JN5148 NXP Semiconductors, JN5148 Datasheet - Page 89

• Manufacturer Part Number: JN5148
• Description: The JN5148 is an ultra low power, high performance MCU combined with an IEEE802
• Manufacturer: NXP Semiconductors

B.1.3 Crystal ESR and Required Transconductance
The resistor in the crystal equivalent circuit represents the energy lost. To maintain oscillation, power must be
supplied by the amplifier, but how much? Firstly, the Pi connected capacitors C
apply an impedance transformation to Rm, when viewed from the amplifier. This new value is given by:
The amplifier is a transconductance amplifier, which takes a voltage and produces an output current. The amplifier
together with the capacitors C1 and C2, form a circuit, which provides a negative resistance, when viewed from the
crystal. The value of which is given by:
Where
Derivations of these formulas can be easily found in textbooks.
In order to give quick and reliable oscillator start-up, a common rule of thumb is to set the amplifier negative
resistance to be a minimum of 4 times the effective crystal resistance. This gives
This can be used to give an equation for the required transconductance
Example: Using typical 32MHz crystal parameters of
capacitance of 9pF), the equation above gives the required transconductance (
typical value for transconductance of 4.3mA/V
The example and equation illustrate the trade-off that exists between the load capacitance and crystal ESR. For
example, a crystal with a higher load capacitance can be used, but the value of max. ESR that can be tolerated is
reduced. Also note, that the circuit sensitivity to external capacitance [ C
Meeting the criteria for start-up is only one aspect of the way these parameters affect performance, they also affect
the time taken during start-up to reach a given, (or full), amplitude. Unfortunately, there is no simple mathematical
model for this, but the trend is the same. Therefore, both a larger load capacitance and larger crystal ESR will give a
longer start-up time, which has the disadvantages of reduced battery life and increased latency.
© NXP Laboratories UK 2011
ω
g
m
is the frequency in rad/s
is the transconductance
g
m
≥
C
T
4
1
R
×
R
m
C
×
NEG
g
R
ω
T
ˆ
m
JN-DS-JN5148-001 1v7
m
2
2
×
[
=
=
C
ω
C
R
S
R
(
2
m
T
m
C
C
=40Ω,
1




T
T
×
C
≥
1
1
×
+
C
S
4
C
g
C
+
C
C
T
R
m
L
C
T
2
T
S
m
2
×
2
=1pF and
L




)




C
ω
+
2
.
1
S
C
C
, C
2
+
T
L
C
2
1
×
] is a square law.
L
C
1
g
C
and C




T
m
2
1
T
) as 2.59mA/V. The JN5148 has a
=
2
C
]
2
2
T
with C
2
=18pF ( for a load
S
from the crystal,
89