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PERMFILE44309
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Last modified
8/24/2016 10:46:44 PM
Creation date
11/20/2007 11:53:20 AM
Metadata
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Template:
DRMS Permit Index
Permit No
C1982057
IBM Index Class Name
Permit File
Doc Date
12/11/2001
Doc Name
OIL WELL SITE BLASTING
Section_Exhibit Name
TAB 14 ATTACHMENT 14-4
Media Type
D
Archive
No
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Compared to previous studies, strains were relatively low for given <br />particle velocities. Tlie large blasts involved in this study produced high <br />• particle velocities at relatively large distance. Hence, the pipelines <br />experienced Nigh vibration amplitudes at distances beyond the inelastic zone. <br />In addition, charges are in blastlioles, being vertical columns which are long <br />compared to the closest blast to pipeline separations. 8y contrast, the <br />previous studies involved close-in "point" sources. Interesting is the <br />apparent limiting effect of pipeline responses. Circumferential strains, in <br />particular, do not continue to increase in proportion to increasing surface <br />particle velocity. This could be from lack of total coupling with the ground. <br />Another possibility is that the spatially extended charge with its <br />relatively long detonation time impacts the pipeline less than a point source <br />type blast. Tl~e hypothesis requires further analysis. <br />Stresses <br />Stresses were calculated for each blast using maximum circumferential <br />and longitudinal strains (table 4). As with previous SwAI studies by Esparza, <br />these were assumed to be principle plane strains, and represent a type of <br />worst case (as in pseudo vector sum compared to true vector sum). Esparza's <br />values of Young's modulus (29.5 x 106) and Poisson's Ratio (0.3) were used <br />(Ref. 5). Stress values calculated from these tests are based on pseudo sums <br />of longitudinal and circumferential. An initial examination of time- <br />. correlated strain components found that peaks did not occur at the same tune. <br />Phase is also important in calculating the stresses corresponding to given <br />strain states. If the two component are opposite (one tensile and one <br />comprehensive at any instant), the calculated stresses are actually less than <br />would correspond to either uniaxial strain. <br />Circumferential or hoop stresses from internal pressurization can•be <br />easily calculated from the thin-walled cylinder equation; <br />Stress (lb/inz) = PD/2t <br />where P is pressure, lb/inz; D is inside diameter and t is wall thickness, <br />both in inches. Table 5 lists pipeline specifications and hoop stresses <br />produced by internal pressurization. As the table shows, the pressurization= <br />induced circumferential or hoop stresses are close to 72 pct of yield <br />strengths (and would be exact if D was set to outside diameter). The PVC is <br />also an exception for reasons unknown to the authors. Also in table 5 are <br />both stresses and strains equivalent to 18 pct of yield strength. This 18 pct <br />level is used by some transmission companies as an informal guideline for <br />transient environmental effects such as traffic over a pipeline beneath a <br />highway. <br />The minimum biaxial strain values in table 5 (last column) were <br />calculated from the stress-strain equation in table 4 based on the worst-case <br />assumption that the two strain components peak at the same time and are the <br />same peak amplitude. They are minimums in that they are tl~e lowest (most <br />restrictive) values that correspond to the 18 pct of SP1YS stress. <br />134 <br />
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