3.1 Airguns for Non-Experts The airgun has long been the most popular marine seismic source.
Double, double, toil and trouble; airguns fire and ocean bubble. With apologies to Shakespeare’s three witches in Macbeth,
and thanks to our colleagues Bill Dragoset and Jan Langhammer.
A seismic source is defined as any device which releases energy into the earth in the form of seismic waves. Te major source type in marine exploration is the airgun array, which since the 1970s has been by far the most popular. Te airgun can be described as a chamber of compressed air that is released rapidly into the surrounding water to create an acoustic pulse. Te airgun is the most commonly used source because the pulses are predictable, repeatable and controllable, it uses compressed air which is cheap and readily available, and it has only a minor impact on marine life.
3.1.1 Size and Geometry
An airgun volume is measured in litres (l) or more commonly, by the conservative petroleum geophysicist, in cubic inches (in3
Typical volumes of individual airguns used by the exploration industry vary from 20 in3
(0.3 litres) to 800 in3 ). (13.1 litres), while
academic seismic refraction studies can use volumes up to 1,600 in3
(26.2 litres). An airgun array consists of 3–6 subarrays called
strings, each string containing 6–8 individual guns, so that the array usually involves between 18 and 48 guns, although in special cases as many as 100 guns an array can be used. Te airgun array volume is the sum of the volumes of each gun, and is typically in the range 3,000–8,000 in3
(49.2–131.6 litres). Te airguns hang in the sea beneath floats between 3m and
10m below the sea surface, generally at about 6m, except in refraction studies when a deeper deployment is needed. Te gun pressure most commonly used by the seismic industry is 2,000 psi (138 bar). During a survey the guns fire every 10–15 seconds. It is common to arrange several (2–4) airguns in a cluster,
with the guns so close together that they behave as a larger single gun. Te main purpose of clustering is to improve signal characteristics, since the bubble motion (see Section 3.1.2.1) is reduced by this configuration. Te energy sent out by airgun arrays is predominantly
directed vertically downwards. Te broad band of frequencies from the array form a pulse with peak-to-peak amplitude in the range 14–28 bar-m, corresponding to 243–249 dB re 1 μPa-m vertically downward. Te amplitude levels emitted horizontally tend to be 15–24 dB lower. Tese numbers are frequency dependent. By filtering out high frequencies there is less deviation between amplitude levels vertically and horizontally. Here, ‘dB re 1 μPa-m’ means decibel value peak-to-
peak relative to the reference pressure one micropascal at a reference distance of one metre. Confusing units? Read the box on definitions and for a guide of the physical principles of airguns and the basic sound measurement units. Our focus for the moment is on the vertically downward travelling ‘far- field’ signature of an airgun array as this signature provides a quantitative measure of the array’s performance.
94
Figure 3.1: Deployment of airgun subarray (or string). 3.1.2 Bubble Oscillations
When compressed air is suddenly released into the water an oscillating bubble forms. Tis process is described in Parkes and Hatton (1986): “Initially, the pressure inside the bubble greatly exceeds the
hydrostatic (external) pressure. Te air bubble then expands well beyond the point at which the internal and hydrostatic pressures are equal. When the expansion ceases, the internal bubble pressure is below the hydrostatic pressure, so that the bubble starts to collapse. Te collapse overshoots the equilibrium position and the cycle starts once again. Te bubble continues to oscillate, with a period typically in the range of tens to hundreds of milliseconds.” Te oscillation is stopped due to frictional forces, and the buoyancy of the bubble causes it to break the sea surface. If
PGS
Page 1 |
Page 2 |
Page 3 |
Page 4 |
Page 5 |
Page 6 |
Page 7 |
Page 8 |
Page 9 |
Page 10 |
Page 11 |
Page 12 |
Page 13 |
Page 14 |
Page 15 |
Page 16 |
Page 17 |
Page 18 |
Page 19 |
Page 20 |
Page 21 |
Page 22 |
Page 23 |
Page 24 |
Page 25 |
Page 26 |
Page 27 |
Page 28 |
Page 29 |
Page 30 |
Page 31 |
Page 32 |
Page 33 |
Page 34 |
Page 35 |
Page 36 |
Page 37 |
Page 38 |
Page 39 |
Page 40 |
Page 41 |
Page 42 |
Page 43 |
Page 44 |
Page 45 |
Page 46 |
Page 47 |
Page 48 |
Page 49 |
Page 50 |
Page 51 |
Page 52 |
Page 53 |
Page 54 |
Page 55 |
Page 56 |
Page 57 |
Page 58 |
Page 59 |
Page 60 |
Page 61 |
Page 62 |
Page 63 |
Page 64 |
Page 65 |
Page 66 |
Page 67 |
Page 68 |
Page 69 |
Page 70 |
Page 71 |
Page 72 |
Page 73 |
Page 74 |
Page 75 |
Page 76 |
Page 77 |
Page 78 |
Page 79 |
Page 80 |
Page 81 |
Page 82 |
Page 83 |
Page 84 |
Page 85 |
Page 86 |
Page 87 |
Page 88 |
Page 89 |
Page 90 |
Page 91 |
Page 92 |
Page 93 |
Page 94 |
Page 95 |
Page 96 |
Page 97 |
Page 98 |
Page 99 |
Page 100 |
Page 101 |
Page 102 |
Page 103 |
Page 104 |
Page 105 |
Page 106 |
Page 107 |
Page 108 |
Page 109 |
Page 110 |
Page 111 |
Page 112 |
Page 113 |
Page 114 |
Page 115 |
Page 116 |
Page 117 |
Page 118 |
Page 119 |
Page 120 |
Page 121 |
Page 122 |
Page 123 |
Page 124 |
Page 125 |
Page 126 |
Page 127 |
Page 128 |
Page 129 |
Page 130 |
Page 131 |
Page 132 |
Page 133 |
Page 134 |
Page 135 |
Page 136 |
Page 137 |
Page 138 |
Page 139 |
Page 140 |
Page 141 |
Page 142 |
Page 143 |
Page 144 |
Page 145 |
Page 146 |
Page 147 |
Page 148 |
Page 149 |
Page 150 |
Page 151 |
Page 152 |
Page 153 |
Page 154 |
Page 155 |
Page 156 |
Page 157 |
Page 158 |
Page 159 |
Page 160 |
Page 161 |
Page 162 |
Page 163 |
Page 164 |
Page 165 |
Page 166 |
Page 167 |
Page 168 |
Page 169 |
Page 170 |
Page 171 |
Page 172 |
Page 173 |
Page 174 |
Page 175 |
Page 176 |
Page 177 |
Page 178 |
Page 179 |
Page 180 |
Page 181 |
Page 182 |
Page 183 |
Page 184 |
Page 185 |
Page 186 |
Page 187 |
Page 188 |
Page 189 |
Page 190 |
Page 191 |
Page 192 |
Page 193 |
Page 194 |
Page 195 |
Page 196 |
Page 197 |
Page 198 |
Page 199 |
Page 200 |
Page 201 |
Page 202 |
Page 203 |
Page 204 |
Page 205 |
Page 206 |
Page 207 |
Page 208 |
Page 209 |
Page 210 |
Page 211 |
Page 212 |
Page 213 |
Page 214 |
Page 215 |
Page 216 |
Page 217 |
Page 218 |
Page 219 |
Page 220 |
Page 221 |
Page 222 |
Page 223 |
Page 224 |
Page 225 |
Page 226 |
Page 227 |
Page 228 |
Page 229 |
Page 230 |
Page 231 |
Page 232 |
Page 233 |
Page 234 |
Page 235 |
Page 236 |
Page 237 |
Page 238 |
Page 239 |
Page 240 |
Page 241 |
Page 242 |
Page 243 |
Page 244 |
Page 245 |
Page 246 |
Page 247 |
Page 248 |
Page 249 |
Page 250 |
Page 251 |
Page 252 |
Page 253 |
Page 254 |
Page 255 |
Page 256 |
Page 257 |
Page 258 |
Page 259 |
Page 260 |
Page 261 |
Page 262 |
Page 263 |
Page 264 |
Page 265 |
Page 266 |
Page 267 |
Page 268 |
Page 269 |
Page 270 |
Page 271 |
Page 272 |
Page 273 |
Page 274 |
Page 275 |
Page 276 |
Page 277 |
Page 278 |
Page 279 |
Page 280 |
Page 281 |
Page 282 |
Page 283 |
Page 284 |
Page 285 |
Page 286 |
Page 287 |
Page 288 |
Page 289 |
Page 290 |
Page 291 |
Page 292 |
Page 293 |
Page 294 |
Page 295 |
Page 296 |
Page 297 |
Page 298 |
Page 299 |
Page 300 |
Page 301 |
Page 302 |
Page 303 |
Page 304 |
Page 305 |
Page 306 |
Page 307 |
Page 308 |
Page 309 |
Page 310 |
Page 311 |
Page 312 |
Page 313 |
Page 314 |
Page 315 |
Page 316 |
Page 317 |
Page 318 |
Page 319 |
Page 320 |
Page 321 |
Page 322 |
Page 323 |
Page 324 |
Page 325 |
Page 326 |
Page 327 |
Page 328 |
Page 329 |
Page 330 |
Page 331 |
Page 332 |
Page 333 |
Page 334 |
Page 335 |
Page 336 |
Page 337 |
Page 338 |
Page 339 |
Page 340 |
Page 341 |
Page 342 |
Page 343 |
Page 344 |
Page 345 |
Page 346 |
Page 347 |
Page 348 |
Page 349 |
Page 350 |
Page 351 |
Page 352