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Figure E1. Tree structure for the Array source node - The Domain Data nodes are described separately in figure E2. Figure E2. Tree structure with the details of the Domain Data node. This note comes in two versions depending on weather Domain=Octave or Domain=Frequency. App-10
Figure E3 Images of the Mono, Dipol, Quadropol and Octopol directivity patterns installed with <strong>Odeon</strong> Auditorium and Combined, as viewed in the Far field balloon tab in the <strong>Odeon</strong> Array Source Editor. App-11
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ODEON ROOM ACOUSTICS SOFTWARE Versi
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ODEON Room Acoustics Software Versi
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Introduction This manual is intende
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SOFTWARE LICENSE AGREEMENT The foll
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Contents Introduction .............
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1 Installing and running the progra
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applied to all surfaces. In these c
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Update option Update to most recent
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2 Short guided tours This chapter w
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Define a line source (Combined edit
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Define a receiver grid and calculat
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Single Point response receiver and
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defined before ODEON can calculate
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Point Response calculations The Poi
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Archiving project files in one sing
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Define a multi surface source Click
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Other facilities in ODEON Apart fro
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2-34 Copenhagen Central Station Arr
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3 Modelling rooms Creating new room
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Experiences from tests with the fir
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3.2.2 ODEON Extrusion Modeller A sm
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The drawing has now been scaled and
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By checking Move all layers on laye
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To rotate a surface around a point
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BLOCK’s are not supported ODEON c
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Geometric rules, glue surfaces Surf
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3.4.1 Viewing the room in a 3DView
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Surfaces are missing from the model
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4 Materials This chapter covers mat
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Another option is to change the abs
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utton for finding material in the l
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5 Auralisation (Combined and Audito
Page 65 and 66: frequency response inverse to that
Page 67 and 68: are simulating an ordinary stereo s
Page 69 and 70: 6 Calculation Principles 6.1 Global
Page 71 and 72: The calculations carried out are di
Page 73 and 74: eflection order and up to the trans
Page 75 and 76: Scattering coefficient S s Surface
Page 77 and 78: oom; such as windows, doors, painti
Page 79 and 80: A last remark on Oblique Lambert is
Page 81 and 82: 6.9 Calculation method for Reflecto
Page 83 and 84: 7 Calculated Room Acoustical parame
Page 85 and 86: The calculated value of Lj(Average)
Page 87 and 88: 8 Calculation Parameters - Room Set
Page 89 and 90: Screen diffraction If this option i
Page 91 and 92: 9 Achieving good results The follow
Page 93 and 94: 9.1.3 Materials /absorption data Wr
Page 95 and 96: 10 Directivity patterns for point s
Page 97 and 98: inary and have the extension .SO8.
Page 99 and 100: An example; Full_Omni.dat on the fu
Page 101 and 102: 11 Line array sources This section
Page 103 and 104: 11.2 Playing with delay One advanta
Page 105 and 106: Figure 11-6. The radiation in octav
Page 107 and 108: Appendix A: References Affronides,
Page 109 and 110: Kristensen, J. (1984). Sound Absorp
Page 111 and 112: Appendix B: Vocabulary The techniqu
Page 113 and 114: Appendix C: Specify Transmission th
Page 115: Appendix D: Description of XML form
Page 119 and 120: When developing export facilities f
Page 121 and 122: InvertPhase="false" - If phase is i
Page 123 and 124: speaker deliver 1W. The reason why
Page 125 and 126: You may describe coordinates using
Page 127 and 128: Example 1: Const CeilingHeight 3.4
Page 129 and 130: As a special option for multi point
Page 131 and 132: 5411>5401 5512>5522 Elevation surfa
Page 133 and 134: If an elevation surface has 22 surf
Page 135 and 136: Name of counter to be used by the F
Page 137 and 138: The UCS command is used to create a
Page 139 and 140: As another option the colour of the
Page 141 and 142: Width is oriented in the Y-directio
Page 143 and 144: The Cone statement The Cone stateme
Page 145 and 146: ### Const N 16 Const W 10 Const H 3
Page 147 and 148: Surf 2 ceiling 11 12 13 14 Surf 3 e
Page 149 and 150: Surf 100 Circular floor 100>100+N-1
Page 151 and 152: The window example shows how a cyli
Page 153: Appendix G: Importing geometries -
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