Dutt, S K

Gupta, M M Sen

English

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40 APPLICA TION OF THE THEORY OF RANDOM SCATTERING ON THE INTENSITY V ARIA TIONS OF THE DOWN-COMING WIRELESS. W A YES OVER LONG TRANSMISSION PATHS By M. M. SEN CUPTA 1": AND S. K. DUTT' ABSTRACT. Pawse.,·'s theory of random s{,!Itterint to explain the variation of the ampli-tude of dowll-coming radio waves was applied in thp case: of transmission over l110dnately great distances in the mediulII wave hand Rt;sults ilJ(lkate that while random scattering is a predomi-lIant factor in determining the- strength of the down-coming waves, the ohst'rvational data cannot b(' flllly accounted for h.\' this th('ory alone. It is suggested tlmt for long transmission paths the presence of other factors mils! also he taken into consideration. INTRODUCTION Pawseyl has shmvn that a single reflected ray from ionosphere does not consist of a single ray but is huilt up of elementary contributions from u series of dit1racting centres distributed l1lorc or less at random in the ionosphere. Working with a wavelength in the medium band (200 111. to 500 m.), he found that the variation of the amplitude of the down-coming wave is consistent with the probability formula given by I~ord Rayleigh. The result of his experiments, was obtained with a transmission path of 56 KillS. (London Regional Transmitter --Sydney Sussex College Receiving Station); it was thought desirable to test whether the theory of random scattering as given hy Pawsey is applicahle even when the transmission path is made considerably great. The present communi-cation gives an account of the study of variation of intensity of down-coming waves in the medium band (wavelengths 370.4111. and 257.1 m.) from two lndian Broadcasting stations, Tiz., Calcutta and Dacca, at distances as great as 480 and 610 Kms. * All the data for meastllements "were obtained in our case from auto-matic photographic records of received siJ.wals taken between the hours 6 P.M. and 10-30 P.M. over a reriod of about two years. • Recently a paper has been published by Kho~tgir and Ray (I/ldiall .To"lIlllal of Physics, 11, 283, 1940), hut here also the di~tnn("1' was not more than 245 Kms Moreover, the data \V~rt' secured from visual observation of galvanometer deflections 448 M. M. Sen Gupta and S. K. Dutt AUTOMATIC Rr~CORDING The automatic recording was made as follows :-A bromide paper was fixed on a drum rotated by a clockwork, the whole system being put hlside a light-tight box. On one side of the box there was a fine horizontal slit which could be opelll·d or dosed. The vertical image of the straight filament of a lamp formed by retLctioll frolll the galvanometer mirror was allowed to fall on the slit. The deflection of the s)lot of light at any instant was thus automatic-aIly recorded. The vcrticallil1es in the photographic records of Fig. 4 were obtained by weaus of another clockwork making contacts of an electric circuit containing a 4-volt lump every 4 minutes. RECRIVTNn SYSTEM The receiver was a battery set of the superheterodyne type cOllsistitlg of two stag-es of H. F. amplification preceding an octcc'lc fn.:queucy·c:l!anger with a separate oscillator and one stage of 1. II. amplification followed by a second detector which was a douh1e·diodl'·triodc giving a linear detection. The relation bet\\~ell the input voltage and the ddlectioll ill the gulvanom<.:tcr is showlJ in Fig. T. It will be observed thut it is practicaliy linear withiu the working rallg<: i-S 8 IlO .5 Calibrating H. F. ('urrt'llt in the coil of :1 turns. (I) Diode bias ... (. volt. (21 niode hi as ... ".$ volt. FIG. I except for field strengths below 70 detector in some of om measurements. detection are shown in Figs. 2 and 3· ,.,.1'/ Ill. We had also llSl'd Ii sQuare-la\\ The circuit di~grall1s of hoth types of Application 0/ Theory 0/ Random Scattering, etc. 449 FIC. 2 ...r .. -, L .. L--_ .. - .. --- ---'\"NVV 1,._ ... -00.....--- + ~'l"aH' ,JIlII' J It'l~( It '1". (]D~r ,; ,> ~!C.~\ll).I.J. < 'L, 1:'0 v 1 Tile calibration of Ihe receiving sci (f'/lOlo,R'rajJhically) and calculaliotl 0/ the jidd strellglhs.--Thc calibration of the receiving set was done by the method adopted by the Standardization Committee of Radio Engineers (Rund's High Frequency Measurements, page 346). A small coil of 2 turns was placed along the axis of the loop aerial. The deflections d 1, d2 , d3 [ Fig. 4 (b)] in the output galvanometer (G) corresponding to known H. F. currents in miiliamps. of the same frequency as that of the signal in suitable steps were photographed. This was done both in the beginning and at the end of each observation with the loop set hI the minimum position. The line joining the spots. in the beginning and end of each observation for a particular H. F. current thus gave the strength level when reduced to micro-volts per metre. A graph walrplotted with galvano-meter deflection against calibrated field strength, from which the desired field strength corresponding to any deflection could be easily evaluated. It will be observed from photographic records that the zero setting remained almost undisturbed throughout the period of observation which was 2 hours ~"387P'-Vl 450 M. M. Sen Gupta and S. K. Dutt generally and ahout 30 minutes in some cases. In some of the records of the spots, changes of deflection could be noticed in the beginning but this invari-ably settled down to constant values. The variations noticed were due to the movement of the spot while setting the loop from maximum to minimum position or due to fluctuation of H. F. current while adjusting to a particular value [Fig. 4(b)]. The he am of light giving the spot \vhen switched off while bringitlg the loop to minimum position ?r adjusting the H. F. current and switched on again after a minute or so, the variations disavpear. The level line in each case was dravm along horizontal portion of the path traced by the spot. The frequency of the calibrating H. F. currents was set by adjusting the local oscillator to exact no beat condition with the help of a very slow motion vernier dial of ratio I : 80 operated by a long earthed handle outside the shielded cover of the oscillator. The strength of the H. F. current (I mAl passing through the inducing coil of N turns and radius r was measured by Cambridgc' Vacuum Junc-tion of 5 rnA range which had been previously calibrated by comparison with ?lIoullin's Multi-range Thermal Milliammeter. Tht; voltage E induced in the loop at a perpendicular distance d from the coil was then calculated from the formula* , r8840 I t 2 N L=k _.-_.-. -!,-1.'/II/. (d 2 +r2 ).1,/2 The deflections due to the calibrating fields ill thc case of the diode detector were found to be linear except for very I()w field strengths. All our observations excepting a few ill the beginning were, thereforc, taken with tlIl' diode detector. This facilitated evalllation with greater accmacy of resl1lt~ thall was possible with the slJllare-law detector. GROUND WAVr.; Sl'I'I'RESSTI)N r'\>r n:liablc re:>ults due consideration 11111st he paid to the ground wavc e!Teet as well as tht; antenna effect. In our experimcnts the magnitudc of the grouud wave was found to be negligible relative to that of the sky wave. This is quite in accord:ll1cc with the experimental results given hy Sommerfield and Eckersley. The distances of the two broadcasting statiolls Ca1cntta ('\=370-4111.) and Dacca ('\=257.1 111.) are 480 Kl11. and 610 K1l1. respectively. Corresponding to these dista11ces and wavelengths the strength of the ground wave field intensities given are 40(J.'V / 111 for good ground and 1.4 !'-'V / m for poor ground assuming power output in the transmitter to be 2 kilowatts for Calcutta; for Dacca these are zero for distances over 500 Km. for good ground and also zero for dista11ces over 350 Rm. for poor ground. These values are obtained from unmodified Sommer-Held curves and if diffraction corrections are applied according to Eckersley, I • As d was not very large in comparison with the dimensions of the loop, the ('orrectiop factor Ii WIlS Hit'todllced in the actual calculation. Application of Theory of Random Scattering, etc. 451 these become still less. The length of the horizontal slit in front of the bromide paper was 130 nllns. only and so the output galvanometer G had to be adjusted in our case for 130 mm. deflection for the maximum field intensity in any setting. This maximum field intensity recorded was of the order of 300 }l7) / m for Dacca and 600 f.J.V / m for Calcutta. Thus even assuming the ground wave intensity for good conducting grounds, the deflection that will be recorded will not be more than I H1In. for Calcutta, while for Dacca it'.would be still less. In Pawsey's experiments the ground wave component wa(as much as 20 times stronger than the sky wave componellt~· and hence the groun~wave suppression was absolutely llecessary in his case. From the above cOllsiierations it will be seen that at the transmission distances with which we worked, tile ground wave component being practically negligible cOl11vared to tile sky wate component 110 special arrange-ment was necessary for its suppressioll. , In order to millimise the antenna effect as ~uch as possible, the dimensions of the loop were Illade purposely small. The loo~iwas nearly 86 cm. square and had 6 to 8 turns of wire. The effective height "\'$ about 100 ems. The following procedure was adopted to test the magnitudes of both the ground wave effect and the antenna effect relative to tIle maximum sky wave component :-During day-time the zero position of the galvanometer was noted with all the high tensions of the set switched on except tbat of the oscillator valve. The reading in the galvanometer (C) gave the actual zero of the graph, i,e., the real zero signal strength level [H ill Fig. ,1 (a)]. The 11. 1'. of the oscillator valve \Vas then switched on with the lool! set both in the maximullI and minimulll positions. It was seen that there was absolutely no change reconk<l ill the zero readillg B ill Fig. 4(a) for the wbole veriud of observation which ,\"as not less than half an hour indicatillg that boll I the gr0l1l1d and antelllJa eiTec1s wele practically negligible. The readings for different strellgth. levels wert' then takE'n in steps in the way ex-plained before {ullder the heading 'Calibratioll (If tlw Set'). Without disturbing the adjustl11ellts made during the daytinle, the abovc procedure was repeated during the night-time reception jJeriod 6.00 to ](),30 1'.1\1., but now with the loop ill the minimuIIJ position only, The records showed agaill the absence of any appre-ciable change either in the zero level or in those for the differellt strength levels both in the beginning as weJl as at the cud of the period of observatioll (Fig, 4). 'rhus it will be seen that in our arrangelllCnts the antclIlla dft'ct \\"as negiigiblc even during the night time. Some typical records givillg the variatIOn of galvanollleter deflection with time are shown in Plaie XIV. The ordinate r represel1ting the galvanOllletcr deflectioll \Vas di\'ided into a large number of small parts each representing equal challgc of field irltellsity by • In Khastgir and Ray's work the ground wave COlllp011cnt was 3 to 4 times ~trol1ger than the sky wave componrnL \, 452 M. M. Sen Gupta and S. K. Dutt utilising the calibration graph plotted with field intensity against galvanometer deflection. The abscissa representing time was also divided into half-minute intervals. The number of a particular alllvlitude bctween rand r + dr that occurred during the period was counted, the amplitude within the range occuning for half a miul1te being counted as one. From this the fraction of the total time during which the amplitude lay between rand 1 + dT was determined. As men-tioned before, all our records were taken for periods varying from half an hour to two hours. * Distribution curves were then ura wn with values of fractions so ob-tained against average amplitudes of 1 and r + dr. Fr0111 these curves the vaiue of the 1110st probable alllplitude r", was obtained; this value of rll, \\'as used in draw-ing the theoretical probability curves ill accordance with Rayleigh's expression (where R 2 ... the Stull of the squares of thc cOlllponcnts I"dr ... the prohahility of a resultant amplitude betweclJ 7 and 7 + dr) for the probability of occurrcnce of any resultant amplitude Oil the assumption of a large llulllhcr of componcnts of random pbases. The maxilllum value of 1" corresponds to R 2 = 21;' where rIll is the most probabic value of r in the eXlleri-t .~" I 110 , \ '+, " ',+< '"k o~----~----__ ~. ____ -L!_~~=h~_+~ __ o 4 for S r~ (a) Calcutta 2-12-37 FIG. 5(a) 16 fur r~ (b) Dacca 16-1-40 FIG. 5(b) • The chief L'tJllsidemtiol1H being practical ('()mcniellce and sufficient number of readings, we made the total period of observation half an hour and more, Fig. 4(a)-Calcutta, 18. 1. 39. Fig. 4(b)-Dacca, 12. 2. 40. Time ~ Time~ Fig. 4(c)-Calcutta, 7. 12. 37. 749 P.M. en [1":1 Z C") c :s "l> At ~ ~ 3> pj X :< Application of Theory of Random Scattering. etc. 453 mental distribution curves. The scales in the figures have been adjusted to give the best fit. Figs. 5 and 6 give the typical results in which the experimental curves are shown as full-line curves and the theoretical ones as dotted. It will be seeu from the experimental results that the agreement between the theoretical and exp~rimelltai curves are not as good as ill cases of experiments* with smaller transmission distances. We have, therefore, sbown the results in two broad representative types, 'Viz., those with fair agree.ent (Fig. 5) and those showing ,~. great divergence (Fig. 6). It may, therefore, bel concluded on the basis of our observations that for long trausmission paths ~e intensity ofJhc down-coming waves is 110t determined only by irregular scatteri4g at the ionosphere but also by r~ for (al Calcutta 7- I 2-37 FIG. 6(a) for ,~ (b) Dacca 12-2-40 FIG.6(b) the existence of other fadors; the: effect of the latter sometimes becomes quite appreciable as may be found ill the :.md lype of curves (Fig. ()). Observations are being continued to study fully the l1ahire of these factors. 111 conclusion, the authors take this opportunity to thank Principal R. Prosad, LE.S , who has taken lIlud, iuterest in OUf work. One of I1S (5. R. D.) is grate-ful to the Government of Bihar for the grant of a research scholarship which has enabled him to take part in this work. PHYSICAl. LABORATORY, PATNA SClIlNCE COI.I.I!CE. * Experiments by Pawseyl and by Khastgir and Ray.S RBFBRENCBS I Pawsey, Proc. Camb. Phil. Soc., 81, 125 (1935). , Eckersley, Proc. I.R.E., SO, 1555 (1932). 3 Khastgir and Ray, Indian Jour. of Phys., iI, 283(1940) 

Application of the Theory of Random Scattering on the Intensity Variations of the Down-Coming Wireless Waves Over Long Transmission Paths

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Application of the Theory of Random Scattering on the Intensity Variations of the Down-Coming Wireless Waves Over Long Transmission Paths

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