| Electronic Components Datasheet Search |
|
NE564 Datasheet(PDF) 5 Page - NXP Semiconductors |
|
|
|||||||||||||||||||||||||||||
NE564 Datasheet(HTML) 5 Page - NXP Semiconductors |
|
5 / 9 page ![]() Philips Semiconductors Product specification NE/SE564 Phase-locked loop 1994 Aug 31 5 FUNCTIONAL DESCRIPTION (Figure 6) The NE564 is a monolithic phase-locked loop with a post detection processor. The use of Schottky clamped transistors and optimized device geometries extends the frequency of operation to greater than 50MHz. In addition to the classical PLL applications, the NE564 can be used as a modulator with a controllable frequency deviation. The output of the PLL can be written as shown in the following equation: VO = (fIN - fO) KVCO (1) KVCO = conversion gain of the VCO fIN = frequency of the input signal fO = free-running frequency of the VCO The process of recovering FSK signals involves the conversion of the PLL output into logic compatible signals. For high data rates, a considerable amount of carrier will be present at the output of the PLL due to the wideband nature of the loop filter. To avoid the use of complicated filters, a comparator with hysteresis or Schmitt trigger is required. With the conversion gain of the VCO fixed, the output voltage as given by Equation 1 varies according to the frequency deviation of fIN from fO. Since this differs from system to system, it is necessary that the hysteresis of the Schmitt trigger be capable of being changed, so that it can be optimized for a particular system. This is accomplished in the 564 by varying the voltage at Pin 15 which results in a change of the hysteresis of the Schmitt trigger. For FSK signals, an important factor to be considered is the drift in the free-running frequency of the VCO itself. If this changes due to temperature, according to Equation 1 it will lead to a change in the DC levels of the PLL output, and consequently to errors in the digital output signal. This is especially true for narrowband signals where the deviation in fIN itself may be less than the change in fO due to temperature. This effect can be eliminated if the DC or average value of the signal is retrieved and used as the reference to the comparator. In this manner, variations in the DC levels of the PLL output do not affect the FSK output. VCO Section Due to its inherent high-frequency performance, an emitter-coupled oscillator is used in the VCO. In the circuit, shown in the equivalent schematic, transistors Q21 and Q23 with current sources Q25 - Q26 form the basic oscillator. The approximate free-running frequency of the oscillator is shown in the following equation: fO ≅ 1 22 RC (C1 + CS) (2) RC = R19 = R20 = 100Ω (INTERNAL) C1 = external frequency setting capacitor CS = stray capacitance Variation of VD (phase detector output voltage) changes the frequency of the oscillator. As indicated by Equation 2, the frequency of the oscillator has a negative temperature coefficient due to the monolithic resistor. To compensate for this, a current IR with negative temperature coefficient is introduced to achieve a low frequency drift with temperature. Phase Comparator Section The phase detection processor consists of a doubled-balanced modulator with a limiter amplifier to improve AM rejection. Schottky-clamped vertical PNPs are used to obtain TTL level inputs. The loop gain can be varied by changing the current in Q4 and Q15 which effectively changes the gain of the differential amplifiers. This can be accomplished by introducing a current at Pin 2. Post Detection Processor Section The post detection processor consists of a unity gain transconductance amplifier and comparator. The amplifier can be used as a DC retriever for demodulation of FSK signals, and as a post detection filter for linear FM demodulation. The comparator has adjustable hysteresis so that phase jitter in the output signal can be eliminated. As shown in the equivalent schematic, the DC retriever is formed by the transconductance amplifier Q42 - Q43 together with an external capacitor which is connected at the amplifier output (Pin 14). This forms an integrator whose output voltage is shown in the following equation: VO = gM C2 (3) VINdt gM = transconductance of the amplifier C2 = capacitor at the output (Pin 14) VIN = signal voltage at amplifier input With proper selection of C2, the integrator time constant can be varied so that the output voltage is the DC or average value of the input signal for use in FSK, or as a post detection filter in linear demodulation. The comparator with hysteresis is made up of Q49 - Q50 with positive feedback being provided by Q47 - Q48. The hysteresis is varied by changing the current in Q52 with a resulting variation in the loop gain of the comparator. This method of hysteresis control, which is a DC control, provides symmetric variation around the nominal value. Design Formula The free-running frequency of the VCO is shown by the following equation: (4) fO ≅ 1 22 RC (C1 + CS) RC = 100Ω C1 = external cap in farads CS = stray capacitance The loop filter diagram shown is explained by the following equation: (5) fS = 1 1 + sRC3 (First Order) R = R12 = R13 = 1.3kΩ (Internal)* By adding capacitors to Pins 4 and 5, a pole is added to the loop transfer at ω = 1 RC3 NOTE: *Refer to Figure 6. |
|
|
Link URL |
| Does ALLDATASHEET help your business so far? [ DONATE ] |
About Alldatasheet | Advertisement | Contact us | Privacy Policy | Link to Datasheet | Link Exchange | Manufacturer List All Rights Reserved©Alldatasheet.com |
| Russian : Alldatasheetru.com | Korean : Alldatasheet.co.kr | Spanish : Alldatasheet.es | French : Alldatasheet.fr | Italian : Alldatasheetit.com Portuguese : Alldatasheetpt.com | Polish : Alldatasheet.pl | Vietnamese : Alldatasheet.vn Indian : Alldatasheet.in | Mexican : Alldatasheet.com.mx | British : Alldatasheet.co.uk | New Zealand : Alldatasheet.co.nz |
|
Family Site : ic2ic.com |
icmetro.com |