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Related Concept Videos

Calculating Standard Free Energy Changes02:49

Calculating Standard Free Energy Changes

The free energy change for a reaction that occurs under the standard conditions of 1 bar pressure and at 298 K is called the standard free energy change. Since free energy is a state function, its value depends only on the conditions of the initial and final states of the system. A convenient and common approach to the calculation of free energy changes for physical and chemical reactions is by use of widely available compilations of standard state thermodynamic data. One method involves the...
Free Energy Changes for Nonstandard States03:25

Free Energy Changes for Nonstandard States

The free energy change for a process taking place with reactants and products present under nonstandard conditions (pressures other than 1 bar; concentrations other than 1 M) is related to the standard free energy change according to this equation:
Gibbs Free Energy02:39

Gibbs Free Energy

One of the challenges of using the second law of thermodynamics to determine if a process is spontaneous is that it requires measurements of the entropy change for the system and the entropy change for the surroundings. An alternative approach involving a new thermodynamic property defined in terms of system properties only was introduced in the late nineteenth century by American mathematician Josiah Willard Gibbs. This new property is called the Gibbs free energy (G) (or simply the free...
Thermodynamic Potentials01:26

Thermodynamic Potentials

Thermodynamic potentials are state functions that are extremely useful in analyzing a thermodynamic system. They have dimensions of energy. The four important thermodynamic potentials are internal energy, enthalpy, Helmholtz free energy, and Gibbs free energy. These thermodynamic potentials can be expressed using two of the following variables: pressure, volume, temperature, and entropy. These two variables are expressed as the rate of change of the thermodynamic potential with respect to other...
Free Energy01:21

Free Energy

Free energy—abbreviated as G for the scientist Gibbs who discovered it—is a measurement of useful energy that can be extracted from a reaction to do work. It is the energy in a chemical reaction that is available after entropy is accounted for. Reactions that take in energy are considered endergonic and reactions that release energy are exergonic. Plants carry out endergonic reactions by taking in sunlight and carbon dioxide to produce glucose and oxygen. Animals, in turn, break down the...
Free Energy and Equilibrium00:55

Free Energy and Equilibrium

The free energy change for a process may be viewed as a measure of its driving force. A negative value for ΔG represents a driving force for the process in the forward direction, while a positive value represents a driving force for the process in the reverse direction. When ΔG is zero, the forward and reverse driving forces are equal, and the process occurs in both directions at the same rate (the system is at equilibrium).
The reaction quotient, Q, is a convenient measure of the status of an...

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Related Experiment Video

Updated: Jun 8, 2026

Multiscale Sampling of a Heterogeneous Water/Metal Catalyst Interface using Density Functional Theory and Force-Field Molecular Dynamics
10:52

Multiscale Sampling of a Heterogeneous Water/Metal Catalyst Interface using Density Functional Theory and Force-Field Molecular Dynamics

Published on: April 12, 2019

Enhanced free-energy calculation using multiscale simulation.

Hiromitsu Shimoyama1, Yasushige Yonezawa, Haruki Nakamura

  • 1Laboratory of Protein Informatics, Research Center for Structural Biology Institute for Protein Research, Osaka University, 3-2 Yamadaoka, Suita, Osaka 565-0871, Japan. shimoyama@protein.osaka-u.ac.jp

The Journal of Chemical Physics
|October 15, 2010
PubMed
Summary

We developed a multiscale simulation method combining coarse-grained models and all-atom models to efficiently calculate protein free-energy landscapes. This approach significantly reduces computational time for protein folding studies.

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Realistic Membrane Modeling Using Complex Lipid Mixtures in Simulation Studies
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Realistic Membrane Modeling Using Complex Lipid Mixtures in Simulation Studies

Published on: September 1, 2023

Area of Science:

  • Computational biology
  • Biophysics
  • Molecular modeling

Background:

  • Calculating protein free-energy landscapes is crucial for understanding protein folding and function.
  • Traditional all-atom simulations are computationally expensive, limiting their application to large systems or long timescales.
  • Coarse-grained models offer efficiency but often lack the accuracy needed for detailed landscape analysis.

Purpose of the Study:

  • To develop and validate a novel multiscale simulation method for efficient and accurate protein free-energy landscape calculation.
  • To combine the strengths of coarse-grained models (CGM) and all-atom models (AAM) for enhanced computational performance.
  • To reduce the computational cost associated with determining protein conformational dynamics.

Main Methods:

  • A multiscale simulation strategy integrating CGM and AAM was proposed.
  • Coarse-grained simulations were employed for rapid exploration of protein conformational space.
  • Information from CGM was used to enhance subsequent all-atom simulations for free-energy landscape determination.

Main Results:

  • The multiscale method was successfully applied to the chignolin protein folding system.
  • A significant reduction in computational time, up to 90%, was achieved compared to traditional methods.
  • Accurate free-energy landscapes were obtained, demonstrating the efficacy of the combined approach.

Conclusions:

  • The proposed multiscale simulation method offers a computationally efficient and accurate approach for protein free-energy landscape calculations.
  • This method holds promise for advancing the study of protein folding, dynamics, and function.
  • The integration of CGM and AAM provides a powerful tool for molecular modeling in biophysics.