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PCF5079 Datasheet(PDF) 9 Page - NXP Semiconductors |
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PCF5079 Datasheet(HTML) 9 Page - NXP Semiconductors |
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9 / 28 page ![]() 2001 Nov 21 9 Philips Semiconductors Product specification Dual-band power amplifier controller for GSM, PCN and DCS PCF5079 7.7 Considerations for ramp-down Referring to Fig.5, the i-th code can be programmed to have either the CODEEND or CODESTART value or any code between, depending on the application preferences. These codes do not produce any power at the output of the PA, as CODESTART has been chosen to keep the PA isolation. The proper conclusion of the ramp-down is ensured by choosing CODEEND < CODESTART so that the discharge of the integration capacitance is controlled until the control voltage on pin VCD or VCG goes below the PA conduction threshold and by applying at this time the PU transition from logic 1 to logic 0. At the beginning of a burst, the VDAC signal steps applied at OP1 are not compensated by any signal at the sensor input up to when pin VCD or VCG voltage is greater than the PA conduction threshold voltage. In any case, the initial DAC voltage steps are stored in the capacitance of amplifier OP1. CODEEND has to be chosen so that the energy inside the shaded zone cancels the energy accumulated in the summing node (OP1) at the start of a burst and not balanced by a feedback signal at the sensor input. The exact value of the energy required depends on the specific PA, on the characteristics of the overall loop and on the values chosen for the settable parameters inside the loop. A rough idea can be derived with a simplified analysis of a ramp-up, ramp-down cycle using the following simplifications: • The starting conditions for OP1 and OP4 are biasing at Vhome with zero charge on capacitances • The initial rising of pin VCD or VCG voltage from Vhome is caused only by the integration of the constant CODEKICK • VDAC is treated as applied directly at the summing node, initially neglecting the transmission delay through the internal low-pass filter. Generally, the integrator OP4 input can be expressed as (1) where gs and gd are respectively the gains of sensor input and DAC input in the summing amplifier OP1. Equation (1) holds for closed loop operation. In the time interval between the rising of pin VCD or VCG voltage due to CODEKICK (t = 0) and when Vconduction for the PA is reached (t = t1), ∆Vs is 0 and operation is open loop. In this time interval, a charge accumulates in the summing node, which remains uncompensated. Time t1 can be calculated with the preceding simplification. Now, to define the quantity (2) the current/voltage equations around the integrator OP4 can be solved by forcing the current through R1 to be equal to the current through the integration capacitance and calculating the ∆V generated on CINT, then (3) where (4) Substituting equation (4) into equation (3) (5) Under the hypothesis the voltage is constant: (6) Equation (6) can be used to calculate time t1 at which the conduction of the PA is reached, considering that (7) (8) Time t1 depends on the time constant of the integrator, by the PA and by ∆VKICK. The condition to be fulfilled is that the energy contained in the shaded zone (Fig.5) is at least equal to the energy accumulated at the beginning: (9) where k is the number of quarter-bits during which CODEEND is applied. V in integrator () g s ∆V s × g d ∆V VDAC × – = ∆V KICK CODE KICK CODE START – = ∆V CINT 1 C CINT --------------- i τ () τ d 0 t ∫ × = i τ () g d ∆V KICK × R1 ------------------------------- = ∆V CINT 1 C CINT R1 × ----------------------------- g 0 t ∫ d ×∆V KICK × d τ = ∆V CINT 1 C CINT R1 × ----------------------------- g d ×∆V KICK × t × = tt 1 V home ∆V CINT V conduction = + ⇒ = t 1 R1 C CINT × V conduction V home – g d ∆V KICK × ----------------------------------------------- × = V out OP1 2 (t) dt = k QB CODE END CODE START – () 2 × × 0 t 1 ∫ |
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