common time division systems
(e.g. GSM/EDGE, DECT)
◆ Handling of external components
through Γ and s-parameter correction
◆ Simultaneous operation of up to
4 sensors on basic unit
◆ Operation of sensor directly from PC
via USB interface
◆ 2-year calibration cycle
Ready for a wide variety of applications
The RF and microwave Power Meter
Designed for R&D
R&S NRP is always the right choice:
It is ideal for daily use in research and
development, production or mobile
service, not to mention when analyzing
broadband modulation signals of thirdgeneration mobile radio. The versatility
of the novel R&S NRP power meter
series is primarily due to the newly
developed sensors in
. These sensors are intelligent standalone instruments that communicate with the
basic unit or a PC via a digital interface.
The , now
implemented for the first time, sets
Top measurement accuracy plus a
dynamic range of 90 dB for broadband
signals of any modulation are the most
requested characteristics of a modern
power meter. The versatile R&S NRP
sensors in
feature exactly these characteristics and
are a priceless investment if you wish to
meet future requirements such as the
broadband modulation types of thirdgeneration mobile radio. In addition, they
are also capable of handling the RF bandwidths beyond 100 MHz that are already
under discussion for wireless LAN.
new standards in terms of universality
and accuracy. The R&S NRP basic unit
offers exactly what you expect for
today’s needs: compact size, intuitive
user interface and multichannel capability.
A power meter must of course be easy to
operate: The numerous sensor functions
can be activated via an intuitive user
interface, and the high-resolution display
indicates up to 4 measurement results at
a time. As with other power meters from
Rohde&Schwarz, all calibration data is
stored in the sensor, which ensures highprecision measurements by minimizing
operating errors.
Sensor connectors on front
panel, channel B: option
R&S NRP-B2
Built-in test generator
(option R&S NRP-B1)
Display of up to
4 measurement
results
Softkeys and window-oriented
menu technique
Power sensor in
with 90 dB dynamic range
Function keys for fast access to
important functions
2 Power Meter R&S NRP
Ideal for production
S
n
Mobile use
For any type of test signal:
If you have ever dealt with microwave
power measurements, you know that the
necessary filtering of results due to the
noise characteristics of the sensor as well
as delays in measurement range selection and command/result processing can
have negative effects on throughput in
production. And this is where the R&S
NRP with its innovative features offers
straightforward solutions:
◆ Autofilter
◆ Parallel processing
◆ Speed
It goes without saying that the basic unit,
which can accommodate up to 4 sensors
at the same time, can be fully remotecontrolled. In addition, the sensors can
directly be connected to a PC. It is good to
know that the sensors can perform reliable measurements for an extended
period of time owing to the long calibration interval of 2 years.
The handy, lightweight and sturdy instrument, which can also be powered from
the optional battery for several hours,
makes mobile use a pleasure. With an
operating temperature range from 0°C to
50°C, the Power Meter R&S NRP can be
used under almost any conditions.
allows every
R&S NRP sensor to be operated directly
from a PC, making it the smallest and
most lightweight microwave measuring
instrument available.
Microwave power meters have historically required a multitude of different
sensors to cover all applications. Thermal
sensors, diode sensors as well as peak
power sensors were used to handle the
various measurement tasks. The sensors
of the R&S NRP family now make life
much easier – in many cases, a single
sensor can perform all necessary measurements (see table 1).
Table 1: Sensor technologies and their applications
Application ↓Sensor → Thermoelectric sensor Diode sensor (CW) Peak p ower sensor Sensor in
Average power
Burst power––––
Time gating––––
Signal with extremely high bandwidth ––
Measurement over wide dynamic range ––
optimal possible–– not possible
Summary
◆ One power sensor
◆ 90 dB dynamic range
◆ CW and broadband-modulated signals
◆ Time-gating applications
◆ High measurement accuracy and speed
ensor i
Power Meter R&S NRP3
High system accuracy through
Plug in and measure
The accuracy of microwave power measurements essentially depends on the
characteristics of the sensor, but it is
impossible to eliminate level, temperature and frequency influences by traditional means. Rohde&Schwarz solved
this problem years ago by introducing a
novel approach: Measure the deviations
of each manufactured sensor from the
ideal characteristics and then store the
values in the sensor as a data record. This
means that you do not have to bother
with calibration data. Instead, you simply
plug in the sensor and start the measurement, which is a significant advantage in
day-to-day work.
Precise calibration
High measurement accuracy –
even with modulated signals
Benefitting from all the factors described
above, Rohde& Schwarz broadband
power meters have a very low measurement uncertainty, which is still the decisive argument in their favour. In the past,
however, the data sheet specifications of
about 2% (0.09 dB) could seldom be
achieved in practice. This was due to error
sources associated with the test signal or
external circuitry: harmonics and nonharmonics, modulation, mismatch of the
source, and the influence of attenuators
and directional couplers connected
ahead of the sensor for level matching.
The R&S NRP sensors represent a big step
forward in solving these problems. The
concept of
(see page 5) comprises an entire series of
measures intended to make the sensors
similar to thermal sensors in behaviour.
This includes very accurate measurement
of average power, regardless of modulation (FIG 1), as well as high immunity to
incorrect weighting of harmonics, spurious and other interference signals. The
maximum speed of 1500 measurements
per second (in buffered mode, measurement interval 2 x 100 µs) nevertheless
equals that of diode sensors.
A power sensor can only be as good as
the measuring instruments used to calibrate it. This is why the standards
employed by Rohde& Schwarz are directly
traceable to the power standards of the
German Standards Laboratory (PTB).
0.2
0.15
0.1
0.05
Error in dB
0
–0.05
–0.1
–0.15
–0.2
–60–300–10–50–20–402010
Power level in dBm
FIG 1: Modulation-related errors of an R&S NRP-Z11 or R&S NRP-Z21 power sensor for a 3GPP test
signal (test model 1-64) compared to a CW signal of the same magnitude.
Red: default setting; yellow: transition area between measurement paths shifted by –6 dB;
light blue: uncertainty caused by noise (modulation effect below –30 dBm negligible).
4 Power Meter R&S NRP
The Power Sensors R&S NRP-Z11 and R&S NRP-Z21 fuse
multiple-path architecture, multiple-diode technology and a
simultaneously scanning multichannel measurement system
into a unique high-performance concept.
Multiple-path architecture is the combination of two or three
diode detectors to obtain a large dynamic range for modulated signals. This is achieved by operating each detector
exclusively in the square-law region and by using only the
optimally driven detectors for the measurement.
Multiple diodes comprise several zero-bias Schottky diodes
connected in series and integrated on one chip. When used
in an RF detector, they expand its square-law region, because
the measurement voltage is split among several diodes – so
that each one is driven less – while at the same time the
detected voltages of the individual diodes are added together.
Rohde&Schwarz's multiple-path architecture (patent
pending) is characterized by the following features (FIG 2):
◆ 3 signal paths, each fitted with triple diodes
◆ 6 dB wide overlap ranges, smooth transitions
◆ Simultaneous scanning and analysis
◆ Chopper stabilization of signal paths for recurring signals
The advantages over conventional technology are obvious:
high signal/noise ratio throughout, low modulation effect,
negligible delays and discontinuities when switching signal
paths, as well as the ability to perform a time-domain analysis of the test signal within the available video bandwidth.
As a consequence, these sensors not only compete with peak
power meters – they are indeed superior in two respects:
◆ No restrictions on the RF bandwidth of the test signal
◆ Wider dynamic range
As a result, it is already possible today to analyze extremely
broadband signals, such as are planned for wireless LAN or
will be created by combining several carriers in accordance
with 3GPP.
A
14 dB
–19 dBm to +7 dBm
P
i
–67 dBm to –13 dBm
34 dB
+1 dBm to +23 dBm
Chopper
FIG 2: Sensor architecture in R&S NRP-Z11 and R&S NRP-Z21.
D
A
D
A
D
Error
correction
Weighting
External trigger
Power Meter R&S NRP5
Power Meter R&S NRP5
+
P
m
Power measurement without external influences
Γ correction – accounting for
the source mismatch
The most important source of error in
power measurements on RF and microwave signals is the mismatch of source
and sensor. Due to reflections that cannot
be eliminated, it is not the nominal power
of the source that is transmitted to
P
GZ0
the power sensor, but the power P
that deviates to a certain extent from the
nominal value. To minimize the influence
of mismatched sources, the standing
wave ratio (SWR) at the sensor end was
reduced to the extent technically feasible
(1.11). However, asignal source with an
SWR of 2, for example, still leads to an
additional uncertainty of the measurement result of ±3.5% (0.15 dB). Although
this error normally is decisive for total
measurement uncertainty, it was frequently not taken into account because it
could not be specified for the sensor
alone.
Here the R&S NRP sensors boast another
innovation: To reduce the mismatch, the
complex reflection coefficient of the
source is transmitted to the sensor via the
USB data interface, and the sensor corrects the matching error by means of
Γ correction, taking into consideration its
own low impedance mismatch. This
approach yields a measurement result of
significantly higher precision.
(FIG 3)
i
P
GZ0
G
≠ 0Γ
Γ
L
Source
FIG 3: Γ correction function: By taking into account the complex reflection coefficient ΓG of the source,
the measurement result (P
displayed.
) is corrected in such a way that the nominal power of the source P
i
≠ 0
G
P
i
Power Sensor
R&S NRP-Z11/-Z21
is
GZ0
S-parameter correction –
accounting for additional
components
A similar mismatch problem is encountered in test setups where the sensor
cannot be connected directly to the
source to be measured. Especially in production facilities, it is often necessary to
connect a cable or an attenuator for level
matching. In this case, the interactions
between three components must be
taken into account – a non-trivial bit of
mathematics involving complex numbers.
Here, too, the R&S NRP offers a straightforward, standardized solution to the
user. With the help of a small software
tool that runs on any PC, the complete
s-parameter data set of the twoport connected ahead can be loaded into the sensor's memory via the USB data interface.
The data format required (s2p/Touchstone) is provided by any vector network
analyzer.
After the source's complex reflection
coefficient has been transmitted (optionally), a perfectly corrected reading is
obtained; the sensor practically behaves
as if it were connected directly to the
source (FIG 4).
6 Power Meter R&S NRP
P
GZ0
G
Source
FIG 4: Shifting the measurement plane from 1 to 2 by means of s-parameter correction. The influence
of the additional component is compensated for, so that the nominal power P
sured.
Plane 2Plane 1
Attenuator
Measured
s-parameters
P
i
Power Sensor
R&S NRP-Z21
of the source is mea-
GZ0
Throughput is essential in production
New autofilter function –
averaging made simple
The setting of the display filter is essential
for the measurement speed that can be
attained. As a rule, noise is superimposed
on the signal to be measured. The relative
noise content increases as power
decreases. To obtain a noise-reduced
display, an averaging factor has to be
selected for low signal levels, but such a
factor increases the measurement time.
Therefore a compromise must be made
between sufficient signal/noise ratio and
acceptable measurement time. The following rule of thumb applies: Reducing
the noise by a factor of 10 increases the
measurement time by a factor of 100.
With the classic autofilter function, the
averaging factor is, therefore, only
increased gradually, which keeps the
measurement time acceptable but does
not make it possible to maintain a specific
noise level.
The enhanced autofilter function, now
implemented in a power meter for the
first time, mitigates this problem. In addition to the classic autofilter function, a
Fixed Noise mode is available. Using this
mode, the sensor will maintain the userdefined S/N ratio as long as the maximum
measurement time (to be defined by the
user) is not exceeded. Consequently, the
instrument provides stable measurement
results exactly matched to the user’s
needs.
FIG 5: Autofilter menu of the R&S NRP.
Measurement range selection
without delay
Multipath concepts for diode sensors
often have the disadvantage of hard
switching from path A to path B in the
case of level changes, which interrupts
measurement data acquisition and introduces large differential linearity errors.
This disadvantage has been eliminated in
the R&S NRP diode sensors in
owing to
parallel signal processing in the three
paths and soft transitions from one path
to the other.
User-definable measurement
window
Measurements on very low-frequencymodulated signals are typically performed using large averaging factors to
keep the display stable. This, however,
extends the measurement time. The R&S
NRP uses a different approach: The measurement time interval is adapted to the
signal period by means of windowing.
The use of an integer multiple of the
period yields a perfectly stabilized
measurement result.
High measurement speed
All these requirements, i.e. optimum
filtering and fast range selection, must be
met before a power meter can make full
use of its measurement speed under any
conditions. If filtering is not necessary
and the size of the measurement window
is not critical, the R&S NRP excels with its
1500 measurements per second (in
buffered mode, measurement interval
2 x 100 µs).
Power
FIG 6: Parallel signal processing and soft transitions between measurement
paths owing to
Path APath B
1
0
P
x
.
4xPxPower
FIG 7: Windowing technique used on a low-frequency-modulated signal.
Power Meter R&S NRP7
Signal-synchronized measurements
Power
Trigger
event
Measured burst average power
Last falling slope
in the burst
In addition, unwanted power components at the beginning or end of the burst
can be excluded from the displayed result
by using the commands EXCLUDE START
and EXCLUDE END (FIG 8).
Trigger threshold
Time
EXCLUDE START EXCLUDE END
Measurement interval
FIG 8: Modulated burst of an EDGE signal and relevant parameters for measuring burst average power.
Just in time
Automatic burst acquisition and
measurement
The R&S NRP-Z11 and R&S NRP-Z21 sensors can measure the average power not
only in the classic manner, i.e. continuously without temporal reference to the
signal content, but also synchronized
with the signal over definable periods of
time. Power measurements on signal
bursts and within individual timeslots of
time division systems are important applications. A fundamental prerequisite for
signal-synchronized measurements is the
availability of extensive trigger capabilities. The Power Meter R&S NRP can
derive the trigger time from the test
signal (internal triggering) or from an
external trigger signal.
The internal trigger capabilities of the
Power Meter R&S NRP are particularly
useful for burst measurements. Depending on the trigger level previously
defined, the sensor automatically determines the beginning and the end of the
burst. This is even accomplished for modulated bursts by defining of a dropout
parameter, i.e. a minimum signal-off
period that must be detected by the sensor to reliably determine the end of the
burst.
Multislot measurements
This function enables the R&S NRP to
carry out measurements on signals with
complex timeslot structure. Up to 128
intervals (26 when controlled by the basic
unit) can be acquired and measured at
the same time (FIG 9). This allows entire
frames of GSM/EDGE signals to be analyzed. The user can select the number and
the timing of the timeslots relative to the
trigger event; up to 4 results can simultaneously be displayed on the basic unit.
The unwanted portions in the transition
from one timeslot to the next can be
blanked by user-definable exclusion
periods.
The internal trigger capabilities of the
R&S NRP can also be used in this context.
In the case of TDMA signals, using an
external frame trigger is often beneficial
to generate the temporal relation to
timeslot 1. The basic unit is fitted with the
appropriate connector on the rear panel;
if the sensor is operated from a PC,
triggering via the Adapter R&S NRP-Z3 is
possible.
FIG 9: Multislot measurement: for the most
common time division methods (e.g. GSM/EDGE,
DECT), average power can be measured in all
timeslots at the same time.
8 Power Meter R&S NRP
Power
P
P
1
P
2
Exclusion period
P
3
P
4
P
5
P
6
7
Time
P
8
Power/time template
If the R&S NRP-Z sensors are operated
from a PC (see page 10), more in-depth
analysis functions are available. Recurring or non-recurring waveforms can be
displayed as power/time templates
(FIG 10). The number of test intervals
(points) can be increased to 1024; signal
details down to a duration of about 10 µs
can thus be resolved. Extensive trigger
functions, derived from an external
source or the test signal, again ensure
stable conditions.
Outstanding dynamic range
FIG 10: Power/time template of a nonrecurring RF burst for an application
in medical electronics, measured with the R&S NRP-Z11 (LabView application without basic unit; readings in W and ms, no averaging).
In the past, the limited dynamic range of
standard sensor technologies forced
many users to employ sensors of different
sensitivity (nominal power) to handle the
power range of the test items. This was
especially true if average power of modulated signals had to be measured.
achieved, while the lower measurement
limit (defined by noise and zero offset)
remains a very respectable –67 dBm.
With signal-synchronized measurements,
the difference between the new sensors
and previous power sensors is most
evident.
Although conventional multipath sensors
were able to attain respectable values,
their dynamic range was limited to 80 dB,
not to mention the slow response times
and the significant measurement errors in
the transition regions of the individual
For signal-triggered measurements of the
average power of single bursts or the
generation of a power/time template, a
wider dynamic range is available than
with all existing conventional designs.
paths. The R&S NRP-Z11 and R&S
NRP-Z21 are the first sensors with
outstanding values: For the first time, a
dynamic range of 90 dB for broadband
signals of any modulation has been
Table 2: Dynamic range for measuring average power (bandwidth of test signal 100 MHz/5 MHz/0 (CW))
Technology ↓Mode ↓
ContinuousTimeslot
1 out of 8 (external trigger)
Thermoelectric sensor50/50/50 dB–––
Diode:
Sensor in square-law region
Diode: CW sensor43/43/90 dB–––
Diode: Peak sensor33/50/80 dB–/50/57 dB–/33/37 dB–/50/57 dB
Diode: Multiple-path sensor80/80/80 dB–––
43/43/50 dB––
Burst
duty cycle 1:8 (internal trigger)
Power versus time
256 points (external trigger)
–
Diode:
90/90/90 dB85/85/85 dB60/60/60 dB70/70/70 dB
Power Meter R&S NRP9
Sensor with PC interface
P
GZ0
G
USB Adapter
R&S NRP-Z4
Sensor connected directly to the
R&S NRP basic unit
Sensor connected via the passive
USB Adapter R&S NRP-Z4
Source
FIG 11: Three ways of displaying results with an R&S NRP sensor.
Miniature power meter
The sensors of the R&S NRP-Z series can
be used as standalone measuring instruments without the basic unit. In addition
to the power sensor itself, they include a
CPU that controls the sensor, processes
the measurement results and operates
the interface: a complete miniature
power meter. All measurement data and
settings are transmitted via a digital USB
interface. This concept, with which
Power Sensor
R&S NRP-Z21
USB Adapter
R&S NRP-Z3
Trigger signalPower supply
Use on a PC
The most cost-effective method for highprecision power measurements is to connect the sensors directly to a PC, especially if data acquisition and evaluation
take place via a PC. The main area of
application is production, since production environments usually include a process controller. The fact that the basic
unit can be omitted saves space in the
rack and reduces costs.
Rohde&Schwarz already set the pace in
the field of directional power meters, is
now being used for the first time in
classic microwave power measurements.
Sensor connected via the active
USB Adapter R&S NRP-Z3
Service technicians will also appreciate
this option since the power meter fits into
a trouser pocket and can easily be
operated from a laptop.
10 Power Meter R&S NRP
FIG 12: The Power Viewer turns any PC (under Windows98/2000/ME/XP)
into a power meter.
The software toolkit supplied as standard
with every R&S NRP sensor is required in
order to control the R&S NRP power sensors via a PC. The software toolkit comes
with both a DLL (dynamic link library), for
individualized use of the entire sensor
functionality under Windows, and the
Power Viewer, a virtual power meter with
basic measurement functions (subset of
the R&S NRP functionality) for the PC
workstation (FIG 12).
Two adapters are available for connection
to the hardware:
◆ The passive USB Adapter R&S NRP-Z4
provides all basic functions, as it
handles the transmission of settings
and measurement data as well as the
power supply of the sensor.
◆ The active USB Adapter R&S NRP-Z3
has been developed for applications
requiring external triggering of the
power sensor. It also offers a separate
power supply.
Universal basic unit
For applications requiring a basic unit,
the R&S NRP offers everything that is
expected from a modern power meter –
and much more. It is small, lightweight
and rugged, and the optional battery
pack ensures several hours of operation
without line power. Depending on
requirements, it can be fitted with one,
two or four measurement inputs (options
R&S NRP-B2 and R&S NRP-B5).
The IEC/IEEE bus connector is a standard
feature as are the trigger input and the
analog measurement output.
The user interface of the power meter
takes its cue from the PC world: The basic
unit is controlled via menu bars, menus
and dialog boxes, and uses only three
menu levels despite the large number of
functions. The self-explanatory operating
concept makes the R&S NRP a pleasure
to use.
The high-resolution graphical display can
show as many as four measurement
results at the same time. The user can
choose which results to display – either
the data from different sensors (with a
maximum of four connected simultaneously) or from different timeslots of a
TDMA signal measured by means of one
sensor. Even values obtained by calculation, such as SWR or return loss, can be
displayed. For immediate clarity, each
data window can be assigned a specific
name.
FIG 13: The Power Meter R&S NRP can be equipped with one, two or four measurement inputs (two on rear panel, see red frame).
Power Meter R&S NRP11
Specifications
Burst Average function
Power Sensors R&S NRP-Z11/-Z21 (specifications from 8 GHz to
18 GHz apply only to R&S NRP-Z21)
Bold: Parameter 100% tested.
Italics: Uncertainties calculated from the test assembly specifications
and the modelled behaviour of the sensor.
Normal: Compliance with specifications is ensured by the design or
derived from the measurement of related parameters.
Sensor type3-path diode sensor
Measurandaverage power of incident wave or
average power of source into 50 Ω
Frequency range10 MHz to 8 GHz (R&S NRP-Z11)
10 MHz to 18 GHz (R&S NRP-Z21)
Matching (SWR)values in () for temperature range 15°C
to 35°C
10 MHz to <30 MHz
30 MHz to 2.4 GHz
>2.4 GHz to 8.0 GHz
>8.0 GHz to 18.0 GHz
Level-dependent matching change
Measurement error due to harmonics n xf0 of carrier frequency
Values in []: typ. standard uncertainty
n = 3, 5, 7, ...
n = 2, 4, 6, ...
Modulation influence
20)
20)
21)
–30 dBc
–20 dBc
–10 dBc
–30 dBc
–20 dBc
–10 dBc
<0.003 dB [0.0015 dB]
<0.010 dB [0.005 dB]
<0.040 dB [0.015 dB]
<0.001 dB [0.0003 dB]
<0.002 dB [0.001 dB]
<0.010 dB [0.003 dB]
values in []:
User def'd crossover ≤–6 dB
General
measurement errors in subranges are
proportional to power and depend on
CCDF and modulation bandwidth of
test signal
WCDMA (3-GPP Test Model 1-64)
Worst case
–0.02 dB to +0.07 dB [–0.02 dB to
+0.02 dB]
Typ ica l
–0.01 dB to +0.03 dB [–0.01 dB to
+0.01 dB]
Averaging filter
Duration
as specified for the individual measure-
ment functions
Shape
rectangular (integrating behaviour;
available for all measurement func-
tions)
Von Hann (smoothing filter, for effi-
cient suppression of result variations
due to modulation
26)
; only for Continu-
ous Average function)
Measurement times
19)
Continuous Average
Buffered, without averaging
Burst Average
Timeslot, Scope
27)
N x (duration of measurement
7)
+ 0.2 ms) + tz
window
buffer size x (duration of measurement
7)
+ 0.5 ms) + tz
window
(2 to 4) x N x burst period + t
(2 to 4) x N x trigger period + t
tz: <1.6 ms (0.9 ms on average)
z
28)
z
Tr ig ge r in g
Source
Slope (external, internal)
Bus, External, Hold, Immediate, Internal
pos./neg.
Level
Internal
External
–40 dBm to +23 dBm
see specs of R&S NRP and
USB Adapter R&S NRP-Z3
Delay
Holdoff
Hysteresis
–5 ms to +100 s
0 s to 10 s
0 dB to 10 dB
Attenuation correction
Function
correcting the measurement result by
means of a fixed factor (dB offset)
Range
–100.000 dB to +100.000 dB
Modes
AUTO mode
Reference power
Continuous Average
Burst Average
Timeslot
22)
Scope
Normal operating mode
Resolution
Fixed Noise operating mode
Noise content
Max. measurement time
Averaging factor N
Result output
Moving Average
Repeat
AUTO OFF (fixed averaging factor)
AUTO ON (continuously auto-adapted)
AUTO ONCE (automatically fixed once)
S-parameter correction
Function
taking into account a component con-
nected ahead of the sensor by loading
its s-parameter data set into the sensor
non-averaged result in measurement
window
non-averaged result in measurement
Number of frequencies
Parameters
Download
window
non-averaged result in reference
25)
timeslot
non-averaged result at reference
25)
23)
point
setting of filter depends on power to be
measured and resolution
1 (1 dB), 2 (0.1 dB), 3 (0.01 dB),
Γ correction
Function
Parameters
4 (0.001 dB)
filter set to specified noise content
24)
0.0001 dB to 1 dB
0.01 s to 999 s
16
(number of averaged measure-
1 to 2
ment windows)
Download
Frequency response correction
Function
1 to 1000
, s21, s12 and s22 (in s2p format)
s
11
with R&S NRP toolkit (supplied with
sensor) via USB Adapter R&S NRP-Z3
or R&S NRP-Z4
reducing the influence of mismatched
29)
sources
magnitude and phase of reflection
coefficient of source
see under S-parameter correction
taking into account the calibration
factors relevant for the test frequency
continuous with every newly evaluated
measurement window (e.g. in case of
manual operation via R&S NRP)
only final result (e.g. in case of remote
Parameter
Permissible deviation from actual
value
carrier frequency (center frequency)
50 MHz (0.05 x f below 1 GHz) for
specified measurement uncertainty
control of R&S NRP)
Power Meter R&S NRP13
Interface to host
Power supply
+5 V/200 mA typ. (USB high-power
device)
Remote control
as a USB device (function) in full-speed
mode, compatible with USB 1.0/1.1/
2.0 specifications
Trigger input
differential (0/+3.3 V)
Dimensions (W x H x L)48 mm x 31 mm x 170 mm
length incl. connecting cable:
approx. 1.6 m
Weight<0.3 kg
30)
0.175
0.071
0.048
0.164
0.081
0.063
0.184
0.110
0.096
in dB
0.147
0.072
0.056
–40 to –19to+1 to +23
(–67)
0.160
0.096
0.083
–40 to –19to+1 to +23
(–67)
0.188
0.133
0.123
–40 to –19to+1 to +23
(–67)
0.159
0.069
0.047
0.170
0.089
0.072
0.196
0.120
0.103
31)
in dB
0.159
0.069
0.048
0.174
0.097
0.082
0.210
0.142
0.128
0°C to 50 °C
15°C to 35 °C
20°C to 25 °C
dBm
0°C to 50 °C
15°C to 35 °C
20°C to 25 °C
dBm
0°C to 50 °C
15°C to 35 °C
20°C to 25 °C
dBm
Calibration uncertainty
10 MHz to <20 MHz20 MHz to <100 MHz
Path 1Path 2Path 3Path 1Path 2Path 3
0.0560.0470.0480.0560.0470.04720 °C to 25°C
100 MHz to 4 GHz>4 GHz to 8 GHz
Path 1Path 2Path 3Path 1Path 2Path 3
0.0660.0570.0570.0830.0710.07220 °C to 25°C
>8 GHz to 12.4 GHz>12.4 GHz to 18 GHz
Path 1Path 2Path 3Path 1Path 2Path 3
0.0940.0760.0760.1230.0990.09920 °C to 25°C
Uncertainty for absolute power measurements
10 MHz to <20 MHz20 MHz to <100 MHz
0.174
0.075
0.056
–40 to –19to+1 to +23
(–67)
100 MHz to 4 GHz>4 GHz to 8 GHz
0.150
0.081
0.066
–40 to –19to+1 to +23
(–67)
>8 GHz to 12.4 GHz>12.4 GHz to 18 GHz
0.168
0.106
0.094
–40 to –19to+1 to +23
(–67)
0.175
0.070
0.047
0.162
0.077
0.058
0.176
0.096
0.079
Uncertainty for relative power measurements
10 MHz to <20 MHz20 MHz to <100 MHz
+23
0.226
0.229
0.027
0.084
0.080
0.046
+8
±0
–13
–19
–40
+23
+7
+1
–13
–19
–40
+23
+7
+1
–13
–19
–40
0.044
0.226
0.027
0.083
0.022
0.045
0.022
0.023
0.226
0.022
0.083
0.022
0.045
–40 –19 /–13 ±0 /+8 +23
Power level in dBm
100 MHz to 4 GHz>4 GHz to 8 GHz
0.209
0.218
0.088
0.085
0.055
0.047
0.206
0.028
0.083
0.022
0.048
0.022
0.023
0.206
0.022
0.083
0.022
0.048
–40 –19 /–13 +1 /+7 +23
Power level in dBm
>8 GHz to 12.4 GHz>12.4 GHz to 18 GHz
0.224
0.231
0.111
0.106
0.084
0.077
0.216
0.034
0.096
0.027
0.063
0.025
0.024
0.216
0.022
0.096
0.022
0.063
–40 –19 /–13 +1 /+7 +23
Power level in dBm
0.206
0.022
0.082
0.022
0.046
0.229
0.205
0.080
0.081
0.044
0.044
0.226
0.023
0.084
0.022
0.046
0.022
–40 –19 /–13 +1 /+7 +23
Power level in dBm
0.031
0.215
0.032
0.097
0.038
0.066
0.218
0.210
0.085
0.088
0.047
0.054
0.209
0.024
0.088
0.022
0.055
0.022
–40 –19 /–13 +1 /+7 +23
Power level in dBm
0.064
0.244
0.061
0.135
0.060
0.110
0.231
0.230
0.106
0.112
0.077
0.079
0.224
0.024
0.111
0.022
0.084
0.022
–40 –19 /–13 +1 /+7 +23
Power level in dBm
32)33)
0.215
0.078
0.044
0.027
0.022
0.022
0.205
0.081
0.044
0.233
0.093
0.059
0.030
0.022
0.022
0.210
0.088
0.054
0.245
0.128
0.102
0.040
0.034
0.033
0.230
0.112
0.079
in dB
0.027
0.022
0.022
0.215
0.078
0.044
0.206
0.082
0.046
0.049
0.044
0.043
0.218
0.085
0.047
0.215
0.097
0.066
0.086
0.084
0.083
0.245
0.128
0.102
0.244
0.135
0.110
0°C to 50 °C
15°C to 35 °C
20°C to 25 °C
0°C to 50 °C
15°C to 35 °C
20°C to 25 °C
0°C to 50 °C
15°C to 35 °C
20°C to 25 °C
0°C to 50 °C
15°C to 35 °C
20°C to 25 °C
0°C to 50 °C
15°C to 35 °C
20°C to 25 °C
0°C to 50 °C
15°C to 35 °C
20°C to 25 °C
0°C to 50 °C
15°C to 35 °C
20°C to 25 °C
0°C to 50 °C
15°C to 35 °C
20°C to 25 °C
0°C to 50 °C
15°C to 35 °C
20°C to 25 °C
14 Power Meter R&S NRP
Accessories for sensors
R&S NRP-Z2
Extension cablefor connecting the sensor to the basic
Length
Model .05
Model .10
Total length incl. sensor cable5 m (model .05) or 10 m (model .10)
R&S NRP-Z3
Active USB adapter with trigger
input and plug-in power supply
Trigger input
Maximum voltage
Logic level
Low
High
Input impedance
Plug-in power supply
Voltage/frequency
Tol era nce
Current consumption
Connection
Connecting cable to PC
USB interface
Length
Dimensions (W x H x L)
USB adapter
Plug-in power supply
Weig ht
USB adapter
Plug-in power supply
R&S NRP-Z4
Passive USB adapter (cable)for connecting a sensor to the USB
unit or a USB adapter
3.5 m
8.5 m (not in conjunction with
R&S NRP-Z4)
for connecting a sensor to the USB
interface of a PC
±15 V
<0.8 V
>2.0 V
approx. 5 kΩ
100 V to 240 V, 50 Hz to 60 Hz
±10% for voltage, ±3 Hz for frequency
25 mA typ. with sensor connected
via adapter to all common AC supplies
(Europe, UK, USA, Australia)
type A
approx. 2 m
48 mm x 45 mm x 140 mm
52 mm x 73 mm x 110 mm
length of line to adapter: 2 m
<0.2 kg
<0.3 kg
interface of a PC
Measurement functionality
Single-channel
Display
Absolute
Relative
Multichannel
Display
Difference
Ratio
Relative ratio
Display
Typ eLC graphics screen ¼ VGA (320 x 240)
Backlightingbrightness adjustable
Measurement results
Representation
Resolution
Digital values
Analog display
Manual operationWindows-oriented menus with hot-
Remote control
see sensor specifications6), plus:
relative measurement referenced to result or user-selectable reference value,
storage of minima and maxima (Max,
Min, Max-Min), limit monitoring
in W, dBm and dBµV
in dB, as change in percent (∆%) or as
quotient
simultaneous measurement in up to
4 channels; ratio, relative ratio
difference of results of 2 channels can
be displayed (for all functions except
Scope)
in W
in dB, as change in percent (∆%), as
quotient or as one of the following
matching parameters: SWR, return
loss, reflection coefficient
in dB, as change in percent (∆%) or as
quotient
pixel, monochrome, transflective
up to 4 results with additional information (Min, Max, Max-Min, frequency)
can simultaneously be displayed in
separate windows
digital, digital and analog
selectable in 4 steps:
0.001 dB/0.01%/4½ digits (W, quotient)
0.01 dB/0.1%/3½ digits (W, quotient)
0.1 dB/1.0%/2½ digits (W, quotient)
1 dB/1.0%/2½ digits (W, quotient)
depending on user-definable scale end
values
keys for the most important functions
34)
or
USB interface
Length
type A
approx. 2 m
R&S NRP basic unit
Applicationmultichannel power meter
SensorsR&S NRP-Z series
Measurement channels
Basic version
Basic version + R&S NRP-B2
Basic version + R&S NRP-B2 +
R&S NRP-B5
1
2
4
SystemsIEC 60625.1 (IEEE488.1) and
Command setSCPI-1999.0
IEC/IEEE bus
Interface functions
Connector
Firmware downloadwith a Windows-compatible program
from the R&S NRP toolkit via the rearpanel USB interface (type B)
Power Meter R&S NRP15
Inputs/outputs (rear panel)
OUT1
Modes
Analog
Pass/Fail
Off
Voltage range
Setting accuracy
Resolution
Output impedance
Connector
Analog, Pass/Fail, Off
recorder output; user-definable linear
relation to measurement result (display
windows 1 to 4)
limit indicator with two user-selectable
voltages for identifying the Pass and
Fail states in the case of limit monitoring
0 V
0 V to +3.3 V
±1% of voltage reading + (0/+8 mV)
12 bit (monotone)
1 kΩ
BNC (female)
Options for R&S NRP
R&S NRP-B1
Power reference
Power
Uncertainty
20°C to 25 °C
0°C to 50°C
Frequency
SWR
RF connector
R&S NRP-B2
1.00 mW
0.85%
1.00%
50 MHz
<1.05 typ.
N (female)
IN/OUT 2
Modes
Analog Out
Electrical characteristics
Trigg er In
Maximum voltage
Logic level
Low
High
Impedance
Connector
Power supply
Voltage, frequency
Tol era nce
Apparent power
Dimensions (W x H x D)274 mm x 112 mm x 267 mm
Weight<3.0 kg
Analog Out and Trigger In
recorder output; user-definable linear
relation to measurement result (display
windows 1 to 4)
see OUT1
input for trigger signal to sensors
–7 V/+10 V
<0.8 V
>2.0 V
10 kΩ//100 pF
BNC (female)
220 V to 240 V, 50 Hz to 60 Hz
100 V to 120 V, 50 Hz to 400 Hz
±10% for voltage and frequency
<80 VA
Second test input (B)for R&S NRP-Z sensors (available as
standard on front panel)
R&S NRP-B5
Third (C) and fourth (D) test inputs for R&S NRP-Z sensors (only on rear
panel)
R&S NRP-B6
Rear-panel assemblyfor test inputs A and B (only possible if
the R&S NRP-B5 option is not installed)
General specifications
Temperature loading
Operating range and permissible range
(in [] if different)
R&S NRP with options
R&S NRP-Z2, -Z11, -Z21
R&S NRP-Z3
Storage range
R&S NRP with options
R&S NRP-Z2, -Z3, -Z11, -Z21
Climatic resistancemeets IEC 60068
35)
meet IEC 60068
0°C [–5°C] to +50°C
0°C [–10 °C] to +50°C [+55°C]
0°C to +40°C
–20°C to +70°C
–40°C to +70°C
Damp heat
R&S NRP-Z3, -Z11, -Z21
Mechanical resistance
Vibration, sinusoidalmeets IEC 60068
Vibration, randommeets IEC 60068
Shockmeets IEC 60068; 40 g shock spectrum
Air pressure
Operation
Tra nsp or t
Electromagnetic compatibilitymeets EN 61326, EN 55011
Safetymeets EN 61010-1
+25°C/+40 °C cyclic at 95% relative
humidity
with restrictions: non-condensing
5 Hz to 55 Hz, max. 2 g
55 Hz to 150 Hz, 0.5 g constant
10 Hz to 500 Hz, 1.9 g (rms)
795 hPa (2000 m) to 1060 hPa
566 hPa (4500 m) to 1060 hPa
Power Meter R&S NRP 16
1)
Γ correction activated.
2)
Referenced to 0 dBm.
3)
Specifications apply to timeslots with a duration of 12.5% referenced to the sig nal period (duty
cycle 1:8). For other waveforms the following equation applies:
lower measurement limit = 200 pW x measurement time/integration time
For measurement time, see specifications. For integration time, see footnote
4)
With a resolution of 256 points.
5)
Transition regions can be shifted by up to –20 dB if automatic path selection has been chosen.
6)
The Scope function will be available for the R&S NRP basic unit as of spring 2003.
7)
Portion of signal that is the subject of measurement (sampling). The factor of 2 is due to the
16)
.
measurement being performed in two equal periods of time (chopper amplifier) separated by
100 µs. If averaging is activated, the averaging factor determines the number of measurement
windows to be averaged.
8)
For calculating the pulse power of periodic bursts from an average power measurement.
9)
To increase measurement speed, the power sensor can be operated in buffered mode. In this
mode, measurement results are stored in a buffer of user-definable size and then output as a
block of data when the buffer is full. To enhance measurement speed even further, the sensor
can be set to record the entire series of measurements when triggered by a single event. In this
case the power sensor automatically starts a new measurement as soon as it completes the
preceding one.
10)
This parameter enables power measurements on modulated bursts. The parameter must be
longer in duration than modulation-induced power drops within the burst, but at least 10 µs
shorter than the gap between the end of one burst and the beginning of the next one.
11)
To exclude unwanted portions at the beginning or end of the measurement window from the
measurement result.
12)
Portion of signal that is the subject of measurement (sampling). Periodic signals are measured
in t wo eq ual p erio ds of time (cho pper ampl ifie r) separated by 100 µs. If averaging is activated,
the averaging factor determines the number of measurement windows to be averaged.
13)
To prevent aliasing in the case of signals with discrete modulation frequencies between
100 kHz and 1 MHz.
14)
Two standard deviations, 10.24 s integration time (see footnote
16)
). Multiplying noise specifications by 10.24 s/integration time yields the noise contribution at other integration times.
Smoothing (see under Measurement window) increases noise by 22%.
15)
Two standard deviations, for power leve ls gr eate r tha n 500 nW (– 33 dBm ) in C onti nuou s
Average mode with automatic path selection (User def'd crossover deactivated or set to 0 dB).
Within a measurement subrange, relative measurement uncertainty due to noise is inversely
proportional to the measured power. The specified values refer to 500 nW (–33 dBm) and the
lower limits of paths 2 and 3 at 50 µW (–13 dBm) and 5 mW (+7 dBm) respectively.
16)
Integration time is defined as the total time used for sampling the signal. It can be calculated by
multiplying the duration of the measurement window by the averaging factor.
17)
Expanded uncertainty (k = 2) after zeroing (for 4 s). Zeroing for more than 4 s lowers uncertainty
correspondingly (half values for 16 s).
18)
Within 1 hour after zeroing, permissible temperature change ±1°C, following 2-hour warm-up
of power sensor.
19)
Magnitude of measurement error with reference to an ideal thermal power sensor that measures the sum power of carrier and harmonics. Specified values apply to automatic path selection (User def'd crossover deactivated or set to 0 dB) and power levels up to +20 dBm. Above
+20 dBm, specified values must be multiplied by a factor of 1.25 per 1 dB rise in power level.
Within a measurement subrange, errors (uncertainties) are proportional to the measured
power in W. The specified values refer to 10 µW (–20 dBm) for path 1, 1 mW (0 dBm) for path 2
and 100 mW (20 dBm) for path 3.
20)
Adhering to specified error limits implies that harmonics above 25 GHz (R&S NRP-Z11) and
56 GHz (R&S NRP-Z21) are at least 20 dB lower than required at other frequencies.
21)
Measurement error with reference to CW signal of equal power and frequency. Specified
values apply to automatic path selection (User def'd crossover deactivated or set to specified
val ue) a nd po wer l evel s up t o (+2 0 dBm + Use r def'd crossover). Above this level, specified
val ues m ust b e mul tipl ied b y a fa ctor of 1. 25 per 1 dB r ise i n pow er le vel. In th e mea sure ment
subranges, the specified values apply to –20 dBm for path 1, 0 dBm for path 2 and +20 dBm for
path 3.
22)
The AUTO mode is not available in conjunction with the R&S NRP basic unit.
23)
Characteristics like for a conventional power meter. The averaging factor increases continuously as power decreases, but not to the extent that would be necessary to keep the relative
noise content at the same level.
24)
Limits the averaging factor when measuring very low powers or when the noise content is set
to a very small value (status information available).
25)
Reference timeslot and reference point are user-definable.
26)
Preferably used with determined modulation, when the duration of the measurement window
cannot be matched to the modulation period. Compared to a rectangular window, display noise
is about 22% higher.
27)
Valid for Repeat mode, extending from the beginning to the conclusion of all transfers via the
USB interface of the power sensor. Measurement times under remote control of the R&S NRP
basic unit via IEC/IEEE bus are approximately 2.5 ms longer, extending from the start of the
measurement until the measurement result is supplied to the output buffer of the R&S NRP.
28)
For calculation of measurement time, N must be set to twice the averaging factor if the expression (number of timeslots x nominal width + 100 µs + trigger delay) exceeds the trigger period.
29)
This function can be used to counteract interactions between the signal source and the input of
the power sensor (input of a component ahead of the power sensor if s-parameter correction is
activated). By using this function, the nominal power of the source into 50 Ω can be measured
(without this correction: power of the incident wave).
30)
Expanded uncertainty (k = 2) for absolute power measurements on CW signals at calibration
levels (–20 dBm for path 1, 0 dBm for paths 2 and 3) and the calibration frequencies (10 MHz,
15 MHz, 20 MHz, 30 MHz, 50 MHz, 100 MHz; from 250 MHz to 8 (18) GHz in increments of
250 MHz). Specifications include zero offset and display noise (up to a 2 σ value of 0.004 dB).
31)
Expanded uncertainty (k = 2) for absolute power measurements on CW signals with automatic
path selection. Specifications include display noise with a 2 σ val ue up to 0. 01 dB and z ero o ff-
set for levels from –40 dBm to +23 dBm. Higher display noise and the effect o f zer o off set a t
lower levels must be considered separately.
Exa mple : Pow er to be me asur ed is 3.2 n W (–55 dBm) at 1.9 GHz; ambient temperature is 29 °C;
automatic path selection is set. Typical absolute uncertainty due to z ero o ffs et eq uals 64 pW ,
corresponding to a relative measurement uncertainty of .
3.2 nW + 64 pW
10 x lg
(
Combined with the specified value of 0.081 dB for the uncertainty of absolute power measurements, the total uncertainty is 0.086
should be considered in the same way.
32)
Expanded uncertainty (k = 2) for relative power measurements on CW signals with automatic
2
= 0.086 dB
)
3.2 nW
+0.0812 dB = 0.12 dB. Noise content exceeding 0.01 dB
path selection. Specifications include display noise with a 2 σ value up to 0.01 dB for both the
measurement and the reference level as well as zero offsets for all levels from –40 dBm to
+23 dBm . Bel ow –4 0 dBm , the effec t of i ncre ased rela tive zero offs et mu st be take n int o
account (only for the lower level, if both levels are below –40 dBm). Display noise exceeding
0.0 1 dB m ust b e con side red s epar atel y for both the measurement level and the reference level
(if applicable). See example in footnote
33)
Reading the measurement uncertainty for relative power measurements
31)
for calculation of total uncertainty.
The example shows a level step of approx. 14 dB (–4 dBm → +10 dBm) at 1.9 GHz and an
ambient temperature of 28°C.
100 MHz to 4 GHz
+23
Power level 1:
–4 dBm
34)
Quotient of a measured and a stored reference power ratio, e.g. for measuring gain compression of amplifiers.
35)
The operating temperature range defines the span of ambient temperature in which the instru-
+1
–19
–40
+7+23–13
+23
+7
0
0
–13
+1+23–19–40
Power level 2: +10 dBm
0°Cto50°C
15 °C to 35 °C
20 °C to 25 °C
ment complies with specifications. In the permissible temperature range, the instrument is still
functioning but adherence to specifications is not warranted.
Power Meter R&S NRP 17
Ordering information
DescriptionTypeOrder No.
Basic Unit
Power MeterR&S NRP1143.8500.02
Power Sensors
200 pW to 200 mW,
10 MHz to 8 GHz
200 pW to 200 mW,
10 MHz to 18 GHz
Options
Sensor Check SourceR&S NRP-B11146.9008.02
Second Sensor Input (B)R&S NRP-B21146.8801.02
3rd and 4th Sensor Inputs (C, D)
Rear-Panel Sensor Inputs A and B
Battery SupplyR&S NRP-B31146.8501.02
Recommended extras
Sensor Extension Cable to 5 mR&S NRP-Z21146.6750.05
Sensor Extension Cable to 10 mR&S NRP-Z21146.6750.10
USB Adapter (active)R&S NRP-Z31146.7005.02
USB Adapter (passive)R&S NRP-Z41146.8001.02
19" Rack Adapter (R&S NRP + dummy)
19" Rack Adapter (two R&S NRPs)
R&S NRP-Z111138.3004.02
R&S NRP-Z211137.6000.02
1)
R&S NRP-B51146.9608.02
2)
R&S NRP-B61146.9908.02
R&S ZZA-T261109.4387.00
R&S ZZA-T271109.4393.00
Printed in Germany1202 (Bi sk)
1)
Option R&S NRP-B2 required.
2)
Not in conjunction with the R&S NRP-B5.
Certified Environmental System
ISO 14001
REG. NO 1954
Certified Quality System
ISO 9001
DQS REG. NO 1954
PD 0757.7023.21 ⋅ Power Meter R&S NRP ⋅ Trade names are trademarks of the owners ⋅ Subject to change ⋅ Data without tolerances: typical values
ROHDE& SCHWARZ GmbH & Co. KG ⋅ Mühldorfstraße 15 ⋅ 81671 München ⋅ Germany ⋅ P.O.B. 80 14 69 ⋅ 81614 München ⋅ Germany ⋅ Telephone +49 89 4129-0