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NXP Semiconductors UM10301 PCF2123 User Manual

Page 13

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NXP Semiconductors

UM10301

User Manual PCF85x3, PCA8565 and PCF2123, PCA2125

UM10301_1

© NXP B.V. 2008. All rights reserved.

User manual

Rev. 01 — 23 December 2008

13 of 52

Now in order to determine the value of C

L

resulting from C

IN

, C

OUT

(plus C

T

if mounted)

and C

STRAY

it is necessary to realize that seen from the crystal, C

IN

and C

OUT

are

effectively in series; the 32 kHz signal goes from OSCI through C

IN

to ground, via ground

to C

OUT

and then through C

OUT

to OSCO. In parallel with this series circuit is C

STRAY

. For

the remainder of this discussion, whenever in formulas C

OUT

is written this represents

either the value of C

OUT

only, or in case a trimming capacitor C

T

is present too, the sum of

C

OUT

and C

T

. Now the load capacitance C

L

is given by:

STRAY

OUT

IN

OUT

IN

L

C

C

C

C

C

C

+

+

=

Since C

0

is in parallel with C

L

the total capacitance in parallel with the motional arm

L

1

-C

1

-R

1

is given by

0

C

C

C

C

C

C

C

STRAY

OUT

IN

OUT

IN

PAR

+

+

+

=

The motional arm is a series circuit, which forms a closed circuit because there is a
capacitance C

PAR

connected in parallel to this series circuit. Of course the crystal itself

can’t oscillate stand alone, but the equivalent capacitance C which determines together
with L

1

the resulting resonance frequency is now given by the series circuit of C

PAR

and

C

1

. Thus C is given by

⎪⎭

⎪⎩

+

+

+

+

⎪⎭

⎪⎩

+

+

+

=

0

1

0

1

C

C

C

C

C

C

C

C

C

C

C

C

C

C

C

STRAY

OUT

IN

OUT

IN

STRAY

OUT

IN

OUT

IN

Typical values for crystal parameters are given in Table 4. From these values it is clear
that C

1

is several orders of magnitudes smaller than the other capacitances in this

expression and therefore C

1

dominates. C will be in the order of magnitude of C

1

but it

will be a bit smaller as a result of C

PAR

in series.

With

LC

1

=

ω

and

1

1

1

R

C

Q

=

ω

the resulting resonance frequency and quality

factor can be calculated.

Because C

1

is orders of magnitude smaller than the other capacitances Q can be

approximated by

1

1

1

1

R

C

Q

a

=

ω

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