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Theses

Thesis/Dissertation Collections

1-1-1988

Optimizing tone production on a 300 spot per inch

laser printer

James R. Hamilton

Follow this and additional works at:

http://scholarworks.rit.edu/theses

This Thesis is brought to you for free and open access by the Thesis/Dissertation Collections at RIT Scholar Works. It has been accepted for inclusion in Theses by an authorized administrator of RIT Scholar Works. For more information, please contactritscholarworks@rit.edu.

Recommended Citation

(2)

by

James R. Hamilton

Athesissubmittedinpartialfulfillmentofthe

requirements forthedegreeofMasterofScience inthe

Schoolof

Printing

andManagementSciences intheCollegeofGraphic Arts and

Photography

oftheRochesterInstituteof

Technology

January,

1988
(3)

School of Printing and Management Sciences

Rochester Institute of Technology

Rochester, New York

CERTIFICATE OF APPROVAL

MASTER'S lHESIS

This is to certify that the Master's Thesis of

James

R.

Hamilton

With a major in Printing Technology

has been approved by the Thesis Committee as

satisfactory for the thesis requirement for the

Master of Science

degree

at the convocation of

January, 1988

Thesis Committee:

Frank Cost

--~~---')=Th::re-s"""'is-A"""""-:-dv--;i"-so-r---Joseph

L. Noga

Graduate

Pro~am Coor~ator

Miles Southworth

(4)

OPTIMIZING TONE PRODUCTION

ON A 300 DOT PER INCH LASER PRINTER

I, James R. Hamilton, hereby grant permission to the Wallace Memorial Library, of

R.I.T, to reproduce my thesis in whole or in part. Any reproduction will not be for

commercial use or profit.

(5)

Iwouldliketo thank the

following

people:

Prof. Frank

Cost,

whoseinsightandinterest inspiredthisproject

Dr.JosephDeLorenzoandProf. Michael Kleper for

lending

theirexpertisetothis

undertaking

RochesterInstituteof

Technology

professorsJoseph

Brown,

Robert

Chung,

Marie

Freckleton,

C.R.Meyers,

Joseph

Noga,

Michael

Peres,

Bob TompkinsaswellasDavid CohnoftheT&ECenterwho allhelpedinnumerous stages oftheproject

Mark

Curby

andIshmael J. Stevanov-WagneroftheEaton

Peabody

Laboratory

for

answerstotechnicalquestions aboutlaser printing

Betty

GreenawaltandPamelaOriansofBoise

Cascade,

andJohnGorskiand

Judy

Palucki

ofHammermillfor arrangingpaperdonations

Lisa DigginsofData

Recording

Systemsfor providingtranscriptsofDavidSpencer'stalks

Greg

Haddam,

whoseunderstandingoftheMacintosh greatlyaidedthisproject
(6)

List ofTables v

ListofFigures vi

Abstract 1

ChapterOne 1

Introduction 1

Footnotes forChapter One 6

Chapter Two 7

Theoretical Basis 7

TheLaser Printer 8

PostScript 9

Footnotes for ChapterTwo 10

Chapter Three 11

Review oftheLiterature 11

Footnotes forChapter Three 13

ChapterFour 14

Hypothesis 14

ChapterFive 16

Methodology

16

TheDevelopmentoftheTests 16

Density

Measurements 21

Testing

oftheDensitometer 21

Testing

oftheLaser Printer 22

Comparing

theStandard Deviations 23

Microscopic Studies 23

Footnotes for ChapterFive 24

Chapter Six 25

Results 25

Tone Production 25

Microscopic Studies 26

PaperTests 29

Maximum

Density

Tests 29

Gray

Production Tests 30
(7)

PaperTests 33

Chapter 8 50

Discussion 50

ToneProduction 50

MicroscopicStudies 52

PaperTests 53

Maximum

Density

53

Gray

Production 54

Chapter 9 56

Summary

56

Conclusions 56

Recommendations for Further

Study

57

EquipmentUse 57

Bibliography

59

Appendices 62

A Tone Production Data 63

Condensed 63

Diamond 67

Open 70

B

-Paper Tests 74

Density

-Part One 75

Maximum

Density

- Part Two

. . . . 76

Gray

Production 77

Grading

Grays 78

C

-Consistency

Tests 79

LaserWriter 80

Densitometer 83

D- BartlesonandBreneman 84

E- Spot Sequence 88

Condensed Dot Form Sequence 89

Diamond Dot Form Sequence 90

Open Dot Form Sequence 91

F - Sample Output- 3x3 Condensed 92

3x3 Condensed 93

(8)

Pagenumber

Table 1 - Matrix

size,number of grays possible andlinescreenat300spotsperinch. ..11

Table 2

-Summary

of spots in matrix, gray

level, linescreen,

and screen angle 20

Table 3 - Comparison

oftestsquareswith 50% spots on 26

Table 4 Dot size measurements 27

Table5

-Testing

the accuracy ofthemicroscopic measurements 28

Table 6 Results ofthe firstpapertest 29

Table 7

-Results ofthe second papertest 29

Table 8 - Results

ofthethirdpapertest 30

Table 9 - Overview

of paper characteristics 31

Table 10

-50%spots onwithinformation concerning areabetweenspots 51

Table 1 1

(9)

Pagenumber Figure 1 - 3x3

matrix of squares 3

Figure 2 - Grays

possibleversus linescreen at300 spots perinch 11 Figure 3-

Comparison

of4x4open and condensed matriceswith eight spots on 14 Figure 4 - 3x3

open matrix 18

Figure 5 - 3x3

condensed matrix 18

Figure 6 - 13

spotdiamond matrix 19

Figure 7 - Spot

sequence in 13 spotdiamond matrix 20

Figure 8 - Irregular

nature ofthe dot 27

Figure 9

Illustrating

dotsize 28

Figure 10 Graph of

2x2, 3x3, 4x4,

and 6x6open matrices 35 Figure 1 1 - Graphof

2x2, 3x3, 4x4,

and 6x6condensed matrices 36 Figure 12 - Graph

of

5,

8, 12,

and24 diamondmatrices 37

Figure 13 - Graph of matrices

containing 25 spots 38

Figure 14- Graphof open and condensed 8x8matrices (withcolumn

breaks)

39

Figure 15 Graphofidealtonal scale versus 8x8condensed matrix 40 Figure 16 - Microphotoofparallel lines atfinestresolution 41

Figure 17 Microphoto of1/25 5x5 open matrix 42

Figure 18 - Microphoto of6/25 5x5 open matrix

43

Figure 19

-Microphotoof 12/25 5x5 openmatrix 44

Figure 20 - Microphotoof 13/25 5x5 openmatrix 45

Figure 21 Microphotoof 18/25 5x5 open matrix 46

Figure 22 - Microphotoof24/25 5x5 openmatrix 47

Figure23 - Microphotoof 12/25 5x5 condensed matri 48

Figure 24 - Microphotoof 12/25 25 diamond matrix 49

(10)

Digitalhalftonesas output on plain paper arethefocusofthisstudy. Anew

terminology

issuggestedtoallow properdescriptionofdigital halftones. Themost importantofthese termsistheuse of

"addressability"

toreplacetheoften misusedterm "resolution."

Also important istheuseoftheterm"spot" ratherthan"dot" todescribe addressability. Ameans ofproperly

describing

digitalhalftonesissuggestedtoavoid confusion withanalog

(ie.,

conventionalphotographic)halftones.

Halftonepatterns were createdto test theefficiencyofdifferent designsat300spot perinch addressabilityon alaserprinter.Thepagedescription language PostScriptwas usedtocreatethehalftonepatternswhichweremodeled onthreebasic designs.

Ithasbeenestablishedthat twohalftone dotpatternsconstructed onthesamematrix andcontainingthesame number of spots will producedifferent densities ifthe

configuration ofthespotswithinthematrixisdifferent This has beentested

by

comparing theresults ofthe toneproductioncurves ofthecondensedand openhalftone dot designs. Thesepatterns were output on alaserprinterand measuredfor density. Toneproduction curves weredrawnand compared.Eventhougheachmatrix containsthesame numberof spots,it hasbeenshownthatdifferent densitiesresult.This is solelya consequence ofthe dotdesign.

Microscopicstudies wereconductedtoillustratethenature ofthefilling-in inthe non-image area.Microscopicmeasurements werealso madetoascertainthesize of an individualspotatvarious screen rulings. Itwasfoundthat thespot,whichwasvery irregulartobeginwith,actually begantobreak upasthelinescreenapproached150 lines perinch.

Papertestswere runtogaugethemaximum

density

andthe toneproduction capabilities ofvarious papers.Although theresults were

inconclusive,

they

point out anotherflawofdigital halftoneswhichareoutputon plain paper.Thenumber of grays predictable,givenamatrixsize,isgreaterthanwhatisachievableinpractice.
(11)
(12)

INTRODUCTION

Theideaofcombiningtextandillustrationswithout

having

tocut and pasteisa conceptthathas intriguedtheauthor sincehis daysas a mechanical artist.

However,

tobe

abletoachievethis goal,both digitaltypeandhalftonesare necessary.Inaddition,a "type-"

or"image-"setterisrequiredthatcan receive and createbothtypesof output

Devicesandtechniqueshave been developedthatcan now achievethesegoals, and what's

more,since

they

output onplainpaper,

they

mayevenleadto theelimination offilmas a

step intheproduction process.This study investigates digital halftonesandthewaythese

halftones are output onplainpaper. Suggestionsare madetooptimizethedesignanduse

ofdigital halftones.

Consistency

interminology isstrivedforthroughoutthisproject Someoftheterms

thatare usedrepeatedlyare:

addressability

-the

frequency

withwhichthelasermarks thephotoconductive surface

dot- theone or more spotsusedtoformthebasicunit of ahalftonepattern

halftone

-atechniqueusedtosimulate continuoustoneimages ina processthatcan

onlyprint or not print at all

latent image- animagethatis

present,butnot yet visible

(ie.,

beforeapplicationof

toner)

linescreen- alsoknownaslineruling; themeasure ofthedistance between halftone

dots inahalftone

linesperinch- thetermusedtodescribethelinescreenof ahalftone

matrix- a

groupingof spots

photoconductivity- the

propertyofconductingelectricityuponexposuretolight

(13)

orsharpness

spot

-thesmallest mark alaserprinter can make on paper spots perinch- theterm

usedtodescribe addressability

Toconduct adiscussionoftheissuesinthisthesis, it isoftheutmostimportanceto

maintainconsistencyinterminology. Thereare a number ofmisleading terms which,

poorly

defined,

haveresultedinmuch confusion.Oneofthemostimportantoftheseterms

is"resolution."

Resolutionisoften

incorrectly

describedintermsofthenumber of marks that thelasercan makein creatinganinchoflatent image. Thislatent

image, however,

is subsequentlytonedandtransferredtopaper, andany degradationoftheimagethatoccurs

inthis processisunaccountedfor. Sincethisdegradationtends tobemuchlargerthanina

photographicprocess,itmakestheuseofthe term"resolution" quite misleading. Ifa number valueistobeassigned,the term"addressability" ismore accurate.

Addressability

isthecapabilityofthelasertomark alatent imageonthephotoconductive surface.This canbedescribedmoreaccurately numericallythanresolution sincethereisnodegradation

oftheimagetoaccountfor.

Keep

inmindthataddressability describesthelatentimage

whereas resolutiondescribestheimageonpaper.

Unfortunately,

"resolution" isthe term thatismostcommonly usedtodescribethe

imaging

capabilityof aprinter, andit isoften

described intermsof "dotsper

inch",

anotherconfusingterm.Printersare accustomedto

theterm"linesperinch" todescribehalftonescreens.

However,

300"dotsperinch" and

300"linesperinch"donotmeanthesamething.Inhalftones a300lineperinch linescreen wouldbeof extremefineness. 300 dotsperinchontheother

hand,

producesimagesthat

arerelativelycrude

(keep

inmindthat72dotsperinchis dotmatrix printerqualitywhile

1000dotsperinch isthe

beginning

oftypesetquality.) Theword"dot" alsoisassociated withhalftonescreens,as in "halftone

dot."

Thepotentialforconfusionis

limidess,

and

solelya result of

faulty

terminology.

Tounderstandthisproblemitisnecessary tohavea generalunderstandingofthe nature ofhalftones.

They

existtoproduceanillusionofgrayness ina processthatcanonly printblackornot print at all.Halftonescanbe describedas

being

analogordigital. In

using theterm

"analog

halftone"

(14)

the dots inch. Confused?Youhavea reasontobeconfused sincetheword "dot"

hastwomeanings withinthelastsentence.First it isusedas"halftonedot" which

may vary insize,andthenit isused as"dot" in dotsperinchwhereitmeanstheminimum markablespot(a constant)inalaserprintingsystem.

Toalleviate some oftheconfusionbetween digitalandanalog

halftones,

itwillbe

necessarytorevise some commonly-used vocabulary. Theterm"addressability" shouldbe

usedwhennumerically

describing

thecapabilities of a plainpaperprinter.

"Addressability"

and"resolution"which arevirtually identical inreferencetophotographic processes arein

factquitedifferentwhen usedtodescribeplain paper processes.

Furthermore,

"spotsper inch,"

not"dotsperinch," shouldbethe termusedfor

describing

addressability.Theword "dot"

simply hastoomanyother connotations."Spotsperinch" willbethe termusedto

describe addressability fortherest ofthisstudy. "Linesperinch" shouldbeusedsolely for

describing

halftones.

Analog

halftonesareadequately described

by

thetermlinesper

inch;

however,

digital halftonesrequirefurtherexplanation.

Abasic descriptionofadigital halftonewill

help

illustratethepointFigure 1

illustratesa3x3matrixof squares:

X

m

X

X

X

X

X

X

X

Figure 1 - 3x3matrixof squares

Using

this tobuildadigital

halftone,

black,

whiteand eight shades ofgraycanbe
(15)

shades ofgraythantheexample above. In

fact

it'slaughableto

try

and comparethem. Yet ifthedigital screenisdescribed as a100 linescreen,theimmediateassumptionisthatit is

equivalenttoa100lineanaloghalftone.

Therefore,

toadequatelydescribeadigital

halftone,

itisnecessarytostate notonlythelinescreenbutalsotheaddressabilityofthe

outputdevice.

So,

where 100 lines perinch

justly

describesananalog

halftone,

100lines perinchat300spots perinchwould

justly

describeadigital halftone.

This bringsupanother point.Oneofthecharacteristicsthatcanmakeanalog

halftonessuperiortodigitalhalftones isthat

they

are outputonphotographicpaperwhich,

ofcourse,hasgreatsensitivitytoverysubtiedifferences. Whenphotographicpaperis

usedtocapturedigital

halftones,

much moredetailcanbe heldthanifthesamehalftone were outputon plainpaper.Thus ifadigital halftonewereoutput onbothplainand photographicpaper,much moredetailwouldbe heldonthephotographic paper. This seems quite obvious.Butitisalsotrue thataslaserprinters gainhigherandhigher addressabilities(intermsofspotsper

inch),

themain

limiting

factorwillbethepaper,not thenumberof spots perinch.

Theuse ofdigitalhalftones is goingto

increase,

and as aresult,the"look"of

halftoneswillchange.Digitalhalftonesthatarecreatedforoutput ondotmatrix orlaser

printersalreadystart out at a markeddisadvantagetoanalog halftones:

they

simply fall far short ofphotographic resolution.Even digitalhalftonesthatare output onlasertypesetters havelowerresolutionas comparedtoanalog halftones.There is a simple explanationfor

this: thesmallestmarkalaserphototypesettercan createislimited

by

thesizeofthelaser

spotwhile,on theother

hand,

lighton photographicfilmorpaperis limited only

by

the grainsize ofsilverhalidewhichismuchsmallerthan laserspot size(silverhalidecrystals

rangefrom0.05 to2

microns1

whilelaserspot size at300spots perinchis around85

microns.2)Thereisanother complication: thesmallerthelaserspotsize, thelargerthe amount ofinformationtobeencoded,and, thelargerthe amount of

information,

thelarger thecost andtimeinvolved. Forexample, at300spotsper

inch,

90,000

(300x300)

bitsof informationareneededtoencodea squareinchofimage. At 1000spotsper

inch,

1,000,000

(1000x1000)

bits arerequired. Thusthereis atradeoffbetweencost and
(16)

addition, there for using digital halftones.

Among

advantages are ease ofdata transmission,electronic storage of

images,

and electronicdata manipulation.

Itshouldbestressedthatalloftheexperimentationinthis studywasdoneona

singleAppleLaserWriter. The limitedscope oftheexperimentswillgive someinsight into

thestrengths and weaknesses oflaserprinting;

however,

these tests are notintendedtobe

usedtodrawconclusions about the capabilities ofanymanufacturer'sproduct.Thereis

simplynotenoughdatatosupportthose sorts of claims.Thisisalsotrueofthetestsonthe

X-Rite densitometerandtheHammermillandBoise Cascadepapers. Thesetestshave been

(17)

JMcGraw

Hill EncyclopediaofScienceandTechnology. 6thed.S. v.

"Photography,"

by

Vivian K. WalworthandRobert D.

Anwyl,

p.405.

2Author's

calculation:

1/300"

(18)

THEORETICAL BASIS

In 1937Chester Carlson inventedthefirstelectrostatic process (latercalled xerography.)1

Thiswas thebirthof part of the

technology

forthelaserprinter.Patents

wereissuedin 1942and

1944,

and

by

1950Xeroxhadthefirstcommercial copieronthe market.The Xerox 914office copier was introducedin

1960,

and sincethen,electrostatic copiershavebecomeanintegralpart ofAmericanbusiness life. Inthelate

1950's,

Dr. CharlesTownesandDr. Arthur Schawlow laidthefoundations fortheconstructionforthe

firstlaser.2

The firstworking laserwas constructed

by

Dr. Therodore Maiman in I960.3 The laserhas broadenedtheapplication ofthecopier.The devicecan nowbeusedas an

imagesetter/typesetter. Aprime exampleofthisistheApple LaserWriter.The LaserWriter ismorethanalaserprinter;it isacomputing devicewith 1.5megabytes ofrandomaccess memory.Ithasbeen describedasthemostpowerfulcomputerthatApplemakes.4

And

yeteven withthatamount ofmemorytheLaserWriteris limitedtoanaddressabilityof300

spots perinch. This makesitan excellent choicefor business applications,butsubstandard

forthegraphicarts (where 1000spotsperinchis arguablythe standard.)Larger

addressabilityrequires morememory,butthishasnot preventedtherecentintroductionof 400and600spot perinchprinters.Ofcourse,laserphototypesettershave beenused with

great success ataddressabilities of muchhigherthan300spotsperinch

but,

forthemost part,thesesystems usephotographicpaper.5Companiesare anxioustoperfect a plain

papersystemdueto thehighexpense ofphotographicpaper.

Oneofthemost

interesting

developmentshas beenthatofthepagedescription

language PostScript.

Previously,

each

typesetting

manufacturerhaditsowncoding

language fortheirmachinery.Acomputerfile forone manufacturer'stypesetterwouldbe

useless onanother's.

However,

through theuse of

PostScript,

a single computerfilecan berun on anumberofdifferentoutputdevices attheresolutionofthatoutputdevice. This

is what

is

knownas deviceindependence.

PostScript,

thoughnottheonlypagedescription
(19)

Sincethelaserprinter and pagedescription languageare ofimportancetothis

project,

they

willbe discussedinthe

following

sections.

The Laser Printer

Tounderstand whatthelaserprinterdoestoproduce an

image,

it is necessaryto

haveanunderstandingoftheelectrostatic process.Inthis

discussion,

theelectrostatic

process(ormorespecifically,transferxerography)willbe describedas atoner-based

system.Theelectrostaticprocess,as usedinconventionalphotocopiers,isrelatively

simple.Adrumor

belt,

often constructed ofselenium,is charged.This surfaceisa

photoconductor whichloses itscharge when exposedtolight. When oppositelycharged

tonerparticles arebroughtincontact withthesurfaceofthe

drum,

they

adhereto the

charged areas

(ie.,

theareasthathavenotbeenstruck

by

light.)

Inthenextstep,a pieceof

paperisbrought incontactwiththedrumatthesametimethata chargeisappliedto the

backside ofthepaper,removingthetonerfromthedrumandpassingitto thepaper. The

toneristhenfusedto thepaper,completingtheprocess.7

Considerfora moment a conventional copier.Toobtain acopy,light isreflectedoff

theimagethatis

being

reproduced.Where light fromthenon-image area reflects ontothe

surface ofthe

drum,

thechargewillbe

lost,

andthereforenotonerwillbeattracted.The

reverseistrueintheimagearea;nolightreflectsfromtheblackoftheimageandtherefore

thedrumstays charged and attractstoner.Inalaserprinter,whereyouare notworking

fromreflectioncopy,thelasercanbeused eithertoerasethenon-image areaintheway

thatlight does in theconventionalcopier,oritcanbeusedtocreate animagearea.Ifthe

laseris usedtoerasethenon-imageareaitisknownaswhitewriting;if itcreatestheimage

areait isknownasblackwriting.The

image-creating

part of alaserprinteriscalledthe

"engine."

The CanonengineintheApple LaserWriterusedforthisexperimentis

blackwriting.8

The laser inalaserprinteriscontrolled

by

a polygon-shaped mirrorthat

aimsthelaser beamatthedrum.Thepathofthebeamishorizontalacrossthedrum

surface.The drum in theLaserWriterischargedandthechargesdissipatewhenstruck

by

thelaser. It becomesclearatthispointthatiftoneristhenattractedto thechargedareas, a

negativeimagewillresult

However,

sincethetonerhas thesame charge asthecharged

areas ofthe

drum,

tonerwillonlygotonon-chargedareas

(ie.,

wherethelaser has struck.)

Thusthe tonersystemsare quitedifferent betweenblack- and whitewriters.

(20)

creating finehalftonea similar problem arises.The halftone

dotscreateslittleislandsoflike-chargethatbegintoaffect each other asthelinescreen

increases.

PostScript

In

1982,

ChuckGeschkeandJohn WarnockformedAdobe

Systems,

Inc. Their product

PostScript

isdescribedas "aprogramming language designedtoconvey a descriptionofvirtually anydesiredpagetoaprinter."9

PostScript's syntax resembles the

programminglanguage

Forth,

butthereare also similaritiestoLisp10. The PostScript imageoperator was usedexclusively forthisproject Adescriptionofhow itwasusedis

containedinthe

Methodology

section,page 16. Forthepurposes ofthisproject,
(21)

FOOTNOTES

FORCHAPTER TWO

-J.J.RheinfrankandL.E.

Walkup,

"Current Status ofElectrostaticReproduction Processes,"

1961 TAGA Proceedings.TechnicalAssociationoftheGraphic

Arts,

Rochester,

NewYork: n.p.,

1961,

p.114.

2Allen

Maurer,

Lasers - Light Wave

oftheFuture. NewYork: Arco

Publishing, Inc.,

1982,

p.2.

-Ibid., p.39.

4Bruce

Blumberg,

"Page Printersfor LowCost ElectronicPublishing,"

The Fourth

National Print

Quality

Seminar.

Newtonville,

Massachusetts:Datek Information

Services,

Inc., 1985,

p.237.

5One

exceptionistheTegraGenesissystemwhichclaimsaddressabilityof1012spotsper

horizontal inchon plainpaper,Tegrapromotional material.

6"...PostScript

hasnow emerged as'the'pagedescriptionlanguage. Atthemoment,

AdobeSystems isalmostinamonopoly

position."

TheSeyboldReporton

Publishing

Systems."Competitors for AdobeSystems," 16

(May

11,

1987): 49.

Encyclopedia

ofPhysicalScienceandTechnology. 1987ed.S. v."Photographic

Materialsand

Processes,"

by

P.S.

Vincent,

pp.484-494.

8Personal

letterfrom Mark

Curby

andIshmael Stevanov-Wagner.

9Adobe

Systems, Inc.,

PostScript Language Tutorial andCookbook.

Reading,

Mass.:

Addison

Wesley Publishing

Co.

Inc., 1985,

p. 1.

10Adobe

Systems, Inc.,

PostScript LanguageReferenceManual.

Reading,

Mass.:
(22)

CHAPTER THREE

REVIEWOFTHE LITERATURE

In an articleinthe

February

16,

1987 Seybold Reporton

Publishing

Systems1,

David R.

Spencer,

chairmanofData

Recording

Systems,

uses a charttoillustratea point

aboutthe tradeoffsbetweenshades ofgrayandthefinenessoflinescreens. Theresultsfor 300spots perinchare summarizedin Table 1 and shown graphically in Figure 2.

Table 1 - Matrix

size,number of grays possibleandlinescreenat300spotsperinch

MatrixSize 2x2 3x3 4x4 5x5 6x6 8x8 10x10

GraysPossible* 5 10 17 26 37 65 101

Linescreen 150 100 75 60 50 37.5 30

?this isatheoreticalcalculationofgrays,

including

blackandwhite

Grays

100-75

-50

-25

-Grays

Possible

vs. Linescreen

at 300 spi

I

90

T

T

n

r

30 60 90 120 150

Linescreen in lines perinch

(23)

Figure2showsthat thelargerthenumber of graysproducible, thefewerthelines in

thelinescreen. Spencergoes ontosaythatat300spots per

inch,

therejust isnota

satisfying tradeoff; hiscutoffis thepoint at which64shades ofgrayareachievable, and thelinescreenis atleast65linesperinch.In

fact,

thiscombination offactors isnot possible untiltheaddressabilityreaches600spots perinch. StephenRoth2 ,inthe

May

1987issueofPersonal

Publishing

magazine,makes a similar statement aboutthenumber

of grays producible. Bothauthors haveassumedthat theseprojections arein facttrue.

Whilethelinescreen informationisaccurate, thenumber of grays achievableis debatable

(refertodiscussionongrayproductioninthepapertests,page

54.)

Itisthis

discrepancy

betweenwhatiscalculable and whathappensinreality thatprovidedtheimpetus forthis thesis.

A goodunderstandingofdigital

halftoning

isimportantto thisstudy. Some

referencesthatarehelpfulareJarviset al

(1976),

StoffelandMoreland

(1981),

and

AnastassiouandPennington(1982).Morerecently,GoertzelandThompsonofIBM

(1987),

havewrittenaboutdigital halftonesontheIBM4250printer.David Spencer

(1985, 1987)

andAmnon Goldstein

(1985),

bothofData

Recording Systems, Inc.,

have

bothpublishedthought-provokingarticlesontheissues

involving

printqualityoflaser

printers.Dr. William White hasalsowritten

lucidly

ontonersand resolutions(ofparticular

notearethemicrophotographs.)His

book,

Laser Printing: The

Fundamentals,

has good

basic informationonlaserprinters.

For informationon

PostScript,

thebooks

by

Adobe Systems Inc. formedthe

startingpointforthe programmingnecessarytobuildthetestpatterns.PostScripthas been

thefocusof quite alotofinterestrecently,seeDennis Pelli'scontributionto the

Berkeley

Macintosh Users

Group

Newsletter,

Fall

1986,

pp.35-44.For informationabout

numerouspagedescription languagesseetheApril

14,

1986issueoftheSeybold Report

on

Publishing

Systems.

ForinformationonBartlesonandBreneman'sdarknessvalues, referto their

originalarticle

(1967),

andalsothoseofArcher

(1978)

andR. E. Maurer (1982). In

addition,anunpublishedhandout

by

Prof. Robert

Chung

ofRITwas instrumentalin
(24)

FOOTNOTESFORCHAPTER THREE

!David

R.

Spencer,

"OutputTechnologiesandHigh

Resolution,"

The Seybold Reporton

Publishing. 16

(February

16 1987):p.5.
(25)

CHAPTERFOUR

HYPOTHESIS

Thehypothesisofthisproject canbestated asfollows:

Twohalftonedotpatterns constructed onthesame matrix andcontainingthesamenumber

of spots will producedifferent densitiesiftheconfiguration ofthespotswithinthematrix

is different

Togive anexample, a4x4condensed matrixcontainingeight spotswillproduce a

different

density

than a4x4open matrixcontainingeight spots (see Figure3).

Open

Condensed

Figure 3 - Comparisonof4x4openand condensedmatriceswitheight spots on

The 4x4open matrixcontainingeight spotswillproduceadarker

density

becauseofthe

tendency

oftonertofill inthenon-image area.Whatisofimportance here isthatjudicious

designof matrices canbeusedtocontroltoneproduction.

This hypothesiswillbetested

by

comparingtheresults of condensed versus open dot forms. Thenature ofnon-square matrices willbetestedwith thediamond dot forms. Theeffect ofpaper ontheseprocesses willalsobetested.

Firstand

foremost,

it istheintentofthisprojecttoshowthatwhatmight appearto beachievablewiththelaserprinterisnot always whathappens inpractice.Theconfusion

between300spotsperinchaddressabilityand300spots perinchresolutionis an example

(26)

mathematicallypossible,but

they

havenottested theactual outputItis theauthor'sbelief

thatfewergrays areactuallypossiblethanSpencerandRothestimate.

Testing

how many

gray levelscanbeproduced wouldbeathesisin

itself,

butitwillbeaddressedinsome
(27)

CHAPTER FIVE

METHODOLOGY

Abasic method was usedforallthe

testing

inthisproject.

First

aPostScript file wascreatedthat,when output onthelaserprinter,would resultinahalftonetestpattern. Thesetestpatternsweremeasured

by

densitometerandtheresults recorded.Inthis

section, thenature ofthecreation ofthe testswillbe

discussed,

aswellastests toascertain

thevariationinthedensitometerandthelaserprinter.

Finally,

thetechniquesusedforthe

microphotographyand microscopic measurementswillbe discussed.

TheDevelopmentoftheTests

The

feasibility

ofthisprojecthingedonthecreationofthevarioustestpatterns.

Prof. FrankCostsuggestedthat thesepatterns couldbecreated on anApple Macintosh personal computerusingthepagedescription language PostScript Continuedresearch

revealedthatthe"imageoperator"

described inthePostScript CookbookandTutorial1

alongwiththesoftware programsJustTextandSendPostScriptwould allowthecreation of theprogramsandtheir transferto theLaserWriter.Thecreationoftheindividualpatterns wastime-consuming.

First,

thedotpatternhadtobe broken downintoa series oflaser spotsthatcouldberepeatedtoproducetheactualdot.Thisseriesthenhadtobetranslated

intoahexidecimalformat foruseintheimageoperator.

Finally,

thehexidecimalnumbers wereinputontheMacintoshand proofedontheLaserWritertoensurethat thecorrectdot

pattern was produced.

Aportionofatypicalprogramlooks likethis:

150 650translate 69 69scale

288288 1 [288 0 0288

00]

(28)

B6DBB6DBB6DBB6DBB6DBB6DBB6DBB6DBB6DB

B6DBB6DBB6DBB6DBB6DBB6DBB6DBB6DBB6DB

FFFFFFFFFFFFFFFFFFFFFFFFFFFFFFFFFFFF

>}image

showpage

Thisprogram would create a3x3matrix with one spot on out of nine.The firstcommand,

"translate",

determineswheretheimagewillbeplacedusingx andycoordinates.The

secondcommand,

"scale",

determinesthata squareimage 69x69units willbeproduced

(thereare72unitstoan

inch.)

Thenext sevenlinesarethe"image" command.The first

threenumbers ofthefirst line indicatethat theimagewillbe 288x288pixels wide and each

pixel willberepresented

by

onebit Thesix numbersinthesquarebracketsscaletheimage

tofittheunitsquaredescribed inthe"scale" command.2

Thenext sixlinesare a

hexidecimalrepresentation of ahalftone.PostScript hexisthereverse of normalhex so

thatF =0000where0represents non-image area.Thetwolines ofsolidF's (the F's

repeat72

times)

represent onehorizontalscanline.Thesameistrueofthe twolinesof

B's,

6'sandD's. The lasttworows ofF's completethe thirdrow ofthe3x3 matrix.

Whenthatiscompleted, thecycleisrepeateduntiltheunitsquareis filled.Atthatpoint,

theimageis actuallycreatedusingthecommand

"showpage."

Appendix

F,

page

93,

containsa sampleofa3x3condenseddottestpattern.Note

thatthe 10squares(oneis

blank)

representthetengray levels. The foursmallblackcorner

squares appearin every testimage.

Using

thiskindofprogram,severaldotshapes were produced.

They

are categorized

underthenames

"condensed", "open",

and"diamond".Thefigures thatfollow illustrate

thedifferences inthevariousdotshapes.Theopendotshapedescribesadotthatis

(29)

X

X

X

?x?

X

X

X

X

Figure4- 3x3

open matrix

Thecondenseddotshapedescribesadotthatis builtaround a central spot:

Z

1

Figure5 - 3x3

condensed matrix

Thesquare nature oftheseopenandcondenseddotformsmakesitpossibletostackthem

one on

top

ofanother. Thisallows ascreenangle of zero(therows couldbestaggeredto

createscreenanglesotherthan zero;howeverthiswasnotdone inthisexperiment.)

Screenanglebecomesafactor inthediamondclassofdotshapes sincethesedots

are notformedonasquare matrixanddon'tstackup neatly like boxes.

However,

inthe

sensethat

they

buildonacentralspot,

they

are similartocondensed spots.Figure6
(30)

X

EX

*P

KN

X

Hxil^

_*<*

i***

(31)

Therelationbetweenspotsinthematrix,number ofgray

levels,

and screen angleisshown

inthe tablebelow:

Table2

-Summary

of spotsin matrix, gray

levels,

linescreenand screen angle

Condensed/Open

2x2

3x3

4x4

5x5

6x6

8x8

Diamond

5

8

12

13

24

25

?includesblackand white(rememberthatthis iswhatis mathematicallypossible)

Thespot patternsdescribed inthe chart above canbe described inavisualshorthand

thatdescribesthewaythedotis formed:

Grays+

Linesperinch ScreenAngle

5 150 0

10 100 0

17 75 0

26 60 0

37 50 0

65 37.5 0

6 134.2 63.4

9 106.1 45

13 83.2 33.7

14 83.2 56.3

25 60 36.9

26 60 36.9

13

7 8 9

12

6

1 2 10

5 4 3

11

Figure7

(32)

For informationonthespot sequence of alldot

forms,

seeAppendix

E,

pages 88-91.

Sincethereare somanypossible combinations ofdot formationsonlyafewcould

bechosenfortesting.Theseparticular condensed and open patterns were chosento

comparetheaffect oftonerspreading intonon-image area.Thediamondpattern was

chosentolookattheeffect of anotherdotform(onewitha non-squarematrixandascreen

angle.)Screenangle couldhavebeenisolatedas afactor

by

creating screen anglesforthe

openand condensed

dots,

butthiswasnotdone inthisstudy.

Density

Measurements

All

density

measurements were madewithanX-Rite 309reflectiondensitometer.

Calibrationwashandledas specified

by

themanufacturer.Measurementswere madeon a

tablesurface with ablanksheet ofpaper

backing

upthetest.Threemeasurementswere

made on each l"xl"

testsquare.Themeasurementsequencewithinthesquarewas: upper

rightcorner,leftcenterandlowerrightcomer. Thesemeasurementswererecorded

direcdy

onthesheetandlateraveraged.Theseaverages wereusedforanalysis.

Thetestsforthisresearch wererunon anApple LaserWriter. When runninga series

oftests,

they

were rununinterrupted.Paperforthese testshas beensupplied

by

Boise CascadeandHammermill.

They

have been labeled "A-E".

"A"

representsHammermill

Laser

Copy,

"B"representsHammermillLaser

Print,

"C"

representsHammermill Laser

Plus,

"D"representsBoise CascadeLaserPaperand "E"

representsBoiseCascade Cotton

LaserPaper. Paper"C" waschosentobeusedforalltestswhere paper was notthe

variable.

Twoparametersare ofparticularimportanceinthisstudy.The first istheabilityof

the densitometer togivereproducibleresultswithinan acceptabletolerance,andthesecond

istheabilityofthelaserprintertoproducethesamepattern(froma sourcecomputer

file)

within reasonabletolerances. Theresultsforthe

following

sections aretobefound in

Appendix

C,

page79.

Testing

ofthe Densitometer

The X-Rite309manual3

statesthatmeasurementofthecalibrated reference check

(33)

inthisstudy

by

thehalftonenature ofthetestpatterns andthevariationsthatcanoccur

within a giventestpattern.Measurementswere recordedin

density,

notdotarea. Inan efforttomaintainthehighest accuracywhile

keeping

theprocedure

feasible,

three measurementshavebeenmade on eachtestsquare.Totest therepeatabilityof

measurements madeinthis manner,an experiment wasconducted.Threetestsquares were chosen andmeasured35timeseach.Thefirstsquarehadan average

density

of.26,the

second squarehadan average

density

of.78,andthe thirdsquarehadanaverage

density

of1.13. The standarddeviationsare asfollows: lightpatch .006,medium patch .010and

solid patch.018.Whatthisimplies isthat thelowerdensitiesare measured more

accurately

thanthehigherones.

Testing

oftheLaser Printer

AsingleAppleLaserWriterwasusedforalltests;

initially

itwastestedfor

consistency. Theconsistency test(see Appendix

C,

page

80)

showedtheextentof variationpossiblewithinrepetitions ofthesamefile. This testhad

thirty

solidblack

squares(each

l"xl")

infivecolumns of six squares each.Thissamefilewasprintedthree

timeswiththeresults asfollows.

Density

measurements rangedfrom.88to 1.30 (arange

of.42).Thiswide rangeisaccentuated

by

thevariationsin

density

on a givenpage;

however,

ifa squareiscomparedtoa squareinthesamepositiononthe

following

page

thenthevariations wentonlyas highas.26.

Following

inthismanner ofonly comparing

thesame square ondifferentpages showsthat 100%ofthemeasurementsfallwithin.243

ofthemean. Inotherwords,there isastandarddeviationof.081.

Itwasdiscoveredthat thereisa

tendency

fortheprintertoprintdarkerontheleft handside ofthepage(thisisclearlyshown

by

theaverages of pages

1-3,

Appendix

C,

page

81.)

The

top

was alsoslighdy darkerthanthebottom. Generalobservations revealed

thatsheets were oftenmarked withtracesofapreviousimage. Inaddition,adarkimageon

a single sheet could affectthedarknessachievableinother areas ofthesheet.It became clearthatseveral stepswouldhavetobetakentoadjustforthesevariations.

First,

corner testsquares wereincludedoneachimagesothatageneral comparisoncouldbemade

between any twotestsheets.

Secondly,

thepositioningofthesquares was reconsidered. Greaterspace wasleft betweentest

images,

fewer imageswereincludedon apage, and

testimageswerekept away fromtheedge areas of pages wherevariationwasgreatest.

Thirdly,

whenanumberoflike-tests weretoberun,a

"sample"

(34)

theghosting effect of a previousimage.Evenwiththeseadjustments,itwas clearthata

certain amount ofvariationwasinherentintheprocess which could notbeavoided.

Comparing

theStandard Deviations

Itfollowsthata comparison canbemadebetweenthedensitometerandthelaser

printer.Thedensitometermeasured a solidtestsquarein35trialswitha standarddeviation

of.018(mean

density

= 1.13). The LaserWritercreatedthesame solidtestsquare90times

witha standarddeviationof.081 (mean

density

=1.14.) Althoughit istruethatthe

variationcaused

by density

measurementwillbereflectedinthis .081 standarddeviation

forthe

LaserWriter,

it isstill quite clearthat thevariationintheLaserWriterisof amuch

greatermagnitudethaninthedensitometer.

MicroscopicStudies

Themicrophotos were shotusinganOlympus BH-2microscopewith

Tungsten-Halogen

lamp

and aNikonMultiphotphotographic attachmentThe

magnification was80x (Vonthephotograph = onthe

original.) Allphotographs

representPaperC. Polaroid Type 55 Positive/Negative Instantsheetfilmwasused.

Exposuretimewasfourminutes anddevelopmentwas handledas prescribed

by

Polaroid.

These4x5negatives werethencontact printedforreproductioninthis thesis.

They

have

beenmounted on a grid

illustrating

thematrix.

Microscopicmeasurementsweretakentodeterminetheactualsize of adot

consistingofonespot.The instrumentused wasaBauschandLomb lightmicroscope

witha lOx

lens,

zoom adjustmentand acalibratingeyepiece.Theeyepiecewascalibrated

toan etched slidewithdivisionsof.001".Themarkingsintheeyepiece were adjustedto

(35)

FOOTNOTESFOR CHAPTERFTVE

1Adobe

Systems, Inc.,

PostScript LanguageTutorial andCookbook.

Reading,

Mass.:

Addison

Wesley Publishing

Co, Inc., 1985,

p.l1 1-116.

2Surprisingly,

whenthescale was setto72x72and a300x300pixelimagewascreatedthe

resultingtestpatterndisplayed repeatingpatternsthatstreakedtheimage vertically

andhorizontally. Trial and errortestsconfirmedthat thecombination of69x69

scalingplus a288x288pixelimageresultedinnon-streakedtestpatterns.288 is a

multiple of72whichmay be whyiteliminatesthe streaking,althoughno

explanationfora unit square of69x69was everdetermined.

(36)

CHAPTERSIX

RESULTS

Besidestheconsistencytests(referto the

Methodology

section),a numberof

differenttests were conducted.

They

canbe divided intogroups: tone production,

microscopicstudies,and papertests. Alldata forthe toneproduction and papertestsare

includedintheAppendices.Theresults ofthemicroscopic studies areincludedinthis

chapter(withtheexception ofthemicrophotographs.)

Tone Production

Toneproduction curves were producedfor

2x2, 3x3, 4x4, 5x5, 6x6,

and8x8

matrices.Withineach ofthesematrix structurestwodotformswerecompared: open and

condensed.Thesetests were run onPaperC. Thegraphs ofthese testsappearonpages35

to40intheAnalysissection. (Thegraphs record

density

onthey-axisandnumberof

spots ondivided

by

totalspotsinthematrix onthex-axis.)Severaltrends becomeclear.

Thecondenseddot

forms,

Figure

11,

tend toproducea slight s-shaped curvethatbecomes

lessandlessaccentuated as thematrix sizeincreases.

Conversely

theopendot

forms,

Figure

10,

produces an exaggerated s-curvethatactually developsa

hump

nearthe50%

spots on region.

Density

continuesto

drop

untilaround70%. Thiscurvebecomesmore

exaggeratedas matrix sizeincreases.

Toneproductioncurves were alsoproducedforthediamond dot forms. These dot

forms(see Figure

12)

produced curves quitesimilarinshapetothecondenseddotforms

(ie.,slightly

s-shaped.)Themidtones(fromapproximately 30%to

70%)

are covered

by

lowerandlower densitiesasthenumberof spotswithinthediamondmatrixincreases.

Wheredirectcomparisonispossible(see

below)

itcanbeseenthateventhoughthe

samepercentageof spots are oninthematrix,alarger

density

is achievedwherethematrix
(37)

Table 3 Comparisonoftestsquares with50%spots on

Spotson

Density

Maximum

Density

AdjustedDensity*

2/4 .71 .93 .76

4/8 .63 .85 .74

6/12 .56 .95 .60

8/16 .49 .89 .55

12/24 .47 .94 .50

18/36 .42 .91 .46

32/64 .45 1.15 .39

?Forthepurpose ofcomparison,the

density

isadjustedto themaximum

density

achieved

by

theLaserWriteron a givenday.Allofthedensitieshave beenadjusted

toa maximum

density

of1.00. Inthecase of2/4spots onthismeansthatthe

density,

.71,ismultiplied

by

1.00/.93togive an adjusted

density

of.76.The

assumption madehere isthatifthe

density

had been

1.00,

the2/4 stepwouldhave

been.76.Yeteven withoutadjustingthe

density

thereisa gradualdeclinein

density

asthenumber of spotsincreases.

Thedotshapes usedforthis testwerethe

8,

12 and24 diamondshape,andthe

2x2, 4x4,

6x6and8x8condenseddotshapes.Theopendotshapes at

50%,

since

they

are all

checkerboards,are all quite similar.

They

averageat about.82adjusteddensity.

Microscopic Studies

Microscopicmeasurements weremadetodeterminetheactual size ofthedot. The

markingsin theeyepiece were adjustedtobeequalto through theuseofthe zoom

adjustment. Theactualdotsare quiteirregular innature(see

below),

sothesediameter
(38)

3 units =

Figure8- Irregular

nature ofthedot

Thecriterion used wasthatthebulkofthedotshouldfallwithinthestated

measurementMeasurements weremade on

2x2, 3x3, 4x4, 5x5, 6x6,

and8x8 matrices

usingthe testsquare whereonlyonespotinthematrix was on.Inthismanner,thevariable

betweenthe testsisthedistancebetweenadjacent spots. Itshould alsobenotedthatasthe

dotscome closer and closertogether,the

irregularity

inthedotshapeincreases. The

measurementsfortheindividualspots are asfollows:

Table 4- Dot

size measurement

Matrix

2x2

3x3

4x4

5x5

6x6

8x8

Diameterofthedot

Ameasurementwas also made ofthe2x2opendot formwheretwoout offourspotsare

oninthematrix.Thischeckerboardpatternhasquite anirregulardotwhichmakesexact

measurement

difficult

howeverthediameterisnogreaterthan.003".

Graphically

thedata
(39)

5x5 4x4 3x3 2x2 2x2

*

?

Side

of boxequals

Figure9

-Illustrating

dotsize

(Thesecond2x2matrix representsthe twospots on situation.Ineach case thenearest

adjacentdotsare alsoshown.)

The accuracyofthemeasurements wastested

by

measuringthedistance betweenthe

dotsandcomparingitwiththeknown linescreenvalues:

Table5

-Testing

theaccuracyofthemicroscopic measurements

Distance betweenspots(midpointto midpoint)

Matrix Measured Calculated

2x2

3x3

4x4

5x5

6x6

8x8

Microphotographs weretakentogive avisualillustrationofwhatis

happening

atthe

levelofasinglespot.Thephotos areshownon pages41 to49.

They

have beenmounted

on a gridtoillustratetherelationship between thespot andthematrix. Thephotos were

shot at amagnificationofapproximately80x (one inchonthephotographisequalto

.0125").Thephotos willbe

discussedintheanalysissection,butpleasenotetwo things:

first

therelativesize of anindividual spotandsecond, therelationofthematrixtothe
(40)

PaperTests

Twofactorsrelatingtopaper weretestedas part ofthisresearch.The firstisthe

ability toachieve ahighmaximumdensity.Thesecondistheabilitytoproduceatonal

curvethrough a range of grays.

Maximum

Density

Tests- The

density

testconsisted oftaking

density

measurements

from 12solidblackpatches,aswellasrecordingthe

density

ofthewhite ofthepaper.

Threesheets were runforeach paper sample.Theresults werethenaveragedand shown

below (rankingsareinparentheses):

Table6- Resultsofthefirstpapertest

Paper Dmax Paper White Range St. Dev.

A

1.114(2)

0.089(1)

1.025(2)

.030(5)

B

1.134(1)

0.090(2)

1.044(1)

.034(3)

C

1.102(3)

0.095(4)

1.007(3)

.035(1-2)

D

1.069(5)

0.102(5)

0.967(5)

.035(1-2)

E

1.061(4)

0.093(3)

0.968(4)

.031(4)

Ave. 1.096 0.094 1.002 .043

Thetestwas repeatedat alater datewiththe

following

results:

Table 7- Resultsofthesecond papertest

Paper Dmax PaperWhite Range St. Dev.

A

0.887(4)

0.089(1)

0.798(3)

.033(2-3)

B

0.908(2)

0.096(4)

0.812(2)

.035(1)

C

0.913(1)

0.092(2)

0.821(1)

.033(2-3)

D

0.897(3)

0.103(5)

0.794(4)

.022(5)

E

0.846(5)

0.093(3)

0.753(5)

.025(4)

Ave. 0.890 0.095 0.796

(41)

Itis

interesting

tonotethat themaximum

density

achieved onthe

day

ofthefirsttest

is 1.096comparedto0.890onthesecondday. Eachtestrepresents,inthecase of maximum

density,

36measurements(gleaned from 108 actual measurements onthe36

squares.)

Gray

Production Test- Totest the

abilityof a papertoproduce grays(andalsoto

gaugetheamount of

filling in)

anothertestwas run. The 5x5open matrixpatternwasrun

threetimeson each paper.

Density

measurements weretakenand averaged. Sincethis

particulardot formationformsa characteristichump-shapedtoneproductioncurve, itwas decidedtocomparethepoints wherethecurve peaks and whereitreachesthebottom. Thesepeaks,bottomsandcorrespondingspot numbers are recordedbelow:

Table8- Resultsofthethirdpapertest

Peak

Density

Bottom

Density

Difference between Paper andSpot # andSpot # PeakandBottom

A .70/12,14 .64/17 .06

B .72/12 .66/16,17 .06

C .69/12 .63/16 .05

D .69/14 .67/16,17 .02

E .69/14 .64/16 .05

Ave. .69/14 .65/17 .04

Thisparticulartestwillbeofimportancenotonly in

determining

a paper'sabilityto

reproduceatonecurveaccurately, butalsotoget alookatthenature ofthis hump/bottom

phenomenon. Thisis becausetheaverages oftheresultsof all papersshowthat

steps 14

and 17arethekeysto solvingthepuzzle.Thenatureofthegrayproduction willbe discussed

by

theuseofseveral methodstogradetheproductionofgrays.Referto the Analysis section,page32 foranexplanationofthesemethods.
(42)

Table 9- Overview

of papercharacteristics

A B C D E

Weight(in

lbs.)

20 24 24 20 20

Opacity

87 90 92 86+ 85+

Brightness 89 89 90 85.5 91

Brightness* 89

93 89.5 85 90

?brightnessmeasurements made on aPhotovolt Model 670reflection meter(the

(43)

CHAPTER

SEVEN

ANALYSIS

Thissectionis divided intothreeparts: toneproduction,microscopicstudies,and

papertests.The datafromtheResultssectioniscontainedintheAppendices.The data has

beenusedtocalculatemeans andstandarddeviations. Theraw

data,

alongwiththemeans

and standarddeviations isshownintheseAppendices. Graphs havebeen drawnto

illustratesome ofthedata. Thegraphs are on pages35 to40attheend ofthischapter.

ToneProduction

Thebulkofthissection consists ofthegraphical representation oftheResults

section. Figures 10through 15are graphs ofthetoneproduction curves.

Density

is

recorded onthey-axis while percent of spotsoninthe matrixisrecordedonthex-axis.

Percentof spots on inthematrixsimplyisa calculation of spotsondivided

by

spotsinthe

matrix. Forexample,one spot onina25spotmatrixyieldsa valueof4%spots oninthe

matrix.Wherecertain curveswithinacategory showed greatsimilarity (asis thecaseinthe

diamondmatrixforexample)onlyone curvewas showntopreservetheclarityofthe

graph.Forexample, the 12 diamondand 13 diamondareverysimilar andthereforeonly

the 12diamondisshown on the graph (thesameistruefor 24and

25,

only 24 diamond is

shown.) This adjustmenthas beenmadein figures 10through 12.

Agoodcomparisoncanbemadeofthe25

diamond,

5x5condensed andthe5x5

open matrices since

they

allcontain25 spotswithinthematrix. Forthisreasontheyhave

allbeenshowntogetherin figure 13. Thecurvesinthegraphs havebeen drawnto

representthedatapoints.Itshouldbenotedthatinthematricescontaining fewspots

(ie.,

2x2, 3x3,

5

diamond)

thismeansthat thecurvehas been drawn using relatively few data

points.Nocurves aredrawn in figure 14. Allthedatapoints are showntoillustratethe

unevennature ofthedata. Column breaksare showntoshowtheeffectthatpagelocation

hasonthetest.Inthe8x8 test, 24testsquaresfiton a pagein fourcolumns of sixsquares

each. Threepageswere requiredtofitalltestsquares. 8x8openisrepresented

by

(44)

and8x8condensedisrepresented

by

"c's". Wherethevalues arethesame an

"x"

appears.

BartlesonandBrenemanvalues were usedtocreatetheidealtonalscalein Figure

15. Thissystem relateshumanperceptionto

density

values.Inthismanner,stepsofequal

visualdifferencecanbecreated.

Therefore,

ifthemaximum

density

ofthe8x8condensed

matrixis 1.

15,

anidealcurve of65steps canbecreatedusing 1.15as the maximum

density

and0.10astheminimumdensity. See Appendix

D,

page84 forcalculations and

anin-depthexplanation.

MicroscopicStudies

Themicroscopic measurement results are shownintheresults sectionintheir

entirety.No furtheranalysishasbeenperformed onthisdata.

Themicrophotographs have beenmountedongridswhichrepresentthematrices on

which

they

arebuilt The"x's" representthespotswhichare on. Figure 16 includesa

microphotograph of parallellinesattheirfinestresolution(thereisnounderlyingmatrixfor

this.)

Figures 17through22shouldbeviewedas a series.

They

allrepresentthe5x5open

matrix with anywherefromoneto24spots on. Figures 18and21 are remarkablefortheir

similaritythough 18 has six spots on while21 has 18spots on. Figure 23representsthe

12spots on square ofthe5x5condensed matrix.Figure 24represents 12 spotson,inthis

caseinthe25 spotdiamondmatrix.Both23and24shouldbecomparedtoFigure

19,

sinceineach ofthesecases 12out of25 ofthespots areoninthematrices.

Paper Tests

Appendix

B,

page

74,

givesthefullextent ofdataand calculations.The gray

production part ofthepapertestsrequiresan analysis todetermine how manygrayswere

produced.Therearecertainly many waystodothiskindof analysis.Theauthorhas developedthreemethods of

doing

thisand eachwillbe lookedat separately.

First,

it is

possibletomeasurethenumberoftimes thatavalueofagivenstepislessthanor equalto theprevious value.

Certainly

ifavalue inanascending gray scaledoesnotexceedthe

previous valueitcannotbeconsideredaseparategray. ThismethodwillbecalledMethod

One.Anothermethod wouldbetocountthenumberoftimes that thevalue of a givenstep

doesnotexceedthehighestpreviousvalue.Thismethod will accountfor dips ina curve

(likeintheopencurves) where valuesmay be ascending but have actuallybeenexceeded

(45)

countingthenumber oftimesthat thevalue ofanystep inthe testisrepeated.Thismethod

willbereferredtoasMethod Three.Toreview:

MethodOne

-thenumber oftimesthatthevalue ofa givenstepislessthanorequal

to thepreviousstep

MethodTwo

-thenumber oftimesthat thevalue of a givenstepis lessthanorequal

to thehighestprevious value

MethodThree- the number oftimes that thevalue of a

steprepeats

Thesecalculations havebeenmadenotonly forthepapertests,butalsoforthe tone

(46)

LU

o

DC

h-<

LU

D-O

o o

o a.

o CO

o

o (o E c c o o ID W O Q. l/>

OJ O ^r cj 0_

o co

o CO

rtJ I

CM

t-<J> 00 to to CO CJ

to QJ

D

Figure 10 - Graphof

2x2, 3x3, 4x4,

and6x6
(47)

co hi o cn h-< D LU CO -z. LU D O o

J I I L

o a. o oo o X to -rt rt* ro E c c o o u. to c> Q. to c OJ o y rtf OJ 0-o CO o C\J CJ

T-Oi CO to io CO CM

-to c

OJ O

Figure 1 1 - Graphof

2x2, 3x3, 4x4,

and 6x6
(48)

CM PcDooi^-to-O'-;

c0.CN.,r"-cz

CD D

Figure 12- Graphof

5, 8,

12,

and24diamond
(49)

o Q-00 in CM CD 2 2 O O C/0 LU o cc h-< o o CD O CO o to ~ ro o o -m o Q. V) C CD O ^ ^ CD CL O CO o CM

1 I I L

CM

t-CD oo r^ co io CO CM

to c CD Q

Figure 13 - Graph

(50)

o u o CO O O o o o o o o o o CJ o O o o o u o u u o CJ o o o o u o u o cj o o o u CO o CJ o o u o o CJ o o o o o u <J o o o D LU

00 . .

7- c

III rti

Q or

S <<o O C/J UJ o V) O ro z cc OJ

<. < c z rt E

UJ m 3

LL V O

u oo u

o o u o u o o o o CO "o CJ u Irt) o o o o o o OO CO -CD Ol ro CL CM CD ro Crtrtl. <D O) ro a. CJ o o OO CO OO o o o o o 05 o CO o o co o CO o CM ro E o <r> O Q. to CD CJ krt Q) 0. CM

t-O) oo CD IO CO CM

to c

CD Q

Figure 14- Graph

(51)

-O

LU 00

z

UJ UJ _J Q

< z

o

00 o

o

_l

<

z

oo

X

CO

u

1- 00

rtrt-J

<

LU

Q

00

cc

UJ

>

1 I

CM cn oo to m CO CM

c CD

O

(52)
(53)

X

X

X

it

<

X

X

X

X

X

X

X

x:

e

E

x

(54)
(55)
(56)
(57)
(58)

k. ^rtk. rtrtAk.__*^ ... ^rtrtrtrtirtk.^^^fc.^^rtrtirtk.^'_ k.^jLrt<rtk^rtirtL^ikv. .^^rt*rtk.^^rtrt*k.^"rt^fc.^F^W^^rti rtk.^^rtrtrtk^^^fc.^ik.VAl^^r.

***

?!-?!

?>:

?>T.tt.>:

.*

T<iT

*_;?::?:

*l*

?!<>*.**>*

a<

?X*>>5

&2&3Z

(59)
(60)
(61)

CHAPTEREIGHT

DISCUSSION

Thischapteris divided intothreesections:tone production, microscopicstudies and

papertests.

ToneProduction

Forthisdiscussionplease refertoFigures 10through 15on pages35to40. An

inherentcharacteristic ofthecurves oftheopen matricesbecomesclearin Figure 10. The

curve (of6x6 forexample)reaches aninitialpeakatabout50% spots on andthendrops

until 70%spots on at which pointitincreasesagain.This isapparentin Figures 13and 14

as well.Thecurves ofthecondensed matrices ontheother

hand,

tend towardan s-curve

shapewhichisrelatively flat inthe midtones.The diamondmatricesare quite similarto the

condensedas agroup (seeFigure 12).Thethree typesofcurves canbecomparedin

Figure 13.

Clearly

themoststriking aspectofthisgraphisthehumped-shapeofthe5x5

opencurve.Itmightbesurmisedthat theopenmatriceswouldfill in causingtherapidrise

indensitiesshown;howeverit iscuriousthatthedensities decreasepast50%as more

spots are added. Thisquestionisanswered

by

themicrophotographs andwillbe discussed

inthemicroscopic studiessectionofthis chapter.Rememberin

looking

atFigure 13 that

theopenand condensed5x5 matricesdiffer only inthewaythespots are configured.

Thegeneralshape of open versus condensed curvesiswelldocumented in Figure

14.Inaddition, theinfluenceof pagelocationisindicated

by

themarkingofthecolumn

changes.The datapointsdonotformaperfecdy smoothcurve.Inpartthisiscaused

by

thecolumn changes.

Note,

inparticular,page

3,

column 1 wherebothopen and condensed

rise

by

considerable amounts.Thesameistruetoa somewhatlesserextentinpage

3,

column2. This emphasizesthepoint madeinthe

Methodology

section, that

is,

thatpage

locationplays alargeroleinthe

density

ofagiventestsquare.

Thefinalgraph,Figure

15,

comparesanideal BartlesonandBrenemancurveto the
(62)

facts

shouldbenoted.

First,

the

8x8

condensedmatrix represents alinescreenof37.5

which while

affording

numerous grays,sacrificesdetail. Secondofall, the8x8curveis

toosteep inthe

highlight

andshadow,andtooflatinthemidtone.Thismeansthat the

midtoneareafromabout.3to.6in

density

(

a range of

.3)iscovered

by

moregrays than

theentire rest oftherange(about.75).Lastofall,duetothedigitalnature ofdigital

halftones,

thefirst few steps are of greater magnitude thantheonesthatfollow. Thevalues

of

0/25,1/25,2/25,3/25

and4/25 are asfollows:

0.10, 0.14,

0.17, 0.19,

and0.20.

Ideally

thesteps mightbe

0.10, 0.12,

0.14, 0.16,

and0.18. Ifthiswerethecase, therewould

notbesuch alarge

jump

fromthepaper whitetothefirstgray.In addition,itwould

facilitatethespreadingout oftheflatareainthemidtone.Theseconditions,

however,

are

difficulttoachieveinadigitalhalftone.Rememberthat theaddition ofa spotwithinthe

matrix will make a greaterdifferenceif very fewspots arealreadythere.Forexample,

fromoneto twospotsthereis a100% increaseinthenumber ofspots,fromtwo tothree

onlya50% increase and so on.

Pulling

data fromthevariouscurvesthe

following

comparison canbemadebetween

all ofthedatapointsatwhich50%ofthespots are on(see

Results,

page26):

Table 10- 50%spots onwithinformation concerningareabetweenspots

Spotson Area betweenspots Docomerstouch? Adjusted

density

2/4 2units Yes .76

4/8 4units Yes .74

6/12 6units Yes .60

8/16 8units No .55

12/24 12units No .50

18/36 18 units No .46

32/64 32units No .39

Eventhoughthesame percent of spots areon,itisclearthatthe

density

increasesas the

areabetweenthespotsincreases.

Why

shouldthisbe? Therearecertainly manyfactorsat

play

here,

twoofthem

being

laserspot size andtheamount of overlap. Onepossible

explanationis thatastheline ruling

increases, toning

willbeless

likely

inthenon-image
(63)

Microscopic Studies

Themicroscopicmeasurementsrevealthat thediameterof adot consistingof a

single spot remains at aconstant untilthematrix sizeisreducedto4x4.Atthatpoint

thedotcontinuestoshrink untilit

becomes

soirregularthatit is difficulttomeasure.This

destruction

oftheunit

building

blockof a

halftone

isof utmost concerntodesignersof

digital

halftones.

Forthe

following

discussionofthemicrophotographsplease refertoFigures 16

through

24,

pages41 to49. Figure 16isa goodillustrationofthemannerinwhichtoner

fillsinthenon-imagearea.ThesearethefinestparallellinesthattheLaserWritercan

create.Ina unit

inch,

onehundredand

fifty

oftheseblacklineswouldbe bordered

by

one

hundredand

fifty

whitelines.Ifitwere possibletooutputthis imagetophotographic paper

thenature oftheimagewouldbemuchdifferentThespread oftonerwould notbea

problem andthedefinitionoftheedge wouldbemuchfiner. Thishigherresolutionis

reflectedinthehighercost of photographic paper andfilm.

Thenextsequence,Figures 17through

22,

isofinterestforseveral reasons. Note

thedecreaseinspot sizebetween Figure 17and 19. The individualspots are visiblein

Figure 19andhaveshrunkenremarkablyas comparedtoFigure 17. Figures 18and 21

make another

interesting

comparison.Ineffect, six spots (in Figure

18)

dotheworkof18

spots(in Figure21).This isdueto toner

filling

inthenon-image areainFigure 18. Toner

falls intothenon-imagearea;however becauseit issurrounded

by

moretonerthathas

alreadymadeits wayto theimagearea,itcan't makeitswayoutandisultimatelytrapped.

The

hump

shaped curvein Figure 13canbeexplainedwiththe microphotographs.

Figure 19representsthepeakofthe curve,Figure 20representsthepoint

immediately

after.Figures 19and20illustratethedecrease in

density

thatoccurs.Notehow Figure 20

appearslighterthanFigure 19eventhoughan extra spothasbeenadded. Whatappearsto

be

happening

hereis that theextraspot,whichissurrounded

by

fourotherspots,forms a

largecharged areawithitsneighbors.Thischarged areaappearstodrawthetonerfromthe

non-image area

thereby

creatingahigher density. Thisextraspothastheeffect ofcleaning

upthenon-image area ofstray toner; howeveritalsoappearstomakeitmoredifficultfor

tonertobeattractedto theimageareasthatareisolated.Thisprocess continuesuntilthis

largecentral charged areahasbecome largeenoughitselftobeginanincreasein

density

(seeFigure

21.)

ItissurprisingthattoreachFigure21 it is necessarytopass through
(64)

toeach otherinsequence, andyet, thecentraldot in Figure 18 virtually decomposes before

being

built

upagain in Figure 21.

Figure

22represents one spot short of a solidblack.

Notethat thesize oftheopen

(non-image)

areais quite similarinsizetothatoftheimage

areain Figure 17.

Figures

19,

23 and24make an

interesting

comparison of25 spot matriceswith 12

spotson. The resulting densities (.42

diamond,

.53 condensed,and.88open,referto

Appendix

A)

show a

difference

thatisalso quite visible onthemicroscopiclevel. In Figure

19,

theopen areas betweenspotshave filledintoa great extent In Figure23thegreatest

amount offilling-intakesplace atthepoint wherethehalftone dotsare endtoend. In

Figure24the

halftone

dots onlyapproach each other atthecomers andit isatthesecorners

thatsomefilling-intakesplace.This limited filling-inthat takesplaceinFigure24isa

result ofthescreen anglethatexistsinthe25diamondmatrix. Thisisanimportant factor

to

keep

inmind while

designing

matrices sinceitcanbeusedtocontrolfilling-in. These

microphotographsshowthatconfigurationwithinthe matrix, and, theshape ofthematrix

itselfplayalargeroleintheresultingdensities.

Paper Tests

Maximum

Density

-Achieving

ahighmaximum

density

isimportantintone

productionsinceitallows a greater range of valuestobecovered

by

various grays. Alow

maximum

density

willcompress thegrayscale sothatadjacent graysbecomemore similar.

Theotherfactorinrangeistheminimumdensity. What is

being

comparedinthispapertest

istherangefrommaximumtominimumdensity. InthefirsttestTable

6,

page 29the

papers are ranked

by

rangeinthe

following

order: Bthen

A,

C, E,

andD. Itwouldbe

statisticallypossibletojudgetheaccuracyofthisrankinggiventhemeans and standard

deviations.

However,

thesecondtest,Table

7,

page

29,

gives arankingofCthen

B, A,

D,

andE. This rankingthrowssomedoubtontoanyjudgementsof orderthatmightbe

drawn fromtheserankings.Itshouldbenotedthatonthe

day

ofthefirst test,theaverage

maximum

density

was 1.096while onthe

day

Figure

Figure 1 - 3x3 matrix of squares
Table 1 - Matrix
Figure 6-13 spot diamond matrix
Table 3 Comparison of test squares with 50% spots on
+7

References

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