURNAL DE PHYSIQUE
According t o Rosencwaig-Gersho t h e o r y a compound s h a l l be photo a c c o u s t i c a l l y opaque i f t h e t h e r ma1 d i f f u s i o n l e n g t h i s l e s s t h a n t h e o p t i c a l a b s o r p t i o n l e n g t h 1/B, S i n c e it r e q u i r e s modulation f r e q u e n c i e s i n excess o f 1
o4
HZt o b r i n g t h e s e p a r t i c l e s o u t of S a t u r a t i o n ( l / B ) , such samples w i l l appear t o be i n h e r e n t l y opaque, even from photo a c c o u s t i c p o i n t of view(4). I n s u c h c a s e s , t h e r e f o r e , P.A. S a t u r a t i o n s h a l l p r e v e n t r e c o r d i n g of a meaningful
spectrum.
SPECTROSCOPY
The PA spectrum o f t h e dye was o b t a i n e d u s i n g t h e normal s e t t i n g s of t h e i n s t r u m e n t as per d e t a i l s given below:
Modulation frequency : A s p e r d e t a i l s g i v e n i n f i g u r e s Scan r a n g e ; uv-vi s i b l e
Scan r a t e 100 nm/minute
S e n s i t i v i t y Phase
Lamp C u r r e n t
A s p e r d e t a i l s g i v e n i n f i g u r e s 90%
19 Am
The d i f f e r e n t s p e c t r a o f t h e dye recorded have been shown f i g u r e s 1-4.
WAVELENGTH
Figure-I: Photo Acoustic Spectrum of Congo Red.
Figure-1 shows t h e P.A S p e c t r a r e c o r d i n g w i t h normal ins'nrmental s e t t i n g s at a modulation frequency of 240 HZ A s m a l l hump a t 470-480m a l o n g - w i t h a r a p i d d e c r e a s e i n
P.A s i g n a l around 590 nm can be c l e a r l y d i l i n e a t e d from t h i s f i g u r e . A s no comparable spectrum was a v a i l a b l e i n t h e l i t e r a t u r e , it was very d i f f i c u l t t o a n a l y s e t h e
s p e c t m s p e c i a l l y t h e absence of any s t r o n g a b s o r p t i o n peak.
A s a l r e a d y mentioned even modulation frequency of 240 HL i s t o o low t o b r i n g t h e sample o u t of s a t u r a t i o n .
The P.8. s p e c t r a of t h e s o l i d d y e , t h e r e f o r e , were recorded a g a i n u s i n g s l i t widths f o u r times t h e normal used f o r r e c o r d i n g of t h e spectrum i n f i g u r e - I .
A t h i n l a y e r of t h e powdered sample Was spread on t h e bottom s u r f a c e of t h e c a v i t y i n t h e sample h o l d e r . The P.A.
s p e c t r a of t h e sample was t h e n recorded at d i f f e r e n t modulation f r e q u e n c i e s v i z . 10,20,40,80,160 and 240 1%
reproduced i n figure-2.
! 10 H z at 10mV 1100 n m l s e c 1 2 20 H Z at lorn" 1100 nm1s.cI I. '0 H Z 01 l a m " l , O o n m l r = c l
' 8 0 H Z m t 1 mV 1100nmf S.c 1
5. 20 H. .t 10 mv l l o o n m / s e ~ 2LoHz 1 m~ 1100om/..c 1 2i0 nZ I 1 2 0 nmf s * c 1 g smmpLa hold-r 100 P V I ~ ~ ~ ~ ' ~ '
(5111 w l t h L X ' 1
WAVELENGTH
Figure-2: Photo Acoustic S p e c t r a of Congo-Eied(so1id s t a t e ) a t d i f f e r e n t modulation f r e q u e n c i e s ;
The P.A. s p e c t r a of t h e sample h o u e r has been i n c l u d e d i n t h e above f i g u r e . The spectmun a t 240 HZ recorded a t two d i f f e r e n t s c a n r a t e s ( 100 and 2C nm/rainute) t o l o c a t e any peak which might have been missed a t h i g h e r s c a n r a t e . I t ma be n o t i c e d from t h e above f i g u r e ( d p e c t r a N6s. 182fthat t h e two s p e c t r a a r e r e p r o d u c i b l e and t h u s excludes t h e p o s s i b i l i t y of any a d d i t i o n a l band/peak. The s p e c t r a a t o t h e r modulation f r e q u e n c i e s , t h e r e f o r e , were recorded a t 100 nm/minute s c a n r a t e only.
I t may a l s o be mentioned t h a t t h e s p e c t r a a t d i f f e r e n t moduiation f r e q u e n c i e s a r e s i m i l a r e x c e p t t h a t i n t e n s i t y of t h e bands(peak h e i g h t ) a r e reduced due t o s a t u r a t i o n e f f e c t s .
T h i s s t u d y t h u s shows t h a t t h e P.A. s p e c t r a of o p t i c a l l y opaque samples(without any s u b s t r a t e / d i l u e n t ) can a l s o be recorded b y a d j u s t m e n t of c e r t a i n i n s t r u m e n t a l s e t t i n g s , F u r t h e r work a l o n g t h i s l i n e i s i n progress.
A corn a r i s o n of t h e PA spectrum o f t h e dye i n s o l i d s t a t e y f i g u r e - 2 ) w i t h t h a t of t h e d i l u t e aquous s o l u t i o n
( t r a n s m i s s i o n spectrum reproduced i n f i g m e - 3 ) .
JOURNAL DE PHYSIQUE
C R = C o n g o r o d
Ftg 3. T r o n s m ~ s s i o n s p e c t r a of Dyes
Figure.5: Transmission Spectrum o f t h e aquous s o l u t i o n of t h e dye.
F i g u r e . 3 shows t h a t t h e broad band around 495 n m p r e s e n t i n t h e t r a n s m i s s i o n spectrum seems t o be a combination of t h e 2 bands a t 465 and 495 nm(weak) p r e s e n t i n t h e PA spectrum.
I 1
2W 100 L 00 5W 600 700 800
WAVELENGTH
Figure-4: Photo Acoustic Spectrum of t h e f i l t e r paper w i t h and without dye.
The e f f e c t of s u b s t r a t e on t h e PA Spectrwn o f t h e dye was a l s o s t u d i e d . A p i e c e of 't!hatman(~o. 42) f i l t e r paper w a s soaked i n a d i l u t e aquous s o l u t i o n of t h e dye and d r i e d i n a i r , The s p e c t r a o f t h i s a s w e l l as
t h a t of t h e f i l t e r paper a s s u c h were r e c o r d e d ( f i g u r e - 4 ) . The E.A spectrum of
t h e dye soaked f i l t e r paper gave qnly one v e r y broad band between 420 and 600 nm. It may be mentioned t h a t t h i s spectrum, i s comparable t o t h a t of t h e t r a n s m i s s i o n spectrum(figure-3).
2
1 conpo r e d 2 F0II.r paper 3 *.lhyl=ne blue
Y e t h ~ I ~ ~ . blue o f f e r OIIosU,S
Conclusions : The above s t u d y i n d i c a t e s t h a t
( i ) t h e PA spectrum of h i g h l y a b s o r b i n g compounds can be recorded a t lower modulation f r e q u e n c i e s .
( i i ) The P.A. spectrum of t h e dye i n s o l i d s t a t e i s b e t t e r r e s o l v e d t h a n that of t h e t r a n s m i s s i o n spectrum of t h e dye s o l u t i o n .
( i i i ) ~ h e P.A. spectrum o f t h e aquous s o l u t i o n of t h e dye on a s u b s t r a t e ( f i 1 t e r paper) seems t o r e p l i c a t e i t s t r a n s m i s s i o n spectrwn. The d i l u e n t / s u b s t r a t e appear t o a f f e c t a change i n t h e P.A. spectrum of t h e dye.
T h i s work i s a p a r t of t h e p r o j e c t supported by Department of Environment, Government of I n d i a .
1
.
P&DhY G.C. ,Proc. 3 r d I n t e r n a t i o n a l Neeting o n Photo a c c o u s t i c and photo Thermal Spectroscopy, P a r i s 19832. BOBEITCWAIG A . , i n "Advances i n E l e c t r o n i c and E l e c t r o n P h y s i c s w Vol-46 ( e d . ~ . ~ o r t o n )
Academic p r e s s (N.Y.) 1978.
3. LIN J . W . and DUDEK L.P. Anal. Chem.
2
1627(1979]4. ROSElhCWAIG A., "Photo Accoustics and Photo Accoustics Spectroscopyn John. ~ i l l e y ( l ~ . Y ) 1980 P . 170