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					 Lithology from Matrix
					TRAVEL TIME "Slowness" is the new word for sonic or acoustic travel
					time. The inverse of slowness is speediness or velocity. We
					continue to use travel time in this Handbook - it's hard to
					teach old dogs new tricks.
 
					The
			apparent matrix travel time can be calculated in a similar fashion
			to the matrix density, again by rearrangement of the response
			equation.
 
			Calculate Matrix Travel 
			Time: 1: IF Vsh + PHIe < 0.95
 2: THEN DTCma = (DTC - PHIe * DTCW - Vsh *
			DTCSH) / (1 - PHIe - Vsh)
 3: OTHERWISE DTCma = DTC
 
 Calculate mineral volumes (relative to each other)
 4: Vmin1 = (DTCma - DTC2) / (DTC1 - DTC2)
 5: Vmin2 = 1.00 - Vmin1
 
 Calculate mineral volumes (relative to total rock volume)
 6: Vrock = (1.0 - Vsh - PHIe)
 7: V1 = Vmin1 * Vrock
 8: V2 = Vmin2 * Vrock
 
 Where:
 DTC = sonic log reading (usec/ft or usec/m)
 DTCma = computed matrix travel time (usec/ft or usec/m)
 DTC1 = matrix travel time for first mineral (usec/ft or usec/m)
 DTC2 = matrix travel time for second mineral (usec/ft or usec/m)
 DTCSH = sonic log reading in shale (usec/ft or usec/m)
 DTCW = sonic log reading in water (usec/ft or usec/m)
 PHIe = effective porosity from any method (fractional)
 Vsh = volume of shale (fractional)
 Vrock = rock volume (fractional)
 Vmin1 = volume of first mineral (fractional)
 Vmin2 = volume of second mineral (fractional)
 Volumes for lithology track
 V1 = volume of first mineral (fractional)
 V2 = volume of second mineral (fractional)
 
 
  COMMENTS: This
			equation breaks down with high values of PHIe + Vsh, so we set
			DELTma = DELT when PHIe + Vsh > 0.95.
 This
			model is not very sensitive in carbonates - the matrix density model
			is better, if data is available. The
			matrix travel time can be obtained graphically from the chart below. 
			
			 Sonic neutron crossplot to find DELTma
 
					
					 NUMERICAL
			EXAMPLE: 1. Assume
			Sand D in Example 1.
 DTC = 300 usec/m
 DTCSH = 328 usec/m
 Vsh = 0.33
 DTCW = 616 usec/m
 PHIe = 0.11
 DTCma = (300 - 0.11 * 616 - 0.33 * 328) / (1 - 0.11 - 0.33) = 229
			usec/m
 This
			value falls in the impossible area and is too high because the sonic
			log reads high compared to effective porosity found from the density
			neutron crossplot. If porosity was 0.16, the matrix travel time
			would be 183 usec/ft (close to the sandstone value). This
			is another quality control indicator, and in this example
			demonstrates a lack of coherence between the sonic and density
			neutron data, when the matrix, shale and fluid assumption are as
			given above. Either these parameters, or the log data, or the whole
			rock model are in error. 
  Sonic Lithology Codes Lithology codes are more difficult to generate with sonic data then
			with density data.
 
 
  SlithCode - Sonic Lithology Codes
 
				
					| DELTma |  |  |  
					| English | Metric | SlithCode |  
					| usec/ft | usec/m |  |  
					| < 41 | < 134 -- | ---- |  
					| 41 - 45 | 134 - 147 | DOLO |  
					| 45 - 49 | 147 - 160 | LIME |  
					| 49 - 51 | 160 - 167 | ANHY |  
					| 51 - 58 | 167 - 190 | QRTZ |  
					| 58 - 65 | 190 - 213 | ---- |  
					| 65 - 68 | 213 - 223 | SALT |  
					| 68 - 72 | 223 - 236 | ---- |  
					| 72 - 76 | 236 - 249 | SYLV |  
					| 76 - 80 | 249 - 262 | CARN |  
					| 80 - 120 | 262 - 393 | COAL
					(only if trigger set) |  
					| 120 - 124 | 393 - 406 | SULF |  
					| > 124 | > 406 - | ---- |  
					| if Vsh >
					0.85 |  | SHLE |  COMMENTS:The bad
			hole code does not intervene in sonic calculations.
 Should
			not be used in shallow unconsolidated sandstones. 
  SONIC PARAMETERS 
  
  
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