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LTC486I Fiches technique(PDF) 6 Page - Linear Technology |
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LTC486I Fiches technique(HTML) 6 Page - Linear Technology |
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6 / 8 page ![]() LTC486 6 S APPLICATI I FOR ATIO When using low loss cables, Figure 8 can be used as a guideline for choosing the maximum line length for a given data rate. With lower quality PVC cables, the dielectric loss factor can be 1000 times worse. PVC twisted pairs have terrible losses at high data rates (>100kbs) and greatly reduce the maximum cable length. At low data rates however, they are acceptable and much more economical. Cable Termination The proper termination of the cable is very important. If the cable is not terminated with its characteristic impedance, EN 12 EN 4 LTC486 • TA07 120 Ω DX 1 2 3 SHIELD 120 Ω RX RX SHIELD 3 DX EN 12 EN 4 2 EN EN 4 1 2 3 RX RX 3 DX EN 12 EN 4 1 DX 1/4 LTC488 1/4 LTC486 1/4 LTC488 1/4 LTC486 2 1 12 Losses in a transmission line are a complex combination of DC conductor loss, AC losses (skin effect), leakage, and AC losses in the dielectric. In good polyethylene cables such as the Belden 9841, the conductor losses and dielec- tric losses are of the same order of magnitude, with relatively low overall loss (Figure 7). FREQUENCY (MHz) 0.1 0.1 1 10 1 10 100 LTC486 • TA08 Figure 7. Attenuation vs Frequency for Belden 9841 DATA RATE (bps) 10k 10 100 1k 10k 100k 1M 10M LTC486 • TA09 2.5M distorted waveforms will result. In severe cases, distorted (false) data and nulls will occur. A quick look at the output of the driver will tell how well the cable is terminated. It is best to look at a driver connected to the end of the cable, since this eliminates the possibility of getting reflections from two directions. Simply look at the driver output while transmitting square wave data. If the cable is terminated properly, the waveform will look like a square wave (Figure 9). If the cable is loaded excessively (e.g., 47 Ω), the signal initially sees the surge impedance of the cable and jumps to an initial amplitude. The signal travels down the cable and is reflected back out of phase because of the mistermination. When the reflected signal returns to the driver, the amplitude will be lowered. The width of the pedestal is equal to twice the electrical length of the cable (about1.5ns/ft). If the cable is lightly loaded (e.g., 470 Ω), Figure 8. Cable Length vs Data Rate Figure 6. Typical Connection |
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