ICEA P-47-434-1965 Pressurization Characteristics of Polyethylene-Insulated and - Jacketed Telephone Cables《聚乙烯绝缘护套电话电缆的耐压特性》.pdf
《ICEA P-47-434-1965 Pressurization Characteristics of Polyethylene-Insulated and - Jacketed Telephone Cables《聚乙烯绝缘护套电话电缆的耐压特性》.pdf》由会员分享,可在线阅读,更多相关《ICEA P-47-434-1965 Pressurization Characteristics of Polyethylene-Insulated and - Jacketed Telephone Cables《聚乙烯绝缘护套电话电缆的耐压特性》.pdf(26页珍藏版)》请在麦多课文档分享上搜索。
1、ICEA P-47-434 65 m 9007034 0000223 723 = PRESSURIZATION CHARACTERISTICS OF POLYETHYLENE - INSULATED AND -JACKETED TELEPHONE CABLES PUBLICATION P-47-434 JUNE i965 INSULATED POWER CABLE ENGINEERS ASSOCIATON ICEA P-47-434 65 = 7007034 OOOOLL4 65T Copies of this Publication can be obtained by addressing
2、 The Insulated Power Cable Engineers Association 283 Valley Road Montclair, N. J. 07042 Area Code 201 Phone 744-3786 Price $1.50 per copy ICEA P-47-434 65 W 90070LY OOOOL15 57b = PFESSURIZATION CHARACTERISTICS OF POLYETHYLENE one was kept at conditioned room temperature, approximately 23 C, and the
3、other placed in an oven at 50 to 53 C. - i3 - ICEA P-47-434 b5 7007034 OOOOL29 080 = These tests were conducted to show what can be expected to happen to a pressurized cable stored out of doors in the winter, inside a plant or storage area, or out of doors in the summer. The test resuits, charted in
4、 Figure 2-4 show: for -2 to +4 C - 50 percent pressure loss occurred in over i40 days. for approximately 23 C - 50 percent pressure loss occurred in approximately for 50 to 53 C - 50 percent pressure loss occurred in approximately 32 days. 4 days. Calculated values (Kca for dimensions of above sampl
5、e = 0.027) are: Temperature, Degrees C Kg (see Figure 2-2) T.5, Days 1 23 52 4000 to 6000 130 to 200 800 to 1200 i08 to 162 3.5 to 5.4 21 to 32 The above indicates that the measured values are withinthe calculated range. II. with air. in Fig. 2-3. be.used, since this would hold only for a single gas
6、. data with calculated values, the percent pressure drop for air during the initial time, T,S (calculated for nitrogen), can be determined. sure drop for air is 59 percent, resulting in a pressure equal to bl percent of the original (nitrogen pressure drops from 80 percent to 40 percent; oxygen pres
7、sure from 20 percent to approximately 1 percent.) values for T-5, based on cable dimensions and nitrogen with actual measured time for air drop to 41 percent of original pressure as indicated by curves in Figure 2-5 and Figures 2-5 and 2-6 show results on direct burial and aerial cables pressuriaed
8、These tests show a pattern for pressure drop similar to that developed As these cables were pressurized with air, the T.5 concept could not In order to compare measured Figure 2-3 shows the pres- The tabulation below compares calculated 2-60 Cable T. 5 Calculated for N2, DaP Time for Air Pressure Dr
9、op to .hl Percent, Days 100 pair 22 Awg direct burial 25 pair 22 Awg direct Curial 6 pair 19 Awg direct burial 100 pair 22 Awg aerial and duct 25 pair 22 Awg aerial and duct 6 pair i9 Awg aerial and duct 43 to 65 19 to 30 15 to 23 65 to 97 32 to 48 24 to 36 23 18 84 h6 38 Examination of the above ta
10、bulation indicates time for pressure drop to 41 per- cent for direct burial cable to be somewhat less than the average of the calculated range for T.5, but for aerial cables these times are greater than the average of the calculated range for T.5 for 6 pair 19 Awg cable this time exceeds the calcula
11、ted maximum. - 14 - ICEA P-47-434 6.5 m 9007034 OOODL30 BT2 m It is noted that in direct burial type cables the corrugated shield is formed over the inner jacket, resulting in little area of contact between thetwo components. In contrast to this, the outer jackets of either aerial or direct burial c
12、able are extruded over the formed shield, resulting in good conformance and substantial con- tact area. Reeling and handling of the cable does result in some nonelastic shield defor- mation reducing conformance to and area of contact with the jacket. shield and jacket would be expected to reduce the
13、 effective area for gas diffusion through this jacket, and the difference in correlation between calculated and measured pressure drop in the two types of cables is attributed to the difference in shield-to= jacket contact. reels of each cable sise to provide data for within-reel and between-reel co
14、mparisons and to determine the effect of straight or coiled cable configuration on cable pressure- drop rate. Contact between In another independent set of measurements7 samples were taken from at least two For all cables tested, the rate of pressure drop was much greater for the direct This trend a
15、grees with results reported burial cable than for the aerial cable. increased with decreasing cable pair count. y Reference 1. Within one cable construction, this rate Comparative results are listed as follows: Time Required for Air Pressure Drop to 50 Percent of Original Cable Pressure, Days Coiled
16、 Cable Pair Count /AWE Reference 7 Reference 1 Aerial It II 6/19 15, 18 25/22 19, 20, 21, 22 100/22 53 Direct Burial 6/19 942 Il It 25/22 13 H II 100/22 28, 38 28 34 60 1242 17 36 Differences in air diffusion through jackets may be due to test temperatures utilized and to differences in the polyethy
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