1
θ θ' 0 360 360 180 180 0 −1500 −750 0 Min kJ.mol − 1 Generating potential energy landscapes for membrane proteins Nandhini Rajagopal and Shikha Nangia Department of Biomedical and Chemical Engineering, Syracuse Biomaterials Institute, Syracuse University Lipid Bilayer Top view • Protein-protein interactions have high clinical significance • Especially, integral membrane proteins occupy 30-50% of the cell surface area in mammals • Mutations in proteins affect protein associations • Resulting pathological conditions include neurodegenerative diseases, cancers, autoimmune diseases, genetic diseases, and many more • Experimental methods - Resolution - Extraction methods for membrane proteins Methods Results & Analysis θ θ' 0 360 360 180 180 1 110 55 0 Ma x Potential energy 1D variable Funnel Saucer − <0 • Protein LJ+Coulombic interaction energies for 360×360 rotational states • Relative thermodynamic stabilities • Visiting frequency of 360×360 rotational states • Relative kinetic stabilities Funnels and Saucers References 1. Wassenaar, T. A., Pluhackova, K., Moussatova, A., et. al. High-Throughput Simulations of Dimer and Trimer Assembly of Membrane Proteins. The DAFT Approach. J. Chem. Theory Comput. 2015, 11, 2278−2291. 2. Suzuki, H., Nishizawa, T., Tani, K., Yamazaki, Y., Tamura, A., Ishitani, R., Dohmae, N., Tsukita, S., Nureki, O., Fujiyoshi, Y. Crystal structure of a claudin provides insight into the architecture of tight junctions. Science 2014, 344: 304-307. Syracuse University Research Computing: Academic Virtual Hosting Environment (AVHE) Acknowledgements 3. Hiroshi S., Kazutoshi T., Atsushi T., Sachiko T., Yoshinori FModel for the architecture of claudin-based paracellular ion channels through tight junctions. J. Mol. Biol. 2015, 427(2):291-7. 4. Tamura A, Hayashi H, Imasato M, et al. Loss of claudin-15, but not claudin-2, causes Na+ deficiency and glucose malabsorption in mouse small intestine. Gastroenterology. 2011, 140(3):913-923. 5. Rajagopal, N., Nangia, S., Obtaining Protein Association Energy Landscape (PANEL) for Integral Membrane Proteins. J. Chem. Theory & Comp. 2019. 6. Rajagopal N., Nangia S. Exploring the “Funnels” and “Saucers” of Protein Interaction Landscapes. Manuscript in preparation. θ θ' S1 S3 S4 S5 F2 F1 S3 S4 S2 S2 -1 -0.5 0 0.5 1 S1 S2 S3 S4 S5 F1 F2 Relative Frequency Relative Energy S1 S4 S5 S1 S4 S5 Crystal lattice-based claudin-15 strand Motivation PANEL (Protein AssociatioN Energy Landscape) 0˚ 360˚ 90˚ 180˚ 270˚ P1 (θ) P2 (θ') Rotational space schematic (Proteins as seen from the top view) Claudin-15 – Representative protein 0˚ 90˚ 180˚ 360˚ 270˚ Uniform stochastic distribution of seed geometries (schematic) Often due to local landscape features, energy and frequency landscapes exhibit mismatch in dimer favorability. • “Funnels”— thermodynamically favored states • “Saucers”— kinetically favored states • Significant dimer regions—Grids retaining seed geometries greater than initial value throughout the MD simulation Min Energy Max Frequency • Computational methods: - Difficult to obtain comprehensive data - High computational cost This work: • Exhaustively explore membrane protein interactions • Quantify the interaction stability • Computationally affordable • Identify key dimers • Using coarse-grained MD simulations Approach : • Rotational space: Defined by axial rotation of an interacting pair of proteins (θ,θ'), in the membrane plane • Uniform stochastic distribution: Rotational space (θ,θ’) divided into equal, non-overlapping segments (Ω)—each segment Ω i comprised of a selected number of random seed configurations. • Equilibrium conformations: Independent and parallel unconstrained MD simulations of seed geometries • Non-bonded interaction energy: Computed between P1 and P2 proteins for each equilibrium conformation • PANEL Landscapes: Minimum energy and Frequency contour plots for each degree rotation of P1 and P2 • S4: Crystal lattice protomeric unit • S1 and S5: Dimer orientations across antiparallel strand assembly • Role of other Saucers need to be explored. • Comprehensive, robust and versatile method to generate potential energy and frequency landscapes • Highly parallelized workflow • Computationally inexpensive short simulations—high throughput. • Validated for dimer and trimer interactions • Enabled Identification physiologically relevant key dimer interfaces • Enabled identification of aggregation patterns • Applicable to any membrane protein Key dimer orientations Critical need to understand protein interactions Limitations: Funnels and Saucers Minimum Energy Landscape Frequency Landscape Membrane Protein Ranking Conclusions NSF CAREER CBET-1453312

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Page 1: Generating potential energy landscapes for membrane proteins...Saucer 𝐸 𝑢𝑛𝑛 ... NSF CAREER CBET-1453312. Title: PowerPoint Presentation Author: Nandhini Rajagopal Created

θ

θ'

0

360

360

180

180

0

−1500

−750

0

Min

kJ.mol−

1

Generating potential energy landscapes for membrane proteins Nandhini Rajagopal and Shikha Nangia

Department of Biomedical and Chemical Engineering, Syracuse Biomaterials Institute, Syracuse University

Lip

id B

ilaye

r

Top view

• Protein-protein interactions have high clinical significance

• Especially, integral membrane proteins occupy 30-50% of

the cell surface area in mammals

• Mutations in proteins affect protein associations

• Resulting pathological conditions include

neurodegenerative diseases, cancers, autoimmune

diseases, genetic diseases, and many more

• Experimental methods

- Resolution

- Extraction methods

for membrane proteins

Methods

Results & Analysis

θ

θ'

0

360

360

180

180

1

110

55

0

Ma

x

Po

ten

tia

l e

ne

rgy

1D variable

Funnel

Saucer

𝐸𝑓𝑢𝑛𝑛𝑒𝑙 − 𝐸𝑠𝑎𝑢𝑐𝑒𝑟 < 0

• Protein LJ+Coulombic interaction energies

for 360×360 rotational states

• Relative thermodynamic stabilities

• Visiting frequency of 360×360 rotational

states

• Relative kinetic stabilities

Funnels and Saucers

References1. Wassenaar, T. A., Pluhackova, K., Moussatova, A., et. al. High-Throughput Simulations of Dimer and Trimer

Assembly of Membrane Proteins. The DAFT Approach. J. Chem. Theory Comput. 2015, 11, 2278−2291. 2. Suzuki, H., Nishizawa, T., Tani, K., Yamazaki, Y., Tamura, A., Ishitani, R., Dohmae, N., Tsukita, S., Nureki, O.,

Fujiyoshi, Y. Crystal structure of a claudin provides insight into the architecture of tight junctions. Science 2014, 344: 304-307.

Syracuse University Research

Computing: Academic Virtual

Hosting Environment (AVHE)

Acknowledgements3. Hiroshi S., Kazutoshi T., Atsushi T., Sachiko T., Yoshinori FModel for the architecture of claudin-based

paracellular ion channels through tight junctions. J. Mol. Biol. 2015, 427(2):291-7.4. Tamura A, Hayashi H, Imasato M, et al. Loss of claudin-15, but not claudin-2, causes Na+ deficiency and

glucose malabsorption in mouse small intestine. Gastroenterology. 2011, 140(3):913-923.5. Rajagopal, N., Nangia, S., Obtaining Protein Association Energy Landscape (PANEL) for Integral Membrane

Proteins. J. Chem. Theory & Comp. 2019. 6. Rajagopal N., Nangia S. Exploring the “Funnels” and “Saucers” of Protein Interaction Landscapes. Manuscript

in preparation.

θ

θ'

S1

S3

S4

S5

F2

F1

S3

S4

S2

S2

-1

-0.5

0

0.5

1

S1 S2 S3 S4 S5 F1 F2

Re

lative

Fre

qu

en

cy

Re

lative

En

erg

y

S1 S4 S5

S1

S4S5

Crystal lattice-based claudin-15 strand

Motivation

PANEL

(Protein AssociatioN Energy Landscape)

0˚

360˚

90˚

180˚

270˚

P1 (θ) P2 (θ')

Rotational space schematic (Proteins as seen

from the top view)

Claudin-15 – Representative protein

0˚

90˚

180˚360˚

270˚

Uniform stochastic distribution of seed

geometries (schematic)

Often due to local landscape features,

energy and frequency landscapes exhibit

mismatch in dimer favorability.

• “Funnels”— thermodynamically

favored states

• “Saucers”— kinetically favored states

• Significant dimer regions—Grids

retaining seed geometries greater than

initial value throughout the MD

simulation

Min

Energy

Max

Frequency

• Computational methods:

- Difficult to obtain

comprehensive data

- High computational cost

This work:

• Exhaustively explore

membrane protein

interactions

• Quantify the interaction

stability

• Computationally

affordable

• Identify key dimers

• Using coarse-grained

MD simulations

Approach:

• Rotational space: Defined by axial rotation of an interacting pair of

proteins (θ,θ'), in the membrane plane

• Uniform stochastic distribution: Rotational space (θ,θ’) divided into

equal, non-overlapping segments (Ω)—each segment Ωi comprised of a

selected number of random seed configurations.

• Equilibrium conformations: Independent and parallel unconstrained MD

simulations of seed geometries

• Non-bonded interaction energy:

Computed between P1 and P2 proteins

for each equilibrium conformation

• PANEL Landscapes: Minimum energy

and Frequency contour plots for each

degree rotation of P1 and P2

• S4: Crystal lattice protomeric unit

• S1 and S5: Dimer orientations across antiparallel

strand assembly

• Role of other Saucers need to be explored.

• Comprehensive, robust and versatile method

to generate potential energy and frequency

landscapes

• Highly parallelized workflow

• Computationally inexpensive short

simulations—high throughput.

• Validated for dimer and trimer interactions

• Enabled Identification physiologically

relevant key dimer interfaces

• Enabled identification of aggregation

patterns

• Applicable to any membrane protein

Key dimer orientations

Critical need to understand protein interactions

Limitations:

Funnels and SaucersMinimum Energy Landscape Frequency Landscape

Membrane

Protein

Ranking

Conclusions

NSF CAREER

CBET-1453312