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ADV3201ASWZ Datasheet(PDF) 34 Page - Analog Devices |
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ADV3201ASWZ Datasheet(HTML) 34 Page - Analog Devices |
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34 / 36 page ![]() ADV3200/ADV3201 Rev. 0 | Page 34 of 3 6 Effect of Impedances on Crosstalk Input side crosstalk can be influenced by the output impedance of the sources that drive the inputs. The lower the impedance of the drive source, the lower the magnitude of the crosstalk. The dominant crosstalk mechanism on the input side is capacitive coupling. The high impedance inputs do not have significant current flow to create magnetically induced crosstalk. However, significant current can flow through the input termination resistors and the loops that drive them. Thus, the PCB on the input side can contribute to magnetically coupled crosstalk. From a circuit standpoint, the input crosstalk mechanism looks like a capacitor coupling to a resistive load. For low frequencies, the magnitude of the crosstalk is given by [ s C R XT M S × = ) ( log 20 10 ] (5) where: RS is the source resistance. CM is the mutual capacitance between the test signal circuit and the selected circuit. s is the Laplace transform variable. From the preceding equation, it can be observed that this crosstalk mechanism has a high-pass nature; it can also be minimized by reducing the coupling capacitance of the input circuits and lowering the output impedance of the drivers. If the input is driven from a 75 Ω terminated cable, the input crosstalk can be reduced by buffering this signal with a low output impedance buffer. On the output side, the crosstalk can be reduced by driving a lighter load. Although the ADV3200/ADV3201 are specified with excellent differential gain and phase when driving a standard 150 Ω video load, the crosstalk will be higher than the minimum obtainable due to the high output currents. These currents induce crosstalk via the mutual inductance of the output pins and bond wires of the ADV3200/ADV3201. From a circuit standpoint, the output crosstalk mechanism looks like a transformer with a mutual inductance between the windings that drives a load resistor. For low frequencies, the magnitude of the crosstalk is given by ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ × = L XY R s M XT 10 log 20 (6) where: MXY is the mutual inductance of Output X to Output Y. RL is the load resistance on the measured output. s is the Laplace transform variable. This crosstalk mechanism can be minimized by keeping the mutual inductance low and increasing RL. The mutual inductance can be kept low by increasing the spacing of the conductors and minimizing their parallel length. PCB Layout Extreme care must be exercised to minimize additional crosstalk generated by system circuit boards. The areas that must be carefully detailed are grounding, shielding, signal routing, and supply bypassing. The input and output signals have minimum crosstalk if they are located between ground planes on layers above and below and are separated by ground in between. Locate vias as close to the IC as possible to carry the inputs and outputs to the inner layer. The input and output signals surface at the input termin- ation resistors and the output series back-termination resistors. To the extent possible, separate these signals as soon as they emerge from the IC package. PCB TERMINATION LAYOUT As frequencies of operation increase, proper routing of trans- mission line signals becomes more important. The bandwidth of the ADV3200/ADV3201 is large enough so that using high impedance routing does not provide a flat in-band frequency response for practical signal trace lengths. It is necessary for the user to choose a characteristic impedance suitable for the application and to properly terminate the input and output signals of the ADV3200/ADV3201. Traditionally, video applications use 75 Ω single-ended environments. For flexibility, the ADV3200/ADV3201 does not contain on- chip termination resistors. This flexibility in application comes with some board layout challenges. The distance between the termination of the input transmission line and the ADV3200/ ADV3201 die is a high impedance stub and causes reflections of the input signal. With some simplification, it can be shown that these reflections cause peaking of the input at regular intervals in frequency, dependent on the propagation speed (vP) of the signal in the chosen board material and the distance (d) between the termination resistor and the ADV3200/ADV3201. If the distance is great enough, these peaks can occur in band. In fact, practical experience shows that these peaks are not high-Q, and should be pushed out to three or four times the desired bandwidth in order to not have an effect on the signal. For a board designer using FR4 (vP = 144 × 106 m/s), this means that the ADV3200/ADV3201 input should be placed no farther than 2 cm after the termination resistors and, preferably, should be placed even closer. Therefore, 2 cm PCB routing equates to d = 2 × 10−2 m in the calculations. ( ) d v n f P PEAK 4 1 2 × + = (7) where n = {0, 1, 2, 3, …}. In some cases, it is difficult to place the termination close to the ADV3200/ADV3201 due to space constraints and large resistor footprints. A better solution in this case is to maintain a controlled transmission line past the ADV3200/ADV3201 inputs and to terminate the end of the line. This method is known as fly-by termination. The input impedance of the ADV3200/ADV3201 is large enough, and the stub length inside the package is small enough, that this works well in practice. |
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