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DP8459 Scheda tecnica(PDF) 21 Page - National Semiconductor (TI) |
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DP8459 Scheda tecnica(HTML) 21 Page - National Semiconductor (TI) |
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21 / 35 page ![]() The 3 dB bandwidth for requirement #3 is defined by the equation 3: ω −3 dB = ωn [2ζ 2 + 1 +{(2 ζ2 +1)2 +1}0.5]0.5 Requirement #4 has been established in order to maximize the available window margin via PLL dynamics. Conceptually, window margin is preserved if the loop phase response to individually displaced bits (jitter) is not allowed to cause subsequent windows to be readily shifted from the “average” position. Any window movement from nominal position can readily degrade the window margin. It can be seen from Figure 19 that systems employing low values of damping ratio exhibit a reduced instantaneous response to phase step and thus display improved jitter rejection with respect to higher damping ratio systems. Damping ratio, fortunately, is easily regulated by loop filter design. It also follows that a low natural frequency and its associated “slower” instantaneous phase response will assist in achieving the goal of jitter rejection. However, the minimum natural frequency limit for the PLL may actually be imposed on the system by the θ e(t) settling time requirement, the ∆ω L requirement, or the ω−3 dB requirement. Whichever of these produces the highest minimum ω n value must, by necessity, dominate in the design. The goal of minimizing the natural frequency in order to maximize jitter rejection, therefore, may have to defer to one of these other three criteria. Requirement #5 is addressed in three ways: 1) the DP8459 itself engages the frequency discriminating action of the Phase Comparator whenever the READ GATE is deasserted and the PLL locks to the REFERENCE CLOCK signal, thus guaranteeing re-lock regardless of the initial frequency step; 2) tying the HIGH GAIN DISABLE pin to the READ GATE input places the Charge Pump in the high gain mode whenever the PLL is locked to the REFERENCE CLOCK, producing an elevated natural frequency and a more rapid locking action; 3) N = 2 whenever the READ GATE is deasserted, which, in this example, effectively increases the loop gain by another factor of 2 with respect to the gain within the preamble, where N = 4. Determining PLL Response Characteristics It is expected that the minimum value of ω n will be determined by the residual phase error requirement of #1 rather than the lock-in range requirement of #2orthe ω −3 dB requirement of #3. This assumption will be checked at the end of the analysis. System requirements then are as follows: 1. θ e(t) ≤ (2 ns) x (2π rad/ 200 ns) = 0.063 radians, where t = preamble length 8.8 µs 2. ∆ω L ≈ ±KBZf(s)|s→ ∞ ≥ 0.015x5MHzx2π = 471 Krad/sec 3. ω −3 dB = ωn[2ζ 2 +1+{(2 ζ2 +1)2 +1}0.5]0.5 ≥ 2x10kHzx2π = 126 Kr/s Requirement #1 calls for θ e(8.8 µs) ≤ 0.063 radians. Damping ratio ζ varies as the inverse square root of N (see the equation for Damping Ratio in Section 3.0) such that ζ PREAMBLE = √(N MAX/NPREAMBLE)x ζMIN = √2 x 0.5 = 0.707. Solving the appropriate equation for θ e(t) for various values of ωn with ζ = 0.707, t = 8.8 µs and an expected frequency step of 0.01 x 5 MHzx2 π = 314 Kr/s: ω n θ e (8.8 µs) |t e| 200 Kr/s 0.606 rad 19.29 ns 300 Kr/s 0.219 rad 6.97 ns 400 Kr/s 0.056 rad 1.78 ns 500 Kr/s 0.0012 rad 0.038 ns 600 Kr/s −0.0098 rad 0.312 ns ω n θ e (8.8 µs) |t e| 700 Kr/s −0.008 rad 0.026 ns θ e (8.8µs)|400 Kr/s = 0.056 radian < 0.063 radian t e = 0.056 radian x 200 ns/2π radian = 1.78 ns < 2ns Thus 400 Kr/s is chosen as the desired natural frequency within the preamble to satisfy requirement #1. If the assumption that θ e(t) dominates the minimum natural frequency requirement is correct, then the ∆ω L requirement of #2 and the ω −3 dB requirement of #3 should be met by the ωn obtained above. First, examining requirement #2, Z f(s)|s→ ∞ = R1 (C2 neglected). Thus, ∆ω L = KBR1 Rearranging for R 1: R 1 = ∆ωL/KB The equation for R 1 previously derived shows R 1 = 2ζωn/KB Thus, ∆ω L/KB = 2ζωn/KB ∆ω L = 2 ζωn In this case, ω n = 400 Kr/s and ζ = 0.707 (preamble), thus ∆ω L = 400 Kr/sx2x 0.707 = 566 Kr/s > 471 Kr/s Thus, requirement #2 is met. Examining requirement #3, where ω −3 dB ≥ 2x10kHzx2π when N equals its maximum value of 8 (minimum frequency data pattern; ζ = 0.5): ω n(min) = ωn(preamble) x 1/√(NMAX/NPREAMBLE) = 400 Kr/s x 1/ √2 = 283 Kr/s ω −3 dB = ωn(min) [2ζ 2 +1+{(2 ζ2 +1)2+1}0.5]0.5 =283 Kr/s x 1.817 = 514 Kr/s 514 Kr/s ÷ 2 π = 82 kHz > 2x10kHz Thus requirements #1 through #3 are met, and #4 defers to the minimum ω n established by #1. Regarding requirement #5, the DP8459 has been configured externally in this example such that when the READ GATE is deasserted, the loop gain will be increased by a factor of 2 due to the Charge Pump gain switching (R NOM = RBOOST; HGD tied to RG) and by an additional factor of 2 due to the decrease in N from 4 (preamble) to a fixed internal value of 2. The resulting factor of 4 effective gain elevation results in an increase in both the natural frequency, ω n, and the damping ratio, ζ,by √4 = 2. Thus, when READ GATE is deasserted, ω n = 2 x 400 Kr/s = 800 Krad/s ζ = 2 x 0.707 = 1.414 ∆ω L = 2ζωn = 2 x 1.414 x 800 Krad/s = 2.3 Mr/s COMPONENT CALCULATIONS The formulae for the filter components, derived previously, are A 2:1 ratio of high-to-low Charge Pump gain was chosen for the derivation of R NOM and RBOOST. To achieve the 2:1 gain ratio, R NOM must be equal to R BOOST while the parallel http:\\www.national.com 21 PrintDate=1996/07/31 PrintTime=11:06:07 ds009322 Rev. No. 1 Proof 21 |
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