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MRI-Based Computational Torso/Biventricular Multiscale Models to Investigate the Impact of Anatomical Variability on the ECG QRS Complex

Abstract

Aims:Patient-to-patient anatomical differences are an important source of variability in the electrocardiogram, and they may compromise the identification of pathological electrophysiological abnormalities. This study aims at quantifying the contribution of variability in ventricular and torso anatomies to differences in QRS complexes of the 12-lead ECG using computer simulations. Methods:A computational pipeline is presented that enables computer simulations using human torso/biventricular anatomically based electrophysiological models from clinically standard magnetic resonance imaging (MRI). The ventricular model includes membrane kinetics represented by the biophysically detailed O’Hara Rudy model modified for tissue heterogeneity and includes fiber orientation based on the Streeter rule. A population of 265 torso/biventricular models was generated by combining ventricular and torso anatomies obtained from clinically standard MRIs, augmented with a statistical shape model of the body. 12-lead ECGs were simulated on the 265 human torso/biventricular electrophysiology models, and QRS morphology,duration and amplitude were quantified in each ECG lead for each of the human torso-biventricular models. Results:QRS morphologies in limb leads are mainly determined by ventricular anatomy,while in the precordial leads, and especially V1 to V4, they are determined by heart position within the torso. Differences in ventricular orientation within the torso can explain morphological variability from monophasic to biphasic QRS complexes. QRS duration ismainly influenced by myocardial volume, while it is hardly affected by the torso anatomyor position. An average increase of 0.12±0.05 ms in QRS duration is obtained for eachcm3of myocardial volume across all the leads while it hardly changed due to changes in torso volume. Conclusion:Computer simulations using populations of human torso/biventricular models based on clinical MRI enable quantification of anatomical causes of variability in the QRS complex of the 12-lead ECG. The human models presented also pave theway toward their use as testbeds in silico clinical trials Mincholé, Ana; Zacur, Ernesto; Ariga, Rina; Grau, Vicente; Rodriguez, Blanca

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MRI-Based Computational Torso/Biventricular Multiscale Models to Investigate the Impact of Anatomical Variability on the ECG QRS Complex

Author: Mincholé, Ana; Rodriguez, Blanca; Grau, Vicente; Zacur, Ernesto; Ariga, Rina
Year: 2019
DOI: 10.3389/fphys.2019.01103
Source: https://zaguan.unizar.es/record/99441/files/texto_completo.pdf
phys-10-01103 Augus 24, 2019 Time: 16:24 # 1
ORIGINAL RESEARCH
published: 27 Augus 2019
doi: 10.3389/ phys.2019.01103
Edi ed by:
Ja ie Saiz,
Poly echnic Uni e si y o Valencia,
Spain
Re iewed by:
A un V. Holden,
Uni e si y o Leeds, Uni ed Kingdom
Gunna Seemann,
Uni e si y Hea Cen e F eibu g,
Ge many
*Co espondence:
Ana Mincholé
[email p o ec ed]
†These au ho s ha e con ibu ed
equally o his wo k as i s au ho s
‡These au ho s ha e con ibu ed
equally o his wo k as senio au ho s
Special y sec ion:
This a icle was submi ed o
Compu a ional Physiology
and Medicine,
a sec ion o he jou nal
F on ie s in Physiology
Recei ed: 08 Ma ch 2019
Accep ed: 08 Augus 2019
Published: 27 Augus 2019
Ci a ion:
Mincholé A, Zacu E, A iga R,
G au V and Rod iguez B (2019)
MRI-Based Compu a ional
To so/Bi en icula Mul iscale Models
o In es iga e he Impac
o Ana omical Va iabili y on he ECG
QRS Complex.
F on . Physiol. 10:1103.
doi: 10.3389/ phys.2019.01103
MRI-Based Compu a ional
To so/Bi en icula Mul iscale
Models o In es iga e he Impac o
Ana omical Va iabili y on he ECG
QRS Complex
Ana Mincholé1*†, E nes o Zacu 2†, Rina A iga3, Vicen e G au2‡and Blanca Rod iguez1‡
1Depa men o Compu e Science, Uni e si y o Ox o d, Ox o d, Uni ed Kingdom, 2Ins i u e o Biomedical Enginee ing
(IBME), Uni e si y o Ox o d, Ox o d, Uni ed Kingdom, 3Di ision o Ca dio ascula Medicine, Radcli e Depa men
o Medicine, Uni e si y o Ox o d, Ox o d, Uni ed Kingdom
Aims: Pa ien - o-pa ien ana omical di e ences a e an impo an sou ce o a iabili y
in he elec oca diog am, and hey may comp omise he iden i ica ion o pa hological
elec ophysiological abno mali ies. This s udy aims a quan i ying he con ibu ion o
a iabili y in en icula and o so ana omies o di e ences in QRS complexes o he
12-lead ECG using compu e simula ions.
Me hods: A compu a ional pipeline is p esen ed ha enables compu e simula ions
using human o so/bi en icula ana omically based elec ophysiological models om
clinically s anda d magne ic esonance imaging (MRI). The en icula model includes
memb ane kine ics ep esen ed by he biophysically de ailed O’Ha a Rudy model
modi ied o issue he e ogenei y and includes ibe o ien a ion based on he S ee e
ule. A popula ion o 265 o so/bi en icula models was gene a ed by combining
en icula and o so ana omies ob ained om clinically s anda d MRIs, augmen ed
wi h a s a is ical shape model o he body. 12-lead ECGs we e simula ed on
he 265 human o so/bi en icula elec ophysiology models, and QRS mo phology,
du a ion and ampli ude we e quan i ied in each ECG lead o each o he human
o so-bi en icula models.
Resul s: QRS mo phologies in limb leads a e mainly de e mined by en icula ana omy,
while in he p eco dial leads, and especially V1 o V4, hey a e de e mined by hea
posi ion wi hin he o so. Di e ences in en icula o ien a ion wi hin he o so can explain
mo phological a iabili y om monophasic o biphasic QRS complexes. QRS du a ion is
mainly in luenced by myoca dial olume, while i is ha dly a ec ed by he o so ana omy
o posi ion. An a e age inc ease o 0.12 ±0.05 ms in QRS du a ion is ob ained o each
cm3o myoca dial olume ac oss all he leads while i ha dly changed due o changes
in o so olume.
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Mincholé e al. Impac o Ana omy on ECG QRS Complex
Conclusion: Compu e simula ions using popula ions o human o so/bi en icula
models based on clinical MRI enable quan i ica ion o ana omical causes o a iabili y
in he QRS complex o he 12-lead ECG. The human models p esen ed also pa e he
way owa d hei use as es beds in silico clinical ials.
Keywo ds: clinical MRI-based o so/ en icula ana omical models, compu e simula ions, elec oca diog am,
compu a ional modeling, ca diac magne ic esonance imaging
INTRODUCTION
The elec oca diog am (ECG) is he mos widely used clinical
ool o e alua ion o ca diac unc ion. I eco ds he elec ical
ac i i y o he hea om elec odes posi ioned on he pa ien ’s
o so, and he du a ion, ampli ude, and mo phology o ECG
wa e o ms in he di e en leads a e used o pa ien s’ diagnosis
(Mac a lane and Law ie, 2010).
Elec oca diog am ea u es, and speci ically i s QRS complex,
a e a ec ed no only by mic os uc u al and physiological
ac o s such as ibe o ien a ion, Pu kinje, myoca dial conduc ion
pa hways and ionic cu en s (Boineau and Spach, 1968), bu also
by ana omical cha ac e is ics such as hea size and o ien a ion,
en icula wall hickness, and body mass index (Hoekema
e al., 1999, 2001; an Oos e om e al., 2000;Co lan e al.,
2005). Quan i a i e in o ma ion on he la e is, howe e , sca ce.
An expe imen al s udy showed la ge changes in QRS wi h
a ying hea loca ions, using one isola ed pe used dog hea
suspended in an elec oly ic o so ank (MacLeod e al., 2000).
Compu e simula ion s udies a e ideally placed o p o ide
insigh on he unde lying basis o he ECG. Mos o he
p e ious compu a ional s udies ocused on simula ing he ECG
using a single hea ana omy as (Kelle e al., 2010;Zemzemi
e al., 2013;Zemzemi and Rod iguez, 2015;Neic e al., 2017;
Po se, 2018). Mo e ecen ly, a compu a ional s udy using o so-
bi en icula ana omical models o i e pa ien s wi h hea
ailu e showed ha hea posi ion and o ien a ion s ongly
al e ed QRS ampli ude, bu only sligh ly, QRS du a ion (Nguyên
e al., 2015). Sánchez e al. (2018) also p o ided insigh s in o he
key ac o s de e mining he ECG cha ac e is ics based on da a o
six hea ailu e pa ien s. These s udies highligh he po en ial o
compu e simula ion s udies using image-based models o shed
ligh in o he ana omical basis go e ning ECG a iabili y and
he QRS complex.
Whe eas he dense olume ic in o ma ion and high
esolu ion o cu en CT scans is a clea ad an age in he
cons uc ion o ca diac ana omical models (Naza ian and
Halpe in, 2018) o ECG simula ions, he adia ion in ol ed
limi s hei use, o example in heal hy subjec s. The al e na i e
o using magne ic esonance imaging (MRI) scans is e y
a ac i e as hey p o ide good quali y ca diac images sa ely
and non-in asi ely. Clinical p o ocols, howe e , ocus on he
hea and he e o e in o ma ion on he o so is sca ce. This
is why p e ious s udies ha e used MRI scans ob ained using
dedica ed imaging p o ocols, no sui able o ou ine clinical
p ac ice (Po se e al., 2014;Sánchez e al., 2018). Me hodological
ad ances a e he e o e needed o exploi clinically s anda d MRI
da abases in compu e simula ions s udies using image-based
human o so/bi en icula ana omical models.
The goal o his s udy is o conduc a compu e simula ion
s udy using a popula ion o 265 o so- en icula ana omical
models based on clinically s anda d MRI o dissec and quan i y
he indi idual con ibu ion o en icula and o so ana omy on
QRS bioma ke s in he 12-lead ECG. We hypo hesize ha QRS
complexes in each o he s anda d 12-lead ECGs a e a ec ed
di e en ly by geome ical ac o s such as en icula ana omy,
hea o ien a ion and loca ion, o o so ana omy. To es his
hypo hesis, we de elop a compu a ional pipeline o conduc high-
pe o mance compu ing (HPC) elec ophysiological simula ions
using biophysically de ailed compu a ional human models wi h
en icula and o so ana omies ob ained om clinically s anda d
ca diac MRI acquisi ions. In a clinical scena io, he new insigh s
could acili a e an imp o ed disc imina ion in clinical ECG
eco dings be ween he con ibu ions o pa ien ’s ana omical
ea u es and hose a ising om a ca diac condi ion o disease.
MATERIALS AND METHODS
Recons uc ion o Ven icula and To so
Ana omical Meshes F om Clinical MRI
In his s udy, a o al o 265 combined o so- en icles ana omical
models we e conside ed o quan i y he e ec o en icula
and o so olumes, and hea posi ion and o ien a ion on he
QRS complex. Ini ially, as desc ibed in Figu e 1, wen y- i e
human hea - o so models we e gene a ed by combining he bi-
en icula geome ies (H1–H5) and o sos (T1–T5) (including
co esponding hea o ien a ions and posi ions) ex ac ed om
clinical MRI acquisi ion om 5 heal hy subjec s. The MRI
da ase s we e selec ed o include en icula end dias olic
myoca dial olumes be ween 75 and 170 cm3and o so olumes
be ween 23 and 54 dm3. Then, ei he o a ion o ansla ion was
applied o each bi- en icula model wi hin each o so. 5◦s eps
up o (±40◦we e conside ed bo h a ound he long axis (LA) and
a ound he le - o- igh - en icle axis (LR) (Nguyên e al., 2015).
T ansla ion was conside ed in 1 cm s eps up o (±4 cm ei he
along he la e al o along c anio-caudal di ec ions.
The MRI scans we e ob ained in i e heal hy subjec s ( h ee
emales and wo males) wi h a ange o en icula end-dias olic
myoca dial olumes be ween 75 and 170 cm3and o so olumes
be ween 23 and 54 dm3, ec ui ed a John Radcli e Hospi al,
Ox o d, Uni ed Kingdom. Subjec s we e non-smoke s wi hou
ca dio ascula disease, hype ension o diabe es, and no amily
his o y o ca diomyopa hy o sudden ca diac dea h (SCD).
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FIGURE 1 | (A) Compu a ional pipeline om clinical MRI segmen a ions h ough cons uc ion o hea and o so geome ies o he HPC simula ion o
elec ophysiology om ionic o body su ace po en ials. Following MRI segmen a ions, hea su ace is ob ained by emo ing b ea h misalignmen and o so su ace
by using he spa se in o ma ion om he MRI con ou s oge he wi h a s a is ical body shape model. Wi h he olume ic meshes, elec ophysiological p ope ies
such as an ac ion po en ial model and an ac i a ion model a e used o simula e elec ical ac i i y om cell o o so and calcula e he 12-lead ECG. (B) 25
o so- en icula ana omical models combining i e o sos (T1–T5) and i e en icles (H1–H5) o a ying olumes. (C) Hea pose wi hin he o so de ined as he
ans o ma ion om a canonical coo dina e sys em o he en icula geome y o he o so coo dina e sys em.
Clinically s anda d cine ca diac MRI acquisi ion was pe o med
o each subjec , including long axis (LAX) and a s ack o sho
axis (SAX) iews. Mo e speci ically, o each subjec , he da a
includes a 2 chambe LAX iew, 4 chambe iew, and a s ack o
SAX iew om apex o base wi h 10 mm o sepa a ion be ween
adjacen slices in he s ack (8 mm slice hickness plus 2 mm
gap). Image esolu ion anges om 1.4 o 1.6 mm pe pixel. An
expe wi h se e al yea s o expe ience in ca diac MRI segmen ed
he images a end-dias ole including he ollowing s uc u es:
le epica dium, le en icle (LV) endoca dium excluding he
papilla y muscles, and igh en icle (RV) endoca dium (see
Figu e 1A, Segmen a ion). As he image esolu ion in s anda d
MRI acquisi ions does no allow o di e en ia e igh en icula
epica dial and endoca dial con ou s in he igh en icle, we
syn hesized igh epica dial con ou s by a 3.5 mm o se om
he endoca dial con ou s (P akash, 1978). Spa ial misalignmen s
in slice images and spa ial disc epancies be ween he con ou s
due o acquisi ions a di e en b ea h holds we e co ec ed
by aligning in ensi y p o iles o in e sec ing slices using a 3D
igid ans o ma ion o each image (Villa d e al., 2017) (see
Figu e 1A, Con ou s alignmen ). Bi- en icula geome ies we e
buil om he aligned con ou s using he end-dias ole ames
om he s anda d CINE acquisi ion as in Villa d e al. (2018)
and Zacu e al. (2017).
Fo he cons uc ion o he o so geome ies, semi-au oma ic
ools we e de eloped and used o delinea e he o so skin and
lungs (Zacu e al., 2017). In b ie , on each subjec , he scou
images (localize s), as well as, mos o he MRI images (SAX
and LAX images) wi h a la ge enough ield o iew we e used
and con ou ed. The spa se 3D geome ical in o ma ion om he
o so images is insu icien o he use o classical segmen a ion
o su ace me hods such as isocon ou ing ools (Figu e 1A,
3-Dimensional o so a angemen ). Thus, we de eloped and
applied a me hodology o i a s a is ical shape model o he
human body o he skin con ou s (Zacu e al., 2017). The
o so con ou s oge he wi h subjec heigh , weigh and gende
in o ma ion we e used o econs uc a body su ace belonging o
a lea ned class o plausible body shapes om he s a is ical shape
model (Pishchulin e al., 2017;Zacu e al., 2017). The a e age
disc epancy be ween MRI-based con ou s and model su ace is
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FIGURE 2 | (A) Endoca dial ac i a ion maps o he i e en icula geome ies. In o ma ion abou en icula olumes is also p o ided. (B) Homologous 12-lead
elec ode posi ions o he i e i ualized subjec s. In o ma ion abou he o so olumes is p o ided.
FIGURE 3 | E ec o en icula geome y on QRS du a ion, and S and R wa e ampli ude. (A) Simula ed QRS complexes ob ained o i e en icula geome ies
placed in he o so-pose o Subjec 3 (T3). (B) QRS du a ion (le ), S and R ampli ude (middle and igh , espec i ely) ob ained om simula ions using he i e
en icula geome ies (H1 o H5) placed in each o he i e o so-poses (T1 o T5). The e m “a.u.” s ands o a bi a y uni s.
3 mm in e ms o oo mean squa e, being he 90 h pe cen ile
5 mm. A empla e-based app oach was used o place o he
in e nal s uc u es such as he lungs and he ibs (Figu e 1A,
Su ace meshes). Full de ails abou he p ocedu e a e p o ided
in Zacu e al. (2017).
All su aces we e emeshed wi h di e en elemen sizes
o ensu e nume ical con e gence o he ini e elemen
so wa e Chas e o elec ophysiological simula ions (Pi -
F ancis e al., 2009;Du a e al., 2016) as desc ibed in
Supplemen a y Ma e ial S1. Finally, e ahed al olume ic
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Mincholé e al. Impac o Ana omy on ECG QRS Complex
meshes we e cons uc ed om hese su aces (see
Supplemen a y Ma e ial S1). The su ace and olume ic meshes
can be downloaded om h p://www.cs.ox.ac.uk/ccs/home.
Figu e 1B shows he econs uc ed en icula geome ies
and, he o so geome ies including hei co esponding hea
o ien a ions and posi ions, cons ained by ches bounda ies.
The gene a ion o a new i ual o so- en icula geome y
equi es he ans o ma ion o he en icula geome y om a
canonical e e ence ame o he posi ion de ined by he o so
(pose, see Figu e 1C). He eina e , o so-pose is de ined as
he o so geome y including he hea pose, which ep esen s
he coo dina e sys em and loca ion o he hea . This o so-
pose linking is suppo ed by physical cons ain s such as ches
bounda ies, since one speci ic o so ana omy does no allow any
hea posi ion (Engblom e al., 2005). Fu he in o ma ion is
ound in Supplemen a y Ma e ial S1.
Elec ophysiological Simula ions
The ana omical o so- en icula model combina ions desc ibed
abo e we e used o compu e 265 QRS complexes om compu e
simula ions as ollows. The p opaga ion o he elec ical
ac i i y in he human en icles and o so was modeled using
he ully coupled hea - o so bidomain equa ions and sol ed
wi h he Chas e so wa e (Pi -F ancis e al., 2009). Human
en icula memb ane kine ics we e simula ed wi h a modi ied
e sion o he O’Ha a-Rudy ac ion po en ial model (O’Ha a
e al., 2011) published in Du a e al. (2017). Myoca dial and
o so conduc i i ies, and, myoca dial ibe s uc u e we e se
as desc ibed in Supplemen a y Ma e ial S2. An aniso opic
myoca dial ibe a chi ec u e was implemen ed using he S ee e
ule (S ee e e al., 1969). The h ee o ho opic in acellula
and ex acellula myoca dial conduc i i ies we e se as in
Ca done-Noo e al. (2016). T ansmu al, apex- o-base and
in e en icula cell elec ophysiological he e ogenei ies we e
in oduced based on expe imen al and clinical da a and as
desc ibed in Supplemen a y Ma e ial S2. The QRS complex
is ha dly a ec ed by he elec ophysiological he e ogenei ies
included in ou models as hey mainly a ec he epola iza ion
p ope ies and he T wa e. Howe e , hey p o ide ou
compu a ional pipeline wi h all he s a e o he a capabili ies o
ex end he wo k o in es iga e a iabili y in T wa e mo phology,
as well as unde disease and d ug ac ion.
Sinus hy hm was simula ed using a phenomenological
ac i a ion model wi h ea ly endoca dial ac i a ion ini ia ed by
oo nodes and a as endoca dial laye ep esen ing a igh ly
packed endoca dial Pu kinje ne wo k (Ca done-Noo e al.,
2016). In sho , 7 oo nodes a e posi ioned in he en icles on
he endoca dium: ou in he LV (LV mid sep um, LV an e io
pa asep al, and wo LV mid-pos e io ) and h ee in he RV (RV
mid sep um, wo RV ee wall), as shown in Supplemen a y
Ma e ial S2. Simula ed en icula ac i a ion imes o hese
models show he LV endoca dial su aces a e ully ac i a ed
wi hin a ange o 39 o 51 ms, and he la es momen s o ac i a ion
occu s in a ange om 57 o 76 ms. This is in ag eemen wi h
he ex i o mic oelec ode eco dings by Du e e al. (1970)
epo ing a ound 45 ms in endoca dial LV ac i a ion, and om
60 o 80 ms he la es momen s o whole en icula ac i a ion.
The aim o his s udy is o in es iga e, analyze and
quan i y he e ec o ana omical/geome ical a iabili y on he
QRS complexes in an elec ophysiological compu e simula ion
amewo k. I is no o cons uc pe sonalized elec ophysiology
models o eplica e each o he pa ien s’ da a. In o de o isola e
he e ec o en icula ana omy om di e ences in ac i a ion
pa e ns, he endoca dial speed was se o 120 cm/s in all
models, and he loca ions o he oo nodes we e mapped o
ana omically homologous loca ions om he geome y used in
a p e ious s udy (Ca done-Noo e al., 2016). The coupled
epica dial, RV and LV endoca dial su aces and en icula
inse ion poin s om he o iginal geome y (Ca done-Noo
e al., 2016) we e di eomo phically egis e ed o each en icula
geome y using a composi ion o app oxima ed Thin-Pla e
Splines (TPS) de o ma ions (Roh e al., 2001). The de o ma ion
me hod was guided by an i e a ed closes poin be ween he
co esponding sou ce and a ge su aces/s uc u es (le and
igh endo- and epica dial su aces, a io- en icula planes, and
an e io and pos e io in e en icula g oo es). The successi e
de o ma ions we e pe o med by ollowing an annealing p ocess
in he smoo hness pa ame e o app oxima ed TPS (Ambe g
e al., 2007). The esul ing egis e ed de o ma ion was applied
o he ea ly ac i a ion si es om he o iginal geome y esul ing
in he ana omically homologous loca ions ha lead o simila
ac i a ion sequences (see Figu e 2A). The esul ing de o ma ions
and he mapped ac i a ion si es we e isually e alua ed and
app o ed by an expe ca diologis . This echnique was used
gi en i s b oad accep ance and success in he medical imaging
and shape analysis ield bu he uni e sal en icula coo dina es
could ep esen an al e na i e (Baye e al., 2018).
QRS complexes om he 12-lead ECGs we e simula ed
by placing i ual elec odes in he s anda d 12-lead ECG
posi ions o each o so. Since he s a is ical shape model
used o econs uc ing he o sos is based on ana omical
co espondences, he i ual elec odes a e loca ed in
ana omically homologous loca ions o all he o sos (see
Figu e 2B). These elec ode posi ions co espond o analogous
in e cos al spaces o all subjec s. Elec ode coo dina es a e gi en
o each o he o so geome ies, and can be downloaded om
h p://www.cs.ox.ac.uk/ccs/home.
To simula e he QRS complex o 265 combina ions o
en icula / o so posi ions and o ien a ions while minimizing
he numbe o expensi e HPC simula ions, ex acellula
po en ials we e compu ed om he en icula po en ials
ollowing he in eg al o dipole sou ce densi y o mula ion
(Gima and Rudy, 2002;Plonsey and Ba , 2007) as:
φ(e)=Z

−D∇Vm·∇1
|| −e||d ,
whe e e=ex,ey,eza e he elec ode posi ion coo dina es, Dis
he di usion enso , and Vmis he memb ane po en ial. The
in eg al is calcula ed o e he whole myoca dium olume, .
Bidomain simula ions coupled wi h he Poisson equa ion o
p opaga e he elec ical ac i i y o he body su ace we e
compa ed o he in eg a ion o dipole sou ce densi y o mula ion
o he o so p opaga ion. The esul ing QRS complexes we e
e y simila as shown in Supplemen a y Figu e S3 om
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Mincholé e al. Impac o Ana omy on ECG QRS Complex
Supplemen a y Ma e ial S2. The p opaga ion model based
on he in eg a ion o dipole sou ce densi y o mula ion was
chosen in o de o simpli y he nume ical complexi y o he
compu a ions and o a oid e-meshing he o so olume o
each scena io in which he en icula geome y was o a ed,
ansla ed o pe mu ed. Al hough his me hod does no allow
he inclusion o issue inhomogenei ies in he o so, se e al
s udies sugges minimal di e ences in he esul ing body su ace
po en ials and he QRS complex when assuming homogeneous
o inhomogeneous o so models (Ramana han and Rudy, 2001;
Genese e al., 2008).
Quan i ica ion o QRS-Based Fea u es
and Desc ip o s
Clinically used ea u es om he QRS, such as du a ion and
ampli ude, we e ex ac ed o each o he simula ed 12-lead
ECGs. QRS du a ion is calcula ed by using a ela i e h eshold
on he absolu e alue o he slopes o he ECG signal o
iden i y QRS onse and o se as in Ma ínez e al. (2004).
We compa ed he simula ion esul s wi h hose epo ed in
he li e a u e and also clinical ECG eco dings om heal hy
olun ee s, as pa o a p ospec i e s udy app o ed by he
Na ional Resea ch E hics Commi ee (REC e 12/LO/1979).
In o med w i en consen was ob ained om each pa icipan
(Lyon e al., 2018a).
Fu he mo e, in o de o quan i y he e ec o ana omical
a iabili y in QRS mo phology, we p oposed a simila i y
measu e o quan i y QRS mo phological di e ences, in a ian
o QRS ampli ude and du a ion. The new me ic (PC∗)
is based on a con inuous gene aliza ion o he Pea son
coe icien (PC), which in o de o ensu e independence
om QRS du a ion, includes he in a iance o a uni o m
wa ping ( ime scaling) in ime o he QRS complex.
The e o e, PC∗be ween wo QRS complexes is 1 when
hese ha e he same mo phology ega dless o he ampli ude
o he du a ion.
Le and gbe wo unc ions de ined on he domains
dom( )=h
0,
1iand dom(g)= g
0, g
1, espec i ely.
Le ’s assume ha dom( )∩dom(g)6= ∅ and le ’s conside
he combined domain [ 0, 1]= dom( )∪dom(g), whe e
0= min
0, g
0and 1= max
1, g
1. On his combined
domain, le ˜
be he eplica ed ex ension o he o iginal
unc ion ,
˜
=






( )i ∈h
0,
1i
(
0)i <
0
(
1)i <
1
and equi alen ly o ˜
g.
Ou p oposed gene alized PC is gi en by
PC ,g=1
1− 0
1
Z 0
˜
( )−µ˜
σ˜
·˜g( )−µ˜g
σ˜g
d (1)
whe e µ˜
and µ˜ga e means, and σ˜
and σ˜ga e he s anda d
de ia ions o he unc ions ˜
( ) and ˜
g( ), espec i ely,
µ˜
=1
1− 0
1
Z 0
˜
( )d , σ˜
=
u
u
u
1
1− 0
1
Z 0˜
( )−µ˜
2d
and equi alen ly o µ˜gand σ˜g. The sub ac ion o he means µ˜
and µ˜gin Eq. (1) ensu es he in a iance o PC unde changes in
he baseline le els. Likewise, no maliza ions by σ˜
and σ˜g, endow
PC wi h in a iance o scaling. The no maliza ion by ( 1− 0)
allows independence om ime uni s. Thus, PC alues a e wi hin
he [–1, 1] in e al.
In o de o ensu e independence om QRS du a ion, we
include he in a iance o a uni o m wa ping ( ime scaling)
in ime h ough he ollowing simila i y measu emen PC∗:
PC ∗
,g= max
s∈R+PC (·),g(s·),
whe e g(s·) is a uni o mly ime-wa ped e sion o g.
I is wo h men ioning ha since domg(s·)= 1/s·
dom(g)= g
0/s, g
1/s, he in eg al in e al in Eq.(1) is
upda ed acco dingly, and he esul ing PC∗keeps ha ing
compa able alues.
In he ollowing, we will explain how o quan i y a global
simila i y o a se o N unc ions  1(·), 2(·),· · · , N(·). We
p opose o compu e, he bes ime wa ping ac o s o he N
unc ions simul aneously, in o de o op imally align he se .
The e o e, we sea ch o
{s1,s2,...,sN}= a gmax
s1,...,sN∈R+
min
i= 1...N
j=i+1...N
PC i(si·), j(sj·)
Once hese op imal ime wa ping ac o s ha e been compu ed,
he global simila i y o he unc ions  1(·), 2(·),· · · , N(·)
is gi en by
PC∗
1, 2,... N= max
i= 1...N
j=i+1...N
PC i(si·), j(sj·)
wi h his, he wo s aligned pai de ines he simila i y
o he whole se .
RESULTS
E ec o Ven icula Geome y on QRS
Du a ion and Ampli ude
Figu e 3 illus a es he e ec o di e en en icula geome ies
wi hin he same o so wi h co esponding hea posi ion
(he eina e e e ed o as o so-pose) on QRS du a ion and
ampli ude. Figu e 3A shows he QRS complexes ob ained in
leads I, II and V1–V6 o each o he i e en icles (H1–H5)
placed in he o so-pose o Subjec 3 (T3). Figu e 3B shows
QRS complex du a ion as well as S and R wa e ampli ude o all
25 o so-pose and en icula combina ions. Fo all o so-poses,
QRS complexes dec ease in ampli ude and inc ease in du a ion
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Mincholé e al. Impac o Ana omy on ECG QRS Complex
wi h an inc ease in myoca dial olume (g een e sus black
aces co esponding o he la ges e sus he smalles en icula
olumes, espec i ely). An a e age inc ease o 0.12 ±0.05 ms
in QRS du a ion o each cm3o myoca dial olume ac oss all
he leads was ound. Rela ionships be ween QRS du a ions and
en icula myoca dial olumes o each o he leads is shown in
Supplemen a y Ma e ial S4.Supplemen a y Figu e S4 shows
he 12 lead QRS complexes o di e en en icula geome ies
wi hin he same o so-pose o each o he i e subjec s.
E ec o To so-Hea Posi ion on QRS
Du a ion and Ampli ude
Figu e 4 shows he e ec o di e en o so-poses on QRS
du a ion and ampli ude. Figu e 4A shows as an example,
he QRS complexes ob ained o he en icula geome y H3
when placed in all he o so-poses, and Figu e 4B p o ides
quan i ica ion o QRS du a ion and R and S wa e ampli udes o
he i e en icula geome ies. QRS du a ion does no change
subs an ially o di e en o so-poses, and his sugges s ha
QRS du a ion is mainly de e mined by he en icula geome y.
Indeed, a sligh inc ease in QRS du a ion o 0.01 ±0.03 ms
o dm3o o so olume ac oss all leads is obse ed ( u he
in o ma ion ega ding he ela ionship be ween QRS du a ion
and o so olume can be ound in Supplemen a y Ma e ial S4).
Howe e , bo h S and R wa e ampli udes a e mainly de e mined
by o so olumes, wi h la ge QRS ampli udes co esponding o
smalle o so olumes. Excep ionally, QRS complexes in T4 wi h
a o so olume o 27 dm3exhibi la ge ampli udes in V1 o V3
compa ed o T5 (23 dm3) ha exhibi la ge ampli udes in V4
o V6. Fo hese wo o sos wi h simila olumes, hea posi ion
plays an impo an ole in QRS ampli ude. By compa ing he
en icula posi ions o T4 and T5 (see Figu e 2), we obse e
ha o T5, V5 and V6 elec ode posi ions a e close o he
en icles esul ing in la ge QRS ampli udes, whils V2 and V3
elec odes a e u he away, esul ing in smalle ampli udes.
E ec o Ven icula Geome y and
To so-Pose on QRS Mo phology
Figu e 5A displays he simila i y measu emen compu ed
om he modi ied Pea son co ela ion PC∗, which measu es
di e ences in QRS mo phology due o di e ences in en icula
geome y and o so-pose.
Resul s show ha o limb leads (I, II, aVR, aVL and aVF),
and V5, QRS mo phology is mo e simila (and PC∗highe ) o
ixed en icula geome y (wi h a ying o so-pose) han o
ixed o so-pose (wi h a ying en icula geome y). The e o e,
in hese leads, he en icula geome y mainly de e mines
he QRS mo phology.
On he con a y, o leads V1 o V4 and V6, QRS mo phology
is mo e simila (as shown by he highe PC∗ alues) o ixed
o so-poses han o ixed en icula geome y. Thus, in hese
leads, QRS mo phology is mos ly de e mined by o so-pose
a he han by en icula geome y.
These esul s a e u he illus a ed in Figu es 5B,C o wo
ep esen a i e leads, aVL and V1. Simula ed QRS mo phology
is mos ly de e mined by he en icula geome y and o so-
pose in leads aVL and V1, espec i ely. Simula ed QRS
complexes ob ained wi h he same en icula geome y a e
shown in he same ow while hose ob ained wi h he same
o so-pose a e shown in he same column. The wa ped
QRS complexes om which PC∗is compu ed a e shown in
Supplemen a y Ma e ial S5.
E ec o Hea O ien a ion and Posi ion
on he QRS Mo phology
Figu es 6,7illus a e he esul s ob ained om he 265
simula ions conduc ed o e alua e he e ec o o a ion a ound
he long axis and le - o- igh en icle di ec ions and ansla ion
along he la e al and c anio-caudal di ec ions o he en icles
wi hin he o so in he QRS complex. Figu e 6 displays simula ed
QRS complexes ob ained o a ep esen a i e ana omical model
(H3 wi hin T3), whe eas Figu e 7 shows quan i ica ion o he
QRS mo phology simila i y me ic (PC∗) o all subjec speci ic
o so- en icula geome ies.
As shown in Figu es 6A,7A, o a ion along he long axis
mainly a ec s he R and S ampli udes o leads V1 o V3. The
ampli ude o he R wa e is la ge when he LV aces he ches
plane (o ange aces) and dec eases as he RV ge s posi ioned
be ween he LV and he ches (blue ace). The ampli ude o
he S wa e also dec eases in he p eco dial leads in en icula
posi ions whe e he RV aces he ches . Quan i a i e esul s
ega ding changes in QRS ampli udes wi h hea o ien a ion and
posi ion can be ound in Supplemen a y Ma e ial S6.
Figu es 6B,7B show ha o a ion a ound he le - o- igh
en icle axis se e ely a ec s he QRS mo phology in leads II,
and V1 o V5. Mo e ho izon al hea s (o ange aces) esul in
la ge R wa e ampli udes in leads I, V1, and V6 while mo e
e ical ones (blue aces) esul in la ge R and S wa e ampli udes
in leads V2 o V5.
Figu es 6C,7C show ha hea s loca ed in mo e medial
posi ions esul in alle R and S wa es in sep al V1 o V3 leads
while sho e R wa es a e obse ed in he p eco dial la e al leads
V5 and V6. This is due o he close en icula loca ion o V1
o V3 elec ode posi ions and u he om V5 and V6. On he
o he hand, hea s loca ed in mo e la e al posi ions ( owa d he
le -a m) displayed nega i ely de lec ed S o e en QS complexes
in he sep al V1 o V2 leads and la ge R wa e ampli udes in V5
o V6 (blue solid lines).
Figu es 6D,7D show he e ec o shi ing he en icles
up along he c anio-caudal (supe io -in e io ) di ec ion leads o
la ge R wa e ampli udes in lead I, and longe R and S wa es in
V1 o V5 (blue lines). Howe e , shi ing he hea down leads
o sho e R wa es in leads I, V1 and V6 (o ange line). The
changes would be equi alen o changing he elec ode posi ion
wi h espec o he en icles.
Compa ison o Clinical Da a
Simula ed ECGs ob ained om ou popula ion o models exhibi
QRS axis (compu ed om QRS complexes in leads I and III)
anging om 50◦ o 75◦[no mal ange –30◦ o 90◦as shown
in Engblom e al. (2005)], QRS du a ions pe lead om 45 o
80 ms [no mal ange including all leads 78 ±8 ms as shown in
an Oos e om e al. (2000)], and ampli udes om 0.5 o 3.5 mV
[heal hy: 2 ±0.6 mV as shown in an Oos e om e al. (2000)].
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Mincholé e al. Impac o Ana omy on ECG QRS Complex
FIGURE 4 | E ec o o so-pose on QRS du a ion, and S and R wa e ampli ude. (A) Simula ed QRS complexes ob ained using he en icula model om Subjec 3
(H3) placed in he i e di e en o sos-poses. (B) QRS du a ion (le ), and S and R ampli udes (middle and igh , espec i ely) om simula ions using each o he i e
hea s (H1 o H5) placed in he di e en o so-poses (T1 o T5).
Thus, all hese quan i a i e measu emen s a e in ag eemen
wi h clinical ECGs om heal hy subjec s ( an Oos e om e al.,
2000;Engblom e al., 2005;S ewa e al., 2011), suppo ing he
c edibili y o he simula ions.
Figu e 8 shows a compa ison o he a iabili y exhibi ed in
simula ed and clinical 12 lead ECG QRS complexes. Simula ed
QRS complexes show a iabili y in e ms o mo phology,
especially in he p eco dial leads. The no mal up igh (posi i e)
QRS complexes in bo h, lead I and lead aVF, esul in a
no mal QRS axis. Fu he mo e, simula ed QRS complexes
show posi i e de lec ion wi h la ge, up igh R wa e in leads
I, II, V4–V6 and a p edominan nega i e de lec ion wi h a
la ge, deep S wa e in aVR, V1 and V2 (see Figu e 8A).
This is in ag eemen wi h he h ee clinical eco dings
shown in Figu e 8B. Lead III in simula ed ECGs shows
biphasic QRS complexes wi h a nega i e de lec ion ollowed
by a posi i e one as in he clinical eco ding o Subjec 1
(Figu e 8B). On he con a y, simula ed lead aVL shows
biphasic QRS complex wi h i s a posi i e de lec ion ollowed
by a nega i e one, as in clinical eco dings o Subjec s 1
and 3 (Figu e 8B).
P eco dial QRS complexes show R wa e p og ession om
V1 o V6, wi h an inc easing R wa e and a dec easing S wa e
when mo ing om V1 o V6. This p og ession is obse ed
in bo h simula ed (Figu e 8A) and clinical ECGs (Figu e 8B).
QRS complexes in lead V1 show mo phological a iabili y
om biphasic QRS complexes (posi i e-nega i e de lec ions) o
down igh QRS complexes (Figu e 8A). This is in ag eemen wi h
he a iabili y in clinical eco dings (Figu e 8B).
DISCUSSION
The p esen s udy demons a es he compu a ional e alua ion
o he e ec o hea - o so posi ion and ana omy on he
QRS complex using human o so/bi en icula elec ophysiology
models de i ed om clinically s anda d MRI. The i s
con ibu ion o he s udy is he compu a ional pipeline o
build he o so/bi en icula ana omies ini ia ing om s anda d
clinical ca diac MRI augmen ed wi h a s a is ical shape model
o he body (Zacu e al., 2017). This me hodology enables
exploi ing clinical da abases o e alua e he unc ional impac
o MRI-ex ac ed ana omical and s uc u al ea u es (Lyon
e al., 2018b). Fu he mo e, human MRI-in o med modeling
and simula ion based on his echnology could accele a e he
de elopmen o ailo ed pha macological and elec ical he apy
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Mincholé e al. Impac o Ana omy on ECG QRS Complex
FIGURE 5 | (A) Simila i y measu emen (PC∗) o he simula ed QRS mo phologies o ixed en icula geome y (and a ying o so-pose) (blue), and o ixed
o so-pose (and a ying en icula geome y (g ay). Panels (B,C) Simula ed QRS mo phologies ob ained wi h he i e en icula geome ies (H1 o H5) placed in he
i e o so-poses (T1 o T5) o leads aVL (B) and V1 (C).
and he goal o p ecision ca e. Fi s ly, being able o econs uc
he pa ien ’s speci ic o so and en icula model om s anda d
ca diac MRI is a s ep o wa d o pe sonalized compu e
modeling and simula ion. The human models cons uc ed ha e
he biophysical de ail equi ed o enable u u e simula ion
s udies in o he esponse o disease and pha macological
ea men . Addi ionally, he simula ion esul s demons a e he
in luence o ana omical ea u es on he QRS complex in heal hy
con ol condi ions. This quan i ica ion o no mal QRS complex
a iabili y is impo an o in o m he e alua ion o esponse o
disease and ea men .
Analysis o he simula ed QRSs yields he ollowing indings:
(i) QRS mo phologies in limb leads I and II a e mainly
de e mined by he geome y o he en icles whe eas QRS
mo phologies in he p eco dial leads, and especially V1 o V4,
a e de e mined by he o so-pose. (ii) QRS du a ion is mainly
in luenced by myoca dial olume while i is ha dly a ec ed
by he o so geome y o hea posi ion; (iii) QRS ampli ude
inc eases wi h la ge en icula olumes and dec eases wi h
la ge o so olumes. Quan i ica ion o he con ibu ion o he
indi idual hea s uc u e, o ien a ion and body habi us on he
ECG is c i ical o aid he clinical in e p e a ion o po en ial ECG
abno mali ies d i en by disease o pha macological ea men .
In syne gy wi h clinical da abases, hey could also d i e
he pe sonaliza ion o sco e me ics o isk s a i ica ion by
disc imina ing in clinical eco dings be ween he con ibu ion
o each pa ien ’s speci ic ana omy and hose a ising om
hei disease s a e.
Popula ions o Hea -To so
Elec ophysiological Models F om
S anda d Clinical MRI
In his pape , we p esen mul iscale elec ophysiological
simula ions using hea - o so ana omical models om s anda d
ca diac MRI acquisi ions (Figu e 1). The gene a ion o he
subjec -speci ic geome ies is pe o med om s anda d ca diac
MRI acquisi ions allowing o be used di ec ly on a ailable
clinical da ase s. The sca ce in o ma ion o o so ana omy om
s anda d ca diac MRI acquisi ions makes he use o adi ional
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Con lic o In e es S a emen : The au ho s decla e ha he esea ch was
conduc ed in he absence o any comme cial o inancial ela ionships ha could
be cons ued as a po en ial con lic o in e es .
Copy igh © 2019 Mincholé, Zacu , A iga, G au and Rod iguez. This is an open-
access a icle dis ibu ed unde he e ms o he C ea i e Commons A ibu ion
License (CC BY). The use, dis ibu ion o ep oduc ion in o he o ums is pe mi ed,
p o ided he o iginal au ho (s) and he copy igh owne (s) a e c edi ed and ha he
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