25
2015-10-17 ISBS 2015, Medan, Indonesia 1 In Searching of Trees Natural Vibration Frequency Based on Granular Particles Interactions and Vibration S. Viridi 1,* , P. Patana 2 , S.A. Subrata 3 , H. Hertiasa 1 , M. Abdullah 1 1 Institut Teknologi Bandung, Jl. Ganesha 10, Bandung 40132, Indonesia 2 University of Sumatera Utara, Jl. Biotechnologi 1, Medan 20155, Indonesia 3 Gadjah Mada University, Jl. Agro 1, Bulaksumur, Yogyakarta 55281, Indonesia *[email protected]

In Searching of Trees Natural Vibration Frequency Based on Granular Particles Interactions and Vibration

Embed Size (px)

Citation preview

2015-10-17 ISBS 2015, Medan, Indonesia 1

In Searching of Trees Natural Vibration Frequency Based on Granular Particles

Interactions and Vibration

S. Viridi1,*, P. Patana2, S.A. Subrata3, H. Hertiasa1, M. Abdullah1

1Institut Teknologi Bandung, Jl. Ganesha 10, Bandung 40132, Indonesia2University of Sumatera Utara, Jl. Biotechnologi 1, Medan 20155, Indonesia

3Gadjah Mada University, Jl. Agro 1, Bulaksumur, Yogyakarta 55281, Indonesia*[email protected]

2015-10-17 ISBS 2015, Medan, Indonesia 2

Outline

• Introduction• Model• Molecular dynamics method• Nomenclature of tree model• Simulation parameters• Results and discussion• Summaries

2015-10-17 ISBS 2015, Medan, Indonesia 3

Introduction

• A tree is an interesting entity from physics point of view

• Morphology of a tree is influenced by factors that is inducing stresses on tree diameter variation (Dassot et al., 2015)

• Even in details, angle of individual leaf inclination is under influence of its weight and wind (Tadrist et al., 2014)

2015-10-17 ISBS 2015, Medan, Indonesia 4

Introduction (cont.)

• These factors also induce the density and strength of the wood (Fournier et al., 2013)

• Various branch diameters of a tree are response to winds from its surrounding and also other factors such as rains, snows, fruits, and upper parts of the tree, since a branch must support the stress induced by this loads (Eloy, 2011)

2015-10-17 ISBS 2015, Medan, Indonesia 5

Introduction (cont.)

• Tree damage after a storm can be used to predict the wind velocity (Frelich and Ostuno, 2012)

2015-10-17 ISBS 2015, Medan, Indonesia 6

Model

• Two dimension model

2015-10-17 ISBS 2015, Medan, Indonesia 7

Model (cont.)

• Push-pull spring force

ijijijSij rlrcS ˆ

2015-10-17 ISBS 2015, Medan, Indonesia 8

Model (cont.)

• Bending spring force

ijkijkBijk c

2015-10-17 ISBS 2015, Medan, Indonesia 9

Model (cont.)

• Gravitation force

• Wind force

gmG ii

wiFi vvDcF

2015-10-17 ISBS 2015, Medan, Indonesia 10

Model (cont.)

• Neighbor particles interaction

2015-10-17 ISBS 2015, Medan, Indonesia 11

Molecular dynamics method

• Newton’s second law of motion

trtrtrB

trtrS

tvtvDcm

gta

kjiijk

ikijjiij

wiFi

i

,,

,

1

,

2015-10-17 ISBS 2015, Medan, Indonesia 12

Molecular dynamics .. (cont.)

• Euler algorithm

ttatvttv iii

tttvtrttr iii

2015-10-17 ISBS 2015, Medan, Indonesia 13

Nomenclature of tree model

2015-10-17 ISBS 2015, Medan, Indonesia 14

Simulation parameters

2015-10-17 ISBS 2015, Medan, Indonesia 15

Simulation parameters (cont.)

2015-10-17 ISBS 2015, Medan, Indonesia 16

Results and discussion

• Unstable configuration: N = 9, λijk = 0.1164

2015-10-17 ISBS 2015, Medan, Indonesia 17

Results and discussion (cont.)

• Stable configuration: N = 9, λijk = 0.0873

2015-10-17 ISBS 2015, Medan, Indonesia 18

Results and discussion (cont.)

2015-10-17 ISBS 2015, Medan, Indonesia 19

Results and discussion (cont.)

• Introducing wind v = 1 on N = 9 (stable)

2015-10-17 ISBS 2015, Medan, Indonesia 20

Results and discussion (cont.)

• Introducing wind v = 16 on N = 9 (unstable)

2015-10-17 ISBS 2015, Medan, Indonesia 21

Results and discussion (cont.)

• Introducing wind v = 64 on N = 9 (stable)

2015-10-17 ISBS 2015, Medan, Indonesia 22

Results and discussion (cont.)

2015-10-17 ISBS 2015, Medan, Indonesia 23

Summaries

• A tree model based on granular particle has been constructed

• Relaxation process small value of λijk in order to give stable tree configuration

• There is certain value of wind velocity that turn the stable configuration into unstable one resonance frequency

2015-10-17 ISBS 2015, Medan, Indonesia 24

Acknowledgements

• DAAD and Committee of ISBS 2015 is supporting dissemination part of this work

• Riset Unggulan Perguruan Tinggi - Desentralisasi Dikti in year 2015 with contract number 310i/I1.C01/PL/2015 is supporting calculation part of this work

2015-10-17 ISBS 2015, Medan, Indonesia 25

Thank you