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5962R9672201QCC Datasheet(PDF) 5 Page - Intersil Corporation |
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5962R9672201QCC Datasheet(HTML) 5 Page - Intersil Corporation |
5 / 8 page 5 Transmitter Operation The transmitter alternately applies the current to each of the two conductors in the twisted pair line such that the total current in the twisted pair is constant and always in the same direction. This current flows through either of the two 50V terminating resistors at the receiver and returns to the transmitter as a steady DC current on the transmission line shield. The DC power supply return for the transmitter is through the receiver terminating resistors (the transmitter ground pin is only a substrate ground). Therefore, it is essential that the shield be connected to the power supply common at both the transmitter and receiver, preferably at the integrated circuit “ground” pin. More than fifteen twisted pair lines can share the same shield without crosstalk. Receivers The HS-248RH “party-line” receiver presents a high impedance load to the transmission line allowing as many as ten HS-248RH receivers to be distributed along a line without excessive loading. Figure 3 shows a typical system of a transmitter, a terminating receiver and a party-line receiver. The transmission line is terminated in its characteristics impedance by an HS-246RH or by a pair of 50 Ω resistors connecting each line to the ground return shield. Transmission Lines The maximum frequency (or minimum pulse width) which can be carried by a certain length of a given transmission line is dependent on the loss characteristics of the particular line. At low frequencies, there will be virtually no loss in pulse amplitude, but there will be a degradation of rise and fall-time which is roughly proportional to the square of the line length. This is shown in Figure 5. If the pulse width is less than the rise-time at the receiver end, the pulse amplitude will be diminished, approaching the point where it cannot be detected by the receiver. The transmission line used with the Intersil HS-245RH series transmitter and receivers can be any ordinary shielded, twisted pair line with a characteristic impedance of 100 Ω. Twisted pair lines consisting of number 20 or 22 gauge wire will generally have this characteristic impedance. Special high quality transmission lines are not necessary and standard audio, shielded-twisted pair, cable is generally suitable. Since the necessary characteristics for various twisted pair lines are not readily available, it may be necessary to take some measurements on a length of the proposed line. To do this, connect an HS-245RH transmitter to one end of the line (100 feet or more) and an HS-246RH to the other end. The rise and fall-times can be measured on the line at both ends and the constant ‘‘K’’, for that line can be computed as shown in Figure 5 so that the minimum pulse width can be determined for any length of line. Data rates of 2MHz have been obtained using 1,000 feet of standard shielded, twisted pair, audio cable. Data rates of 15MHz are possible on shorter lengths of transmission line (50 feet). Electromagnetic Interference Very little electromagnetic interference is generated by the Intersil current mode system because the total current through the twisted pair is constant, while the current through the shield is also constant and in the opposite direction. This can be verified by observing, with a current probe, the total current through the twisted pair, through the shield and through the complete shielded, twisted pair cable. In each case a constant current will be observed with only small variations. Small pulses may be observed if the complementary inputs to the transmitter do not switch at the same time. The current will decrease during the time both inputs are high, and will increase during the time both inputs are low. These switching pulses may be observed when using the circuit shown in Figure 4. The amplitude and shape of these pulses will depend of the propagation delay of G1, and transition times G2 and G3. These pulses are generally of no concern because of their small amplitude and width, but they may be reduced by increasing the similarity of the waveforms and timing synchronization of the complementary signals applied to the transmitter. In addition to generating very little noise, the system is also highly immune to outside noise since it is difficult to capacitively couple a differential signal into the low impedance twisted pair cable and it is even more difficult in induce a differential current into the line due to the very high impedance of the constant current transmitter. Therefore, differential mode interference is generally not a problem with the Intersil current mode system. Large common mode voltages can also be tolerated because the output current of the transmitter is constant as long as the receiver termination ground is less than 2V positive with respect to TTLH1 TTHL1 LINE VOLTAGE AT RECEIVER TTHL2 0V 150mV WIDE PULSE TTLH2 TTLH2 TTHL1 TTLH2 TTHL2 MINIMUM PULSE WIDTH LINE VOLTAGE AT TRANS- MITTER TRLH2 = TTLH1 KL2 TTHL2 = TTHL1 KL2 Where: L is Line Length K is determined by line loss characteristics 150mV 0V FIGURE 5. TRANSMISSION LINE WAVE-SHAPING HS-245RH, HS-246RH, HS-248RH |
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