APN1005 [SKYWORKS]
A Balanced Wideband VCO for Set-Top TV Tuner Applications; 一个平衡的宽带VCO的机顶盒电视调谐器的应用型号: | APN1005 |
厂家: | SKYWORKS SOLUTIONS INC. |
描述: | A Balanced Wideband VCO for Set-Top TV Tuner Applications |
文件: | 总11页 (文件大小:266K) |
中文: | 中文翻译 | 下载: | 下载PDF数据表文档文件 |
APPLICATION NOTE
APN1005: A Balanced Wideband VCO
for Set-Top TV Tuner Applications
Introduction
VCO Model
Modern set-top TV DBS tuner systems require more channel
coverage, while maintaining competitive prices. This situation
creates tough design goals: to improve performance and simplify
design.
Figure 1 shows the VCO model built for open loop analysis in Libra
Series IV including the SMV1265-011 varactor model.
The circuit schematic in Figure 2 shows a pair of transistors in a
single feedback loop, connected so that collector currents would
be 180° shifted (ideally). A pair of back-to-back connected
SMV1265-011 varactors is used, rather than a single one. This
allows lower capacitance at the high-voltage range, without
changing the tuning ratio. The reason is that, apart from package
capacitance, certain mounting fringing capacitances, though
small, may strongly affect higher frequency margins. The effects
Balanced VCO configuration could be a competitive circuit
solution, since it provides the widest tuning range with practical
circuitry and layout. However, tuning margins would be further
improved by optimizing the varactor manufacturing process.
Skyworks has developed such a process to satisfy the most
ambitious wideband design goals.
of parasitic capacitances were summarized in the model as C
4
In this publication, we will address the design of the balanced-
type voltage control oscillator (VCO) based on the newly
developed varactor SMV1265-011 with the unique set of
capacitance tuning ratios and Q-quality.
and C , valued 0.4 pF each. These values may vary depending on
3
the layout of the board. Varactor DC biasing is provided through
resistors R and R , both 1 k, which may affect the phase noise,
6
8
but eliminate the need for inductive chokes. This minimizes
overall costs and the possibility of parasitic resonances — the
usual cause for frequency instability and spurs.
The phase corrector DC chokes, SRL and SRL , were modeled
1
2
as lossless inductors at 33 nH since their losses are dominated
by the 30 Ω emitter biasing resistors. DC blocking series capaci-
tances (C
and C ) are modeled as an SRC network,
SER2
SER1
including associated parasitics. Their values were optimized to
10 pF providing smooth tuning over the design band.
Skyworks Solutions, Inc. • Phone [781] 376-3000 • Fax [781] 376-3100 • sales@skyworksinc.com • www.skyworksinc.com
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APPLICATION NOTE • APN1005
Figure 1. VCO Model, Including SMV1265-011 Varactor Model
Figure 2. Transistor Pair in Single Feedback Loop
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2
APPLICATION NOTE • APN1005
The pseudo-resonator inductance is formed by microstrip trans-
In the Libra test bench shown in Figure 3 we defined an open
mission line TL , which provides necessary circuit response at
loop gain (Ku = V /V ) as the ratio of voltage phasors at the
2
OUT IN
high frequencies. This has little effect at the lower band due to
the resonator’s dominantly capacitive nature.
input and output ports of an OSCTEST component. Defining the
oscillation point requires the balancing of input (loop) power to
provide zero gain for a zero loop phase shift. Once the oscillation
point is defined, the frequency and output power can be mea-
sured. Use of the OSCTEST2 component for the close loop
analysis is not recommended, since it may fail to converge in
some cases, and doesn’t allow clear insight into the under-
standing of VCO behavior. This property is considered an
advantage of modeling over a purely experimental study.
The function of transmission line TL is both feedback and
1
phase alignment — providing flat power response over the
tuning range.
Power output is supplied from the collectors of X or X through
1
2
the series connected resistance and DC blocking capacitance
SRC and SRC .
2
3
DC biasing for both of the transistors is supplied through a resis-
tive divider R /R /R .
In the default bench shown in Figure 4 the variables used for
more convenient tuning during performance analysis and opti-
mization are listed in a “variables and equations” component.
1
3 2
The NEC NE68119 bipolar transistors were selected to best fit
performances. Note: The circuit is very sensitive to the transistor
choice (in terms of tuning range and stability) due to wide band-
width design requirements.
For the model of NEC NE68119 we used the Gumel Poon model
of Libra IV with the coefficients provided by CEL RF & Microwave
Semiconductors Catalogue,1997-98.
Figure 3. Libra Test Bench
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APPLICATION NOTE • APN1005
Figure 4. Default Bench
SMV1265-011 SPICE Model
Figure 5 shows a SPICE model for the SMV1265-011 varactor
diode, defined for the Libra IV environment, with a description of
the parameters employed.
Figure 5. SMV1265-011 Libra IV SPICE Model
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4
APPLICATION NOTE • APN1005
Parameter
Description
Saturation current (with N, determine the DC characteristics of the diode)
Series resistance
Unit
A
Ω
-
Default
IS
1e-14
R
S
0
N
Emission coefficient (with IS, determines the DC characteristics of the diode)
Transit time
1
TT
S
F
0
C
JO
Zero-bias junction capacitance (with V and M, defines nonlinear junction capacitance of the diode)
0
J
V
J
Junction potential (with V and M, defines nonlinear junction capacitance of the diode)
V
1
J
M
Grading coefficient (with V and M, defines nonlinear junction capacitance of the diode)
-
0.5
J
E
Energy gap (with XTI, helps define the dependence of IS on temperature)
EV
-
1.11
G
XTI
KF
AF
FC
Saturation current temperature exponent (with E , helps define the dependence of IS on temperature)
3
G
Flicker noise coefficient
-
0
Flicker noise exponent
-
1
Forward-bias depletion capacitance coefficient
Reverse breakdown voltage
-
0.5
B
V
Infinity
V
I
Current at reverse breakdown voltage
Recombination current parameter
Emission coefficient for ISR
A
A
-
1e-3
BV
ISR
NR
0
2
IKF
High injection knee current
A
-
Infinity
NBV
IBVL
NBVL
Reverse breakdown ideality factor
Low-level reverse breakdown knee current
Low-level reverse breakdown ideality factor
Nominal ambient temperature at which these model parameters were derived
Flicker noise frequency exponent
1
0
A
-
1
T
NOM
°C
27
1
FFE
Table 1. Silicon Varactor Diode Default Values
Table 1 describes the model parameters. It shows default values
appropriate for silicon varactor diodes which may be used by the
Libra IV simulator.
whole range of the usable varactor voltages is segmented into a
number of subranges each with a unique set of the V , M, C ,
J
JO
and C parameters as given in the Table 2.
P
According to the SPICE model in Figure 4, the varactor capaci-
Voltage Range
(V)
C
V
(V)
C
(pF)
JO
J
P
tance (C ) is a function of the applied reverse DC voltage (V ) and
V
R
(pF)
22.5
21.0
20.0
20.0
M
2.0
25.0
7.3
1.8
may be expressed as follows:
0–2.5
2.5–6.5
6.5–11
11–up
4.00
0.00
0.00
0.90
0.56
C
JO
68.00
14.00
1.85
C =
V
+ C
P
M
V
R
1 +
(
)
V
J
Table 2. Varactor Voltages
This equation is a mathematical expression of the capacitance
characteristic. The model is accurate for abrupt junction varactors
(SMV1400 series); however, the model is less accurate for hyper-
abrupt junction varactors because the coefficients are dependent
on the applied voltage. To make the equation fit the hyperabrupt
performances for the SMV1265-011, a piece-wise approach was
These subranges are made to overlap each other. Thus, if a rea-
sonable RF swing (one that is appropriate in a practical VCO
case) exceeds limits of the subrange, the C function described
V
by the current subrange will still fit in the original curve.
employed. Here the coefficients (V , M, C , and C ) are made
J
JO
P
piece-wise functions of the varactor DC voltage applied. Thus, the
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APPLICATION NOTE • APN1005
100
1.0
0.8
0.6
0.4
0.2
0
2.6
2.4
2.2
2.0
1.8
1.6
1.4
1.2
Approximation
Measured
10
1
RS_PWL
RS Measured
20
0.1
0
5
10
15
20
25
30
0
5
10
15
25
30
Varactor Voltage (V)
Figure 6. SMV1265 Capacitance vs. Voltage
Varactor Voltage (V)
Figure 7. SMV1265 Resistance vs. Voltage
Figure 6 demonstrates the quality of the piece-wise fitting
approach.
Since the epitaxial layer for this kind of hyperabrupt varactor has
relatively high resistivity, the series resistance is strongly depen-
dent on the reverse voltage applied to varactor junction. The
Special consideration was given to the fit at the lowest capaci-
tance range (high-voltage area) since it dramatically affects the
upper frequency limit of the VCO.
value of series resistance (R ) measured at 500 MHz is shown in
S
Figure 7, with a piece-wise approximation of R also given.
S
The piece-wise function may be used as follows:
To incorporate this function into Libra, the pwl() built-in function
was used in the “variables” component of the schematic bench.
R = pwl (V 0 2.4 3 2.4 4 2.3 5 2.2 6 2 7 1.85 8 1.76 9
S
VAR
1.7 10 1.65 11 1.61 12 1.5 40 1.5)
M = pwl (V 0 2 2.5 2 2.500009 25 6.5 25 6.50009 7.3 11
VAR
7.3 11.0009 1.8 40 1.8)
Note: The pwl() function in Libra IV is defined for the evaluation of
harmonic balance parameters rather than variables. Therefore,
although series resistance was defined as dependent on reverse
voltage, for harmonic balance it remains parametric and linear.
The same applies to capacitance, which remains the same as in
V = pwl (V 0 4 2.5 4 2.500009 68 6.5 68 6.50009 14 11
J
VAR
14 11.0009 1.85 40 1.85)
C = pwl (V 0 0 2.5 0 2.500009 0 6.5 0 6.50009 0.9 11
P
VAR
0.9 11.0009 0.56 40 0.56)
the original diode model, but its coefficients (V , M, C , and C )
J
JO
P
C
JO
= pwl (V 0 22.5 2.5 22.5 2.500009 21 6.5 21 6.50009
become parametric functions of the reverse voltage.
VAR
20 11 20 11.0009 20 40 20)*1012
Note: While C is given in picofarads, C is given in farads to
P
GO
comply with the default nominations in Libra. (For more details
regarding pwl() function see Circuit Network Items, Variables and
Equations, Series IV Manuals, p. 19–15).
Skyworks Solutions, Inc. • Phone [781] 376-3000 • Fax [781] 376-3100 • sales@skyworksinc.com • www.skyworksinc.com
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APPLICATION NOTE • APN1005
VCO Design and Performance
Figure 8 shows the VCO schematic.
R10
2.4k
VCC1
5-8 V
R3
C6
1000
R6
820
120
C4
100
R4
120
R7
51
R5
R8
1k
820
C5
100
T1
16 x 0.4 mm
V1
V2
NE68119
NE68119
R1
R2
L2
L1
R12
50
33
33 33 nH
33 nH
A
C2
10
C1
10
T2
15 x 0.7 mm
D2
D1
T3
R9
1k
SMV1265
SMV1265
3 X 0.7 mm
R11
1000
VVAR1
C3
100
Figure 8. VCO Schematic
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200314 Rev. A • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • July 21, 2005
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APPLICATION NOTE • APN1005
Table 3 shows the bill of materials used.
Figure 9 shows the PCB layout. The board is made of standard FR4
material 30 mils thick.
Designators
Comment
Footprint
0603
The results measured with the circuit in Figure 8, as well as the
simulated results obtained with the model in Figure 9, are shown
in Figures 10 and 11.
C
C
C
C
C
C
C
D
D
0603AU100JAT9 (AVX)
0603AU100JAT9 (AVX)
0603AU101JAT9 (AVX)
0603AU101JAT9 (AVX)
0603AU101JAT9 (AVX)
0603AU102JAT9 (AVX)
0603AU102JAT9 (AVX)
SMV1265-011 (Skyworks)
SMV1265-011 (Skyworks)
LL1608-F33NJ (TOKO)
LL1608-F33NJ (TOKO)
CR10-330J-T (AVX)
CR10-242J-T (AVX)
CR10-102J-T (AVX)
CR10-330J-T (AVX)
CR10-121J-T (AVX)
CR10-121J-T (AVX)
CR10-821J-T (AVX)
CR10-821J-T (AVX)
CR10-510J-T (AVX)
CR10-102J-T (AVX)
CR10-102J-T (AVX)
NE68119 (NEC)
1
2
3
4
5
6
6
1
2
1
2
0603
0603
Note: The simulated tuning curve in Figure 10 agrees with mea-
sured data, which proves the effectiveness of the above piece-wise
approximation technique.
0603
0603
0603
Note: In the middle of the tuning range there is disagreement
between our model and the measured results. This could be attrib-
uted to the imperfection of the model, which is highly sensitive to
the way different parasitic effects are treated. The other problem of
modeling this oscillator case was the convergence of the harmonic
balance. To facilitate convergence in this case, we kept the number
of harmonics to at least five. The sweeping frequency range is rec-
ommended to keep as close to the oscillation point as possible —
especially when analyzing the middle band area.
0603
SOD-323
SOD-323
0603
L
L
0603
R
1
0603
R
10
R
11
0603
0603
R
0603
2
3
4
5
6
7
8
9
1
2
In Figure 11, the power response modeled at 7 V was very close to
the measurement. Higher measured power is attributed to the ana-
lyzer calibration (the calibration error of the analyzer is known to be
within a couple of decibels). The general trend of the simulated
results reflects the real VCO response almost exactly, which clearly
demonstrates the model’s effectiveness.
R
0603
R
R
R
R
R
R
0603
0603
0603
0603
0603
0603
V
V
SOT-416
SOT-416
NE68119 (NEC)
Table 3. Bill of Materials
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APPLICATION NOTE • APN1005
Figure 9. PCB Layout
8
6
Measured
2.2
2.0
1.8
1.6
1.4
1.2
1.0
0.8
Measured @ 7 V
Simulated @ 7 V
4
2
Simulations
0
-2
-4
-6
-8
Measured @ 5 V
0
5
10
15
20
25
30
0
5
10
15
20
25
30
Varactor Voltage (V)
Figure 11. Power Response
Varactor Voltage (V)
Figure 10. Frequency Tuning
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200314 Rev. A • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • July 21, 2005
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APPLICATION NOTE • APN1005
Table 4 shows the measurement data and shows a useful tuning range
of 0.84–2.23 GHz for the applied varactor voltage from 1–27 V.
List of Available Documents
1. Balanced Wideband VCO Simulation Project Files for Libra IV.
2. Balanced Wideband VCO Circuit Schematic and PCB Layout for
Protel EDA Client, 1998 version.
V
Frequency
(GHz)
0.788
0.842
0.91
P
OUT
@ 7 V
P
OUT
@ 5 V
VAR
(V)
0
(dBm)
(dBm)
3. Balanced Wideband VCO Gerber Photo-plot Files
4. Detailed measurement and simulation data.
3.5
3.7
3.7
4.8
6.5
6.4
6
-8.3
-7.6
-6.1
-2.8
1
1
For the availability of the listed materials, please call our applica-
tions engineering staff.
2
4
1.144
1.492
1.714
1.848
1.946
2.016
2.066
2.106
2.134
2.198
2.225
2.238
© Skyworks Solutions, Inc., 1999. All rights reserved.
6
8
1.8
10
12
14
16
18
20
25
28
30
1.2
5.2
4.8
4.4
4.3
4.4
3.7
3.5
3.4
-0.1
-0.9
-1.5
-1.8
-2.4
-3.3
-3.7
-4
Table 4. Tabulated Measurement Data
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APPLICATION NOTE • APN1005
Copyright © 2002, 2003, 2004, 2005, Skyworks Solutions, Inc. All Rights Reserved.
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information contained herein. Skyworks may change its documentation, products, services, specifications or product descriptions at any time, without notice. Skyworks makes no commitment to
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Skyworks Solutions, Inc. • Phone [781] 376-3000 • Fax [781] 376-3100 • sales@skyworksinc.com • www.skyworksinc.com
200314 Rev. A • Skyworks Proprietary Information • Products and Product Information are Subject to Change Without Notice. • July 21, 2005
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