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Gain (antenna)

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38: 3684: 95: 1697: 3392: 3375: 1325: 3679:{\displaystyle {\begin{aligned}G_{\frac {\lambda }{2}}&={\frac {60^{2}}{30R_{\frac {\lambda }{2}}}}={\frac {3600}{30R_{\frac {\lambda }{2}}}}={\frac {120}{R_{\frac {\lambda }{2}}}}={\frac {1}{{}^{\int _{0}^{\frac {\pi }{2}}{\frac {\cos \left({\frac {\pi }{2}}\cos \theta \right)^{2}}{\sin \theta }}d\theta }}}\ ,\\&\approx {\frac {120}{73.1296}}\approx 1.6409224\approx 2.15088\ {\mathsf {\ dBi}};\end{aligned}}} 688:
radiator is known to be 1.64 and it can be made nearly 100% efficient. Since the gain has been measured with respect to this reference antenna, the difference in the gain of the test antenna is often compared to that of the dipole. The gain relative to a dipole is thus often quoted and is denoted using dBd instead of dBi to avoid confusion. Therefore, in terms of the true gain (relative to an isotropic radiator)
3965: 2908: 1692:{\displaystyle {\begin{aligned}P_{\text{rad}}&=\int _{0}^{2\pi }\int _{0}^{\pi }U(\theta ,\phi )\sin(\theta )\,d\theta \,d\phi =2\pi B_{0}\int _{0}^{\pi }\sin ^{4}(\theta )\,d\theta =B_{0}\left({\frac {3}{4}}\pi ^{2}\right)\\D&=4\pi \left({\frac {U_{\text{max}}}{P_{\text{rad}}}}\right)=4\pi \left={\frac {16}{3\pi }}\approx 1.698\end{aligned}}} 1830: 827:
Both dBi and dBd are in common use. When an antenna's maximum gain is specified in decibels (for instance, by a manufacturer) one must be certain as to whether this means the gain relative to an isotropic radiator or with respect to a dipole. If it specifies dBi or dBd then there is no ambiguity, but
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headed in a specified direction. In a receiving antenna, the gain describes how well the antenna converts radio waves arriving from a specified direction into electrical power. When no direction is specified, gain is understood to refer to the peak value of the gain, the gain in the direction of the
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However a true isotropic radiator cannot be built, so in practice a different antenna is used. This will often be a half-wave dipole, a very well understood and repeatable antenna that can be easily built for any frequency. The directive gain of a half-wave dipole with respect to the isotropic
3370:{\displaystyle {\begin{aligned}R_{\frac {\lambda }{2}}&=60\operatorname {Cin} (2\pi )=60\left=120\int _{0}^{\frac {\pi }{2}}{\frac {\cos \left({\frac {\pi }{2}}\cos \theta \right)^{2}}{\sin \theta }}d\theta \ ,\\&=15\left\ ,\\&=73.12960\ldots {\mathsf {\;\Omega ;}}\end{aligned}}\ } 2257: 675:
When actual measurements of an antenna's gain are made by a laboratory, the field strength of the test antenna is measured when supplied with, say, 1 watt of transmitter power, at a certain distance. That field strength is compared to the field strength found using a so-called
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Therefore, an antenna with a peak power gain of 5 would be said to have a gain of 7 dBi. dBi is used rather than just dB to emphasize that this is the gain according to the basic definition, in which the antenna is compared to an isotropic radiator.
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Gain or 'absolute gain' is defined as "The ratio of the radiation intensity in a given direction to the radiation intensity that would be produced if the power accepted by the antenna were isotropically radiated". Usually this ratio is expressed in
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differs from gain in that it is "reduced by its impedance mismatch factor." This mismatch induces losses above the dissipative losses described above; therefore, realized gain will always be less than gain. Gain may be expressed as
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is the power supplied to the antenna's terminals. Losses prior to the antenna terminals are accounted for by separate impedance mismatch factors which are therefore not included in the calculation of radiation efficiency.
1063: 226:. Since the directive antenna radiates the same total power within a small angle along the z axis, it can have a higher signal strength in that direction than the isotropic antenna, and so a gain greater than one. 2885: 822: 373: 2135: 3742:(TRP) is the sum of all RF power radiated by the antenna when the source power is included in the measurement. TRP is expressed in watts or the corresponding logarithmic expressions, often dBm or dBW. 666: 2568: 3969: 3397: 2913: 1713: 1330: 2270: 1268: 3906: 549: 2032: 1193: 224: 1314: 835:
imply a comparison of that antenna's gain in each direction to a dipole's gain in that direction. Rather, it is a comparison between the antenna's gain in each direction to the
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The TRP can be used to determine body loss (BoL). The body loss is considered as the ratio of TRP measured in the presence of losses and TRP measured while in free space.
2511: 1094: 2580: 1841: 1121: 468: 898: 2125: 1984: 2092: 2064: 918: 590: 499: 428: 1141: 875: 136: 116: 1825:{\displaystyle {\begin{aligned}G&=\eta D\approx (1)(1.698)=1.698\\G_{\text{dBi}}&\approx 10\,\log _{10}(1.698)\approx 2.30\,{\text{dBi}}\end{aligned}}} 926: 698: 1146:
As a result of this definition, we can conclude that the total gain of an antenna is the sum of partial gains for any two orthogonal polarizations.
1000: 769:= 5 would have a gain with respect to a dipole of 5/1.64 ≈ 3.05, or in decibels one would call this 10 log(3.05) ≈ 4.84 dBd. In general: 828:
if only dB is specified then the fine print must be consulted. Either figure can be easily converted into the other using the above relationship.
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of an antenna is "The ratio of the total power radiated by an antenna to the net power accepted by the antenna from the connected transmitter."
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When testing mobile devices, TRP can be measured while in close proximity of power-absorbing losses such as the body and hand of the user.
294: 2252:{\displaystyle {P \over S}={c_{\circ }\varepsilon _{\circ } \over 2}{E_{\theta }}^{2}={1 \over 2}{{E_{\theta }}^{2} \over Z_{\circ }}\ } 680:
at the same distance receiving the same power in order to determine the gain of the antenna under test. That ratio would be equal to
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gain of the dipole (1.64). In any direction, therefore, such numbers are 2.15 dB smaller than the gain expressed in dBi.
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has been deprecated by IEEE. In a transmitting antenna, the gain describes how well the antenna converts input power into
2340:{\displaystyle Z_{\circ }={\sqrt {{\mu _{\circ } \over \varepsilon _{\circ }}\ }}=376.730313461{\mathsf {\ \Omega \ }}} 3956: 3943: 3879: 3702:
Sometimes, the half-wave dipole is taken as a reference instead of the isotropic radiator. The gain is then given in
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Since the antenna is specified as being lossless the radiation efficiency is 1. The maximum gain is then equal to:
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As an example, consider an antenna that radiates an electromagnetic wave whose electrical field has an amplitude
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The radiated wave can be considered locally as a plane wave. The intensity of an electromagnetic plane wave is:
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Diagram illustrating how isotropic gain is defined. The axes represent power density in watts per square meter.
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The intensity of an isotropic antenna is the power so fed divided by the surface of the sphere of radius
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corresponding to a given polarization, divided by the total radiation intensity of an isotropic antenna.
2465:{\displaystyle \left({P \over S}\right)_{\mathsf {ant}}={1 \over 2Z_{\circ }}{A^{2}I^{2} \over r^{2}}\ } 4006: 1927: 1273:
Let us find the gain of such an antenna. First we find the peak radiation intensity of this antenna:
291:. Since a lossless dipole antenna has a gain of 2.15 dBi, the relation between these units is 380: 168: 141: 2680:{\displaystyle \left({P \over S}\right)_{\mathsf {iso}}={{1 \over 2}R_{s}I^{2} \over 4\pi r^{2}}\ } 46: 2478: 1908:{\displaystyle G_{\text{dBd}}=10\,\log _{10}\left({\frac {1.698}{1.64}}\right)=0.15\,{\text{dBd}}} 283:(dBi). An alternative definition compares the received power to the power received by a lossless 2891: 1072: 3767: 1099: 63: 3772: 851: 444: 883: 3922:
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is the radiation pattern of a directive antenna, which radiates a maximum power density of
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is the radiation pattern of an isotropic antenna which radiates the same total power, and
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When considering an antenna's directional pattern, gain with respect to a dipole does
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represent the radiation intensity in a given direction contained in their respective
559: 555: 264: 3984: 2348: 231: 984:{\displaystyle G_{\theta }=4\pi \left({\frac {U_{\theta }}{P_{\text{in}}}}\right)} 263:. A plot of the gain as a function of direction is called the antenna pattern or 755:{\displaystyle G_{\text{dBd}}\approx 10\log _{10}\left({\frac {G}{1.64}}\right).} 395:, the gain of any antenna when receiving is equal to its gain when transmitting. 239: 94: 376: 284: 138:
watts per square meter at some given distance from the antenna. The green ball
1058:{\displaystyle G_{\phi }=4\pi \left({\frac {U_{\phi }}{P_{\text{in}}}}\right)} 4000: 3842: 3731:
if further clarification is required to differentiate it from realized gain.
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The total radiated power can be found by integrating over all directions:
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IEEE Std 145-2013, IEEE Standard for Definitions of Terms for Antennas
2880:{\displaystyle G={\left \over {\left}}\approx {A^{2} \over 30R_{s}}\ } 817:{\displaystyle G_{\text{dBd}}\approx G_{\text{dBi}}-2.15\,{\text{dB}}} 368:{\displaystyle \mathrm {Gain(dBd)} \approx \mathrm {Gain(dBi)} -2.15} 260: 1835:
Expressed relative to the gain of a half-wave dipole we would find:
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is the power density it radiates. The gain of the first antenna is
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Published numbers for antenna gain are almost always expressed in
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If the resistive part of the series impedance of the antenna is
3874:(Second ed.). Reading, MA: Addison-Wesley. p. 612. 1208:
Suppose a lossless antenna has a radiation pattern given by:
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if the reference antenna were an isotropic radiator (irad).
3951:(3rd edition), by John D. Kraus, Ronald J. Marhefka, 2002, 661:{\displaystyle G_{\text{dBi}}=10\log _{10}\left(G\right).} 267:. It is not to be confused with directivity, which does 2563:{\displaystyle \scriptstyle {1 \over 2}{R_{s}I^{2}}\ .} 2520: 2094:
is a characteristic constant (in Ohm) of each antenna.
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of the antenna's gain for a particular frequency and
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take an antenna's radiation efficiency into account.
171: 144: 124: 104: 554:A transmitting antenna is supplied with power by a 3678: 3369: 2879: 2679: 2562: 2505: 2464: 2339: 2251: 2119: 2086: 2058: 2026: 1978: 1949: 1907: 1824: 1691: 1308: 1262: 1187: 1135: 1115: 1088: 1057: 983: 912: 892: 869: 850:is calculated as power gain, but for a particular 816: 754: 660: 584: 543: 493: 462: 422: 367: 238:is a key performance parameter which combines the 218: 184: 157: 130: 110: 3827:(4th ed.). Hoboken, New Jersey. p. 63. 406:is a unitless measure that combines an antenna's 3998: 2066:is the current (in Amps) fed to the antenna and 2902:(decibels referenced to isotropic radiator): 1263:{\displaystyle U=B_{0}\,\sin ^{3}(\theta ).} 765:For instance, the above antenna with a gain 3938:(3rd edition), by C. Balanis, Wiley, 2005, 379:is proportional to the gain. An antenna's 3855:: CS1 maint: location missing publisher ( 3351: 3818: 3816: 3655: 2332: 2326: 1899: 1861: 1812: 1783: 1486: 1423: 1416: 1234: 808: 544:{\displaystyle \eta ={P_{R} \over P_{O}}} 287:, in which case the units are written as 82:Learn how and when to remove this message 2027:{\displaystyle E_{\theta }={AI \over r}} 692:, this figure for the gain is given by: 375:. For a given frequency, the antenna's 93: 45:This article includes a list of general 3912:from the original on February 16, 2016. 3822: 3734: 1188:{\displaystyle G=G_{\theta }+G_{\phi }} 473: 14: 3999: 3813: 3801: 3799: 3797: 3795: 3793: 3664: 3661: 3658: 3355: 3352: 2611: 2608: 2605: 2392: 2389: 2386: 2329: 3869: 219:{\textstyle {S \over S_{\text{iso}}}} 27:Telecommunications performance metric 3916: 3863: 1309:{\displaystyle U_{\text{max}}=B_{0}} 854:. It is defined as the part of the 31: 3825:Antenna theory: analysis and design 3790: 596: 24: 352: 349: 346: 340: 337: 334: 331: 320: 317: 314: 308: 305: 302: 299: 51:it lacks sufficient corresponding 25: 4028: 1919: 3968: This article incorporates 3963: 3823:Balanis, Constantine A. (2016). 3718: 2513:the power fed to the antenna is 1203: 36: 3981:General Services Administration 3929: 3872:Field and Wave Electromagnetics 2347:is a universal constant called 1950:{\displaystyle \ E_{\theta }\ } 842: 4012:Telecommunications engineering 3888: 3313: 3304: 3287: 3277: 3259: 3249: 3012: 3003: 2985: 2976: 2956: 2947: 1803: 1797: 1750: 1744: 1741: 1735: 1483: 1477: 1413: 1407: 1398: 1386: 1254: 1248: 355: 343: 323: 311: 185:{\displaystyle S_{\text{iso}}} 158:{\displaystyle R_{\text{iso}}} 13: 1: 3783: 3696:are usually the cited values) 564:power accepted by the antenna 3949:Antenna for all applications 2506:{\displaystyle \ {R_{s}}\ ,} 1986:That amplitude is given by: 920:components are expressed as 558:connecting the antenna to a 7: 3751: 1198: 1089:{\displaystyle U_{\theta }} 10: 4033: 2898:equivalency, expressed as 2890:For the commonly utilized 1116:{\displaystyle U_{\phi }} 880:The partial gains in the 3903:Certification Test Plans 3870:Cheng, David K. (1992). 3706:(decibels over dipole): 463:{\displaystyle G=\eta D} 285:half-wave dipole antenna 2690:The directive gain is: 893:{\displaystyle \theta } 398: 383:is proportional to the 66:more precise citations. 3976:Federal Standard 1037C 3970:public domain material 3768:Antenna effective area 3680: 3371: 2881: 2681: 2564: 2507: 2466: 2341: 2253: 2121: 2120:{\displaystyle \ r\ .} 2088: 2060: 2028: 1980: 1979:{\displaystyle \ r\ .} 1951: 1909: 1826: 1693: 1310: 1264: 1189: 1137: 1117: 1090: 1059: 985: 914: 894: 871: 818: 756: 662: 586: 545: 495: 464: 424: 369: 227: 220: 186: 159: 132: 112: 3989: (in support of 3681: 3372: 2882: 2682: 2565: 2508: 2467: 2342: 2254: 2122: 2098:For a large distance 2089: 2087:{\displaystyle \ A\ } 2061: 2059:{\displaystyle \ I\ } 2029: 1981: 1952: 1910: 1827: 1694: 1311: 1265: 1190: 1138: 1118: 1091: 1060: 986: 915: 913:{\displaystyle \phi } 895: 872: 819: 757: 663: 587: 585:{\displaystyle P_{O}} 546: 496: 494:{\displaystyle \eta } 465: 425: 423:{\displaystyle \eta } 370: 221: 187: 160: 133: 113: 97: 3987:on January 22, 2022. 3740:Total radiated power 3735:Total radiated power 3393: 2909: 2697: 2581: 2517: 2479: 2362: 2271: 2136: 2102: 2072: 2044: 1993: 1961: 1928: 1842: 1709: 1326: 1280: 1215: 1153: 1127: 1100: 1073: 1001: 927: 904: 884: 861: 776: 699: 612: 569: 508: 485: 480:radiation efficiency 474:Radiation efficiency 445: 414: 408:radiation efficiency 389:radiation resistance 295: 248:radiation efficiency 196: 169: 142: 122: 102: 3773:Antenna measurement 3542: 3045: 1463: 1382: 1367: 856:radiation intensity 279:with respect to an 4017:Engineering ratios 3905:. CTIA. 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823: 821: 820: 815: 813: 810: 801: 800: 797: 788: 787: 784: 761: 759: 758: 753: 748: 744: 736: 727: 726: 711: 710: 707: 667: 665: 664: 659: 654: 640: 639: 624: 623: 620: 597:Gain in decibels 591: 589: 588: 583: 581: 580: 550: 548: 547: 542: 540: 538: 537: 528: 527: 518: 500: 498: 497: 492: 469: 467: 466: 461: 429: 427: 426: 421: 381:effective length 374: 372: 371: 366: 358: 326: 232:electromagnetics 225: 223: 222: 217: 215: 213: 212: 209: 200: 191: 189: 188: 183: 181: 180: 177: 164: 162: 161: 156: 154: 153: 150: 137: 135: 134: 129: 117: 115: 114: 109: 87: 80: 76: 73: 67: 62:this article by 53:inline citations 40: 39: 32: 21: 4032: 4031: 4027: 4026: 4025: 4023: 4022: 4021: 3997: 3996: 3973: 3964: 3962: 3932: 3927: 3926: 3921: 3917: 3909: 3898: 3894: 3893: 3889: 3882: 3868: 3864: 3848: 3847: 3835: 3821: 3814: 3805: 3804: 3791: 3786: 3754: 3737: 3721: 3673: 3672: 3654: 3653: 3628: 3619: 3618: 3589: 3582: 3558: 3557: 3553: 3552: 3545: 3543: 3532: 3527: 3522: 3520: 3519: 3514: 3498: 3494: 3489: 3472: 3468: 3464: 3459: 3442: 3438: 3434: 3428: 3424: 3422: 3415: 3404: 3400: 3396: 3394: 3391: 3390: 3379:(In most cases 3361: 3360: 3350: 3349: 3334: 3333: 3300: 3290: 3286: 3276: 3274: 3262: 3258: 3234: 3230: 3220: 3211: 3207: 3197: 3188: 3184: 3174: 3165: 3161: 3151: 3142: 3138: 3134: 3130: 3118: 3117: 3092: 3085: 3061: 3060: 3056: 3055: 3048: 3046: 3035: 3030: 2969: 2965: 2931: 2920: 2916: 2912: 2910: 2907: 2906: 2865: 2861: 2857: 2851: 2847: 2845: 2826: 2822: 2815: 2808: 2804: 2798: 2794: 2784: 2783: 2781: 2777: 2776: 2763: 2759: 2752: 2748: 2742: 2738: 2737: 2735: 2726: 2722: 2718: 2713: 2712: 2708: 2706: 2698: 2695: 2694: 2665: 2661: 2654: 2647: 2643: 2637: 2633: 2623: 2622: 2620: 2604: 2603: 2589: 2585: 2584: 2582: 2579: 2578: 2571: 2546: 2542: 2536: 2532: 2531: 2521: 2518: 2515: 2514: 2490: 2486: 2485: 2480: 2477: 2476: 2451: 2447: 2440: 2436: 2430: 2426: 2425: 2423: 2414: 2410: 2406: 2401: 2385: 2384: 2370: 2366: 2365: 2363: 2360: 2359: 2325: 2324: 2305: 2301: 2295: 2291: 2289: 2287: 2278: 2274: 2272: 2269: 2268: 2238: 2234: 2228: 2221: 2217: 2216: 2215: 2213: 2203: 2194: 2187: 2183: 2182: 2181: 2169: 2165: 2159: 2155: 2154: 2152: 2139: 2137: 2134: 2133: 2103: 2100: 2099: 2073: 2070: 2069: 2045: 2042: 2041: 2011: 2009: 2000: 1996: 1994: 1991: 1990: 1962: 1959: 1958: 1938: 1934: 1929: 1926: 1925: 1922: 1900: 1879: 1875: 1866: 1862: 1849: 1845: 1843: 1840: 1839: 1819: 1818: 1813: 1788: 1784: 1773: 1767: 1763: 1760: 1759: 1719: 1712: 1710: 1707: 1706: 1686: 1685: 1669: 1664: 1643: 1639: 1629: 1628: 1624: 1618: 1614: 1613: 1607: 1603: 1601: 1597: 1576: 1572: 1566: 1562: 1560: 1556: 1543: 1537: 1536: 1525: 1521: 1511: 1510: 1506: 1500: 1496: 1468: 1464: 1458: 1453: 1443: 1439: 1377: 1372: 1359: 1354: 1343: 1337: 1333: 1329: 1327: 1324: 1323: 1300: 1296: 1287: 1283: 1281: 1278: 1277: 1239: 1235: 1228: 1224: 1216: 1213: 1212: 1206: 1201: 1179: 1175: 1166: 1162: 1154: 1151: 1150: 1128: 1125: 1124: 1107: 1103: 1101: 1098: 1097: 1080: 1076: 1074: 1071: 1070: 1043: 1039: 1033: 1029: 1027: 1023: 1008: 1004: 1002: 999: 998: 969: 965: 959: 955: 953: 949: 934: 930: 928: 925: 924: 905: 902: 901: 885: 882: 881: 862: 859: 858: 845: 809: 796: 792: 783: 779: 777: 774: 773: 735: 731: 722: 718: 706: 702: 700: 697: 696: 644: 635: 631: 619: 615: 613: 610: 609: 599: 576: 572: 570: 567: 566: 533: 529: 523: 519: 517: 509: 506: 505: 486: 483: 482: 476: 446: 443: 442: 415: 412: 411: 401: 330: 298: 296: 293: 292: 234:, an antenna's 208: 204: 199: 197: 194: 193: 176: 172: 170: 167: 166: 149: 145: 143: 140: 139: 123: 120: 119: 103: 100: 99: 88: 77: 71: 68: 58:Please help to 57: 41: 37: 28: 23: 22: 15: 12: 11: 5: 4030: 4020: 4019: 4014: 4009: 3960: 3959: 3946: 3936:Antenna Theory 3931: 3928: 3925: 3924: 3915: 3887: 3880: 3862: 3833: 3812: 3788: 3787: 3785: 3782: 3781: 3780: 3775: 3770: 3765: 3760: 3753: 3750: 3736: 3733: 3720: 3717: 3716: 3715: 3714: 3713: 3700: 3699: 3698: 3697: 3671: 3666: 3663: 3660: 3649: 3646: 3643: 3640: 3635: 3632: 3627: 3624: 3622: 3620: 3617: 3607: 3604: 3598: 3595: 3592: 3585: 3580: 3576: 3573: 3570: 3565: 3562: 3556: 3551: 3548: 3539: 3536: 3530: 3526: 3518: 3513: 3505: 3502: 3497: 3493: 3488: 3479: 3476: 3471: 3467: 3463: 3458: 3449: 3446: 3441: 3437: 3431: 3427: 3421: 3418: 3416: 3411: 3408: 3403: 3399: 3398: 3387: 3386: 3385: 3384: 3383:, is adequate) 3357: 3354: 3348: 3345: 3342: 3339: 3337: 3335: 3332: 3325: 3318: 3315: 3312: 3309: 3306: 3303: 3296: 3293: 3289: 3285: 3282: 3279: 3271: 3268: 3265: 3261: 3257: 3254: 3251: 3248: 3245: 3242: 3237: 3233: 3227: 3224: 3219: 3214: 3210: 3204: 3201: 3196: 3191: 3187: 3181: 3178: 3173: 3168: 3164: 3158: 3155: 3150: 3145: 3141: 3137: 3133: 3129: 3126: 3123: 3121: 3119: 3116: 3110: 3107: 3101: 3098: 3095: 3088: 3083: 3079: 3076: 3073: 3068: 3065: 3059: 3054: 3051: 3042: 3039: 3033: 3029: 3025: 3022: 3018: 3014: 3011: 3008: 3005: 3002: 2999: 2996: 2993: 2990: 2987: 2984: 2981: 2978: 2975: 2972: 2968: 2964: 2961: 2958: 2955: 2952: 2949: 2946: 2943: 2940: 2937: 2934: 2932: 2927: 2924: 2919: 2915: 2914: 2888: 2887: 2868: 2864: 2860: 2854: 2850: 2844: 2837: 2829: 2825: 2821: 2818: 2811: 2807: 2801: 2797: 2791: 2788: 2780: 2774: 2766: 2762: 2755: 2751: 2745: 2741: 2729: 2725: 2721: 2717: 2711: 2705: 2702: 2688: 2687: 2668: 2664: 2660: 2657: 2650: 2646: 2640: 2636: 2630: 2627: 2619: 2613: 2610: 2607: 2601: 2596: 2593: 2588: 2558: 2549: 2545: 2539: 2535: 2528: 2525: 2502: 2493: 2489: 2473: 2472: 2454: 2450: 2443: 2439: 2433: 2429: 2417: 2413: 2409: 2405: 2400: 2394: 2391: 2388: 2382: 2377: 2374: 2369: 2353: 2352: 2331: 2323: 2320: 2308: 2304: 2298: 2294: 2286: 2281: 2277: 2262: 2261: 2260: 2259: 2241: 2237: 2231: 2224: 2220: 2210: 2207: 2202: 2197: 2190: 2186: 2178: 2172: 2168: 2162: 2158: 2151: 2146: 2143: 2116: 2110: 2096: 2095: 2080: 2067: 2052: 2035: 2034: 2021: 2017: 2014: 2008: 2003: 1999: 1975: 1969: 1957:at a distance 1941: 1937: 1921: 1920:Second example 1918: 1917: 1916: 1898: 1895: 1891: 1886: 1883: 1878: 1874: 1869: 1865: 1860: 1857: 1848: 1833: 1832: 1811: 1808: 1805: 1802: 1799: 1796: 1791: 1787: 1782: 1779: 1776: 1774: 1766: 1762: 1761: 1758: 1755: 1752: 1749: 1746: 1743: 1740: 1737: 1734: 1731: 1728: 1725: 1722: 1720: 1718: 1715: 1714: 1700: 1699: 1684: 1681: 1675: 1672: 1668: 1663: 1659: 1652: 1646: 1642: 1636: 1633: 1627: 1621: 1617: 1610: 1606: 1600: 1596: 1593: 1590: 1586: 1575: 1565: 1559: 1555: 1552: 1549: 1546: 1544: 1542: 1539: 1538: 1534: 1528: 1524: 1518: 1515: 1509: 1503: 1499: 1495: 1492: 1489: 1485: 1482: 1479: 1476: 1471: 1467: 1461: 1456: 1452: 1446: 1442: 1438: 1435: 1432: 1429: 1426: 1422: 1419: 1415: 1412: 1409: 1406: 1403: 1400: 1397: 1394: 1391: 1388: 1385: 1380: 1375: 1371: 1365: 1362: 1357: 1353: 1349: 1346: 1344: 1336: 1332: 1331: 1317: 1316: 1303: 1299: 1295: 1286: 1271: 1270: 1259: 1256: 1253: 1250: 1247: 1242: 1238: 1231: 1227: 1223: 1220: 1205: 1202: 1200: 1197: 1196: 1195: 1182: 1178: 1174: 1169: 1165: 1161: 1158: 1132: 1110: 1106: 1083: 1079: 1067: 1066: 1053: 1042: 1036: 1032: 1026: 1022: 1019: 1016: 1011: 1007: 992: 991: 979: 968: 962: 958: 952: 948: 945: 942: 937: 933: 909: 889: 866: 844: 841: 825: 824: 807: 804: 795: 791: 782: 763: 762: 751: 747: 742: 739: 734: 730: 725: 721: 717: 714: 705: 669: 668: 657: 653: 650: 647: 643: 638: 634: 630: 627: 618: 598: 595: 579: 575: 552: 551: 536: 532: 526: 522: 516: 513: 490: 475: 472: 471: 470: 459: 456: 453: 450: 419: 400: 397: 377:effective area 364: 361: 357: 354: 351: 348: 345: 342: 339: 336: 333: 329: 325: 322: 319: 316: 313: 310: 307: 304: 301: 207: 203: 175: 148: 127: 107: 90: 89: 72:September 2009 44: 42: 35: 26: 9: 6: 4: 3: 2: 4029: 4018: 4015: 4013: 4010: 4008: 4005: 4004: 4002: 3995: 3992: 3986: 3982: 3978: 3977: 3971: 3958: 3957:0-07-232103-2 3954: 3950: 3947: 3945: 3944:0-471-66782-X 3941: 3937: 3934: 3933: 3919: 3908: 3904: 3897: 3891: 3883: 3881:0-201-12819-5 3877: 3873: 3866: 3858: 3852: 3844: 3840: 3836: 3830: 3826: 3819: 3817: 3808: 3802: 3800: 3798: 3796: 3794: 3789: 3779: 3776: 3774: 3771: 3769: 3766: 3764: 3761: 3759: 3756: 3755: 3749: 3746: 3743: 3741: 3732: 3730: 3729:absolute gain 3725: 3724:Realized gain 3719:Realized gain 3711: 3710: 3709: 3708: 3707: 3705: 3695: 3691: 3687: 3686: 3669: 3647: 3644: 3641: 3638: 3633: 3630: 3625: 3623: 3615: 3605: 3602: 3596: 3593: 3590: 3583: 3578: 3574: 3571: 3568: 3563: 3560: 3554: 3549: 3546: 3537: 3534: 3528: 3524: 3516: 3511: 3503: 3500: 3495: 3491: 3486: 3477: 3474: 3469: 3465: 3461: 3456: 3447: 3444: 3439: 3435: 3429: 3425: 3419: 3417: 3409: 3406: 3401: 3389: 3388: 3382: 3378: 3377: 3346: 3343: 3340: 3338: 3330: 3323: 3316: 3310: 3307: 3301: 3294: 3291: 3283: 3280: 3269: 3266: 3263: 3255: 3252: 3246: 3243: 3240: 3235: 3231: 3225: 3222: 3217: 3212: 3208: 3202: 3199: 3194: 3189: 3185: 3179: 3176: 3171: 3166: 3162: 3156: 3153: 3148: 3143: 3139: 3135: 3131: 3127: 3124: 3122: 3114: 3108: 3105: 3099: 3096: 3093: 3086: 3081: 3077: 3074: 3071: 3066: 3063: 3057: 3052: 3049: 3040: 3037: 3031: 3027: 3023: 3020: 3016: 3009: 3006: 3000: 2997: 2994: 2991: 2988: 2982: 2979: 2973: 2970: 2966: 2962: 2959: 2953: 2950: 2944: 2941: 2938: 2935: 2933: 2925: 2922: 2917: 2905: 2904: 2903: 2901: 2897: 2893: 2866: 2862: 2858: 2852: 2848: 2842: 2835: 2827: 2823: 2819: 2816: 2809: 2805: 2799: 2795: 2789: 2786: 2778: 2772: 2764: 2760: 2753: 2749: 2743: 2739: 2727: 2723: 2719: 2715: 2709: 2703: 2700: 2693: 2692: 2691: 2666: 2662: 2658: 2655: 2648: 2644: 2638: 2634: 2628: 2625: 2617: 2599: 2594: 2591: 2586: 2577: 2576: 2575: 2556: 2547: 2543: 2537: 2533: 2526: 2523: 2500: 2491: 2487: 2452: 2448: 2441: 2437: 2431: 2427: 2415: 2411: 2407: 2403: 2398: 2380: 2375: 2372: 2367: 2358: 2357: 2356: 2350: 2322:376.730313461 2321: 2318: 2306: 2302: 2296: 2292: 2284: 2279: 2275: 2267: 2266: 2265: 2239: 2235: 2229: 2222: 2218: 2208: 2205: 2200: 2195: 2188: 2184: 2176: 2170: 2166: 2160: 2156: 2149: 2144: 2141: 2132: 2131: 2130: 2129: 2128: 2114: 2108: 2078: 2068: 2050: 2040: 2039: 2038: 2019: 2015: 2012: 2006: 2001: 1997: 1989: 1988: 1987: 1973: 1967: 1939: 1935: 1896: 1893: 1889: 1884: 1881: 1876: 1872: 1867: 1863: 1858: 1855: 1846: 1838: 1837: 1836: 1809: 1806: 1800: 1794: 1789: 1785: 1780: 1777: 1775: 1764: 1756: 1753: 1747: 1738: 1732: 1729: 1726: 1723: 1721: 1716: 1705: 1704: 1703: 1682: 1679: 1673: 1670: 1666: 1661: 1657: 1650: 1644: 1640: 1634: 1631: 1625: 1619: 1615: 1608: 1604: 1598: 1594: 1591: 1588: 1584: 1573: 1563: 1557: 1553: 1550: 1547: 1545: 1540: 1532: 1526: 1522: 1516: 1513: 1507: 1501: 1497: 1493: 1490: 1487: 1480: 1474: 1469: 1465: 1459: 1454: 1450: 1444: 1440: 1436: 1433: 1430: 1427: 1424: 1420: 1417: 1410: 1404: 1401: 1395: 1392: 1389: 1383: 1378: 1373: 1369: 1363: 1360: 1355: 1351: 1347: 1345: 1334: 1322: 1321: 1320: 1301: 1297: 1293: 1284: 1276: 1275: 1274: 1257: 1251: 1245: 1240: 1236: 1229: 1225: 1221: 1218: 1211: 1210: 1209: 1204:First example 1180: 1176: 1172: 1167: 1163: 1159: 1156: 1149: 1148: 1147: 1144: 1130: 1108: 1104: 1081: 1077: 1051: 1040: 1034: 1030: 1024: 1020: 1017: 1014: 1009: 1005: 997: 996: 995: 977: 966: 960: 956: 950: 946: 943: 940: 935: 931: 923: 922: 921: 907: 887: 878: 864: 857: 853: 849: 840: 838: 834: 829: 805: 802: 793: 789: 780: 772: 771: 770: 768: 749: 745: 740: 737: 732: 728: 723: 719: 715: 712: 703: 695: 694: 693: 691: 685: 683: 679: 673: 655: 651: 648: 645: 641: 636: 632: 628: 625: 616: 608: 607: 606: 604: 594: 577: 573: 565: 561: 557: 534: 530: 524: 520: 514: 511: 504: 503: 502: 488: 481: 457: 454: 451: 448: 441: 440: 439: 437: 434: 430: 417: 409: 405: 396: 394: 390: 386: 382: 378: 362: 359: 327: 290: 286: 282: 278: 272: 270: 266: 262: 257: 253: 249: 245: 241: 237: 233: 205: 201: 173: 146: 125: 105: 96: 86: 83: 75: 65: 61: 55: 54: 48: 43: 34: 33: 30: 19: 3985:the original 3975: 3961: 3948: 3935: 3930:Bibliography 3918: 3902: 3890: 3871: 3865: 3824: 3806: 3747: 3744: 3739: 3738: 3728: 3723: 3722: 3703: 3701: 3693: 3689: 3380: 2899: 2889: 2689: 2474: 2354: 2263: 2097: 2036: 1923: 1834: 1701: 1318: 1272: 1207: 1145: 1068: 993: 879: 852:polarization 848:Partial gain 847: 846: 843:Partial gain 836: 832: 830: 826: 766: 764: 689: 686: 681: 677: 674: 670: 600: 563: 553: 477: 435: 410: 403: 402: 384: 288: 273: 268: 251: 250:. The term 235: 229: 78: 69: 50: 29: 18:Antenna gain 3991:MIL-STD-188 3688:(Likewise, 433:directivity 393:reciprocity 385:square root 256:radio waves 244:directivity 64:introducing 4001:Categories 3784:References 259:antenna's 252:power gain 47:references 3851:cite book 3843:933291646 3645:≈ 3642:1.6409224 3639:≈ 3626:≈ 3606:θ 3597:θ 3594:⁡ 3575:θ 3572:⁡ 3561:π 3550:⁡ 3535:π 3525:∫ 3501:λ 3475:λ 3445:λ 3407:λ 3353:Ω 3347:… 3284:π 3253:− 3244:… 3232:π 3209:π 3195:− 3186:π 3163:π 3149:− 3140:π 3109:θ 3100:θ 3097:⁡ 3078:θ 3075:⁡ 3064:π 3053:⁡ 3038:π 3028:∫ 3010:π 3001:⁡ 2995:− 2992:γ 2983:π 2974:⁡ 2954:π 2945:⁡ 2923:λ 2843:≈ 2820:π 2728:∘ 2659:π 2416:∘ 2330:Ω 2307:∘ 2303:ε 2297:∘ 2293:μ 2280:∘ 2240:∘ 2223:θ 2189:θ 2171:∘ 2167:ε 2161:∘ 2002:θ 1940:θ 1873:⁡ 1807:≈ 1795:⁡ 1778:≈ 1733:≈ 1727:η 1680:≈ 1674:π 1641:π 1595:π 1554:π 1523:π 1491:θ 1481:θ 1475:⁡ 1460:π 1451:∫ 1437:π 1428:ϕ 1421:θ 1411:θ 1405:⁡ 1396:ϕ 1390:θ 1379:π 1370:∫ 1364:π 1352:∫ 1252:θ 1246:⁡ 1181:ϕ 1168:θ 1109:ϕ 1082:θ 1035:ϕ 1021:π 1010:ϕ 961:θ 947:π 936:θ 908:ϕ 888:θ 803:− 790:≈ 729:⁡ 713:≈ 642:⁡ 512:η 489:η 455:η 418:η 391:. Due to 360:− 328:≈ 261:main lobe 3907:Archived 3778:Cardioid 3752:See also 3694:2.15 dBi 3344:73.12960 1199:Examples 603:decibels 562:. The 277:decibels 3809:. IEEE. 3758:Antenna 3648:2.15088 3634:73.1296 2896:decibel 2264:where 2037:where: 240:antenna 60:improve 3955:  3942:  3878:  3841:  3831:  3656:  3651:  3613:  3381:73.130 3365:  3328:  3112:  2875:  2675:  2554:  2498:  2483:  2460:  2333:  2327:  2314:  2247:  2112:  2106:  2082:  2076:  2054:  2048:  1971:  1965:  1945:  1932:  1069:where 49:, but 3972:from 3910:(PDF) 3899:(PDF) 3226:70875 1882:1.698 1801:1.698 1757:1.698 1748:1.698 1683:1.698 3953:ISBN 3940:ISBN 3876:ISBN 3857:link 3839:OCLC 3829:ISBN 3692:and 3690:1.64 3462:3600 2355:and 1897:0.15 1885:1.64 1810:2.30 1096:and 994:and 900:and 837:peak 806:2.15 741:1.64 478:The 431:and 404:Gain 399:Gain 363:2.15 246:and 236:gain 3704:dBd 3631:120 3591:sin 3569:cos 3547:cos 3492:120 3203:630 3180:135 3094:sin 3072:cos 3050:cos 3024:120 2942:Cin 2900:dBi 1902:dBd 1864:log 1851:dBd 1815:dBi 1786:log 1769:dBi 1578:rad 1568:max 1466:sin 1402:sin 1339:rad 1289:max 1237:sin 833:not 798:dBi 785:dBd 720:log 708:dBd 633:log 621:dBi 289:dBd 269:not 242:'s 230:In 210:iso 178:iso 151:iso 4003:: 3993:). 3979:. 3901:. 3853:}} 3849:{{ 3837:. 3815:^ 3792:^ 3466:30 3436:30 3426:60 3236:10 3128:15 2998:Ci 2971:ln 2963:60 2939:60 2859:30 2574:: 1868:10 1859:10 1790:10 1781:10 1667:16 1045:in 971:in 811:dB 724:10 716:10 637:10 629:10 438:: 3884:. 3859:) 3845:. 3670:; 3665:i 3662:B 3659:d 3616:, 3603:d 3584:2 3579:) 3564:2 3555:( 3538:2 3529:0 3517:1 3512:= 3504:2 3496:R 3487:= 3478:2 3470:R 3457:= 3448:2 3440:R 3430:2 3420:= 3410:2 3402:G 3356:; 3341:= 3331:, 3324:] 3317:! 3314:) 3311:n 3308:2 3305:( 3302:n 3295:n 3292:2 3288:) 3281:2 3278:( 3270:1 3267:+ 3264:n 3260:) 3256:1 3250:( 3247:+ 3241:+ 3223:4 3218:+ 3213:8 3200:1 3190:6 3177:4 3172:+ 3167:4 3157:3 3154:1 3144:2 3136:2 3132:[ 3125:= 3115:, 3106:d 3087:2 3082:) 3067:2 3058:( 3041:2 3032:0 3021:= 3017:] 3013:) 3007:2 3004:( 2989:+ 2986:) 2980:2 2977:( 2967:[ 2960:= 2957:) 2951:2 2948:( 2936:= 2926:2 2918:R 2867:s 2863:R 2853:2 2849:A 2836:] 2828:2 2824:r 2817:4 2810:2 2806:I 2800:s 2796:R 2790:2 2787:1 2779:[ 2773:] 2765:2 2761:r 2754:2 2750:I 2744:2 2740:A 2724:Z 2720:2 2716:1 2710:[ 2704:= 2701:G 2667:2 2663:r 2656:4 2649:2 2645:I 2639:s 2635:R 2629:2 2626:1 2618:= 2612:o 2609:s 2606:i 2600:) 2595:S 2592:P 2587:( 2572:r 2557:. 2548:2 2544:I 2538:s 2534:R 2527:2 2524:1 2501:, 2492:s 2488:R 2453:2 2449:r 2442:2 2438:I 2432:2 2428:A 2412:Z 2408:2 2404:1 2399:= 2393:t 2390:n 2387:a 2381:) 2376:S 2373:P 2368:( 2351:. 2319:= 2285:= 2276:Z 2236:Z 2230:2 2219:E 2209:2 2206:1 2201:= 2196:2 2185:E 2177:2 2157:c 2150:= 2145:S 2142:P 2115:. 2109:r 2079:A 2051:I 2020:r 2016:I 2013:A 2007:= 1998:E 1974:. 1968:r 1936:E 1915:. 1894:= 1890:) 1877:( 1856:= 1847:G 1804:) 1798:( 1765:G 1754:= 1751:) 1745:( 1742:) 1739:1 1736:( 1730:D 1724:= 1717:G 1671:3 1662:= 1658:] 1651:) 1645:2 1635:4 1632:3 1626:( 1620:0 1616:B 1609:0 1605:B 1599:[ 1592:4 1589:= 1585:) 1574:P 1564:U 1558:( 1551:4 1548:= 1541:D 1533:) 1527:2 1517:4 1514:3 1508:( 1502:0 1498:B 1494:= 1488:d 1484:) 1478:( 1470:4 1455:0 1445:0 1441:B 1434:2 1431:= 1425:d 1418:d 1414:) 1408:( 1399:) 1393:, 1387:( 1384:U 1374:0 1361:2 1356:0 1348:= 1335:P 1302:0 1298:B 1294:= 1285:U 1258:. 1255:) 1249:( 1241:3 1230:0 1226:B 1222:= 1219:U 1177:G 1173:+ 1164:G 1160:= 1157:G 1131:E 1105:U 1078:U 1065:, 1052:) 1041:P 1031:U 1025:( 1018:4 1015:= 1006:G 978:) 967:P 957:U 951:( 944:4 941:= 932:G 865:U 794:G 781:G 767:G 750:. 746:) 738:G 733:( 704:G 690:G 682:G 656:. 652:) 649:G 646:( 626:= 617:G 578:O 574:P 535:O 531:P 525:R 521:P 515:= 458:D 452:= 449:G 436:D 356:) 353:i 350:B 347:d 344:( 341:n 338:i 335:a 332:G 324:) 321:d 318:B 315:d 312:( 309:n 306:i 303:a 300:G 206:S 202:S 174:S 147:R 126:S 106:R 85:) 79:( 74:) 70:( 56:. 20:)

Index

Antenna gain
references
inline citations
improve
introducing
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electromagnetics
antenna
directivity
radiation efficiency
radio waves
main lobe
radiation pattern
decibels
isotropic radiator
half-wave dipole antenna
effective area
effective length
radiation resistance
reciprocity
radiation efficiency
directivity
radiation efficiency
transmission line
radio transmitter
decibels
polarization
radiation intensity
vacuum impedance

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