The design and construction of a photoelectric spectrophotometer for analytical research

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The design and construction of a photoelectric spectrophotometer for analytical research

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THE DESIGN AND CONSTRUCTION Of I PHOTOELECTRIC SPHJTROHIOTOMETER FOR ANALYTICAL llSIISet

W

A thesis Submitted to the Graduate Faculty

fo r th e S@p*s# o f DOCTOR OF PHILOSOPHY Major Subject t Analytical. 0HMl*tsy

B

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4 4 'a _ T ^c a .« ^ ~ I) \ © L O 3© 5H

I m

State College

1942

R eproduced with perm ission o f the copyright owner. Further reproduction prohibited w ith o u t perm ission.

U M I N u m b e r: D P 1 2 1 0 6

IN F O R M A T IO N TO U SER S

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UMI M icroform D P 12106 C o pyrigh t 2005 by P roQ uest Inform ation and Learning C om pany. A ll rights reserved. T his m icroform edition is protected a g ainst u nauth orized copying u n d e r Title 17, U nited S tates Code.

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tfeaaa aatltoAa fr© « the p o in t af view ©f th e ir appli**

©ability in any but the most rig o r« « s iy jrt«atA«f*isnA taafetttea* The eritioal eratafttM at eolortiaetrle W itte *! Isas been pioneered by H* $* umilmt til) «aft M # Aevaffcosw.* ■ana at ib# present time* there «*» avallalDLa reliable la ta . aaaa«nil«ig a number ©f tbs amat widely m*#t oolorlmetrle aethoA** fllanont wait mm®g%so the photo* ##11.# sat oensogitontto tto tuto whloh they nontno&loA, so that &mt®aatl# toloaoing of toe ©irooit was obtain**#

fh# olllptloOl

»ipp#pg nontlonnA n m m ©«mstr«©t#t fro® atoning* sat w#r# to® otopo of portions of. to# «ftlip«oof owth having n w n m at tho oontor of to# galvanometer alrpor

foono

«n& to# other foono

at #®«h pfeotoooll* ■ fit® to® nftswero w m m |#1»#€ .half way tostotta the too ptotooolto*

fhm» shy toon of light two* to®

taiomonetor striking to# mirror# on# ooflootoft to ©litter on#

op too other of to® ptotoo«&.to* to® paper ownrlogo on to# *o*o»4»r woo flat its tfoowlog in wsy®. pooponAiooior to to® travel litf tor*

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to# paper oorrioge wa« Join©! to to®

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» m ** «•*** of %®mm at p**«*

optioul systeo ©I the vtoualy dssorilnA*

St# traveling oarrlagO'Myittig the ■elegiposwtgiitt «&*o ita« w w tA e» i t

iw -ll» m m m m k m resistor* ant hm&

pmmi.®lm for holding *■ tomtomIft pon of tt» stylus variety* This ante s. tsoo&itg m the *otetei»g pops? of any m m m of I M s tevf&ng* sa& #«*«§#. tep&ot' tipeetay the va#i*tldft« in. ■the positlm of the teffisgs utth the » f t length getting*

B*

«jf tint

ffes sain flisten* gwlteti of the amplifier was tew*#* e». and the M o w pom&tte# to mmm. far five aimitos* of that time, the ttosotriog

A t the end

wm get at so*** «nA the

tettoote potentiometer fop the mmmwrnm : *i#e of the amplifier wm m adjusted with the eoarse ant fine resistors that the galvanometer deflection wm zero,

S i t wag observed by turn-

tag oo the galvanometer lump «t. opeiktag. the trap ten*

of the amplifier box Kftfctag the %%&& % » » visible*

ok

tap

Sis

fpegesi pot * « P # $*te*ti«& & m m m m the eoapeasating resistor.

S e n the i»ea«ip§.iig oooiotor *** set at 100 «tt the

$roess« repeated for ffee oilier half of the amplifier, thus pttftiag « sere potemflal top' onrooo the measuring restates?* Most, with the taste sotting of the Ktasortag resistor, the light in the KOKMlnPOMttep «te turned •lit opoteA to the desired vnl®«*

o k *.

&»#. S t exit

ftsea the ooKpeftMttag

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tlmi lit© tulit* €li snot quit* jars wkp»

fill* netting m % M b i t tsr noting 'th* point at- wtiiiiii:

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Apparent value

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4 9 8 .3

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4 7 1 .3

4 7 0 .8

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4 4 7 .1

4 4 6 .3

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fbo soxt step i» the evaluation of the instrument was the AotoYKinatloit of the aaaeuat of stray light. esergiiig f r m ftoooofavoBator*

the

B trm light Is the light of w r * lengths other

than the®# desire#. It 1# dotova&aoA W Obtaining transmitto&flgr values at vaviouo umvo length# for Materials of which

the t*oiM«lttfi&oioo are feaooii* la this cast too glass filter* which hat boon- ««&&brat*4 by tbo lurecu of Stwistri*,, Ho#*, ever, wton an attoapt to use the opootvepbotoaetor for tfeto purpose wag aafio* it was fiaunt that the erratic behavior of tb* amplifier mat# the results of no value, sine* they were

not reproducible-. The two aoot noticeable difficulties were a raaios variation in the galvaaonotor deflection, which was aoitbe? oonatoat nor irreducible, tut# a slow bat stemAy drift,

which va* always in m e 4i*o*tl«n»

the amplifier was turned

on for a. period of time of twelve hours and at the end. of that

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«*

30



time the drift was as pronounced as it .had been five s i w t « * after the initial weane-up period. slips

mf

Since the symmetrical d#»

the amplifier was intended to. eliminate the tendency

to drift, various parte in the amplifier including the tubes and batteries, 'were latttrtfifcttg«6*

*hie produced

wm

correction,

however.

In order to obtain the transmittaney values for the Stereatt of i t i M l M M fiiter%, it wmm finally w t m $ m a w *®

«ee of a

Weston Type 2 barrier layer cell, wl ich was placed in the posi*

lion of. the flickering' mirror, this being directly behind the exit slit of the monochromator,

this sell was connected dl»

reotly'to the galvanometer previously described, -and the

Wm

flections of the galvanometer wire read on a scale at a Aistsno# of three meters.

For each reading of traasmittanoy, the wave

length scale was adjusted, the slit* opened i® the desired value, and the initial reading: made with an cpaspie object in front of the entrance slit.

This gave the •dark* reading:,

which wm subtracted fro® -all subsequent resting#*

the opaque

object was then removed and the incident light value obtained as a galvsastteter deflection.

Since no constant voltage device

was available from which to operate the light source, an. «*«*« eg# of three readings was taken at each setting of the wave

length seal®.

Warn this average ■value wne obtained, the

filter

ist. a suitable holder was placed in front of the entrance slit, and again an average .reading was taken*,

the second of these

average value# was divided by the first and the rati# multiplied

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*** m ** fey 100*

this gave the p « o«n% t r m m t t t m m for

1» fable g are given the observe! and tame telnet for the treaaelttaiiegr of tee glaee flit®#® obtain.#! from the Buremi ©f gtaftdarda*

fufel® ?♦

crasm® ms suit faiiis ran

or m

m s

Fanis

Wmkiilii*a # of lilt fcitte-filter .1fe« 888*48. : red filter 11©, 0631 Wave length »##*¥#! ' ■ 'rite "ISK®eeii In m;u. .m r.m m t'. » r #s*rt ner eent ©er ©eat. ;

404*? 480.0 438.8 471.3 491.6 601.6 620.0 630.0 848.1 860.0 870.0 878*0 887.6 600.0 620.0 640.0 880,0 667.0 680,0 600.0

77.6 77.8 77.0 60*7 36.8 27.6 10,7 6.4 8,6 7.9

88*06 80.80 81.90 64,40 37.70 28.10 11.00 6.09 4.77 8.80

2.9 1,1 1.3 1.6 0.7 2.2 6.4 22.8 36.0

3.96 1*38 1*80 1.59 1.21 2.40 4.70 16,00 38.00

o.oc

0.00

0*00

0,00

*38 3*70 25.80 88*80 87*80 88.30 88*00

.03 0.45 17.20 69.00 ' 83.50 90.80 91,1C

88,00

91*88

tt##® volttoo when 'plotted in the ffeniller m ore length rareue tmaalttasiey fojne an #Mwa in Figure 10* they repw* e*nt & »@«i«§a rare length tend of 10 millimicrons? actually a aeseetiat larger tend end need atnee the exit edit was opened 'to

4 -wu while the entranee slit laetrwaeet was egeal to M B

mm

f as*

Iti# tlsptwl* «f the

ws* per aillittlereit, eo that the

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total silt wi#fch was aqaiffalaiit to'.o apaatoal twit of arl&th X4*S a&ll&alaroiis. .This is baoauaa ill® total slit witth is a 2. «6-