UHF propagation in indoor hallways

A new model for UHF propagation in large buildings is presented. This model relies on knowledge of the interior arrangement of the building without requiring much detail. The guiding of radiation along hallways is the most significant propagation process at distances of more than 10 m from the transmitter. The waveguide model predicts the power loss rate along the hallways, which is affected by the coupling among the propagating modes. The coupling results from the roughness of the surfaces in the building; it is predicted in an average manner using the average deviation of the walls from perfect smoothness. The model predictions are compared to measurements in an office building and to ray tracing predictions.

[1]  Werner E. Kohler Propagation in a randomly perturbed multimode matched waveguide , 1982 .

[2]  U. Dersch,et al.  Propagation mechanisms in microcell and indoor environments , 1994 .

[3]  J J Burke,et al.  Propagation constants of resonant waves on homogeneous, isotropic slab waveguides. , 1970, Applied optics.

[4]  J. Lee,et al.  Coupling at L, T and cross junctions in tunnels and urban street canyons , 2001, IEEE VTS 53rd Vehicular Technology Conference, Spring 2001. Proceedings (Cat. No.01CH37202).

[5]  M. Lecours,et al.  Measurement and modeling of propagation losses in a building at 900 MHz , 1990 .

[6]  H. L. Bertoni,et al.  Transmission and reflection properties of interior walls , 1994, Proceedings of 1994 3rd IEEE International Conference on Universal Personal Communications.

[7]  D. Marcuse Fluctuations of the power of coupled modes , 1972 .

[8]  G. Cancellieri,et al.  Mode coupling effects in optical fibres: perturbative solution of the time-dependent power flow equation , 1983 .

[9]  Adam E. Heimrath,et al.  Random Multimode Optical Media: I. Mode Coupling Process in Slab Waveguide with Stochastic Wall Perturbations , 1992 .

[10]  F. Kneubühl,et al.  Transversely excited 337 μm HCN waveguide laser , 1975 .

[11]  T. Rappaport,et al.  A comparison of theoretical and empirical reflection coefficients for typical exterior wall surfaces in a mobile radio environment , 1996 .

[12]  Bruno Crosignani,et al.  Theory of time-dependent propagation in multimode lightguides , 1977 .

[13]  William C. Stone,et al.  Electromagnetic Signal Attenuation in Construction Materials , 1997 .

[14]  N. Blaunstein Radio Propagation in Cellular Networks , 1999 .

[15]  Dietrich Marcuse,et al.  Radiation losses of dielectric waveguides in terms of the power spectrum of the wall distortion function , 1969 .

[16]  Donald C. Cox,et al.  Modal analysis of MIMO capacity in a hallway , 2001, GLOBECOM'01. IEEE Global Telecommunications Conference (Cat. No.01CH37270).

[17]  Reinaldo A. Valenzuela A ray tracing approach to predicting indoor wireless transmission , 1993, IEEE 43rd Vehicular Technology Conference.

[18]  D. Marcuse Derivation of coupled power equations , 1972 .

[19]  Donald C. Cox,et al.  MIMO capacity in hallways and adjacent rooms , 2002, Global Telecommunications Conference, 2002. GLOBECOM '02. IEEE.

[20]  Theodore S. Rappaport,et al.  Wireless communications - principles and practice , 1996 .

[21]  Dietrich Marcuse Higher-order loss processes and the loss penalty of multimode operation , 1972 .

[22]  Henry L. Bertoni,et al.  UHF propagation prediction for wireless personal communications , 1994, Proc. IEEE.

[23]  Dietrich Marcuse,et al.  Mode conversion caused by surface imperfections of a dielectric slab waveguide , 1969 .

[24]  Brian W. Kernighan,et al.  WISE design of indoor wireless systems: practical computation and optimization , 1995 .

[25]  D. Marcuse,et al.  Power distribution and radiation losses in multimode dielectric slab waveguides , 1972 .