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Almost the entire suspended oor load for the renovated structure was supported by the steel columns, while the edge of the oor slab provided lateral bracing to the original exterior brick walls. Replacing the existing oor system with a two-way at-plate structure had structural advantages in that a 6-inch-thick slab could easily support a 100 psf live load with the spans anticipated. An important advantage was the three-hour re rating easily obtained between oors of the building to be used as a dormitory. The major construction advantage of this system is that once the columns, which are spliced with a simple connection at each oor level, are erected and braced, the other construction materials are easily fabricated and placed. Concrete placed for the oor slab can take any shape contained within the exterior walls without a lot of eld measurements required to verify that fabricated components will actually t into the space to be reframed. The typical reinforcing in the oor system consisted of straight #4 bars. Cast-in-place concrete was conveyed into the building by pumping. Construction was simple in the horizontal direction in that large prefabricated structural shapes, dif cult to erect inside an existing building, were not required. Although accurate steel column placement was required for the new structural steel roof system to t, perimeter dimensions between the columns and the periphery of the building were not critical. The most important advantage is that erection of a new structural system within the brick envelope did not require the complete gutting of the building,



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Figure 6.4.9 Brightness tetnperatures of horizontal polarization at 37 GHz as a function of snow depth with various grain sizes based on the sticky particle model with T = 0.1 and fractional volume = 20%. The other parameters are listed in Tablc 6.4.4.

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snow depth (em) Figure 6.4.10 Brightness temperature differences of horizontal polarization as a function of snow depth with various grain sizes ba.'ied on the sticky particle model with T = 0.1 and fractional volume = 20%. The other parameterH are listed in Table 6.4.4.





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Right-Click Menu: JavaCharts allows for the copying and moving of items from list to list, the deletion of an item, and the tagging/untagging of an item. The ProphetCharts menu is similar, but you also have the ability to drag-and-drop items from list to list without having to use the rightclick menu at all. ( 4) Count: Exclusive to ProphetCharts. This provides a quantity count following the name of each watch list and portfolio in your modules. This makes it much easier to get a checksum when comparing portfolios to watch lists. ( 14)

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Baxter, R 1 (1968), Percus-Yevick equation for hard spheres with surface adhesion, J Chern Phys, 49(6), 2770-2773 Baxter, R .J (1970) Ornstein-Zernike relation and PerclU-;-Yevick approximation for fluid mixtures, J Chern Phys, 52, 4559-4562 Born, M and E Wolf (1975), Principles of Optics, 5th edition, Pergamon Press, New York Chow, P L, W E Kohler, and G C Papanicolaou, Eds (1981), Multiple Scattering and Waves in Random Media, North-Holland Publishing Company, Amsterdam Cruzan, O R (1961), Translational addition theorems for spherical vector wave functions, TR-906, Diamond Ordinance Fuse Laboratories, Department of the Army, Washington DC Cruzan, O R (1962), 'n'anslational addition theorems for spherical vector wave functions, Quart J Appl Math, 20, 33-40 Ding, K H (HI89), Electromagnetic wave propagation and scattering in dense media, PhD thesis, University of Washington, Seattle Ding, K H, C Mandt L Tsang, and 1 A.

Kong (1992), Monte Carlo simulations of pair distribution functions of dense discrete random media with multiple sizes of particles, / Eleetromag Waves and Appl, 6(8),1015-1030 Ding, K H and L Tsang (1988), Effective propagation eonHtants of denHe nontenuous media with mldti-HpecieH of partieles, J Elcctnnnag Waves and Appl, 2(8), 757-777 Ding, K H and L Tsang (1989), Progress in Eleetromag Res, 1 A Kong, Eel, 1, Ch 3, Elsevier Science PubliHhing Co, New York Ding K II and L Tsang (1992), IVlonte Carlo simulations of pair distribution functions of dense discrete random media with multiple Hizes of particleI' J Electrornag Waves and Appl, 6(8),1015-1030 Ding, K H, L rvL Znrk, and L THang (1994) Pair diHtribution functions and attenuation rates for Hticky particles in denHe media / Eleetromag Waves and Appl, 8(12), 15851604 Foldy, L L.

(1945), The multiple scattering of waveI', Phys Rev, 67,107-119 Hallikainen, M '1', F T Ulaby, and T E V Deventer (1987), Extinction behavior of dry Hnow in the 18- to 90-GHz range, IEEE Trans Geosei Remote Sens, 25(6), 737-750 Ishimaru, A and Y Kuga (1982) Attenuation constant of a eoherent field in a dense diHtribution of particles J Opt Soc Am, 72,1317-1320 Koh, G (1992), Experimental study of eleetromagnetic wave propagation in dense random media Waves in Random Media, 2, 39--48 Kuga Y, A Ishimaru, and D Rice (1993) Velocity of coherent and incoherent electromagnetic waveI' in a dens(' strongly scattering medium Phys Rev B 48, 13155-13158 Kuga, Y and P Phu (1995) Experimental techniqUE'S in random media and rough surface, Progress in Electromagnetics Resear'ch, 9 Elsevier Science Publishers, Cambridge, Mass Lam, C M and A.

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