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AD8115AST датащи(PDF) 24 Page - Analog Devices |
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AD8115AST датащи(HTML) 24 Page - Analog Devices |
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24 / 32 page ![]() AD8114/AD8115 Rev. B | Page 24 of 32 Effect of Impedances on Crosstalk The 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 PC board 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 will be given by ( ) [ ]s C R XT M S × = 10 log 20 where RS is the source resistance, CM is the mutual capacitance between the test signal circuit and the selected circuit, and s is the Laplace transform variable. From the equation, it can be observed that this crosstalk mechanism has a high-pass nature; it can 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 AD8114/AD8115 is 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 will induce crosstalk via the mutual inductance of the output pins and bond wires of the AD8114/AD8115. From a circuit standpoint, this 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 ) / ( log 20 10 L R s Mxy XT × = where Mxy is the mutual inductance of Output X to Output Y, and RL is the load resistance on the measured output. 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. |
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