scieee Science in your language
[en] (orig)

Meta-model based optimization of hot rolling processes in the metal industry

Abstract

To maximize the throughput of a hot rolling mill, the number of passes has to be reduced. This can be achieved by maximizing the thickness reduction in each pass. For this purpose, exact predictions of roll force and torque are required. Hence, the predictive models that describe the physical behavior of the product have to be accurate and cover a wide range of different materials. Due to market requirements a lot of new materials are tested and rolled. If these materials are chosen to be rolled more often, a suitable flow curve has to be established. It is not reasonable to determine those flow curves in laboratory, because of costs and time. A strong demand for quick parameter determination and the optimization of flow curve parameter with minimum costs is the logical consequence. Therefore parameter estimation and the optimization with real data, which were collected during previous runs, is a promising idea. Producers benefit from this data-driven approach and receive a huge gain in flexibility when rolling new materials, optimizing current production, and increasing quality. This concept would also allow to optimize flow curve parameters, which have already been treated by standard methods. In this article, a new data-driven approach for predicting the physical behavior of the product and setting important parameters is presented. We demonstrate how the prediction quality of the roll force and roll torque can be optimized sustainably. This offers the opportunity to continuously increase the workload in each pass to the theoretical maximum while product quality and process stability can also be improved.

Read accessible full text

Meta-model based optimization of hot rolling processes in the metal industry

Author: Jung, Christian,Zaefferer, Martin,Bartz-Beielstein, Thomas,Rudolph, Günter
Year: 2016
Source: https://cos.bibl.th-koeln.de/files/558/jung14bCOS.pdf
CIplus
Band 6/2017
Me a-model based op imiza ion o ho
olling p ocesses in he me al indus y
Ch is ian Jung, Ma in Zae e e ,
Thomas Ba z-Beiels ein, Gün e Rudolph
The final publica ion is a ailable a Sp inge ia
h p://dx.doi.o g/10.1007/s00170-016-9386-6
Noname manusc ip No.
(will be inse ed by he edi o )
Me a-model based
op imiza ion o ho olling
p ocesses in he me al
indus y
Ch is ian Jung ·
Ma in Zae e e ·
Thomas Ba z-
Beiels ein ·
G¨un e Rudolph
he da e o eceip and accep ance should be inse ed la e
Abs ac To maximize he h oughpu o a ho olling
mill, he numbe o passes has o be educed. This can
be achie ed by maximizing he hickness educ ion in
each pass. Fo his pu pose, exac p edic ions o oll
o ce and o que a e equi ed. Hence, he p edic i e
models ha desc ibe he physical beha io o he p od-
uc ha e o be accu a e and co e a wide ange o di -
e en ma e ials.
Due o ma ke equi emen s a lo o new ma e i-
als a e es ed and olled. I hese ma e ials a e chosen
o be olled mo e o en, a sui able low cu e has o
be es ablished. I is no easonable o de e mine hose
low cu es in labo a o y, because o cos s and ime. A
s ong demand o quick pa ame e de e mina ion and
he op imiza ion o low cu e pa ame e wi h minimum
cos s is he logical consequence. The e o e pa ame e
es ima ion and he op imiza ion wi h eal da a, which
we e collec ed du ing p e ious uns, is a p omising idea.
P oduce s bene i om his da a-d i en app oach and
ecei e a huge gain in lexibili y when olling new ma-
e ials, op imizing cu en p oduc ion, and inc easing
quali y. This concep would also allow o op imize low
cu e pa ame e s, which ha e al eady been ea ed by
s anda d me hods. In his a icle, a new da a-d i en ap-
Facul y o Compu e and Enginee ing Sciences
Cologne Uni e si y o Applied Sciences,
51643 Gumme sbach, Ge many
[email p o ec ed]
Facul y o Compu a ional In elligence
TU Do mund Uni e si y,
44227 Do mund, Ge many
[email p o ec ed]
p oach o p edic ing he physical beha io o he p od-
uc and se ing impo an pa ame e s is p esen ed. We
demons a e how he p edic ion quali y o he oll o ce
and oll o que can be op imized sus ainably. This o e s
he oppo uni y o con inuously inc ease he wo kload
in each pass o he heo e ical maximum while p oduc
quali y and p ocess s abili y can also be imp o ed.
Keywo ds lowcu e ·K iging ·me a-model ·me al ·
ho olling
1 In oduc ion
The complex p ocess o ho olling equi es e y accu-
a e physical models. Se e al di e en physical models
a e used in ho olling mills. These models include he
slab o ingo hea ing a he u nace, whe e he he -5
mal beha io is modeled, as well as he olling p o-
cess i sel . The ask o he di e en models is o p e-
dic he he mal and physical beha io o he p oduc
and se impo an pa ame e s o achie ing maximum
p oduc h oughpu while inc easing he quali y o he10
inal p oduc . The e a e se e al p ocess and p oduc
pa ame e s which play impo an oles. They a e inde-
penden o he plan ype and applicable o s eel and
aluminum ho mills. Some o hem, o example plan
geome ies o d i e pa ame e s, emain cons an du ing15
olling. O he pa ame e s may a y du ing olling bu
a e no domina ed by he ma e ial, e.g., he maximum
possible hickness educ ion depends mainly on he ac-
ual hickness and he wo k olls cu en ly ins alled.
The maximum edcu ion is o cou se also dependen 20
om he ic ion be ween he olls and he ma e ial
bu his e ec is no as huge as he geome ical limi a-
ions. Pa ame e s, which depend on he ma e ial o he
p oduc , a e usually ha d o op imize, because (i) he
numbe o di e en ma e ials is s eadily inc easing due25
o ma ke equi emen s and (ii) measu emen s o he
p ocess a e only indi ec ly co ela ed o he ma e ial.
The mos impo an pa ame e s o he p edic ion
o he oll o ce a e he low cu e pa ame e s o each
ma e ial. A mo e e icien me hod o op imizing hese30
pa ame e s is necessa y o inc ease he lexibili y and
educe he cos o he olling p ocess.
A ecen app oach uses a i icial in elligen ech-
niques o op imiza ion o shape olling sequences [17].
Especially in he ield o cold olling, se e al me hods35
o simula ion and op imiza ion we e published [18, 24].
The e we e also s udies, which we e based on ini e el-
emen me hods [25]. In his pape we p opose me a-
model based op imiza ion s a egies o he ask o ho
olling mill low cu e pa ame e op imiza ion. Me a40
models, also e e ed o as su oga e models, simpli y
2 Ch is ian Jung e al.
he simula ion op imiza ion as he un imes a e gene -
ally much sho e han he o iginal unc ion e alua ions
[1, 16] and a e a p o en s a egy o global op imiza ion
[15]. The esul s a e compa ed o classical op imiza ion45
s a egies. Hence, his pape add esses he ollowing e-
sea ch ques ions:
(R-1) Can he olling p ocess bene i om me a-model
based op imiza ion?
(R-2) How ime- and cos e icien is his app oach in50
compa ison o he es ablished indus y p oce-
du es?
This pape is s uc u ed as ollows. Sec ion 2 in o-
duces echnical e ms and undamen al p inciples o ho
olling and he ela ed pa ame e s. I desc ibes he cu -55
en s a e-o - he-a app oach in indus y. P oblems e-
la ed o he olling p ocess a e desc ibed in Sec. 3. Ou
me hodology is de ailed and compa ed o exis ing ap-
p oaches in Sec. 4. The expe imen al se up is desc ibed
in Sec. 5. Resul s a e p esen ed in Sec. 6. The pape 60
concludes wi h a discussion in Sec. 7.
2 Ho Rolling
2.1 Fundamen als and Technical Te ms
Be o e desc ibing some o he main aspec s, he unda-
men al echnical e minology will be in oduced. Fig-65
u e 1 shows a common ho s ip mill o s eel. The p o-
cess in gene al is e y simila o an aluminum mill. The
wo k low o he p ocess is om he le side o he
igh side. The main componen s a e a ehea ing u -
nace, a e e sing oughing mill, a con inuous inishing70
mill, a cooling line, and a downcoile . The coilbox be-
ween oughing mill and inishing mill is mo e o less
op ional. I is used o achie e be e empe a u e p o-
iles and allows a mo e compac olling mill.
The p ocess s a s wi h he cha ging o he u nace.75
He e, slabs which a e usually a oom empe a u e a e
cha ged and ehea ed o empe a u es a ound 1200 deg
C o s eel mills and 500 deg C o aluminum mills.
Fig. 1 Ho Rolling mill o s eel wi h coilbox. The oughing
mill consis s o one ho izon al s and wi h ou olls, he so-
called qua o s and and an op ional e ical olling s and wi h
wo olls, he so-called edge (no shown in he igu e).
The slab geome ies may a y. Usually, hey ha e
an inpu hickness,hini , be ween 200 mm and 300 mm,80
wid h o 600 mm o 2500 mm and leng h be ween 3 m
and 10 m o s eel p oduc ion. Fo aluminum, he hick-
ness a e discha ge is commonly a ound 600 mm be-
cause he empe a u e loss o aluminum du ing olling is
much less han o s eel. A e discha ging, he i s ma-85
jo p ocess is o educe he hickness o he slab by 30
mm o 40 mm. This is done in a so-called oughing mill
(RM). The oughing mill in a con en ional ho s ip mill
consis s o one ho izon al s and wi h ou olls, which is
hen called qua o s and and an op ional e ical olling90
s and wi h wo olls, he so-called edge (no shown in
he igu e). The edge is op ional and has he ask o
educe he wid h o he slab and o imp o e he shape
o he slab especially a bo h ends.
The educ ion om he ini ial hickness hini down95
o he a ge hickness h a ge is done in se e al de o -
ma ion s eps which a e called passes. In each o hese
de o ma ion s eps, he hickness o he slab will be con-
inuously educed un il he a ge hickness is a ained.
The educ ion has o be spli o se e al passes because100
he easible educ ion in one pass is limi ed. The de-
o ma ion in he oughing mill can be done in bo h
ope a ing di ec ions. Hence, each pass changes he di-
ec ion o mo emen o he slab. The o al numbe o
passes has o be odd, since he slab has o be mo ed o105
he nex p ocess s ep. A e olling in he oughing mill,
he slab is ans e ed in he di ec ion o he inishing
mill. I a coilbox is used, he ma e ial is coiled i s and
hen di ec ly uncoiled o s a he olling in he inish-
ing mill. He e, he p oduc is olled in se e al s ands o110
he inal hickness (speci ied by by he cus ome ) and is
di ec ly cooled a e wa ds. The addi ional cooling line
is only used o s eel mills. Finally, he p oduc is coiled
in he downcoile .
One impo an quali y c i e ion o he inal p od-115
uc is he de ia ion o he ac ual hickness om he
a ge hickness h a ge . The hickness de ia ion a he
head o he p oduc is ypically a esul o he oll o ce
p edic ion accu acy o he physical model. The head
o he p oduc is he i s pa which encoun e s he120
de o ma ion. In inishing mills we will mos o en ind
hickness gauges a e he las s and. These a e used o
con ol he hickness once he head passes he gauge so
he oll o ce de ia ion would mainly be esponsible o
he head hickness. Addi ionally, he oll o ce is used125
as e e ence o he bending and o p o ile con ol and
is he e o e also e y impo an o he p oduc p o ile.
Inline con ol o he hickness is usually no ins alled
in o he mill ypes such as pla e mills. This is because
he o al leng h o he p oduc is much smalle han130
in mills wi h coil p oduc ion, whe e he o al leng h
Me a-model based op imiza ion o ho olling p ocesses in he me al indus y 3
migh accumula e o mo e han 1000m. In ha case, a
eedback o he measu ed hickness du ing olling can
be used o adjus he oll gap and he e o e he inal
hickness. Fo mill ypes wi hou inline con ol, i is135
c ucial o imp o e he oll o ce p edic ion in o de o
minimize he hickness de ia ion.
Ano he aspec is he h oughpu o he mill, which
should always be maximized. To maximize he h ough-
pu , he numbe o de o ma ion s eps, i.e. he numbe 140
o passes, should be minimized wi hou iola ing o he
cons ain s. Two o he mos limi ing pa ame e s when
ying o inc ease he educ ion in each pass a e (i) he
maximum oll o ce capabili y and (ii) he maximum
oll o que capabili y o he s and. The e o e, i is es-145
sen ial o ha e good models o he p edic ion o oll
o ce and o que.
As men ioned abo e, de ia ions in oll o ce p e-
dic ion will also a ec he hickness and he e o e he
quali y o he p oduc . Because cu en ma ke equi e-150
men s co e a e y wide ange o ma e ials and geome-
ies i is impo an o inc ease he model quali y o
he oll o ce p edic ion o all p oduc s which may be
olled on hese mills. Ideally, he oll o ce p edic ion
is comple ely independen o he geome y and o he 155
pa ame e s and will only depend on he quali y o he
ma e ial pa ame e s. Each ma e ial is usually classi ied
acco ding o i s chemis y. A ma e ial da abase s o es
mechanical and he mophysical pa ame e s o he de-
sc ip ion o he di e en p ope ies o each class. These160
pa ame e s a e used o he p edic ion o beha io du -
ing he de o ma ion p ocess and a e he e o e o majo
impo ance o he olling p ocess.
2.2 Flow Cu e and Roll Fo ce Model
The low cu e pa ame e s a e mos ele an o he
oll o ce model. The low cu e exp esses he ma e ial
esis ance du ing plas ic de o ma ion in dependence on
he chemis y, he empe a u e, he de o ma ion and
he de o ma ion a e. The de o ma ion ϕ, also called
e ec i e, loga i hmic de o ma ion o ue s ain is ex-
p essed by:
ϕ= ln h0
h1
.
He e, h0is he inpu hickness and h1is he ou pu
hickness o he pass. The i s low cu e o mulas we e
de eloped by Geleji and Ekelund a ound 1950. These
o mulas we e only linea ly dependen on he empe a-
u e and only alid o s anda d low ca bon s eel [10].
A e wa ds se e al o he o mulas we e de eloped wi h
polynomial componen s and exponen ial e ms which
also ook in o accoun he de o ma ion and de o ma-
ion a e. While he i s o mulas we e only alid o
some low alloyed ca bon s eels, Hajduk de eloped o -
mulas which we e also alid o some medium and high
alloyed ca bon s eels [9],[8]. A good o e iew and de-
sc ip ion o he di e en low cu es can be ound in
[10, 12, 26]. These o mulas model he de o ma ion e-
sis ance,k , in dependence on he de o ma ion ϕ, he
de o ma ion a e, ˙ϕ, and he empe a u e,ϑ. The de-
o ma ion esis ance o low s ess exp esses he s ess
which is needed o sus ain a plas ical de o ma ion. In
gene al, he de o ma ion a e can be o mula ed as:
k =AKϕKϑK˙ϕ,
whe e A∈R+is a cons an ac o and he e ms K(·)
165
ep esen unc ions o he co esponding a iables ϕ,
˙ϕ, and ϑ, espec i ely. The mos common model o
hese o mulas was de eloped by Hensel and Spi el [10].
I was ex ended a he Uni e si y o F eibe g. Thus,
hese ex ensions a e called F eibe ge App oach. The170
ex ended e sions o his low cu e model gi es a be -
e app oxima ion o he low s ess wi hin high de o -
ma ion g ades. Some o he a ailable low cu e mod-
els, which a e ypically used in p ocess models o ho
olling, a e p esen ed in Table 1. Thei co esponding175
equa ions ead as ollows.
k =k ,0A0A1em1ϑA2ϕm2em4
ϕA3˙ϕm3(1)
k =A0em1ϑϕm2em4
ϕ˙ϕm3(2)
k =A0em1ϑϕm2em4
ϕ(1 + ϕ)m5ϑem7ϕ˙ϕm8ϑ(3)
k =k ,0A1em1ϑA2ϕm2A3˙ϕm3(4)
The mul iplie s Ai(i= 0,1,2,3) can be educed o
one pa ame e , A. The pa ame e s mj(j= 1,2,...,8)
a e de ining he exponen ial beha io o he ma e ials
in dependence o he empe a u e ϑ, he de o ma ion180
ϕ, and he de o ma ion a e ˙ϕ. The pa ame e s ϑ,ϕ,
and ˙ϕa e de ining he wo king poin in each de o ma-
ion. The alue k ,0used in he equa ions (1) and (4)
is he basic de o ma ion and is calcula ed by empi ical
o mula ions based on he chemis y. Each ma e ial is185
classi ied acco ding o i s chemis y and ge s i s own
pa ame e se Mwi h pa ame e alues m1 o m8and
A0 o A3, espec i ely. Usually, he e is one pa ame e -
se M o each ma e ial, which is hen alid o a spe-
ci ic equa ion only. Besides he pa ame e alues o 190
he models also he alid egion o hese pa ame e s is
s o ed. Summa izing, he pa ame e s k , ϕ, ˙ϕ, and ϑ,
he mul iplica o s Ai, mj, (i= 0,1,2,3; j= 1,...,8),
and ela ed unc ions k ,0, Kϕ, K ˙ϕ, Kϑ, a e used.
Nowadays, hund eds o di e en ma e ials a e known.195
The pa ame e k is almos linea ly co ela ed wi h he

4 Ch is ian Jung e al.
Table 1 O e iew o ypical equa ions o he eg ession o
he ma e ial low s ess. The mul iplie s Aia e educed o
one pa ame e , A. Pa ame e s mja e de ining he exponen ial
beha io o he ma e ials in dependence o he empe a u e ϑ,
he de o ma ion ϕo he de o ma ion a e ˙ϕwhich de ines he
wo king poin . Pa ame e k ,0is de ined by a simple equa ion
based on he chemis y. En ies in he column ”Equa ion”
e e s o he equa ions de ined on p. 3.
Eq. Name #Pa ams Pa ame e Lis
(1) F eibe g 1 5 A, m1, m2, m3, m4
(2) F eibe g 4 5 A, m1, m2, m3, m4
(3) F eibe g 8 7 A, m1, m2, m4, m5, m7, m8
(4) Hensel
Spi el
4A, m1, m2, m3
oll o ce and oll o que. Thus, he model p edic ion
quali y and he ewi h he p ocess s abili y and p od-
uc quali y a e co ela ed o he pa ame e -se M. I is
he e o e impo an o op imize hose pa ame e s in o -200
de o inc ease he model quali y and o ensu e a s able
p ocess wi h maximum h oughpu and p oduc qual-
i y. A s anda d p ocedu e o ob aining hese pa ame-
e s is he measu emen o he de o ma ion esis ance
in a labo a o y. Those measu emen s can be used o a205
eg ession on o one o he o mulas shown in Equa ions
(1) o (4). O cou se, o he o mulas exis , and migh
be used o eg ession. Especially when ying o model
he de o ma ion o mic o alloyed o high alloyed s eel
o when complex ma e ials wi h phase ans o ma ions210
should be desc ibed hese o he models migh be mo e
sui able.
2.3 Desc ip ion o he analy ical model
The analy ical model used o he calcula ion o he oll
o ce is based on he elemen a y olling heo y [12, 27].215
Some o he limi a ions o ha heo y a e compensa ed
wi h co ec ion unc ions. Fo example, one o he e-
qui emen s o he elemen a y heo y is ha du ing
each pass he e is a comple e plas ic de o ma ion o he
whole ma e ial. Fo p oduc s wi h hickness abo e 500220
mm his is clea ly no gi en. The e o e, a compensa ion
cu e, which is empi ically de e mined, is applied. Fo
he calcula ion o he oll o ce in each pass he de o -
ma ion zone is di ided in o single s ipe-like elemen s
and he o ce balance o each s ipe is calcula ed. The225
solu ion yields o he basic di e en ial equa ion o he
plas ically de o ma ion heo y which was de eloped by
Ka man in 1925. When calcula ing he oll o ce o
one pass, he low esis ance has o be conside ed. This
low esis ance k is ma e ial dependen and is in lu-230
enced by he pa ame e alues o ϕ, ˙ϕand ϑ. Fu he -
mo e, he o ces induce empe a u e in o he ma e ial
so he calcula ion o he nex pass depends on he p e-
ious passes. Op imizing he low cu e by analyzing
he olling esul s is no su icien . I he pa ame e o 235
he low cu e changes, he whole p ocess has o be sim-
ula ed again and hen he calcula ed oll o ces based
on he new low cu e can be compa ed wi h he o ig-
inal eedback, i.e., measu emen s o oll o ce, o que,
empe a u e, and speed. Addi ionally, i is also no su -240
icien o op imize he esul o a single p oduc be-
cause he pa ame e s ϕ, ˙ϕand ϑmay no a y enough
o achie e s able esul s. The e o e i is p e e able o
conside a campaign wi h a wide a ia ion o p oduc
geome ies, empe a u e anges, and de o ma ions.245
2.4 S anda ds in Indus y
Cu en ly, he a ailable concep s o he op imiza ion o
low cu e pa ame e s a e mos ly dealing wi h de e mi-
na ion o hose pa ame e s in labo a o y a he han
op imizing hose pa ame e s wi h eal p ocess da a.250
T adi ionally, he pa ame e s a e measu ed wi h small
samples o one piece in labo a o y and a e hen gene -
alized o e e y ma e ial which is close o he sample
in e ms o ma e ial composi ion. Some companies a e
modi ying he low cu e pa ame e s wi h linea mod-255
els. Tha is, hey a e de e mining he p edic ion accu-
acy o hei model and a e a ying some o he in lu-
ence pa ame e s. Mos o he esea ch in his a ea is on
he de elopmen o sui able low cu e equa ions espe-
cially o high and mic o alloyed s eel [11, 19, 28] a he 260
han using a da a d i en app oach o he op imiza ion
o hose pa ame e s.
3 P oblem Desc ip ion
Acco ding o ou bes knowledge, low cu e pa ame e
de e mina ion in labo a o y as desc ibed in Sec. 2 will265
equi e se e al weeks and cos s se e al housand Eu o
o he equi ed ma e ials. Some imes, his is no a -
o dable and he e o e no a sui able way o de e mine
hose pa ame e s. Hence, we a e looking o a cheape
app oach o pa ame e es ima ion.270
Due o hei highly nonlinea beha io , he low
cu e equa ions canno be sol ed di ec ly. Fu he mo e,
a di e en oll o ce would esul in a di e en empe -
a u e balance o he p oduc and hus he empe a u e
in he nex pass di e s om he o iginal calcula ion.275
Because hese aspec s canno be neglec ed, we ha e o
simula e a whole scena io when es ing new pa ame e
se s o he low cu e o a speci ied ma e ial. The cal-
cula ions o he oll o ces and oll o ques wi hin his
simula ion a e a e wa ds compa ed wi h he measu e-280
men s o ge a quali y c i e ion o he new pa ame e
Me a-model based op imiza ion o ho olling p ocesses in he me al indus y 5
se . The de ailed desc ip ion o he simula ion scena io
is p esen ed in Chap e 4.
I is impo an ha he simula ion scena io beha es
in he same way as he online p ocess. The e o e, he285
simula ion uses eedback o he measu ed speed, he
educ ion, and empe a u e o calcula e he new se -
ings. This enables he simula ion o achie e he same
wo king poin as in he online p ocess. Ano he p ob-
lem can be he amoun o da a. The simula ion o a290
whole ba ch whe e only one ma e ial g oup was olled
consis s o housands o di e en de o ma ion s eps and
will he e o e be highly expensi e in e ms o simula ion
ime. Se e al op imiza ion algo i hms equi e bound
cons ain s o he op imized pa ame e s. In ou case,295
pa ame e s Aand mia e dependen on each o he . The
only limi a ion which can be se is a plausible egion o
he esul ing alue k o he basic de o ma ion. In ho
mills, he maximum basic de o ma ion alue o k is
usually below 300 N
mm2, bu always posi i e. Then, o a300
gi en maximum wo king ange o he de o ma ion, de-
o ma ion a e, and empe a u e, he easibili y o he
pa ame e se can be es ed.
Due o he ac ha e e y company has usually i s
own classi ica ion sys em i migh be ha ma e ials305
which a e g ouped oge he in one company a e sepa-
a ed in o he companies. In his case, he op imiza ion,
which has been done in he i s company canno be di-
ec ly used o o he companies and has o be enewed
e e y ime.310
Summa izing, i is desi able o op imize he p ocess
in o de o
– eliably es ima e alid low cu es,
– educe lab cos s,
–sa e ime,315
–de e mine pa ame e s in hei wo king en i onmen s,
and
–make he p ocess mo e lexible and adap o new
(ma e ial) changes quickly.
4 Me hodology320
4.1 Simula ion en i onmen
The en i onmen o he online p ocess is shown in Fig. 2.
Fi s o all he model ge s in o ma ion abou he p od-
uc which includes ini ial geome y da a, discha ging
empe a u e da a, and in o ma ion abou he chemis y325
o he p oduc . The discha ge empe a u e is an ini-
ial empe a u e ield o he p oduc . One pa o he
olling model calcula es he empe a u es losses du ing
he whole p ocess. Finally, he impo an pa ame e ϑ
is a esul o he empe a u e losses om discha ge o330
ha poin o he p ocess. Fu he mo e, a ge da a is
Fig. 2 Model en i onmen in he eal-wo ld p ocess o each
pass: The p oduc and cus ome da a such as ma e ial de-
sc ip ion, ini ial and a ge geome y (1) a e combined wi h
ope a o da a (2) and a e ed o he model which calcula es
all equi ed se ings (3) o he nex olling pass (se up o
nex pass). A e olling o his pass he model ge s eedback
(4) o he jus olled pass and combines his in o ma ion o
he ecalcula ion o he p e ious pass and o he nex calcu-
la ions (2-4). Addi ionally, changes om he ope a o o he
nex pass a e send o he model. The p oduc and cus ome
da a a e only p oduc and no pass dependen and may only
be send once. To enable a simula ion o his p ocess e e y in-
and ou pu o he model is s o ed in a da abase.
Fig. 3 Model en i onmen o he o line simula ion. The
da a which has been collec ed in he eal wo d p ocess is
send o he model which calcula es a new se up o he nex
pass. This se up may be di e en om he o iginal one. Bu
because o he ac ha we also s o e he eedback om he
d i es and gauges he model will ecei e also he o iginal se -
ing and ecalcula es he pass as i eally has been olled.
also coming om he cus ome . Bo h da a can be seen
as cons an and a e deno ed wi h Ncons , i.e., he ope a-
o canno change hem as hey a e pa o he p oduc-
ion planning sys em which handles he o de s o he335
mill owne . A e wa ds, he Ncons is used o calcula e
he i s se ings o he mill and his esul is shown o
he ope a o . The se ing consis s o oll gap se ings,
speed se ings, geome y, empe a u e and ime calcu-
la ions. Wi h his da a he i s planned se ings NSe ,340
which also include he pa ame e ϕ, ϑ and ˙ϕ, a e calcu-
la ed and a e shown o he ope a o . The ope a o can
in e e e and modi y he way his p oduc is olled. This
is e e ed o as olling s a egy. This olling s a egy
de ines how a p oduc is olled which includes olling345
speed, numbe o passes, de o ma ions, speed se ings,
6 Ch is ian Jung e al.
possible olling b eaks and much mo e. These s a egies
may also be speci ic cons ain s like absolu e educ ion,
de o ma ion ϕ, o ce, o que, bu also o he es ic ions
o he p ocess like d i e limi a ions.350
I he ope a o is sa is ied wi h he se ings NSe
calcula ed by he model, he se ings a e sen o he
plan whe e he i s pass is olled. A e his pass,
all measu emen s collec ed du ing olling which include
o ces, o ques, speeds, empe a u es, gap se ings, de-355
lay imes, and se e al mo e da a, a e sen o he model
and he da abase bu a e also shown o he ope a o .
Now, he ope a o and also he model can adap he se -
ings o he nex passes and eac o any unexpec ed
beha io o he mill. Usually, no big changes a e made360
by he ope a o and he olling o he u he passes is
s a ed di ec ly. Again, o each pass he se ings a e
sen o he plan and he eedback o measu emen s is
ecei ed om he plan . Fo analysis and o line simu-
la ions all inpu s and ou pu s a e s o ed in a da abase.365
This da abase is he basis o he o line simula ion
shown in Figu e 3. He e, we eed he same model which
was used in he online p ocess wi h he da a s o ed du -
ing he eal-wo ld p ocess. The e o e we can gua an ee
ha he model eac s in he same way as i would eac 370
in he olling p ocess. The da a, which was coming om
he ope a o and he geome y da a a e aken om he
da abase. Hence, he model will no ecognize i i is
used o an o line calcula ion o o an online scena io.
Al hough i may calcula e di e en se ings o he p o-375
cess, i will ecei e he o iginal eedback om he plan
and calcula e e e y hing based on he o iginal se ings.
Fo a p oduc wi h 19 passes he model is igge ed
20 imes. The i s igge c ea es he ini ial se up and
all o he igge s a e eedbacks o he 19 passes wi h380
which he o iginal p oduc s we e olled. The only di e -
ence a e he pa ame e s used o he calcula ion o he
oll o ce. The e o e, we ha e a calcula ed and measu ed
alue o he o ce and o que o each p oduc and pass
o e e y un. A e each simula ion un, he pa ame-385
e s may be changed and esul s o di e en pa ame e s
may be compa ed. This enables he op imiza ion o he
low cu e pa ame e s. Minimiza ion o he Roo Mean
Squa e E o (RMSE) o he p edic ed oll o ce is he
op imiza ion objec i e.390
4.2 Su oga e Modeling
I he simula ion uns o he o iginal p oblem in gene al
a e e y expensi e in e ms o e alua ion i would be
e y ime consuming o pe o m pa ame e op imiza-
ion on hose o iginal scena ios. The e o e, we use a395
su oga e-model based op imiza ion app oach. Su o-
ga e models a e supposed o eplace he o iginal, expen-
si e simula ion model and a e expec ed o be cheape
o calcula e.
The analy ical models, as in oduced in Sec. 2.2,400
a e cheape o e alua e in compa ison o he ini e ele-
men me hod models. In his pape , he e m su oga e
model is used o desc ibe da a d i en models, which a e
buil om an analy ical model. The e o e, he simula-
ion uns on he analy ical model wi h a speci ied se o 405
p oduc s is he expensi e model. The p oduc s which
a e simula ed usually belong o he same ma e ial g oup
and ha e p e iously been olled in a se ies on a eal
olling mill. Each p oduc is calcula ed as i would be
done du ing olling. The e o e, ime delays which oc-410
cu ed du ing he eal p oduc ion a e also aken in o
accoun .
Ou da a is sou ced om a e e sing aluminum ho
mill, which has ypically a ound 19 passes. Hence, we
ha e mo e han 20 calcula ions o each p oduc be-415
cause he model is igge ed a e inishing each pass.
The da a o each pass is sen o he model, which may
eac on unp edic ed ci cums ances.
In gene al, da a-d i en su oga e models can be any
kind o models, e.g., a i icial neu al ne wo ks, linea 420
models, K iging, andom o es and o he s. A de ailed
o e iew o su oga e model based nume ical op imiza-
ion is p esen ed by Jin [13] and Jones [15].
One amewo k o su oga e-model based op imiza-
ion is sequen ial pa ame e op imiza ion (SPO) [3].425
SPO combines me hods om classical DoE and mode n
Design and Analysis o Compu e Expe imen s (DACE) [2,
4] based on K iging models.
Algo i hm 1 p esen s he pseudo code o SPO, as
adap ed o he applica ion o ho mill pa ame e op i-430
miza ion. No e, ha we will use he no a ion x(i), y(i)
o he da a om he i- h pass which is passed o he
su oga e model. Du ing he i s s age o expe imen a-
ion, SPO explo es he sea ch space o he op imiza ion
p oblem A, which is ea ed as a black box. A se o in-435
pu design poin s xis passed o A. Usually hese a e
c ea ed by a space illing design, e.g. La in hype cube
sampling. Each call o he objec i e unc ion p oduces
some ou pu y ega ding i s pe o mance.
SPO now ies o de e mine a unc ional ela ion-440
ship be ween xand y.SPO hus uses a model Y(x) as
su oga e o he ho mill simula ion model A. As men-
ioned abo e, he chosen model ype is K iging K iging
is equen ly used o su oga e-model based op imiza-
ion, because i p o ides a powe ul and lexible p edic-445
o . I also p o ides an es ima e o he a iance o e o
o each p edic ion. The obse a ions a e in e p e ed as
ealiza ions o a s ochas ic p ocess. A gaussian ke nel is
used o model he co ela ion be ween obse a ions [23].
Me a-model based op imiza ion o ho olling p ocesses in he me al indus y 7
Algo i hm 1: SPO-based ho mill simula ion
uning.
// phase 1, collec ini ial knowledge abou he
op imized p ocess:
1le Abe he ho mill simula ion model we wan o
une;
2gene a e an ini ial design DES = {x(1),...,x(n)}o n
pa ame e ec o s;
3le k=k0be he ini ial numbe o eplica ions o
de e mining es ima ed esponses;
4 o each x ∈DES do
5 un Awi h x o de e mine he es ima ed esponse
yo x;
// phase 2, building, using and imp o ing a
su oga e model:
6while s op c i e ia no eached do
7build su oga e model Y(x) based on DES and
{y(1),...,y(|DES|)};
8op imize he model w. . some cos unc ion and
cons ain s, hus p oduce a se DES’ o dnew
pa ame e ec o s ;
9 un Awi h each x∈DES’ o de e mine he
esponse;
10 ex end he design by DES = DES ∪DES’;
// phase 3, inal exploi a ion and ine uning:
11 use local op imize o he bes ppa ame e se s
x1...p ∈DES, wi hou cons ain s
In he sequen ial imp o emen loop SPO op imizes450
he su oga e model Y(x) o e he conside ed space o
inpu a iables by means o a cos unc ion. Once he
new se o design poin s DES’ has been selec ed, he
equi ed e alua ions o DES’ a e pe o med. Based on
DES’, he su oga e model Y(x) is upda ed.455
In s ep 8 o Algo i hm 1, a sea ch on he su o-
ga e model is pe o med. He e, he cons ain s o he
mill pa ame e iza ion p oblem ha e o be conside ed.
As he cons ain s a e no expensi e o e alua e, hey
a e e alua ed oge he wi h he su oga e model i sel .460
Fo he inequali y cons ained op imiza ion, we use he
popula me hod de eloped by Powell [21, 22], which
does no equi e any de i a i es o he objec i e unc-
ion o be a ailable. Du ing his op imiza ion s ep 8,
he nex poin x o e alua e in he sequen ial loop o 465
SPO is de e mined. Fo expensi e, global, black-box
op imiza ion Jones [14] in oduced e icien global op i-
miza ion (EGO). EGO exploi s he in o ma ion gi en
om a K iging model, i.e., he p edic ed mean and a i-
ance, o compu e he expec ed imp o emen (EI) o a470
gi en solu ion. EI can hence be used as a cos unc ion
du ing s ep 8, as an al e na i e o he p edic ed alue
o he K iging model.
In s ep 11, he well known downhill simplex algo-
i hm in oduced by Nelde and Mead [20] is used o im-475
p o e he bes ound esul s by a local op imiza ion p o-
cedu e. We choose he downhill simplex implemen a ion
in he nlop R package. Du ing local e inemen , con-
s ain s a e dis ega ded because hey no longe play a
ole in he egion o good solu ions.480
5 Expe imen al Se up
In ou case, he pa ame e op imiza ion was based on
Equa ion (1). The easible ange was 0 ≤k ≤300.
Tha is, solu ions ha esul in o nega i e k alues o
k alues la ge han 300 a e conside ed o be in easible.
The usual wo king poin o ou es da a was in he
ollowing ange:
0≤ϕ≤0.5, 0 ≤˙ϕ≤600, 500 ≤ϑ≤600.
Wi h ha said, he op imiza ion p oblem o be sol ed
in his s udy is de ined as ollows:
–Pa ame e s o be changed a e he low cu e pa am-
e e ec o mand he consolida ed pa ame e Ao 485
he low cu e.
–The de ia ion o simula ed oll o ce om he mea-
su ed oll o ce is minimized.
–Compu a ional cons ain s: The e alua ions o he
objec i e unc ion is expensi e. (see Sec ion 4.2)490
The pa ame e s which ep esen he sea ch space and
we e subjec o op imiza ion in his s udy a e summa-
ized in Table 2.
To e alua e he success o he op imiza ion, he e-
sul ing pa ame e se is compa ed o a well-known, es-495
ablished pa ame e se used in p ac ice so a . This
old pa ame e se has been de e mined by expe s ac-
co ding o bes knowledge om li e a u e on simila
ma e ials.
We ha e chosen he SPO oolbox (SPOT) o con-500
duc he expe imen s [5]. SPOT i sel has pa ame e s
as well ha a e se acco ding o he au ho s expe ience:
–The chosen su oga e model is K iging, based on
code by Fo es e e al. [7].
Pa ame e : seq.p edic ionModel. unc.505
–The ini ial design consis s o 40 candida e solu ions,
which a e c ea ed by La in Hype cube Sampling
(LHS).
Pa ame e : ini .design.size.
Table 2 Uppe and lowe bounds o he pa ame e se M
in oduced in sec ion 2.2 which was used du ing he op imiza-
ion. All pa ame e s a e o ype FLOAT.
Fac o Low High
A0 2
m1-0.01 0
m2-0.3 0.4
m30 0.2
m4-0.1 0.1
14 Ch is ian Jung e al.
8. Hajduk, M., Zidek, M., El ma k, J., Kopec, S.:
De i a ion o mean alues o inhe en de o ma ion
esis ance in ho olling o onnage s eel. Hu nicke825
Lis y 27(8), 567 (1972)
9. Hajduk, M., e al.: E ec o imp ope selec ion o
he pm o e ical and ho izon al d i es on bal-
anced olling o ce dis ibu ion in a uni e sal olling
mill. Hu nicke Lis y 27(8), 259 (1972)830
10. Hensel, A., Spi el, T.: K a - und A bei sbeda
bildsame Fo mgebungs e ah en. Ve lag G und-
s o indus ie (1978)
11. He nandez, C., Medina, S., Ruiz, J.: Mod-
elling aus eni e low cu es in low al-835
loy and mic oalloyed s eels. Ac a Ma-
e ialia 44(1), 155 – 163 (1996). DOI
h p://dx.doi.o g/10.1016/1359-6454(95)00153-4.
URL h p://www.sciencedi ec .com/science/
a icle/pii/1359645495001534840
12. Hink o h, R.: Massi um o mung. Wissenscha s-
e lag, Aachen (2003)
13. Jin, Y.: A comp ehensi e su ey o i ness app oxi-
ma ion in e olu iona y compu a ion. So Compu -
ing 9(1), 3–12 (2005)845
14. Jones, D., Schonlau, M., Welch, W.: E icien
global op imiza ion o expensi e black-box unc-
ions. Jou nal o Global Op imiza ion 13, 455–492
(1998)
15. Jones, D.R.: A axonomy o global op imiza ion850
me hods based on esponse su aces. J. o Global
Op imiza ion 21, 345–383 (2001). DOI h p://
dx.doi.o g/10.1023/A:1012771025575. URL h p:
//dx.doi.o g/10.1023/A:1012771025575
16. Kleijnen, J.P.C.: Design and analysis o simula ion855
expe imen s. Sp inge , New Yo k NY (2008)
17. Lambiase, F.: Op imiza ion o shape olling se-
quences by in eg a ed a i icial in elligen ech-
niques. The In e na ional Jou nal o Ad anced
Manu ac u ing . . . 68(1-4), 443–452 (2013)860
18. Mancini, E., Campana, F., Sasso, M., Newaz, G.:
E ec s o cold olling p ocess a iables on inal su -
ace quali y o s ainless s eel hin s ip. The In-
e na ional Jou nal o Ad anced Manu ac u ing . . .
61(1-4), 63–72 (2012)865
19. Mandal, S., Rakesh, V., Si ap asad, S., Venugopal,
S., Kasi iswana han, K.V.: Cons i u i e equa ions
o p edic high empe a u e low s ess in a Ti-
modi ied aus eni ic s ainless s eel. Ma e ials Sci-
ence and Enginee ing (2009)870
20. Nelde , J., Mead, R.: A simplex me hod o unc-
ion minimiza ion. Compu e Jou nal 7, 308–313
(1965)
21. Powell, M.: A e iew o algo i hms o nonlinea
equa ions and uncons ained op imiza ion. In: P o-875
ceedings ICIAM, pp. 220–232 (1988)
22. Powell, M.: A di ec sea ch op imiza ion me hod
ha models he objec i e and cons ain unc-
ions by linea in e pola ion. Tech. Rep. DAMTP
1992/NA5, Depa men o Applied Ma hema ics880
and Theo e ical Physics, Uni e si y o Camb idge,
England (1992)
23. Sacks, J., Welch, W.J., Mi chell, T.J., Wynn, H.P.:
Design and analysis o compu e expe imen s. S a-
is ical Science 4(4), 409–435 (1989)885
24. Sheu, J.J.: Simula ion and op imiza ion o he cold
oll- o ming p ocess. In: AIP, pp. 452–457. AIP,
Mel ille, NY (2004)
25. Sun, J., Du, F., Li, X.: FEM Simula ion o he Roll
De o ma ion o Six-high CVC Mill in Cold S ip890
Rolling. In: 2008 In e na ional Wo kshop on Mod-
elling, Simula ion and Op imiza ion (WMSO), pp.
412–415. IEEE (2008)
26. Tseliko , A., Niki in, G., Roko yan, S.: The Theo y
o Leng hwise Rolling. Mi Publishe s (1981)895
27. Webe , K.: G undlagen des Bandwalzens. VEB
Deu sche Ve lag ue G unds o indus ie, Leipzig
(1973)
28. Y.C. Lin Ming-Song Chen, J.Z.: P edic ion o
42c mo s eel low s ess a high empe a u e and900
s ain a e. Meachanics Resea ch Communica ions
(2008)

Kon ak /Imp essum
Diese Ve ö en lichungen e scheinen im Rahmen de Sch i en eihe "CIplus". Alle Ve ö -
en lichungen diese Reihe können un e
h ps://cos.bibl. h-koeln.de/home
abge u en we den.
Die Ve an wo ung ü den Inhal diese Ve ö en lichung lieg beim Au o .
Da um de Ve ö en lichung: 14.11.2017
He ausgebe / Edi o ship
P o . D . Thomas Ba z-Beiels ein,
P o . D . Wol gang Konen,
P o . D . Bo is Naujoks,
P o . D . Ho s S enzel
Ins i u e o Compu e Science,
Facul y o Compu e Science and Enginee ing Science,
TH Köln,
S einmülle allee 1,
51643 Gumme sbach
u l:
www.ciplus- esea ch.de
Sch i lei ung und Ansp echpa ne / Con ac edi o ’s office
P o . D . Thomas Ba z-Beiels ein,
Ins i u e o Compu e Science,
Facul y o Compu e Science and Enginee ing Science,
TH Köln,
S einmülle allee 1, 51643 Gumme sbach
phone: +49 2261 8196 6391
u l:
h p://www.spo se en.de
eMail: homas.ba z-beiels ein@ h-koeln.de
ISSN (online) 2194-2870
This wo k has been pa ially suppo ed by he MIWF NRW
unde g an ag eemen FH-STRUKTUR 2014/10 (ISAFAN).