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LTM2889 датащи(PDF) 21 Page - Linear Technology |
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LTM2889 датащи(HTML) 21 Page - Linear Technology |
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21 / 30 page ![]() LTM2889 21 2889fa For more information www.linear.com/LTM2889 APPLICATIONS INFORMATION Figure 13. Slew Rate vs Slew Control Resistor RSL RSL (k) 2889 F13 60 50 40 30 20 10 0 1 10 100 VCC2 = 5V VCC2 = 3.3V When a voltage between 1.1V and VCC2 is applied, the RS pin acts as a high impedance receiver. A voltage above VIH_RS puts the chip in shutdown, while a voltage below VIL_RS but above 1.1V activates the chip and sets the transmitter to the minimum slew rate. TheslewcontrolcircuitontheRSpinisactivatedatapplied voltages below 1.1V. The RS pin can be approximately modeled as a 1.1V voltage source with a series resistance of 2k and a current compliance limit of –100µA, and a 250k pull-up resistor to VCC2 (Figure 14). Lowering the voltage on RS increases the slew control current ISC be- ing drawn from the slew control circuit until the voltage reaches ~0.9V, where the current drawn from the circuit is ~ –100µA. Below an applied voltage of ~ 0.9V, the slew control circuit sources no additional current, and the current drawn from it remains at ~ –100µA down to 0V. The total current IRS drawn from the RS pin for input volt- age 0.9V ≤ VRS ≤ 1.1V is the sum of the internal pull-up resistor current IRS and the slew control current ISC. IRS(0.9V ≤ VRS ≤ 1.1V)=IPU+ISC = VCC2 – VRS 250k + 1.1V – VRS 2k The transmitter slew rate is controlled by the slew control currentISCwithincreasingcurrentmagnitudecorrespond- ing to higher slew rates. The slew rate can be controlled using a single slew control resistor RSL in series with the RS pin. When the RS pin is pulled low towards ground by an external driver, RSL limits the amount of current drawn from the RS pin and sets the transmitter slew rate. Alternatively,theslewratemaybecontrolledbyanexternal voltage or current source. Figure 14. Equivalent Circuit of RS Pin 2889 F14 ISC (–100µA LIMIT) RS IPU VCC2 IRS IDEAL DIODE GND2 2k 1.1V + – V 250k High Symmetry Driver with Variable Slew Rate The electromagnetic emissions spectrum of a differential linetransmitterislargelydeterminedbythevariationinthe commonmodevoltageduringswitching,asthedifferential component of the emissions from the two lines cancel, while the common mode emissions of the two lines add. The LTM2889 transmitter has been designed to maintain highly symmetric transitions on the CANH and CANL lines to minimize the perturbation of the common mode voltage during switching (Figure 15), resulting in low EME. The common mode switching symmetry is guaranteed by the VSYM specification. Figure 15. Low Perturbation of Common Mode Voltage During Switching 200ns/DIV CANL 500mV/DIV COMMON MODE 500mV/DIV CANH 500mV/DIV 2889 F15 1Mbps LTM2889-3 PVCC = VCC = 3.3V |
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