
22.28.02
FS6209
FS6209FS6209
FS6209
Dual PLL VCXO
Dual PLL VCXODual PLL VCXO
Dual PLL VCXO Clock Generator IC
Clock Generator ICClock Generator IC
Clock Generator IC
ISO9001
ISO9001ISO9001
ISO9001
Table 2: Pin Descriptions
Key: AI = Analog Input; AO = Analog Output; DI = Digital Input; DIU = Input with Internal Pull-Up; DID = Input with Internal Pull-Down; DIO = Digital Input/Output; DI-3 = Three-Level Digi tal Input,
DO = Digital Output; P = Power/Ground; # = Active Low pin
PIN TYPE NAME DESCRIPTION
1 AI XIN VCXO Feedback
2 P VDD Power Supply (+3.3V)
3 AI XTUNE VCXO Tune
4 P VSS Ground
5DOCLKAClock Output A
6DOCLKBClock Output B
7 DO VSS Ground
8 A O XOUT VCXO Drive
3.0 Functional Bl ock Descripti on
3.1 Phase-Locked Loop (PLL)
The on-chip PLLs are a standard frequency- and phase-
lock ed loop archi tec tur e. The PLL multiplies t he r ef er enc e
oscillator to the desired frequency by a ratio of integers.
The frequency multiplication is exact with a zero synthe-
sis error.
3.2 Voltage-Controlled Crystal
Oscillator (VCXO)
The VCXO provides a tunable, low-jitter frequency refer-
ence for the rest of the FS6209 system components.
Loading capacitance for the crystal is internal to the
FS6209. No external components (other than the reso-
nator itself) are required for operation of the VCXO.
Continuous fine-tuning of the VCXO frequency is accom-
plished by varying the voltage on the XTUNE pin. The
total change (from one extreme to the other) in effective
loading capacitance is ??? nominal.
W hen using a crystal with a VCXO, it is im portant that th e
crystal load capacitance (as specified in Table 4: Oper-
ating Conditions be matched to the load capacitance as
presented by the VCXO. The crystal must be specified
with the correct load capacitance to obtain the maximum
tuning range.
The oscillator operates the crystal resonator in the paral-
lel-reso nant mode. Cr ystal warpin g, or the “pul ling” of the
crystal oscillation frequency, is accomplished by altering
the eff ective load ca pacitance presented to the crystal b y
the oscillator circuit. T he actual amount that changin g the
load capacitance alters the oscillator frequency will be
dependent o n the charac teristics of the cr ystal as well as
the oscillator circuit itself.
Specifically, the motional capacitance of the cr ystal (usu-
ally referr ed to by cr ystal m anufactur ers as C1), the st atic
capacitance of the crystal (C0), and the load capacitance
(CL) of the oscillator determine the warping capability of
the crystal in the oscillator circuit.
A simple formula to obtain the warping capability of a
crystal oscillator is:
()
()()
CCCC CCC
ppmf LL
LL
1020
6
121
210
)( +×+× ×−×
=∆
where CL1 and CL2 are the two extremes of the applied
load capacitance.
EXAMPLE: A crystal with the following parameters is
used. With C1 = 0.02 pF, C0 = 5pF, CL1 = 10pF, a nd CL2 =
22.66pF, the coarse tuning range is
()
()()
ppm
.
..
f305
105662252 106
106622020 =
+×+× ×−×
=∆ .