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LTC4313-2 Datasheet(PDF) 9 Page - Linear Technology |
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LTC4313-2 Datasheet(HTML) 9 Page - Linear Technology |
9 / 20 page LTC4315 9 4315f The LTC4315 provides capacitance buffering, data and clock Hot Swap capability and level translation of I2C signals on its clock and data pins. The high noise margin of the LTC4315 permits interoperability with I2C devices that drive a high VOL,permitsseriesconnectionofmultipleLTC4315s and provides improved I2C communication reliability. The LTC4315 isolates backplane and card capacitances, provides slew limited acceleration of rising edges and slew control of falling edges while level translating 1.5V, 1.8V, 2.5V, 3.3V and 5V busses. These features are illustrated in the following subsections. RISE TIME ACCELERATOR (RTA) PULL-UP CURRENT STRENGTH After an input to output connection has been established the RTAs on both the input and output sides of the SDA and SCL busses are activated based on the state of the ACC pin and the VCC2 supply voltage. During positive bus transitions of at least 0.4V/μs, the RTAs provide pull-up currents to reduce rise time. Enabling the RTAs allows users to choose larger bus pull-up resistors to reduce power consumption and improve logic low noise margins, to design with bus capacitances outside of the I2C speci- fication and to operate at a higher clock frequency. The function of the ACC pin in setting IRTA is summarized in Table 1. In the strong mode (ACC low) the acceleration is slew limited to a maximum bus rise rate of 75V/μs. The strong mode current is therefore directly proportional to the bus capacitance. The LTC4315 is capable of sourcing up to 40mA of current in the strong mode. If ACC is left open, rise time acceleration is provided by a 2.5mA pull up. TABLE 1: ACC Control of the RTA Current IRTA ACC IRTA Low Strong Hi-Z 2.5mA High None The ACC pin has a resistive divider between VCCandground to set its voltage to 0.5 • VCC if left open. APPLICATIONS INFORMATION Figures 1 and 2 show the rising waveforms of heavily loaded SDAIN and SDAOUT busses with the ACC pin set for strong mode and 2.5mA current source mode respectively. In both figures, during a rising edge, the buffers are active and the input and output sides connected, until the bus voltages on both the input and output sides are greater than 0.33 • VMIN, where VMIN is the lower of the VCC and VCC2 voltages. When each individual bus voltage rises above 0.41 • VMIN, the RTA on that bus turns on. The effect of the acceleration strength is shown in the SDA waveforms in Figures 1 and 2 for identical bus loads. The RTAs supply 10mA and 2.5mA of pull-up current IRTA in the strong and current source modes respectively for the bus conditions shown in Figures 1 and 2. For identical bus loads, the bus rises faster in Figure 1 compared to Figure 2 because of the higher IRTA. Figure 1. Bus Rising Edge for the Strong Acceleration Mode. VCC = VCC2 = 5V Figure 2. Bus Rising Edge for the Current Source Acceleration Mode. VCC = VCC2 = 5V 2V/DIV 1μs/DIV 4315 F01 VCC = VCC2 = 5V RBUS = 20k CIN = COUT = 200pF ACC = 0V SDAIN SDAOUT 2V/DIV 1μs/DIV 4315 F02 VCC = VCC2 = 5V RBUS = 20k CIN = COUT = 200pF ACC = OPEN SDAIN SDAOUT |
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