Rohde and Schwarz NRP-Z4 Data Sheet

Power Meter R&S NRP
in
Innovative multipath sensor
technology
90 dB dynamic range
High measurement speed
Intelligent sensors – simply plug in
and measure
Accurate measurement of average
power regardless of bandwidth and modulation
Multislot measurements for
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 NRP 3
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 –30 0–10–50 –20–40 2010
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 NRP 5
Power Meter R&S NRP 5
+
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, a signal 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
0 Γ
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 2 Plane 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 A Path B
1
0
P
x
.
4xPxPower
FIG 7: Windowing technique used on a low-frequency-modulated signal.
Power Meter R&S NRP 7
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
Continuous Timeslot
1 out of 8 (external trigger)
Thermoelectric sensor 50/50/50 dB
Diode: Sensor in square-law region
Diode: CW sensor 43/43/90 dB
Diode: Peak sensor 33/50/80 dB –/50/57 dB –/33/37 dB –/50/57 dB
Diode: Multiple-path sensor 80/80/80 dB
43/43/50 dB
Burst
duty cycle 1:8 (internal trigger)
Power versus time
256 points (external trigger)
Diode:
90/90/90 dB 85/85/85 dB 60/60/60 dB 70/70/70 dB
Power Meter R&S NRP 9
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 signal Power 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 NRP 11
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 type 3-path diode sensor
Measurand average power of incident wave or
average power of source into 50
Frequency range 10 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
10 MHz to 2.4 GHz >2.4 GHz to 18.0 GHz
2)
<1.15 (1.13) <1.13 (1.11) <1.20 (1.18) <1.25 (1.23)
<0.05 (0.02) <0.10 (0.07)
RF connector N (male)
Power measurement range
Continuous Average
200 pW to 200 mW (–67 dBm to +23 dBm)
Burst Average
200 nW to 200 mW (–37 dBm to +23 dBm)
Timeslot
Scope
650 pW to 200 mW (–62 dBm to +23 dBm) 10 nW to 200 mW (–50 dBm to +23 dBm)
3)
4)
Max. power
Average Peak envelope power
0.4 W (+26 dBm) continuous
1.0 W (+30 dBm) for max. 10 µs
Measurement subranges
Path 1 Path 2 Path 3
–67 dBm to –14 dBm –47 dBm to + 6 dBm –27 dBm to +23 dBm
Tra nsition ranges
With automatic path selection, user def'd crossover
5)
set to 0 dB
(–19 ±1) dBm to (–13 ±1) dBm (+1 ±1) dBm to (+7 ±1) dBm
Measurement functions
Stationary and periodically modulated signals
Continuous Average Burst Average Timeslot
6)
Scope
Non-recurring waveforms
Scope
6)
Continuous Average function
Continuous measurement of average power
Measurement window Duty cycle correction Smoothing
Capacity of measurement buffer
7)
8)
2 x (10 µs to 300 ms)
0.001% to 100.00% see under Measurement window (page 13)
9)
1 to 1024 results
12 Power Meter R&S NRP
Measurement of average burst power with automatic detection of burst (trigger settings required)
Detectable burst width Minimum gap between bursts Dropout tolerance Exclusion periods
10)
11)
Excluded from Start Excluded from End
Measurement window
7)
20 µs to 100 ms 10 µs 0 ms to 3 ms
0 ms to 100 ms 0 ms to 3 ms 2 x (burst width – Excl. from Start – Excl. from End)
1)
Timeslot function
Measurement of average power in one or more equidistant, successive timeslots
Duration (nominal width) Number of timeslots
Exclusion periods
11)
Excluded from Start Excluded from End
Measurement window (per timeslot)
10 µs to 100 ms 1 to 128 (26 in case of operation from R&S NRP basic unit)
0 ms to 100 ms 0 ms to 3 ms
7)
2 x (nom. width – Excl. from Start – Excl. from End)
Scope function
Measurement of power versus time
Modes
Measurement window
12)
Recurring Non-recurring
Number of measurement points M Resolution /M
for recurring and non-recurring wave­forms (single)
2 x (100 µs to 300 ms) 100 µs to 300 ms 1 to 1024 10 µs
Beginning of measurement window (referenced to trigger)
–5 ms to 100 s
Dynamic behaviour of video path values in () for temperature range 15°C
to 35°C
Bandwidth Rise time 10%/90 %
>50 kHz (100 kHz) <8 µs (4 µs)
Sampling frequencies
Frequency 1 (default) Frequency 2
Display noise
13)
14)
15°C to 35 °C Path 1
Path 2 Path 3
0°C to 50°C Path 1
Path 2 Path 3
Display noise, relative
15)
133.358 kHz
119.467 kHz
values in []: 8 GHz to 18 GHz
<60 pW [64 pW] (40 pW typ.) <5.6 nW [6.0 nW] (3.6 nW typ.) <0.56 µW [0.60 µW] (0.36 µW typ.) <65 pW [69 pW] <6.3 nW [6.6 nW] <0.63 µW [0.66 µW]
Measurement window 2 x 100 µs, without averaging
<0.160 dB (0.1 dB typ.) Measurement window 2 x 20 ms, averaging factor 32 (measurement time approx. 1 s)
<0.002 dB (0.001 dB typ.)
Zeroing (duration)
Depends on setting of averaging filter
AUTO ON AUTO OFF
Integration time
16)
<4 s 4 s to 16 s >16 s
4 s
4 s
integration time
16 s
16)
Zero offset
17)
values in []: 8 GHz to 18 GHz
Measurement window
15°C to 35°C Path 1
Path 2 Path 3
0°C to 50°C Path 1
Path 2 Path 3
18)
Zero drift
Path 1 Path 2 Path 3
<96 pW [102 pW] (64 pW typ.) <9.0 nW [9.6 nW] (5.8 nW typ.) <0.90 µW [0.96 µW] (0.58 µW typ.) <104 pW [110 pW] <10.0 nW [10.6 nW] <1.00 µW [1.06 µW]
values in []: 8 GHz to 18 GHz
<35 pW [37 pW] <3.0 nW [3.2 nW] <0.30 µW [0.32 µW]
Measurement error due to harmonics n x f0 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 NRP 13
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 –19 to +1 to +23 (–67)
0.160
0.096
0.083
–40 to –19 to +1 to +23 (–67)
0.188
0.133
0.123
–40 to –19 to +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 MHz 20 MHz to <100 MHz
Path 1 Path 2 Path 3 Path 1 Path 2 Path 3
0.056 0.047 0.048 0.056 0.047 0.047 20 °C to 25°C
100 MHz to 4 GHz >4 GHz to 8 GHz
Path 1 Path 2 Path 3 Path 1 Path 2 Path 3
0.066 0.057 0.057 0.083 0.071 0.072 20 °C to 25°C
>8 GHz to 12.4 GHz >12.4 GHz to 18 GHz
Path 1 Path 2 Path 3 Path 1 Path 2 Path 3
0.094 0.076 0.076 0.123 0.099 0.099 20 °C to 25°C
Uncertainty for absolute power measurements
10 MHz to <20 MHz 20 MHz to <100 MHz
0.174
0.075
0.056
–40 to –19 to +1 to +23 (–67)
100 MHz to 4 GHz >4 GHz to 8 GHz
0.150
0.081
0.066
–40 to –19 to +1 to +23 (–67)
>8 GHz to 12.4 GHz >12.4 GHz to 18 GHz
0.168
0.106
0.094
–40 to –19 to +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 MHz 20 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 cable for connecting the sensor to the basic
Length
Model .05 Model .10
Total length incl. sensor cable 5 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 k
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 e LC graphics screen ¼ VGA (320 x 240)
Backlighting brightness adjustable
Measurement results
Representation Resolution
Digital values
Analog display
Manual operation Windows-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
Application multichannel power meter
Sensors R&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
Systems IEC 60625.1 (IEEE488.1) and
Command set SCPI-1999.0
IEC/IEEE bus
Interface functions
Connector
Firmware download with a Windows-compatible program
IEC 60625.2 (IEEE488.2)
SH1, AH1, L3, LE3, T5, TE5, SR1, PP1, PP2, RL1, DC1, E2, DT1, C0 24-pin Amphenol (female)
from the R&S NRP toolkit via the rear­panel USB interface (type B)
Power Meter R&S NRP 15
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 k 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 k//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 assembly for 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 resistance meets 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, sinusoidal meets IEC 60068
Vibration, random meets IEC 60068
Shock meets IEC 60068; 40 g shock spectrum
Air pressure
Operation Tra nsp or t
Electromagnetic compatibility meets EN 61326, EN 55011
Safety meets 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 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
Description Type Order No.
Basic Unit
Power Meter R&S NRP 1143.8500.02
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 Source R&S NRP-B1 1146.9008.02
Second Sensor Input (B) R&S NRP-B2 1146.8801.02
3rd and 4th Sensor Inputs (C, D)
Rear-Panel Sensor Inputs A and B
Battery Supply R&S NRP-B3 1146.8501.02
Recommended extras
Sensor Extension Cable to 5 m R&S NRP-Z2 1146.6750.05
Sensor Extension Cable to 10 m R&S NRP-Z2 1146.6750.10
USB Adapter (active) R&S NRP-Z3 1146.7005.02
USB Adapter (passive) R&S NRP-Z4 1146.8001.02
19" Rack Adapter (R&S NRP + dummy)
19" Rack Adapter (two R&S NRPs)
R&S NRP-Z11 1138.3004.02
R&S NRP-Z21 1137.6000.02
1)
R&S NRP-B5 1146.9608.02
2)
R&S NRP-B6 1146.9908.02
R&S ZZA-T26 1109.4387.00
R&S ZZA-T27 1109.4393.00
Printed in Germany 1202 (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 0757.7023.21Power Meter R&S NRPTrade names are trademarks of the ownersSubject to changeData 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
www.rohde-schwarz.com Customer Support: Telephone +49 180512 4242, Fax +49 89 41 29-13777, E-mail: CustomerSupport@rohde-schwarz.com
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