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8/18/2019 Fundamentals of UV-Vis Spectrophotometer
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Fundamentals of UV-Vis
Spectrophotometer
13th July 2009
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What is Spectroscopy?
Spectroscopy is the measurement andinterpretation of electromagnetic radiationabsorbed Or emitted when the molecule, or
atom, or ion of a sample moves from oneallowed energy state to another.
Every atom, ion or molecule has a unique andcharacteristic relationship with
electromagnetic radiation. Chemical instrumentation does not createinformation; it refines the information alreadypresent in the signal from some transducer.
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!lectroma"netic radiation
Light as a wave form
avelength, frequency and Speed of
light
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!lectroma"netic radiation
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!lectroma"netic radiation
!requency of light and its Energy
"#article #roperty of Light$
h # $lan%s& constant # '('3 ) 10 -3* Joule + sec
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!lectroma"netic radiation
ave and #article #roperty of Light
h = Planck’s Constant (erg sec)
c = Speed of light (cm/sec)
λ = Wavelength (cm) ν = Frequenc (ccles/sec)
!nerg" ! = =h cλ
h ν
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!lectroma"netic radiation
%he Electromagnetic Spectrum
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!lectroma"netic radiation
%he Electromagnetic Spectrum
Color regionWavelength
(nm)
violet #$% & '#
blue '# & %%
cyan %% & %
green % & *
yellow * & +%
orange +% & *
red * & ,'%
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!lectroma"netic radiation
Complementary colors Sometimes ,hat you actually see is uite une.pected(
/i.in" different ,aelen"ths of li"ht doesn&t "ie you the
same result as mi.in" paints or other pi"ments(
f you arran"e some colors in a circle you "et a color
,heel( 4he dia"ram sho,s one possi5le ersion of this(
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!lectroma"netic radiation
Complementary colors 6olours directly opposite each other on the colour ,heel
are said to 5e complementary colours( 7lue and yello,
are complementary colours8 red and cyan are
complementary8 and so are "reen and ma"enta(
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!lectroma"netic radiation
Complementary colors /i.in" to"ether t,o complementary colours of li"ht ,ill
"ie you ,hite li"ht(
4hat is :4 the same as mi.in" to"ether paint colours(
f you mi. yello, and 5lue paint you don;t "et ,hite paint(
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ust li%e
the anti-5ondin" si"ma one@ at a
hi"her ener"y than the 5ondin" or5ital
- and so isn;t used to hold electrons(
7oth of the electrons in the pi 5ond
are found in the pi 5ondin" or5ital(
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for non-5ondin" -- non-5ondin"
or5itals contain lone pairs of
electrons
4he non-5ondin" or5itals ,e areinterested in contain a lone pair of
electrons - a perfectly sta5le filled
or5ital(
=nti-5ondin" or5itals are normally
empty and lo,er the sta5ility of acompound if they contain electrons(
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=5sorption of Simple isolated
6hromophores
Class -ransition λma. (nm)
& 01
& 0 & & 21 & S1 C = C & C C & & C 2
& 2 = 2 &
σ∗n σ∗n σ∗n σ∗n π∗π
π∗π
σ∗n
σ∗n
3$%
3$%3+%3%3,3,%3*%
#'%
Class -ransition λma. (nm)
& 20
& C10
C0
C001
C00’C021
π∗n π∗π π∗n
π∗π
π∗n π∗n
π∗n π∗n
,3
3+%+%
3$%$%%
%3%
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=5sorption of 6ommon
6hromophoresChromophore Example Solvent
max
(nm)
Type of
transition
4lkene C*13#C1=C1) n&1eptane 3,, π −> π∗
4lkne C(133C C&C1# n&1eptane 3,$
3+*))(
π −> π∗
−−−
−−−
0
55
C1#CC1# 0
55
C1#C1
n&1eptane
n&1eptane
3$*
)$%
3$%
)+#
n −> σ∗
n −> π∗
n −> σ∗
n−> π∗
Car6o.l 0
55
C1#C01
!thanol )%' n −> π∗
≡7
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=5sorption of 6ommon
6hromophores
Chromophore Example Solvent max (nm) Type of
transition
4mido 0
55
C1#C21)
Water )3' n −> π∗
48o C1# 2=2C1# !thanol ##+ n −> π∗
2itro C1# 20) 9sooctane )$% n −> π∗
2itroso C'1+ 20 !thl ether #%%**(
&&&&
n −> π∗
2itrate C)1(020) :io.ane ),% n −> π∗
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=5sorption of /ultichromophores
Compound Type max (nm)
C1#(C1)C1=C1 0lefin 3$'
C1=C1(C1)C1=C1 :iolefin (uncon;ugated) 3$
1C&C1C1&C1 :iolefin (con;ugated) 3,
1C=C1C1=C1C1=C1 -riolefin (con;ugated) %
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=5sorption of /ultichromophores
Compound Type max (nm)
0
55
C1#(C1)#CC1#
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When Bi"ht Stri%es a /olecule
Low energy causes C 4ibrational transitions
C 5otational transitions
+igh energy causes C Electronic transitions
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!lectronic 4ransition
>round state !%
!.cited state !3
∆! = !3 & !% = h ν
!nerg level
Radiation
e!nerg difference
∆!
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=5sorption of
Dadiation!nerg
ibrational transition
Rotationaltransition R
v!
v"
v#
$%&"
!#
Electronictransition
E!
E#
v#
v!
v"
E ' h in ?hich h is Planck’s constant (*7** @ 3%' Aoulesand ν is the frequenc of the radiation
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What causes =5sorption in
UV + VS De"ion?
Some sin"le 5onds
/any dou5le 5onds 6onu"ated dou5le 5onds
Some metal and inor"anic
compounds
: S halo"en
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6ali5ration and 7eer&s Ba,
Cuvette containing analte
9ncident light
9%
-ransmitted light
93
0ptical path length
From light source-odetector
-ransmittance - =9%
93
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Bam5ert C 7eer&s
Ba,46sor6ance 4 = log = ε C l
3
-
?here- B -ransmittance
ε B olar e.tinction coefficient
l B Path lengthC B 4nalte concentration
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6=B7D=4:
ED=$<
4nalte concentration (ppm)
4 6 s o r 6 a
n c e
Slope m = ε l
46s = m@Concentration D
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Deal Bimitations of 7eers
Ba, ncrease in analyte concentration 6hemical deiation due to physico-chemical
interaction
Stray li"ht
Fluorescence 5y the a5sor5in" species 6han"e in refractie inde. of analyte
on-parallel li"ht 5eam
nstrumental limitation due to noise
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!ffect of analyte concentration
=pplica5le to diluted solution eiation from linearity occurs at hi"h concentration
>G 0(01 /@
ilute the sample to a lo,er concentration
C 4he o5tained a5sor5ance alue is multiply 5y thedilution factor
1igh concentrationmore molecules are packed in one volume
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!ffect of chemical interaction
eiation from linearity may caused 5y
C issociation of analytes
C =ssociation of analytes
C 6hemical reactions ,ith solent to produce a
product hain" different a5sorption spectrum from
the analyte