IPC-TM-650 EN 2022 试验方法.pdf - 第437页
Height of base plate from step to top edge Height of clamp block and specimen Height from launcher body to resonator center line Width of clamp block and specimen Horizontal center line distance between probe lines Probe…

The
test pattern card shall have a permittivity equal to the
nominal value of the type being tested with a tolerance of ±
2.5% of the nominal value (measured by stacking sufficient
plies to the total thickness requirement of a specimen as
above. Use a photo resist and etching method capable of
reproducing circuit dimensions with ± 0.025 mm tolerance. All
copper shall be removed from the other side of the test pat-
tern card. See 9.7, Note, for special treatment of ceramic-
PTFE substrate types.
The pattern card of Figure 4 is 68.6 mm wide by 55.4 mm
high and is designed for the fixture hardware in Figure 5
through Figure 14. The length is cut so that when the pattern
card is clamped for the lap joint with the striplines on the base
card, the resonator is centered in the 51 mm high area above
the base plates of the fixture. For materials with permittivity
values higher than the nominal 2.50 shown in Table 1, please
see 5.2 for a discussion of recommended fixture modifica-
tions.
Probe line widths are based on ground plane spacing taken
as twice the nominal thickness of the two specimens plus
thickness of the pattern card and its 0.034 mm copper foil
pattern and computed as if the stripline were centered
between ground planes
(1,3)
.
Chamfer
values are based on published design curves
(2)
.
The
length of the four node resonator is given in Table 1.
Resonators of lower node values for the purpose of measur-
ing ∆L according to 6.1, will be proportionately shorter with
the probe lengths modified so that the gap is the same.
The values for conductor loss, 1/Q
c
,
in Table 1 are calculated
from known properties of copper, the test frequency, the cal-
culated characteristic impedance of the section of stripline
comprising the resonator, and its cross-sectional geometry
using published formulas
(1)
.
The values shown are usually
biased low giving a high bias to loss tangent results, because
conductor actually used may not have a smooth surface and
may include oxides, microvoids, or other sources of higher
resistivity.
5.2
Fixture Modifications for High Permittivity Materi-
als
Modification
of the fixture design of Figure 5 through Fig-
ure 14 and pattern card dimensions in Figure 4 are recom-
mended to overcome problems experienced with extraneous
transmissions and resonances at frequencies near the desired
resonant peak.
5.2.1 Replace
the coax-stripline launcher shown in Figure 7.
The part suggested has a tab width of 1.27 mm and may be
replaced with Omni-Spectra Part No. 2070-5029-02, or
equivalent, intended for 1.57 mm ground plane spacing and
with a tab width of 0.635 mm. A further acceptable alternative
is to redesign the base plates to accept another type of
coaxial fitting such as a flange mount jack, which can be
modified to provide a smooth, low-reflection transition from
3.0 mm semirigid cable with Z
0
=
50 Ohm, low permittivity
insulation into stripline with Z
0
=
50 Ohm, and high permittiv-
ity insulation in the fixture.
5.2.2
If
the stripline launcher in 5.2.1 is used, the edge at
the step to accommodate the launcher body on the base
plate should be machined with a slight undercut for an acute
included angle of about 80°. This, combined with a means to
press the launcher body axially against the edge, will assure a
well-defined ground connection from coax to stripline. A
poorly defined ground connection with ground current path
length varying or longer than that of the signal conductor has
been found to give rise to scattering, reflections, and reso-
nances in the open ended probe line that are evident as extra-
neous fixture transmissions that may distort the resonant peak
to be measured.
5.2.3
Omit
the conductor lap joints but keep the extended
base cards in the fixture assembly. See figures 13 and 14.
With high permittivity materials, the lap joint also gives rise to
unwanted scattering, reflections, and resonances in the open-
ended probe line, as discussed in 5.2.2. For this purpose the
resonator pattern card will have a longer vertical dimension to
extend down to the launcher pin replacing the spacer board
in Figure 13. It should still center the resonator in the clamp-
ing block area. The base dielectric boards will be etched free
of metal. The ground plane foils will also extend down to the
launcher.
The feature of extending the base dielectric boards upward
above the base plates is to be retained as a means to prevent
premature damage to the resonator pattern card with
repeated loading and unloading of the fixture. The base plate
with the deeper step will be on the side toward which the
resonator pattern faces to avoid straining the offset launcher
tab during assembly.
5.2.4
Scale
down the fixture dimensions to move remaining
probe line resonances away from the resonant frequency of
interest. For ε
r
=
10.5 material, the following dimensions were
found effective.
IPC-TM-650
Number
2.5.5.5
Subject
Stripline
Test for Permittivity and Loss Tangent (Dielectric Constant
and Dissipation Factor) at X-Band
Date
3/98
Revision
C
P
age4of25
电子技术应用 www.ChinaAET.com

Height
of base plate from step to top edge
Height of clamp block and specimen
Height from launcher body to resonator
center line
Width of clamp block and specimen
Horizontal center line distance between
probe lines
Probe length from launch to gap
mm
8.53
25.4
21.23
55.9
30.5
25.81
5.2.5 Thinner
copper cladding (weight Q) for the resonator
pattern card is recommended as mentioned in 5.1. If weight
Q is used, the embedding process discussed in note 9.7 can
be avoided. Experience has indicated that this reduction in
thickness has not impaired the loss tangent values obtained
by the method.
5.3
Older Fixture Design
An
older acceptable alternate
test fixture design is shown in Figure 15. This is included since
fixtures of this type are in service at various laboratories. Com-
pared to 5.1, fixtures of this design depend on ambient con-
ditions for temperature control. Changing resonator test pat-
tern cards is less convenient.
5.4
Temperature Control
It
is a well-known fact that PTFE
and composites containing it show a room temperature tran-
sition in the crystalline structure that produces a step-like
change in the permittivity. This temperature region should be
avoided.
Normally, control of ambient temperature is adequate for rou-
tine measurements. A means other than ambient temperature
to control fixture temperature facilitates collecting data on the
variation of permittivity with temperature. With the test fixture
of 5.1., use 6 mm inside diameter tubing for circulating fluid to
control temperature. The following items are needed to com-
plete the temperature control system.
5.4.1
Laboratory
Immersion Heating Bath/Circulator, such
as Haake Model D1, Lauda Model MT, or equivalent and a
small capacity bath. The Immersion Heating Bath/Circulator
shall be connected to the clamping blocks in series with a
return line to the bath.
5.4.2
Two
fine diameter thermocouple probes with leads
and suitable instrumentation for readout or recording of tem-
perature. A digital thermometer, such as Ohmega Model DSS
115 or equivalent, is used for monitoring temperature.
6.0
Measuring Procedure
6.1 Preparation for Testing
The
actual length of the reso-
nator element shall be determined by an optical comparator or
other means capable of accuracy to 0.005 mm or smaller.
Unless otherwise specified, specimens shall be stored before
testing at 23°C + 1-5°C/50% ± 5% relative humidity (RH). The
referee minimum storage time is 16 hours. Shorter times may
be used if they can be shown to yield equivalent test results.
If electronic equipment, as listed in 4.2, is used, it shall be
turned on at least one half hour before use to allow warm-up
and stabilization. The automatic frequency counter listed in
4.2 is provided with temperature control of the clock crystal
that operates even when the power switch is off. Care should
T
able 1 Dimensions for Stripline Test Pattern Cards in Millimeters
Nom. ε
r
Nom.
Thk.
Pattern
Card
Thk.
Probe
Width
Chamfer
X, Y
Probe
Gap
Resonator
Width
Resonator
Length 4
Node
1/Q
C
Conductor
Loss
2.20
1.59 0.22 2.74 3.05 2.54 6.35 38.1 0.00055
2.33 1.59 0.22 2.67 2.92 2.54 6.35 38.1 0.00055
2.50 1.59 0.22 2.49 2.79 2.54 6.35 38.1 0.00055
3.0 1.59 0.22 2.13 2.41 2.54 5.08 31.8 0.00058
3.5 1.59 0.22 1.85 2.16 2.54 5.08 31.8 0.00058
4.0 1.59 0.22 1.62 1.93 2.54 5.08 31.8 0.00058
4.5 1.59 0.22 1.45 1.73 2.54 5.08 31.8 0.00058
6.0 1.59 0.22 1.07 1.30 2.29 3.81 25.4 0.00062
6.0 1.27 0.22 0.86 1.07 2.29 3.81 25.4 0.00072
10.5 1.27 0.22 0.41 0.54 2.03 2.54 17.3 0.00079
Standard
clamp force for all the above is 4.45 ± 0.22 kN
IPC-TM-650
Number
2.5.5.5
Subject
Stripline
Test for Permittivity and Loss Tangent (Dielectric Constant
and Dissipation Factor) at X-Band
Date
3/98
Revision
C
P
age5of25
电子技术应用 www.ChinaAET.com

be
taken to assure that power is continuously supplied to this
unit to avoid a longer warm-up time. Other equipment using
vacuum tube devices will require a longer warm-up time as
specified in the manufacturer’s literature.
The temperature of the test fixture shall be in the range of
22°C to 24°C, unless otherwise specified. If this standard
temperature is to be used and the temperature of the fixture
is to be controlled by the ambient conditions in the testing
laboratory, then the laboratory shall be maintained at 22°C to
24°C and the fixture shall be stored in the laboratory for at
least 24 hours prior to use.
If non-standard temperature is specified and the fixture of 4.1
is used with the temperature control apparatus described in
4.2, then the rest of this paragraph applies. Prior to making
electrical measurements, the circulator is started and adjusted
to within 1°C of the desired test temperature. The time
required for stabilization depends on the specific temperature
control apparatus in use, the size of the circulation bath tank,
and the temperature selected. Additional stabilization time will
be required for each specimen to come to the set temperature
after it has been clamped in the fixture.
The test fixture containing the test specimens shall be placed
in the clamping fixture and the specified force of 4.45 ± 0.22
kN is applied through the calibrated force gauge to the 1290
mm
2
area
centered directly over the resonant circuit as shown
in the assembly of Figure 12, Figure 13, or Figure 15.
6.2
Manual Measurement of the Specimen
The
follow-
ing procedure is applicable where equipment as described in
4.1 is available. The equipment of 4.2 could also be operated
manually. The stripline resonator formed by the fixture pattern
card and ground planes with the specimen cards inserted is
referred to as a cavity. The sweep oscillator is referred to here
as the sweeper.
6.2.1
Determination of Cavity Resonant Frequency
The
resonant
frequency of the circuit shall be found by scanning
the sweeper over the expected transmission range of the test
resonator. The sweeper shall be precisely adjusted to the fre-
quency that produces a maximum reading of the SWR Meter
No. 1. The frequency meter shall then be adjusted for a mini-
mum reading of the SWR Meter No. 2. Record the resonant
frequency. The input selector of the SWR Meter No. 1 should
be set for low impedance input for proper square law detec-
tion.
6.2.2
Determination of Cavity Half-Power Points
With
the
incident signal having been set to maximum resonator
transmission, adjust the gain of the SWR Meter No. 1 until the
meter reads 0 dB. The frequency of the sweeper shall then be
adjusted to give 3 dB readings both above and below the
maximum transmission frequency. Measure each frequency
with the frequency meter and record the results:
• f1: above the maximum transmission frequency
• f2: below the maximum transmission frequency
6.3
Automated Measurement of the Specimen
For
an
automated system to be used in performing the measure-
ment, computer software is needed that will collect paired
values of frequency and transmitted power. From this data,
the frequency for maximum power transmission and the fre-
quencies of the half power points are determined. The com-
puter program may optionally include computation of permit-
tivity and loss tangent as described in 7.0. Results and
collected data may be displayed on the screen, stored in a
disk file, sent to a printer, or any combination of these.
In one possible mode of operation with the equipment
described in 4.2, the following sequence of steps is performed
as many times as necessary to get enough data to complete
the test procedure. The computer is designated as the con-
troller on the GPIB.
6.3.1
The
computer sets the sweeper to a selected carrier
wave frequency without an AM or FM audio signal to a desired
output power level, such as 10 dBm.
6.3.2
The
same frequency is given to the synchronizer with
instructions to lock the frequency of the sweeper to the speci-
fied value.
6.3.3
The
computer checks the synchronizer for status until
the status value drops to zero, indicating the frequency is
locked.
6.3.4
The
power meter reading is obtained by the computer.
Since it takes a finite amount of time for the power sensor to
stabilize, either a delay is used or the reading may be taken
repeatedly until consecutive readings meet a given require-
ment for stability.
6.4
Use of the Network Analyzer for Measurement of
the Specimen
An
automated network analyzer may be
used either by operating the front panel controls manually or
under computer control with suitable specialized software.
The fixture with the specimen is connected by test cables and
adapters as a device under test. Set up the instrument so the
IPC-TM-650
Number
2.5.5.5
Subject
Stripline
Test for Permittivity and Loss Tangent (Dielectric Constant
and Dissipation Factor) at X-Band
Date
3/98
Revision
C
P
age6of25
电子技术应用 www.ChinaAET.com