A thermodynamic theory of microbial growth and its ...

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www.irstea.fr Théodore BOUCHEZ Irstea-Antony, France Hydrosystems and bioprocesses research unit [email protected] A thermodynamic theory of microbial growth and its perspectives for modelling environmental biotechnology processes MELiSSA WORKSHOP 8-9 June 2016, Lausanne Switzerland

Transcript of A thermodynamic theory of microbial growth and its ...

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www.irstea.fr

Pour mieux

affirmer

ses missions,

le Cemagref

devient Irstea

Théodore BOUCHEZ

Irstea-Antony, France

Hydrosystems and bioprocesses research unit

[email protected]

A thermodynamic theory of microbial growth and its

perspectives for modelling environmental biotechnology

processes

MELiSSA WORKSHOP

8-9 June 2016, Lausanne Switzerland

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Microbial successions and energy gradients

http://www.esf.edu/efb/schulz/Limnology/redox.html http://www.hhmi.org/biointeractive/poster-winogradsky-column-microbial-evolution-bottle

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How could all these complex ecological interactions lead to such a

reproducible functional convergence?

C5H7O2N +3 H2O

2,5 CH4 + 2,5 CO2

+ NH3

C5H7O2N + 7 O2

2 H2O + 5 CO2 +

NO3- +H+

+ H2O

Existence of a functional convergence phenomenon of

microbial communities in environmental bioprocesses

« Open diversity systems »

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IS

IX

NOS

HBX ,

NDX

NHS

NDS

PXSX

ABX ,

deathdea

th

death death

death

an,oxicgrowth

anoxic

growth

aerobic

growthaerobic

growth

death

nitrification

aerobic

hydrolysis

anoxic

hydrolysis

ammonification

aerobic

hydrolysis

anoxic

hydrolysis

SSanoxic

growth

aerobic

growth

Soluble inert

organic matter

Particulate

inert organic

matter

Readily

biodegradable

substrate

Slowly

biodegradable

substrate

Particulate products

from biomass decay

Nitrate +

nitrite nitrogen

NH4+ + NH3

nitrogen

Heterotrophic

bacteria Autotrophic

bacteria

Particulate

biodegradable organic

nitrogen

Soluble

biodegradable

organic nitrogen

What do models tell us about this convergence?

Anaerobic Digestion Model N°1 Activated Sludge Model N°1

][

][max

SK

S

s

][

][max

SK

S

s …n1 times …n2 times

=> Current models are not appropriate to handle this question

Bdt

dB. B

dt

dB.and and

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Observed metabolic successions and thermodynamics

Aerobic

Denitrifying

Sulfidogenic

Methanogenic

∆𝑟 𝐺𝑐𝑎𝑡 > ∆𝑟 𝐺𝑐𝑎𝑡 > ∆𝑟 𝐺𝑐𝑎𝑡 > ∆𝑟 𝐺𝑐𝑎𝑡

CO2Glucose

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6 Thermodynamic balances of microbial growth

∆𝑟 𝐺𝑐𝑎𝑡

∆𝐺𝑎𝑛

ΔGmet = ΔGan + λ. ΔrGcat

ΔGmet = ΔGan + λ. ΔrGcat = ΔGdis = f (substrate)

Edis = λ .Ecat - EM

Introducing the exergy concept

From thermodynamic balances to kinetics?

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n = division coordinate

EM

E

EM

Edis

2M

M

Edis

M X‡ 2M μmax K

X‡

E‡=λ . Ecat

A microbial “transition state” theory Desmond-Le Quéméner and Bouchez, The ISME-J, 2014

𝐾 =𝑋‡

𝑀 =𝑁‡

𝑁

𝑑𝑁

𝑑𝑡= 𝜇𝑚𝑎𝑥 ∙ 𝑁

‡ and

𝑁‡ is the number of activated microbes

N is the number of microbes

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Resource allocation among microbes: a statistical question

• Define the spatial distribution of molecules in the medium

• Introduce Vharv « the harvesting volume »

• Compute the distribution of molecules in the various harvesting volumes

𝑁‡ can be deduced from this calculation

𝑁‡

𝑁= exp −

𝐸𝑀 + 𝐸𝑑𝑖𝑠𝑉ℎ𝑎𝑟𝑣 ∙ 𝑆 ∙ 𝐸𝑐𝑎𝑡

Desmond-Le Quéméner and Bouchez, The ISME-J, 2014

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A microbial growth equation and its consequence on isotopic fractionation

𝜇 = 𝜇𝑚𝑎𝑥 ∙ exp −𝐸𝑀 + 𝐸𝑑𝑖𝑠𝑉ℎ𝑎𝑟𝑣 ∙ 𝑆 ∙ 𝐸𝑐𝑎𝑡

• Any further predictions?

Desmond-Le Quéméner and Bouchez, The ISME-J, 2014

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A microbial growth equation and its consequence on isotopic fractionation

𝜇 = 𝜇𝑚𝑎𝑥 ∙ exp −𝐸𝑀 + 𝐸𝑑𝑖𝑠𝑉ℎ𝑎𝑟𝑣 ∙ 𝑆 ∙ 𝐸𝑐𝑎𝑡

• Any further predictions? Challenging these predictions

with real datasets…

Desmond-Le Quéméner and Bouchez, The ISME-J, 2014

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Challenging thermodynamic growth model’s predictions with actual isotopic data

Hydrogenotrophic methanogenesis

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Challenging thermodynamic growth model’s predictions with actual isotopic data

Hydrogenotrophic methanogenesis

D/H

Aerobic phenol

Degradation Kampara et al., 2008

13C/12C

Acetoclastic

Methanogenesis Goevert and Conrad,

2009

13C/12C

Hydrogenotrophic

Methanogenesis Valentine et al., 2004

Penning et al., 2005

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13 How are communities shaped by thermodynamic gradients?

𝜇 = 𝜇𝑚𝑎𝑥 ∙ exp −𝐸𝑀 + 𝐸𝑑𝑖𝑠𝑉ℎ𝑎𝑟𝑣 ∙ 𝑆 ∙ 𝐸𝑐𝑎𝑡

Flux: microbial growth rate Force: catabolic exergy density

Application to activated sludge O2

NH4+ CH3COO- NO2

- NO3-

Heterotrophs Nitrite oxidizers Ammonia

oxidizers

Hadrien

Delattre’s

PhD Project

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Coupled modelling of energy balances, stoichiometry and

microbial dynamics

Hadrien

Delattre’s

PhD Project

−0,525C2H3O2− − 0,2NH4

+ − 0,325H+ + 0,45H2O + 0,05CO2 + 1C1H1,8O0,5N0,2+ λ(−1C2H3O2

− − 2O2 − 1H+ + 2CO2 + H2O)

−0,2NH4+ − 0,6H2O − 1CO2 + 1,05O2 + 0,2H

+ + 1C1H1,8O0,5N0,2

+λ(−4,5𝑂2 − 2𝑁𝐻4+ − 2𝐻+ + 2𝑁𝑂2

−)

−0,2NO2− − 0,8H2O − 1CO2 − 0,2H

+ + 1,35O2 + 1C1H1,8O0,5N0,2+ λ(−1NO2

− − 0,5O2 + 1NO3−)

Application to activated sludgeO2

NH4+ NO2

- NO3-

Heterotrophs Nitrite oxidizersAmmonia

oxidizers

CH3COO-

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Coupled modelling of energy balances, stoichiometry and

microbial dynamics

Hadrien

Delattre’s

PhD Project

−0,525C2H3O2− − 0,2NH4

+ − 0,325H+ + 0,45H2O + 0,05CO2 + 1C1H1,8O0,5N0,2+ λ(−1C2H3O2

− − 2O2 − 1H+ + 2CO2 + H2O)

−0,2NH4+ − 0,6H2O − 1CO2 + 1,05O2 + 0,2H

+ + 1C1H1,8O0,5N0,2

+λ(−4,5𝑂2 − 2𝑁𝐻4+ − 2𝐻+ + 2𝑁𝑂2

−)

−0,2NO2− − 0,8H2O − 1CO2 − 0,2H

+ + 1,35O2 + 1C1H1,8O0,5N0,2+ λ(−1NO2

− − 0,5O2 + 1NO3−)

𝜇 = 𝜇𝑚 𝑒−𝜈𝑖(𝜆)𝑉ℎ∙𝑆𝑖

𝑖

Multisubstrate rate law expression for all groups:

𝜆 is calculated from thermodynamic balances of microbial growth

Application to activated sludgeO2

NH4+ NO2

- NO3-

Heterotrophs Nitrite oxidizersAmmonia

oxidizers

CH3COO-

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Simulating activated sludge batchs fed with wastewater

Simulation conditions: constant supply of air, default ASM chemical species and microbial

composition used for initialization, same default E.coli growth parameters for all groups

CH3COO-

NH4+

NO3-

NO2-

Ammonia oxidizers

heterotrophs

Nitrite oxidizers

=> Proper metabolic succession obtained without parameter fitting

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Simulating « chemostats »

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Varying the loading rate in virtual activated sludge

chemostats

Low loading rate High loading rate

Nitrification

=> Engineering rules as emerging properties of thermodynamic models

No nitrification

Washout

of nitrifiers

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Take home messages…

A consistent framework for coupled modelling of energy

balance, stoichiometry and microbial dynamics

Revisiting the importance of energy drivers for shaping

microbial community structures

Reproducing microbial successions without parameter

fitting

Towards more predictive models?

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Many thanks to… All the BIOMIC team members in Irstea-Antony

http://www.irstea.fr/la-recherche/themes-de-recherche/ted/biomic

Elie Desmond,

postdoc

Microbial

thermodynamics

Hadrien

Delattre, PhD,

Thermodynamic

simulation of

microbial

ecosystems

BIORARE project

ANR-10-BTBR-02

Christian Duquennoi,

multiphysic models

Ahlem Filali,

Activated sludge models

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Thanks for you attention

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Choice of a generic biomass formula

• Hoover and Porges’ biomass: C5H7O2N

• Widely used in wastewater bioprocesses modelling

• Gibbs energy of formation is unknown

• Composition appears to be unrealistic

• Heijnen’s biomass: C1H1.8O0.5N0.2

• Infered from growth data of multiple microbes on multiple substrates

• Gibbs energy of formation is known

• Composition appears to be unrealistic

• Battley’s biomass: C1H1.613O0.557N0.158

• Experimentally measured from Saccharomyces cerevisiae cultures

• Gibbs energy of formation directly measured by calorimetry

• Composition seems to be more realistic

• Hoover S.R. and Porges N. (1952). Assimilation of dairy wastes by activated sludge. II. The equations of

synthesis and rate of oxygen utilization. Sew. Indus. Wastes J., 24, 306-312.

• Heijnen J. and Dijken J. (1991). In Search of a Thermodynamic Description of Biomass Yields for the

Chemotrophic Growth of Microorganisms. biotechnology and bioengineering, 39(8), 833-858.

• Battley E. (1998). The development of direct and indirect methods for the study of the thermodynamics of

microbial growth. Thermochimica Acta, 309, 17-37.

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Estimation of the harvesting volume (Vh)

𝜇 = 𝜇𝑚𝑒𝜈𝑉ℎ𝑆

𝑉ℎ =𝜈

𝑆 ln 𝜇 − ln 𝜇𝑚

Data is from Taheri-Araghi S. et al. (2015). Cell-size control and homeostasis in bacteria. Current Biology, 25(3), 385-391.

Vh estimated for E Coli growing on various substrates ;

• Glycerol : 0.42 m3.C-mol-1 (sphere of radius 14.3 µm around each cell)

• Glucose : 0.74 m3.C-mol-1 (sphere of radius 19.2 µm around each cell)

• Sorbitol : 0.79 m3.C-mol-1 (sphere of radius 17.7 µm around each cell)

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Lambda factor computation

𝑆 : chemical species concentrations vector (Cx1)

𝜈𝑐𝑎𝑡, 𝜈𝑎𝑛: raw stoichiometric coefficients vectors (1xC)

∆𝐺𝑐𝑎𝑡 = ∆𝐺0𝑐𝑎𝑡 − 𝑅𝑇𝜈𝑐𝑎𝑡 ∗ ln 𝑆

∆𝐺𝑎𝑛 = ∆𝐺0𝑎𝑛 − 𝑅𝑇𝜈𝑎𝑛 ∗ ln 𝑆

∆𝐺𝑑𝑖𝑠: energie to dissipate(constant depending on the carbon source)

𝜆 =∆𝐺𝑎𝑛 + ∆𝐺𝑑𝑖𝑠−∆𝐺𝑐𝑎𝑡

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Dissipated energy calculation

Heijnen J. and Kleerebezem R. (1999). Bioenergetics of microbial growth. Encyclopedia of Bioprocess Technology.

Dissipated energy is a constant whose value depends on the anabolic carbon

source, according to Heijnen and Kleerebezem