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Group of Molecular Physic and Modeling Kaline Cou7nho ([email protected]) Ins$tuto de Física, Universidade de São Paulo, São Paulo, SP, Brazil
8

“Simulations of Lipidic Bilayers”. Prof. Dr. Kaline Coutinho – IF/USP.

Aug 15, 2015

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Page 1: “Simulations of Lipidic Bilayers”. Prof. Dr. Kaline Coutinho – IF/USP.

Group  of  Molecular  Physic    and  Modeling  

 Kaline  Cou7nho  ([email protected])  

 Ins$tuto  de  Física,  Universidade  de  São  Paulo,  São  Paulo,  SP,  Brazil  

Page 2: “Simulations of Lipidic Bilayers”. Prof. Dr. Kaline Coutinho – IF/USP.

Molecules  in  phospholipid  bilayer  (~70,000  atoms)  

Molecules  in  solu:on  or  in  mixtures  (~  3,000  atoms)  

Clusters  (~50  atoms)  Theore:cal  methods:  *  Quantum  mechanics  (QM)  *  Molecular  mechanics  (MM)  

Page 3: “Simulations of Lipidic Bilayers”. Prof. Dr. Kaline Coutinho – IF/USP.

Classical  molecular  dynamics  of  lipophilic  nucleoside  (UP)  bilayer

DaVinci  •  1  node  with  12  cores    •   2  GPUs  NVIDIA  Tesla  M2050  •  178458  atoms,  49886  molecules  •  10  ns/day  (1  fs/step)  •  Total  of  30ns  è  4  days  (1  wai:ng)    •  GROMOS  force  field  with  Gromacs  4.6.1*  

 

*www.gromacs.org  

We  studied  structural  proper:es  of  bilayers  with  different  concentra:ons  of  UP  and  DPPC.  

Page 4: “Simulations of Lipidic Bilayers”. Prof. Dr. Kaline Coutinho – IF/USP.

Classical  molecular  dynamics  of  lipophilic  nucleoside  bilayer  and  adenine

DaVinci  •  1  node  with  12  cores    •   2  GPUs  NVIDIA  Tesla  M2050  •  422262  atoms,  27954  molecules  •  2  ns/day  (2  fs/step)  •  Total  of  40ns  è  26  days  (6  wai:ng)    •  GROMOS  force  field  with  Gromacs  4.6.1*  

We  studied  the  interac:on  of  Adenine  with  the  bilayers  with  different  concentra:ons  of  UP  and  DPPC.  

Page 5: “Simulations of Lipidic Bilayers”. Prof. Dr. Kaline Coutinho – IF/USP.

Usually  the  force  field  parameters  of  solvents,  amino  acids  and  nucleic  acids,  sugars  and  carbohydrates  are  good  due  to  the  large  amount  of  experimental  (structural)  informa:on.    But,  what  about  solutes  (inhibitors,  sensors,  anesthe:cs,  drugs,  etc.),  which  in  general  the  experimental  informa:on  are  not  available  ?  The  bonded  and  Lennard-­‐Jones  (LJ)  parameters  are  considered  transferable  from  other  similar  molecules,  however  atomic  charges  are  calculated  using  quantum  mechanical  of  isolated  molecule.    (QM  ⇒  HF/6-­‐31G*  with  MK,  ChelpG  or  RESP)  

 Agen:on  with  this  procedure,  because  it  

does  not  include  polariza:on  !!!!  

[ ]

[ ]

∑⎥⎥

⎢⎢

⎟⎟⎠

⎞⎜⎜⎝

⎛−⎟

⎟⎠

⎞⎜⎜⎝

⎛ε+

∑+

−ϕ+∑+

δ−ϕ+∑+

θ−θ∑+

−∑=

θ

LJ ij

ij

ij

ijij

elec ij

ji

improper

torsions

n

oangles

orbonds

rB

rA

rqq

)cos(V

)ncos(V

)(k

)rr(kU

612

2

2

4

180212

12

2121

r  

U(r)  

Lennard-­‐Jones  

Coulomb  

bonded  

Page 6: “Simulations of Lipidic Bilayers”. Prof. Dr. Kaline Coutinho – IF/USP.

Experimental  data  N

N(CH2)n

CN

NC

I-

N

N

(CH2)n

CN

CN

+

++

+

+ I-

Ab  ini7o  molecular  dynamics  of  pyridinium  iodide  complex  (in  vacuum)

C3bis(4CP)2+  +2I-­‐  

Blue  Gene/P  •  512  cores  (minimum  available)  •  35  atoms,  108  valence  electrons  •  ~  1.2  ps/day  (:mestep  of  0.25  fs)  •  Total  of  20ps  è  20  days  (4  wai:ng)    •  DFT  (PBE)  with  CP2K*  sojware   *www.cp2k.org  

Page 7: “Simulations of Lipidic Bilayers”. Prof. Dr. Kaline Coutinho – IF/USP.

Ab  ini7o  molecular  dynamics  of  pyridinium  iodide  complex  (in  solu7on)

C3bis(4CP)+2  +2  I-­‐  +  80  acetonitrile   •  512  cores    •  515  atoms,  1388  valence  electrons  •  ~  0.5  ps/day  (0.25  fs/step)  •  Total  of  20ps  è  50  days  (10  wai:ng)    •  DFT  (PBE)  with  CP2K*  sojware  

We  explain  that  although  two  I-­‐  bind  with  the  pyridinium  only  one  I-­‐  par:cipates  of  the  electronic  excita:on.  

Blue  Gene/P  

Page 8: “Simulations of Lipidic Bilayers”. Prof. Dr. Kaline Coutinho – IF/USP.

Structural  proper7es  of  the  ab  ini7o  molecular  dynamics  are  used  to  parameterize  classical  force  fields  

Configura:onal  sampling  

Time  evolu:on  of  C  ·∙  ·∙  I  distance  

2.86  ±  0.27  Å    

3.29  ±  0.21  Å