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DS90LV012A Datasheet(PDF) 5 Page - National Semiconductor (TI) |
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DS90LV012A Datasheet(HTML) 5 Page - National Semiconductor (TI) |
5 / 8 page Applications Information (Continued) Power Decoupling Recommendations: Bypass capacitors must be used on power pins. Use high frequency ceramic (surface mount is recommended) 0.1µF and 0.001µF capacitors in parallel at the power supply pin with the smallest value capacitor closest to the device supply pin. Additional scattered capacitors over the printed circuit board will improve decoupling. Multiple vias should be used to connect the decoupling capacitors to the power planes. A 10µF (35V) or greater solid tantalum capacitor should be connected at the power entry point on the printed circuit board between the supply and ground. PC Board considerations: Use at least 4 PCB board layers (top to bottom): LVDS signals, ground, power, TTL signals. Isolate TTL signals from LVDS signals, otherwise the TTL signals may couple onto the LVDS lines. It is best to put TTL and LVDS signals on different layers which are isolated by a power/ground plane(s). Keep drivers and receivers as close to the (LVDS port side) connectors as possible. For PC board considerations for the LLP package, please refer to application note AN-1187 “Leadless Leadframe Package.” It is important to note that to optimize signal integrity (minimize jitter and noise coupling), the LLP thermal land pad, which is a metal (normally copper) rectangular region located under the package, should be attached to ground and match the dimensions of the exposed pad on the PCB (1:1 ratio). Differential Traces: Use controlled impedance traces which match the differen- tial impedance of your transmission medium (ie. cable) and termination resistor. Run the differential pair trace lines as close together as possible as soon as they leave the IC (stubs should be < 10mm long). This will help eliminate reflections and ensure noise is coupled as common-mode. In fact, we have seen that differential signals which are 1mm apart radiate far less noise than traces 3mm apart since magnetic field cancellation is much better with the closer traces. In addition, noise induced on the differential lines is much more likely to appear as common-mode which is re- jected by the receiver. Match electrical lengths between traces to reduce skew. Skew between the signals of a pair means a phase differ- ence between signals which destroys the magnetic field cancellation benefits of differential signals and EMI will re- sult! (Note that the velocity of propagation,v=c/E r where c (the speed of light) = 0.2997mm/ps or 0.0118 in/ps). Do not rely solely on the autoroute function for differential traces. Carefully review dimensions to match differential impedance and provide isolation for the differential lines. Minimize the number of vias and other discontinuities on the line. Avoid 90˚ turns (these cause impedance discontinuities). Use arcs or 45˚ bevels. Within a pair of traces, the distance between the two traces should be minimized to maintain common-mode rejection of the receivers. On the printed circuit board, this distance should remain constant to avoid discontinuities in differential impedance. Minor violations at connection points are allow- able. Termination: DS90LV012A: Use a termination resistor which best matches the differen- tial impedance or your transmission line. The resistor should be between 90 Ω and 130Ω. Remember that the current mode outputs need the termination resistor to generate the differential voltage. LVDS will not work without resistor ter- mination. Typically, connecting a single resistor across the pair at the receiver end will suffice. Surface mount 1% - 2% resistors are the best. PCB stubs, component lead, and the distance from the termination to the receiver inputs should be minimized. The distance between the termination resistor and the receiver should be < 10mm (12mm MAX). DS90LT012A: The DS90LT012A integrates the terminating resistor for point-to-point applications. The resistor value will be be- tween 90 Ω and 133Ω. Threshold: The LVDS Standard (ANSI/TIA/EIA-644-A) specifies a maxi- mum threshold of ±100mV for the LVDS receiver. The DS90LV012A and DS90LT012A support an enhanced threshold region of −100mV to 0V. This is useful for fail-safe biasing. The threshold region is shown in the Voltage Trans- fer Curve (VTC) in Figure 5. The typical DS90LV012A or DS90LT012A LVDS receiver switches at about −30mV. Note that with V ID = 0V, the output will be in a HIGH state. With an external fail-safe bias of +25mV applied, the typical differen- tial noise margin is now the difference from the switch point to the bias point. In the example below, this would be 55mV of Differential Noise Margin (+25mV − (−30mV)). With the enhanced threshold region of −100mV to 0V, this small external fail-safe biasing of +25mV (with respect to 0V) gives a DNM of a comfortable 55mV. With the standard threshold region of ±100mV, the external fail-safe biasing would need to be +25mV with respect to +100mV or +125mV, giving a DNM of 155mV which is stronger fail-safe biasing than is necessary for the DS90LV012A or DS90LT012A. If more DNM is required, then a stronger fail-safe bias point can be set by changing resistor values. 20015029 FIGURE 5. VTC of the DS90LV012A and DS90LT012A LVDS Receivers www.national.com 5 |
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