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Gyrotheodolite

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thereby bring a zero mark on the attachment into coincidence with the gyroscope spin axis. By tracking the spin axis as it oscillates about the meridian, a record of the azimuth of a series of the extreme stationary points of that oscillation may be determined by reading the theodolite azimuth circle. A midpoint can later be computed from these records that represents a refined estimate of the meridian. Careful setup and repeated observations can give an estimate that is within about 10 arc seconds of the true meridian. This estimate of the meridian contains errors due to the zero torque of the suspension not being aligned precisely with the true meridian and to measurement errors of the slightly damped extremes of oscillation. These errors can be moderated by refining the initial estimate of the meridian to within a few arc minutes and correctly aligning the zero torque of the suspension.
20: 127:. For example, where a conduit must pass under a river, a vertical shaft on each side of the river might be connected by a horizontal tunnel. A gyro-theodolite can be operated at the surface and then again at the foot of the shafts to identify the directions needed to tunnel between the base of the two shafts. During the construction of the 97:
to reduce magnetic influence, connected by a spindle to the vertical axis of the theodolite. The battery-powered gyro wheel is rotated at 20,000 rpm or more, until it acts as a north-seeking gyroscope. A separate optical system within the attachment permits the operator to rotate the theodolite and
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of the spinner axis about the meridian repeats with a period of a few minutes. In practice the amplitude of oscillation will only gradually reduce as energy is lost due to the minimal damping present. Gyro-theodolites employ an undamped oscillating system because a determination can be obtained in
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When the spinner is released from restraint with its axis of rotation aligned close to the meridian, the gyroscopic reaction of spin and Earth's rotation results in precession of the spin axis in the direction of alignment with the plane of the meridian. This is because the daily rotation of the
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When not in operation, the gyroscope assembly is anchored within the instrument. The electrically powered gyroscope is started while restrained and then released for operation. During operation the gyroscope is supported within the instrument assembly, typically on a thin vertical tape that
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When available, astronomical star sights are able to give the meridian bearing to better than one hundred times the accuracy of the gyro-theodolite. Where this extra precision is not required, the gyro-theodolite is able to produce a result quickly without the need for night observations.
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Earth is in effect continuously tilting the east–west axis of the station. The spinner axis then accelerates towards and overshoots the meridian, it then slows to a halt at an extreme point before similarly swinging back towards the initial point of release. This oscillation in
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constrains the gyroscope spinner axis to remain horizontal. The alignment of the spin axis is permitted to rotate in azimuth by only the small amount required during operation. An initial approximate estimate of the meridian is needed. This might be determined with a magnetic
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in 1921 to build the first surveying gyro. In 1949, the gyro-theodolite – at that time called a "meridian pointer" or "meridian indicator" – was first used by the Clausthal Mining Academy underground. Several years later it was improved with the addition of
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to the horizontal axis of the spinner and the meridian is undefined. Gyro-theodolites are not normally used within about 15 degrees of the pole where the angle between the earth's rotation and the direction of gravity is too small for it to work reliably.
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telescopes. In 1960, the Fennel Kassel company produced the first of the KT1 series of gyro-theodolites. Fennel Kassel and others later produced gyro attachments that can be mounted on normal theodolites.
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less than about 20 minutes, while the asymptotic settling of a damped gyro-compass would take many times that before any reasonable determination of meridian could possibly be made.
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N. Korittke; H. Klapperich (1998), "Application of high precision gyro-theodolites in tunneling", in Arsenio Negro; Argimiro A. Ferreira (eds.),
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Tunnels and metropolises: proceedings of the World Tunnel Congress'98 on tunnels and metropolises : Sao Paulo, Brazil, 25-30 april 1998
55:. It is the main instrument for orientation in mine surveying and in tunnel engineering, where astronomical star sights are not visible and 346: 398: 372: 320: 294: 265: 239: 419: 72: 167:, a gyro-theodolite cannot be relocated while it is operating. It must be restarted again at each site. 164: 115:, from an existing survey network or by the use of the gyro-theodolite in an extended tracking mode. 362: 336: 310: 284: 229: 388: 255: 8: 429: 208: 394: 368: 342: 316: 290: 261: 235: 212: 424: 200: 147:
and in both the northern and southern hemispheres, it cannot be used at either the
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Gyro-theodolites are primarily used in the absence of astronomical star sights and
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Wang Hong-lan (September 1987), "Analysis of the motion of a gyro-theodolite",
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from France to the UK, gyro-theodolites were used to align the tunnels.
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Introduction to geodesy: the history and concepts of modern geodesy
94: 144: 112: 103: 334: 282: 124: 56: 360: 411: 27:GAK gyroscope mounted on a Wild T-16 theodolite. 234:, Stanford University Press, pp. 169–170, 93:A gyroscope is mounted in a sphere, lined with 190: 51:. It is used to determine the orientation of 143:Although a gyro-theodolite functions at the 75:points north. This principle was adapted by 341:, Butterworth-Heinemann, pp. 519–533, 367:, Taylor & Francis, pp. 823–827, 186: 184: 393:, Taylor & Francis, pp. 55–56, 386: 278: 276: 253: 223: 221: 18: 335:Wilfred Schofield, Mark Breach (2007), 289:, Walter de Gruyter, pp. 112–116, 283:Heribert Kahmen, Wolfgang Faig (1988), 181: 412: 227: 155:, where the Earth's axis is precisely 308: 273: 218: 13: 14: 441: 260:, Walter de Gruyter, p. 18, 193:Applied Mathematics and Mechanics 43:) is an instrument composed of a 163:Unlike an artificial horizon or 71:discovered that a gyro with two 228:Staley, William Wesley (1964), 390:Engineering the Channel Tunnel 380: 354: 328: 302: 247: 231:Introduction to mine surveying 138: 67:In 1852, the French physicist 1: 309:Smith, James Raymond (1997), 174: 88: 7: 387:Kirkland, Colin J. (1995), 315:, Wiley-IEEE, p. 174, 10: 446: 165:inertial navigation system 62: 254:Deumlich, Fritz (1982), 131:, which runs under the 118: 28: 420:Surveying instruments 338:Engineering surveying 257:Surveying instruments 22: 16:Surveying instrument 205:10.1007/BF02019527 73:degrees of freedom 29: 348:978-0-7506-6949-8 437: 404: 403: 384: 378: 377: 358: 352: 351: 332: 326: 325: 306: 300: 299: 280: 271: 270: 251: 245: 244: 225: 216: 215: 188: 445: 444: 440: 439: 438: 436: 435: 434: 410: 409: 408: 407: 401: 385: 381: 375: 359: 355: 349: 333: 329: 323: 307: 303: 297: 281: 274: 268: 252: 248: 242: 226: 219: 189: 182: 177: 141: 133:English Channel 121: 91: 82:autocollimation 65: 59:does not work. 17: 12: 11: 5: 443: 433: 432: 427: 422: 406: 405: 399: 379: 373: 353: 347: 327: 321: 301: 295: 272: 266: 246: 240: 217: 199:(9): 889–900, 179: 178: 176: 173: 140: 137: 129:Channel Tunnel 120: 117: 90: 87: 64: 61: 41:surveying gyro 37:gyrotheodolite 15: 9: 6: 4: 3: 2: 442: 431: 428: 426: 423: 421: 418: 417: 415: 402: 400:0-419-17920-8 396: 392: 391: 383: 376: 374:90-5410-936-X 370: 366: 365: 357: 350: 344: 340: 339: 331: 324: 322:0-471-16660-X 318: 314: 313: 305: 298: 296:3-11-008303-5 292: 288: 287: 279: 277: 269: 267:3-11-007765-5 263: 259: 258: 250: 243: 241:0-8047-0361-2 237: 233: 232: 224: 222: 214: 210: 206: 202: 198: 194: 187: 185: 180: 172: 168: 166: 161: 158: 157:perpendicular 154: 150: 146: 136: 134: 130: 126: 116: 114: 108: 105: 99: 96: 86: 83: 78: 74: 70: 69:Léon Foucault 60: 58: 54: 50: 47:mounted to a 46: 42: 38: 34: 26: 21: 389: 382: 363: 356: 337: 330: 311: 304: 285: 256: 249: 230: 196: 192: 169: 162: 142: 122: 109: 100: 92: 66: 40: 36: 30: 139:Limitations 77:Max Schuler 45:gyrocompass 430:Gyroscopes 414:Categories 175:References 153:South Pole 149:North Pole 53:true north 49:theodolite 286:Surveying 213:121190508 89:Operation 33:surveying 95:Mu-metal 425:Geodesy 145:equator 113:compass 104:azimuth 63:History 39:(also: 397:  371:  345:  319:  293:  264:  238:  211:  209:S2CID 395:ISBN 369:ISBN 343:ISBN 317:ISBN 291:ISBN 262:ISBN 236:ISBN 119:Uses 35:, a 25:Wild 201:doi 151:or 125:GPS 57:GPS 31:In 416:: 275:^ 220:^ 207:, 195:, 183:^ 23:A 203:: 197:8

Index


Wild
surveying
gyrocompass
theodolite
true north
GPS
Léon Foucault
degrees of freedom
Max Schuler
autocollimation
Mu-metal
azimuth
compass
GPS
Channel Tunnel
English Channel
equator
North Pole
South Pole
perpendicular
inertial navigation system


doi
10.1007/BF02019527
S2CID
121190508

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