The medium matrix is given by

where ρ_k,r is the volume density of (inertial) mass and S_t,j,p,q is the compliance.

For electromagnetic waves the spatial differential operator in the system of (3.12) is given by

The medium matrix is found to be

where ε_k,r is the permittivity and μ_J,P is the permeability.

FRONT MATTER (R1-R12)

OPENING REMARKS (1-3)

INTRODUCTION (4-4)

1 HIGH-ORDER, MULTILEVEL, ADAPTIVE TIME-DOMAIN METHODS FOR STRUCTURAL ACOUSTICS SIMULATIONS (5-49)

2 DISTRIBUTED FEEDBACK RESONATORS (50-71)

3 ACOUSTIC, ELASTODYNAMIC, AND ELECTROMAGNETIC WAVEFIELD COMPUTATION - A STRUCTURED APPROACH BASED ON RECIPROCITY (72-88)

4 NUMERICAL MODELING OF THE INTERACTIONS OF ULTRAFAST OPTICAL PULSES WITH NONRESONANT AND RESONANT MATERIALS AND STRUCTURES (89-102)

5 ALGORITHMIC ASPECTS AND SUPERCOMPUTING TRENDS IN COMPUTATIONAL ELECTROMAGNETICS (103-121)

6 ADAPTIVE FINITE ELEMENT METHODS FOR THE HELMHOLTZ EQUATION IN EXTERIOR DOMAINS (122-142)

7 MODELING OF OPTICALLY (143-161)

8 SYNTHESIS AND ANALYSIS OF LARGE-SCALE INTEGRATED PHOTONIC DEVICES AND CICUITS (162-182)

9 DESIGN AND ANALYSIS OF FINITE ELEMENT METHODS FOR TRANSIENT AND TIME-HARMONIC STRUCTURAL ACOUSTICS (183-203)

10 AN OVERVIEW OF THE APPLICATION OF THE METHOD OF MOMENTS TO LARGE BODIES IN ELECTROMAGNETICS (204-220)

11 DISCUSSION (221-240)

APPENDICES (241-242)

A SYMPOSIUM AGENDA (243-245)

B SPEAKERS (246-249)

C SYMPOSIUM PARTICIPANTS (250-252)