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Networking Main | Archive | Feedback Page 1 of 4 Simulating a Phase-Locked Loop Using a Sigma-Delta Modulator to Attain Nearly Arbitrary Frequency Resolution Without Spurs by Andy Howard Introduction It is often desirable to create a phase-locked loop (PLL) with a frequency resolution in steps smaller than the reference
oscillator frequency. This is often accomplished with a fractional-N PLL in which the divide ratio is varied between N and N + 1 at a defined rate. However, this
technique generates undesired spurs. An alternative is to use a sigma-delta modulator, a circuit in which the divide ratio is "dithered" and the spurs are
eliminated. This paper covers the basic phase-locked loop operation, fractional-N PLL simulation, and sigma-delta PLL simulation.
Basic Phase-Locked Loop Operation Figure 1 shows a block diagram of a basic phase-locked loop. This PLL consists of a reference source, a phase/frequency detector, a charge pump, a loop filter,
a voltage-controlled oscillator (VCO), and a divider. If the divide ratio is a constant, the loop forces the VCO signal frequency to be exactly N times the reference
signal frequency. The phase/frequency detector and charge pump deliver either positive or negative charge "pulses," depending on whether the reference signal phase
leads or lags the divided VCO signal phase. These charge pulses are integrated by the loop filter to generate a tuning voltage. The tuning voltage changes the VCO
frequency up or down until the phases of the reference signal and divided signal are synchronized.
Figure 1 - Basic Phase-Locked Loop Phase-locked loops are used as frequency synthesizers in many applications where it is necessary to generate a precise signal frequency with low spurs and good
phase noise. A VCO's signal frequency may be changed by varying either the reference signal frequency or the divide ratio. The reference signal is very often
produced by a stable oscillator whose frequency cannot be varied, so the divide ratio is changed in integer steps to change the VCO frequency, where Fout
= N * Fref.
One limitation with this type of phase-locked loop is that the VCO frequency cannot be varied in steps any smaller than the reference frequency. With a little
more circuit complexity, a 1/M divider could be placed between the reference signal and the phase/frequency detector, in which case the VCO output frequency would be
determined by the ratio of the integer dividers, where Fout = (N/M) * Fref.
Even when the loop is locked, the charge pump still outputs small charge pulses caused by mismatches in the PLL's positive and negative charge pumps and other
factors such as non-ideal phase/frequency detection. These pulses cause sidebands, or spurs, to appear in the VCO output spectrum at offset frequencies equal to the
reference frequency.
Dealing with these spurs requires some design tradeoffs. For a fine frequency resolution, we want a small reference frequency, but this will cause spurs to be
generated at a smaller offset frequency from Fout. This means that a narrower loop filter bandwidth is required to filter them. PLLs with narrower loop
bandwidths have longer transient settling times (the transition time from one frequency to another) and may not operate at the required speed. Reference [1] has a
discussion of PLL settling time requirements. Also, the narrower the PLL's loop bandwidth, the less the VCO's phase noise outside the loop bandwidth is suppressed.
Fractional-N Synthesis to Achieve Finer Frequency Resolution Fractional-N is one popular technique that achieves a frequency resolution that is finer than the reference frequency. In this approach, the divide ratio is varied
periodically between two integer values. Figure 2 shows a block diagram of this type of PLL.
Figure 2 - Fractional-N Synthesizer PLL The average VCO frequency is determined from Equation (2) in Reference [2],
which is repeated here.
which can be reduced to
Therefore, the fractional part of the divide ratio is determined by the duty cycle, the fraction of the time that the divider is dividing by N + 1.
This type of PLL may be modeled using an accumulator that sums the desired fraction to itself each reference clock cycle (Reference [2]). While the accumulator's sum
is less than its total count capacity, the overflow output is 0, and the divider divides by N. When the accumulator reaches its capacity, it overflows and the divide ratio
is set to N + 1. If the desired fraction is 0.1, the accumulator will overflow once every 10th reference clock cycle. If the desired fraction is 0.5, the accumulator will
overflow every other reference clock cycle.
In fractional-N PLLs, the signals at the input to the phase/frequency detector are not at the same frequency. The reference signal is at Fref, and the divided
VCO signal is at (1 + fraction/N) * Fref. Referred to the VCO, this frequency difference means that the phase of the VCO advances at a rate of fraction
radians per reference clock cycle faster than a signal at frequency of N * Fref. The accumulator sums this fraction once per reference clock cycle, so it accumulates
at the same rate that the VCO phase difference advances. An accumulator overflow occurs at the same time the VCO phase difference (relative to a signal at N * Fref)
reaches 2p radians. When the accumulator overflows, the divide ratio is increased to N + 1 for one cycle. This subtracts 2p/N
radians from the divided VCO signal, so the phases of the two signals at the input to the phase/frequency detector are again equal. Thus, the phase difference between the two
signals at the input to the phase/frequency detector should increase and be reset to zero at the same rate that the accumulator sum increases and overflows. A numerical example
is given in Reference [2].
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