F~2,M~2=u3×1⁢q2+M3×3·p2+N3×5·Q^2+T3×10·O^2. ]]>;When the approximations are applied to small or medium-sized molecules, such as biomolecules of current interest such as proteins, the electrostatic force computations according to the approximations of the present invention are faster than the direct or fast multipole methods."/> Method and system for calculating the electrostatic force due to a system of charged bodies in molecular modeling
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Method and system for calculating the electrostatic force due to a system of charged bodies in molecular modeling

机译:在分子建模中计算由于带电体系统引起的静电力的方法和系统

摘要

In the molecular modeling of a molecular system represented by constituent charged rigid bodies, the electrostatic interactions are computed between the rigid bodies, rather than the individual atoms which constitute the bodies. Multipole representations of the charge distribution of the bodies are used, and the total translational force and moment acting on each rigid body are computed using approximations of the form: <mrow><msub><mover><mi>F</mi><mo>~</mo></mover><mn>2</mn></msub><mo>,</mo><mrow><msub><mover><mi>M</mi><mo>~</mo></mover><mn>2</mn></msub><mo>=</mo><mrow><mrow><munder><mi>u</mi><mrow><mn>3</mn><mo>&amp;times;</mo><mn>1</mn></mrow></munder><mo>&amp;it;</mo><msub><mi>q</mi><mn>2</mn></msub></mrow><mo>+</mo><mrow><munder><mi>M</mi><mrow><mn>3</mn><mo>&amp;times;</mo><mn>3</mn></mrow></munder><mo>&amp;CenterDot;</mo><msub><mi>p</mi><mn>2</mn></msub></mrow><mo>+</mo><mrow><munder><mi>N</mi><mrow><mn>3</mn><mo>&amp;times;</mo><mn>5</mn></mrow></munder><mo>&amp;CenterDot;</mo><msub><mover><mi>Q</mi><mo>^</mo></mover><mn>2</mn></msub></mrow><mo>+</mo><mrow><munder><mi>T</mi><mrow><mn>3</mn><mo>&amp;times;</mo><mn>10</mn></mrow></munder><mo>&amp;CenterDot;</mo><mrow><msub><mover><mi>O</mi><mo>^</mo></mover><mn>2</mn></msub><mo>.</mo></mrow></mrow></mrow></mrow></mrow> ;When the approximations are applied to small or medium-sized molecules, such as biomolecules of current interest such as proteins, the electrostatic force computations according to the approximations of the present invention are faster than the direct or fast multipole methods.
机译:在以带电荷的刚体为代表的分子系统的分子模型中,静电相互作用是在刚体之间而不是在构成刚体的单个原子之间进行计算的。使用物体电荷分布的多极表示法,并使用以下形式的近似值计算作用在每个刚体上的总平移力和力矩: <图像文件=“ US20030216900A1-20031120-M00001.GIF” he =“ 16.07445” id =“ EMI-M00001” imgContent =“ undefined” imgFormat =“ GIF” wi =“ 216.027“ /> <![CDATA [ F 2 < / msub> M 2 = u 3 &times; 1 &it; q 2 < mo> + M 3 &times; 3 < / mrow> &CenterDot; p 2 + N 3 &times; 5 &CenterDot; Q ^ 2 + T 3 &times; 10 &CenterDot; O ^ 2 ]]> ;当将近似值应用于小型或中型分子,例如当前感兴趣的生物分子,例如蛋白质,根据本发明的近似值的静电力计算比直接或快速多极方法更快。

著录项

  • 公开/公告号US2003216900A1

    专利类型

  • 公开/公告日2003-11-20

    原文格式PDF

  • 申请/专利权人 PROTEIN MECHANICS INC.;

    申请/专利号US20030371978

  • 发明设计人 DAN E. ROSENTHAL;

    申请日2003-02-21

  • 分类号G06G7/58;G06G7/48;

  • 国家 US

  • 入库时间 2022-08-21 23:16:00

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