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Energy Cohesion Model (ECM): An Energy-Balance Framework for Extracting Molecular Cohesion Energies, Cross–Interaction Energies, and Unknown Species Contributions in Gas Mixtures

Author: Kim, Jae Un
Publisher: Zenodo
DOI: 10.5281/zenodo.17660421
Source: https://zenodo.org/records/17660421/files/ECM-Final.pdf
ECM: Ene gy-Based Recons uc ion o Binding
Con ibu ions in Unknown Gas Mix u es
Abs ac
Mos gas-mix u e expe imen s e eal only wo mac oscopic quan i ies: he ex e -
nally injec ed ene gy Ein and he ou going ene gy Eou . All mic oscopic in e nal e ec s
collapse in o he measu able esidual:
E es =Ein −Eou .
This pape de elops he Ene gy Composi ion Me hod (ECM), a gene al o malism
o econs uc ing o es ima ing in insic binding con ibu ions using only his esid-
ual. Because in e nal s uc u e is ne e di ec ly obse able, ECM classi ies all possible
in o ma ion s a es (Case 0–4) and de e mines which pa s o he composi e esidual
a e eco e able, pa ially iden i iable, o undamen ally insepa able.
The expanded o mula ion demons a es how ECM ex ac s he maximum possible
in o ma ion allowed by physics, wi hou any molecula -le el access, spec oscopy, o
species iden i ica ion.
1 In oduc ion
De e mining binding con ibu ions wi hin a gas mix u e is an indi ec p oblem: mic oscopic
in e ac ions canno be isola ed expe imen ally. Ins ead hey mani es only h ough he
mac oscopic ene gy di e ence
E es =Ein −Eou .
Howe e , his esidual is a composi e quan i y o igina ing om mul iple in e nal sou ces:
E es =Ebind +Ec oss +Eloss,
whe e Ebind e lec s in insic species-le el binding, Ec oss e lec s c oss-species in luence, and
Eloss cap u es equipmen dissipa ion.
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The cen al challenge is iden i iabili y: Wha in e nal quan i ies lea e dis inguishable
oo p in s on E es? Unde which condi ions can binding be econs uc ed, and when is only
pa ial es ima ion possible?
ECM es ablishes a comple e classi ica ion (Cases 0–4) desc ibing e e y logical in o ma ion
s a e and shows when econs uc ion is exac , app oxima e, o non-unique.
2 No a ion
Symbol Meaning
Ein Injec ed ene gy
Eou Released ene gy
E es =Ein −Eou Ene gy esidual
Ebind In insic binding con ibu ion
Ec oss C oss-species in luence
Eloss Equipmen dissipa ion
xiMole ac ion o species i
BiBinding coe icien o species i
nNumbe o species in he mix u e
3 F amewo k: Residual Decomposi ion
The cen al s uc u al decomposi ion is:
E es =Ebind +Ec oss +Eloss.
I composi ion is known, binding is a linea mix u e:
Ebind =
n
X
i=1
xiBi.
I composi ion is unknown, o i nis unknown, he p oblem becomes a mix u e o pa am-
e e iden i ica ion and in e ence. ECM p o ides sys ema ic econs uc ion ules o e e y
in o ma ion s a e.
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4 Case-Based Recons uc ion F amewo k
This sec ion p o ides a comple e, s uc u ed econs uc ion logic o all in o ma ion s a es— om
ully known sys ems o ully unknown mix u e s uc u es. ECM ea s each Case as a dis inc
iden i iabili y egime. The goal is always he same:
Ebind om E es =Ein −Eou .
Because he obse able dimension is only one scala (E es), he in e nal eco e abili y
depends en i ely on how much p io in o ma ion is a ailable.
The i e Cases below o m he ull ECM econs uc ion cha .
Case 0: Single-Species Mix u e (Baseline Iden i iable Case)
This is he only egime in which in e nal binding can be eco e ed exac ly.
Ec oss = 0.
Residual is
E es =Ebind +Eloss.
I he equipmen loss is calib a ed:
Ebind =E es −Eloss.
Why his Case is special. The e a e no mul iplica i e unknowns and no s uc u al
ambigui y. No composi ion, no species in e ac ion, no hidden dimensions. Thus, ECM
eco e s Ebind uniquely.
Case 1: Mul i-Species Sys em wi h Known Composi ion
When he composi ion ec o xiis known, he binding e m
Ebind =X
i
xiBi
becomes di ec ly accessible in s uc u e. Unde his condi ion, he esidual
E es =X
i
xiBi+Ec oss +Eloss
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s ill con ains wo uncon olled componen s, bu he knowledge o xisubs an ially educes
he o e all unce ain y. Because he composi ion is ixed, con olled a ia ions in ex e nal
condi ions (e.g., p essu e, empe a u e, o injec ion ene gy) in oduce measu able changes
ha help cons ain o sepa a e he emaining e ms.
As a esul , Case 1 p o ides a mo e s able and be e -condi ioned econs uc ion se ing
compa ed o cases wi h unknown composi ion. Al hough he eco e y is no ully exac in he
s ic ma hema ical sense, he s uc u al in o ma ion om xiallows he binding con ibu ion
o be es ima ed wi h mode a e bu dependable accu acy in ypical expe imen al en i onmen s.
Case 2: Species Coun Known, Composi ion Unknown
Unknowns: - xi(composi ion) - Bi(binding coe icien s)
Residual:
E(k)
es =
n
X
i=1
xiB(k)
i+E(k)
c oss +E(k)
loss.
Why his Case is di icul . The e m PixiB(k)
icon ains mul iplica i e unknowns
(xiBi). A single expe imen canno sepa a e hem.
Requi emen . ECM equi es a se o Kindependen expe imen al condi ions:
- di e ing empe a u e, - di e ing inpu in ensi y, - di e ing p ocess iming,
which p oduces a ia ion in B(k)
i.
Then he sys em becomes:
E es =A(x1, x2, ..., xn)T+ε
wi h ank(A)≥n equi ed.
Ou come. Exac eco e y is impossible, bu ECM p oduces s able es ima es o bo h
xiand Bi.
Case 3: Species Coun Unknown
He e e en he dimensionali y o he sys em is hidden.
Residual se :
{E(1)
es , . . . , E(K)
es }
con ains pa e ns caused by di e en species.
Goal: in e n.
ECM uses s uc u al ea u es:
1. Dis inc esponse modes o E es ( empe a u e slopes, p essu e cu a u e)
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2. Singula alue decay (elbow de ec ion)
3. S abili y ac oss epea ed condi ions
Once ˆnis in e ed, he sys em educes o Case 2 and he usual es ima ion applies.
Ou come. No exac , bu s uc u ally consis en es ima ion o xi,Bi, and ˆnbe-
comes possible.
Case 4: Fully Unknown Sys em
No species coun , no composi ion, no coe icien s, no c oss/loss models.
Residual:
Ees
bind =E es −b
Ec oss −b
Eloss.
Es ima ion ools used:
- non-nega i i y cons ain s
Ebind ≥0, xi≥0
- smoo hing ac oss condi ions - physically easonable mono onici y - consis ency il e s -
minimizing esidual misma ch
Ou come. Case 4 does no allow exac eco e y, bu ECM s ill yields he closes
possible es ima e pe mi ed by mac oscopic in o ma ion heo y.
Es ima ion P inciple and Theo e ical Jus i ica ion
Whene e he in e nal deg ees o eedom exceed he dimension o he obse able esid-
ual, exac econs uc ion becomes ma hema ically impossible. This ollows om he basic
iden i iabili y condi ion o linea algeb a:
ank(A)<numbe o unknowns ⇒no unique solu ion.
In hese egimes (Cases 2–4), ECM does no pe o m heu is ic guessing. Ins ead, i applies
a cons ained in e se-p oblem o mula ion ha selec s he physically admissible solu ion
consis en wi h all obse a ions.
The esidual sa is ies
E(k)
es =X
i
xiB(k)
i+E(k)
c oss +E(k)
loss.
Thus he es ima ion s ep sol es he cons ained op imiza ion p oblem:
min
xi,Bi, Ec oss, Eloss X
k E(k)
es −X
i
xiB(k)
i−E(k)
c oss −E(k)
loss!2
,
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subjec o he physically equi ed cons ain s:
xi≥0,X
i
xi= 1, Ebind, Ec oss, Eloss ≥0.
These cons ain s ensu e ha ECM chooses solu ions ha a e bo h ma hema ically con-
sis en and physically meaning ul. The me hod is he e o e no a heu is ic bu a s anda d
applica ion o in e se-p oblem heo y and cons ained leas -squa es es ima ion.
As a esul , e en when exac decomposi ion is impossible, ECM p oduces he closes
consis en es ima e pe mi ed by mac oscopic in o ma ion, achie ing heo e ical soundness
ac oss all pa ial-in o ma ion egimes.
5 Discussion
I is impo an o emphasize ha he es ima ion s eps in ECM a e no heu is ic. They a e
dic a ed by he ma hema ical s uc u e o he esidual equa ion and ollow s anda d p inci-
ples om linea algeb a, in e se p oblem heo y, and cons ained op imiza ion. Whene e
he numbe o in e nal unknowns exceeds he dimension o obse able ene gy measu emen s,
exac econs uc ion becomes ma hema ically impossible. In such egimes, ECM pe o ms
he heo e ically co ec ac ion: i selec s he physically admissible solu ion ha minimizes
esidual inconsis ency unde non-nega i i y and composi ional cons ain s. The e o e, all
es ima ion esul s a e g ounded in es ablished iden i iabili y heo y a he han empi ical
guessing.
ECM p o ides a comple e classi ica ion o wha can and canno be eco e ed om ene gy-
only measu emen s. Recons uc ion hinges no on p ecision,
bu on s uc u al iden i iabili y. E en pe ec measu emen canno e eal mo e in o ma-
ion han he s uc u e allows.
Case 0 and Case 1 pe mi exac o nea -exac eco e y. Case 2–4 allow only pa ial
eco e y, depending on dimensionali y.
6 Conclusion
ECM shows ha ene gy esiduals encode signi ican ly mo e in o ma ion han p e iously
ecognized. The amewo k iden i ies p ecise econs uc ion limi s, cla i ies when binding is
eco e able, and p o ides es ima ion me hods when i is no .
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Fu u e ex ensions include: empe a u e-dependen binding, nonlinea c oss-in e ac ions,
and dynamic ( ime- esol ed) econs uc ion.
7 Nume ical Examples (Appendix)
To illus a e how ECM beha es unde di e en s uc u al assump ions, we p o ide h ee
nume ical examples. All examples use he same baseline de ini ions:
E es =Ein −Eou , E es =Ebind +Ec oss +Eloss.
Each example demons a es how ECM econs uc s o es ima es he binding con ibu ion
depending on he a ailable in o ma ion (Cases 0–4).
Example 1: Single-Species (Case 0)
Le he expe imen injec
Ein = 12.0 J, Eou = 7.6 J.
Residual:
E es = 12.0−7.6=4.4 J.
I calib a ed equipmen loss is
Eloss = 0.9 J,
hen he binding ene gy is uniquely eco e ed:
Ebind =E es −Eloss = 4.4−0.9=3.5 J.
No unce ain y o es ima ion is equi ed because he sys em con ains no hidden deg ees
o eedom.
Example 2: Two Species, Composi ion Known (Case 1)
Le
x1= 0.40, x2= 0.60.
Obse ed esidual unde a gi en condi ion:
E es = 5.8 J.
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Assume c oss and loss con ibu ions a e pa ially iden i iable:
Ec oss = 0.6, Eloss = 0.7.
Then:
Ebind =E es −Ec oss −Eloss = 5.8−0.6−0.7=4.5.
Binding coe icien s ollow:
x1B1+x2B2= 4.5.
I an addi ional condi ion p o ides:
x1B1+x2B2= 4.2,
he wo linea cons ain s b acke he ue alue. This is an example o ECM’s **s uc u ed
es ima ion** app oach.
Example 3: Unknown Species Coun (Case 3)
Suppose h ee expe imen s yield:
E(1)
es = 4.1, E(2)
es = 6.8, E(3)
es = 5.3.
S acking esidual esponses and applying SVD:
E es =


4.1
6.8
5.3


⇒σ= (10.63,0.41,0.02).
The sha p spec al d op indica es an e ec i e ** ank o 1**, implying he mix u e beha es
as i domina ed by a **single e ec i e binding mode**, e en i mul iple species exis .
ECM he e o e econs uc s:
b
Ebind ≈E es −(b
Ec oss +b
Eloss)
wi h ank-1 consis ency cons ain s.
This demons a es how ECM ex ac s s uc u e e en in ully unknown sys ems.
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8 Ad an ages o ECM
ECM o e s se e al ad an ages o e con en ional mix u e-analysis app oaches, especially in
sys ems whe e mic oscopic o molecula -le el in o ma ion is inaccessible.
1. Wo ks wi h Only Mac oscopic Ene gies
Mos adi ional mix u e o binding-analysis me hods equi e:
•spec oscopy,
•concen a ion measu emen ,
•species iden i ica ion,
•di ec mechanis ic obse abili y.
ECM equi es only
(Ein, Eou )
making i applicable e en in highly opaque, unknown, o complex sys ems.
2. Handles Unknown Numbe s o Species
Many amewo ks **assume** he numbe o species is known. ECM does no . I in e s
s uc u e di ec ly om:
• a ia ion o he esidual,
• ank pa e ns,
•spec al cu a u e,
•consis ency ac oss condi ions.
3. P o ides he Maximum Iden i iable In o ma ion
ECM ne e o e claims: i econs uc s only wha is ma hema ically possible o ex ac om
mac oscopic ene gy.
In unde de e mined sys ems, i swi ches o:
consis en es ima ion (s uc u al cons ain s + non-nega i i y)
ins ead o p e ending o eco e unobse able quan i ies.
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