Method for calibrating a cable and respective measuring device

Abstract

A measuring device comprises at least one port, an external cable connected to the at least one port, a transmitter connected to the at least one port through a switch, a receiver connected to the at least one port through the switch and a reference path connecting the transmitter with the receiver through the switch. The cable is connected to calibration elements, e.g., short and open. The switch alternately switch in a manner that in a first state the transmitter and the receiver are connected to the at least one port and that in a second state the transmitter and the receiver are connected via the reference path.

Claims

1. A method comprising: providing a first signal, from a transmitter of a measuring device, to a first calibration element connected to a port of the measuring device via one or more cables; receiving, by a receiver of the measuring device, a first return signal reflected by the first calibration element, and measuring the first return signal; providing a second signal, from the transmitter to the receiver, through a reference path of the measuring device, and measuring a reference signal through the reference path; and wherein the measurement of the reference signal is performed via a signal splitter arranged between a switch and the port of the measuring device, wherein the signal splitter comprises a resistive splitter of a star configuration, and wherein a first resistor is connected to the transmitter through the switch, a second resistor is connected to the receiver through the switch and a third resistor is connected to a one of the cables through the port.

2. The method of claim 1, wherein the first calibration element is a short.

3. The method of claim 1, further comprising: providing a third signal, from the transmitter of the measuring device, to a second calibration element connected to the port of the measuring device; receiving, by the receiver of the measuring device, a second return signal reflected by the second calibration element, and measuring the second return signal; providing a fourth signal, from the transmitter to the receiver, through the reference path of the measuring device, and measuring the reference signal through the reference path.

4. The method of claim 3, wherein the second calibration element is an open.

5. The method of claim 3, wherein steps recited by claim 1 and the steps recited by claim 3 are alternately repeated a number of times.

6. The method of claim 3, wherein the steps are repeated for at least one different frequency for one or more of the first signal, the second signal, the third signal and the fourth signal.

7. The method of claim 1, wherein a magnitude and a phase of one or more of the first return signal and reference signal and the second return signal and reference signal are measured, and wherein the measurement of the phase is completed before the measurement of the magnitude.

8. A measuring device comprising a port; an external cable connected to the port; a transmitter connected to the port through a switch; a receiver connected to the port through the switch; a reference path connecting the transmitter to the receiver through the switch; and a signal splitter arranged between the switch and the port, wherein the signal comprised a plurality of resistors in a star configuration, with a first resistor connected to the transmitter through the switch, a second resistor connected to the receiver through the switch and a third resistor connected to the external cable through the port; and wherein the switch is configured to switch between states of the device, wherein in a first state the transmitter and the receiver are connected to the port and in a second state the transmitter and the receiver are connected via the reference path.

9. The measuring device of claim 8, wherein the switch is configured to alternately between the first state and the second state a number of times.

10. The measuring device of claim 8, further comprising: a first calibration element and a second calibration element, wherein the cable is terminated with the first calibration element and the second calibration element.

11. The measuring device of claim 10, wherein the first calibration element is a short and the second calibration element is an open.

12. The measuring device of claim 8, wherein the receiver comprises a first selection device and first phase averaging device configured to evaluate an averaged phase of a return signal reflected by a calibration element connected to the external cable.

13. The measuring device of claim 12, wherein the receiver further comprises a second selection device and a second phase averaging device configured to evaluate an averaged phase of a reference signal provided by the transmitter to the receiver via the reference path.

14. The measuring device of claim 13, wherein the receiver further comprises a subtracting device configured to subtract an output of the second phase averaging device from an output of the first phase averaging device.

15. The measuring device of claim 14, wherein the receiver further comprises a magnitude averaging device configured to evaluate an averaged magnitude of a measuring signal.

16. The measuring device of claim 15, wherein the receiver further comprises a multiplier device configured to multiply an output of the magnitude averaging device with an imaginary exponential output of the subtracting device.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) In the figures of the drawings, example embodiments of the invention are depicted by way of example only, and not by way of limitation. In the drawings:

(2) FIG. 1 illustrates a block diagram depicting an example measuring device and respective cables, in accordance with example embodiments;

(3) FIG. 2 illustrates a vector diagram depicting a quantitative evaluation of the cable loss according to example embodiments;

(4) FIG. 3 illustrates a block diagram depicting a first example of the receiver (Rx) of a measuring device, in accordance with example embodiments;

(5) FIG. 4 illustrates the measurement of the reference signal and the measurement signal, and the measurement of the magnitude of the measurement signal, according to example embodiments;

(6) FIG. 5 illustrates a block diagram depicting a second example of the receiver (Rx) of a measuring device, in accordance with example embodiments;

(7) FIG. 6A illustrates a graph of the phase difference between the averaged reference signal and the averaged measurement signal, where the measurement of the referenced signal and the measurement signal is not done alternatively, in accordance with example embodiments;

(8) FIG. 6B illustrates the phase difference between the averaged reference signal and the averaged measurement signal, where the measurement of the referenced signal and the measurement signal is done alternatively, in accordance with example embodiments; and

(9) FIGS. 7A and 7B illustrate a flow chart a method, in accordance with example embodiments.

DETAILED DESCRIPTION OF THE INVENTION

(10) Aspects of the present invention provide an improved method for calibration and respective measuring devices allowing for calibration with sufficient accuracy. Embodiments of the inventive method achieve improved calibration of the cable for a measuring device, such as a mobile phone testing device. While example embodiments are described with respect to a mobile phone testing device, however, it will be apparent that the approaches of embodiments of the present invention are also applicable to other types of measurement equipment, such as spectrum analyzer or oscilloscope.

(11) According to example embodiments, such measurement devices are connected to the device under test (DUT) through cables. At high frequencies, above 1 GHz these cables have a significant damping even if kept as short as possible. The damping of the cables can be up to 12 dB. Thus, it is very important to calibrate the damping factor of the cables. The error of the result from this calibration procedure should be less than 1 dB. The cable is terminated by a short and a first calibration measurement is done with this short. Then the cable is terminated with an open and a second calibration measurement is done in this open configuration. This is done for several frequency points within the operation range of a measuring device.

(12) According to such example embodiments, the measuring device comprises a transmitter and a receiver. By way of example, for mobile communication testers for testing mobile phones, the starting phase of the transmitter and of the receiver is different to the situation as calibrating the cable with a vector network analyzer because there is no coherence between the oscillators used for the mixers in the transmitter and the receiver. Thus, there is a need for measuring the start phase of the transmitter. According to example embodiments of the invention, a reference path can be alternatively switched between the transmitter and the receiver. By way of example, this may be accomplished by a switch. By way of further example, the reference path is arranged internally in the measuring device.

(13) FIG. 1 shows a block diagram of a simplified model of an embodiment of the inventive measuring device. In this block diagram, only the most essential elements in order to operate the present invention are shown. The model is shown in the equivalent base band which is sufficient to understand the present invention. All mixers and filters for up and down conversion are not shown. It is the task of the present invention to evaluate the unknown cable damping in a calibration procedure, wherein the cables are terminated by calibration elements, especially calibration standards such as open and short. The sending signal a(k) in the equivalent base band is described by the complex vector.

(14) $\begin{array}{cc}a\left(k\right)=\exp \left(j\left[\left(k\right)+{}_0\right]\right)+\stackrel{\stackrel{>=}{}}{n\left(k\right)}& \left(1\right)\end{array}$

(15) The symbols used in this formula describe the following: (i) (k) is a time dependent average free phase noise of the generator of the transmitter with respect to the phase of the oscillator of the receiver; (ii) .sub.0 is an arbitrary starting phase of the oscillator of the transmitter with respect to the oscillator of the receiverfor measuring with an open termination of the cable and for measuring with a short termination of the cable, these starting phases .sub.0 are different; (iii) n(k) is an Additive White Gaussian Noise (AWGN)however, the phase noise is highly dominating the noise so that the AWGN is not considered any further here and is neglected in the above formula.

(16) FIG. 1 shows a relatively simplified embodiment of the inventive measurement device. The embodiment is shown in the equivalent base band. Transmitter 2 transmit a complex sending signal a(k), which in the digital domain is defined at the samples points k, through the first part 3a of switch 3, through a signal splitter 4 and through a port 6 into the cable 5. Actually, this is the case at a first state Meas shown in FIG. 1. The cable 5 is terminated at the end 7 with a short in a first run and with an open in a second run. However, the cable 5 can also be terminated with other calibration elements, such as a match or a specific mismatch.

(17) The wave is reflected at the open calibration element with no phase amendment and is also reflected at the short calibration element with a phase shift of 180. The reflected wave will then propagate back through the cable 5 and through the other branch of the splitter 4 and through the second part 3b of the switch 3 into receiver 8. In the embodiment shown in FIG. 1, the signal splitter 4 is a resistive splitter having three resistors in a star configuration. A first resistor 4a is connected to the transmitter 2 through the first part 3a of the switch 3. A second resistor 4b is connected to the receiver 8 through the second part 3b of the switch 3. By way of example, in the first resistor 4a and the second resistor 4b, the wave receives a damping of 6 dB. A third resistor 4c is connected to the cable 5 through the port 6. By way of further example, the wave receives a damping in each direction (forward and backward) of 3 dB in the third resistor 4c, so that the wave in total is also damped by 6 dB in the third resistor 4c if the forward and backward directions are taken together. In the cable 5 the wave receives a damping of x dB in each direction. It is the task of a measurement to obtain a value of this cable damping x.

(18) The path through the resistors 4a and 4b has a runtime of T.sub.Meas and has a damping of 12 dB. The signal through the port 6 has an additional runtime of T.sub.cable in the forward direction

(19) ##STR00001##
as follows:
a.sub..fwdarw.=3 dB+x[dB](2)
x [dB] is the cable damping which is of interest here. The wave is additionally damped in the backward direction

(20) ##STR00002##
so that the wave running through the port has a total damping, as follows:

(21) ##STR00003##
=2.Math.a.sub..fwdarw.[dB](3)

(22) In order to measure the unknown start phase .sub.0, the sending signal sent by the transmitter 2 is sent directly into the receiver 8 through a reference path 9. In this case, the switch 3 are in a second state designated Ref.

(23) In the following, it is shown that the unknown runtimes T.sub.Meas and T.sub.cable are not needed in order to evaluate the cable damping.

(24) The open-measurement and the short-measurement are considered for an arbitrary frequency .sub.v. The sending signal has arbitrary starting phases and can be defined, as follows:

(25) $\begin{array}{cc}a\left(k\right)=\{\begin{array}{c}\exp \left(j\left[\left(k\right)+{}_0^{\left(\mathrm{Open}\right)}\right]\right)@\mathrm{Open}\\ \exp \left(j\left[\left(k\right)+{}_0^{\left(\mathrm{Short}\right)}\right]\right)@\mathrm{Short}\end{array}& \left(4\right)\end{array}$

(26) By the runtimes, the following phases are created:
.sub.Ref:=.sub.v.Math..sub.Ref
.sub.Meas:=.sub.v.Math..sub.Meas
.sub.Cable:=.sub.v.Math..sub.Cable(5)

(27) In the receiver 8 the following reference signal is received:

(28) $\begin{array}{cc}\begin{array}{c}{b}^{\left(\mathrm{Ref},\mathrm{Open}\right)}\left(k\right)=a\left(k\right).Math.\exp \left(j{}_{\mathrm{Ref}}\right)\\ =\exp \left(j\left[\left(k\right)+{}_0^{\left(\mathrm{Open}\right)}+{}_{\mathrm{Ref}}\right]\right)\\ b^{\left(\mathrm{Ref},\mathrm{Short}\right)}\left(k\right)=\exp \left(j\left[\left(k\right)+{}_0^{\left(\mathrm{Short}\right)}+{}_{\mathrm{Ref}}\right]\right)\end{array}& \left(6\right)\end{array}$

(29) In the receiver 8 also the following measuring signal is received:

(30) $\begin{array}{cc}\begin{array}{c}{b}^{\left(\mathrm{Meas},\mathrm{Open}\right)}\left(k\right)=a\left(k\right).Math.a_{12dB}.Math.\exp \left(j{}_{\mathrm{Meas}}\right).Math.\\ \left[1+a_{.Math.}.Math.\exp \left(j{}_{\mathrm{cable}}\right)\right]\\ =\exp \left(j\left[\left(k\right)+{}_0^{\left(\mathrm{Open}\right)}+{}_{\mathrm{Meas}}\right]\right).Math.\\ a_{12dB}.Math.\left[1+a_{.Math.}.Math.\exp \left(j{}_{\mathrm{cable}}\right)\right]\\ b^{\left(\mathrm{Meas},\mathrm{Short}\right)}\left(k\right)=\exp \left(j\left[\left(k\right)+{}_0^{\left(\mathrm{Short}\right)}+{}_{\mathrm{Meas}}\right]\right).Math.\\ a_{12dB}.Math.\left[1-a_{.Math.}.Math.\exp \left(j{}_{\mathrm{cable}}\right)\right]\end{array}& \left(7\right)\end{array}$

(31) In an ideal case, the reference signal and the measuring signal are received simultaneously. This is assumed in the following as an assumption which makes it easier to understand the measurement principal. First of all, the unknown start phase .sub.0 is eliminated by measuring the reference signal. For the open-measurement we get:

(32) $\begin{array}{cc}\begin{array}{c}{c}^{\left(\mathrm{Meas},\mathrm{Open}\right)}\left(k\right)=b^{\left(\mathrm{Meas},\mathrm{Open}\right)}\left(k\right).Math.\exp \left(-j\arg \left\{b^{\left(\mathrm{Ret},\mathrm{Open}\right)}\left(k\right)\right\}\right)\\ =\exp \left(j\left[\left(k\right)+{}_0^{\left(\mathrm{Open}\right)}+{}_{\mathrm{Meas}}\right]\right).Math.a_{1\mathrm{MB}}.Math.\\ \left[1+a_{.Math.}.Math.\exp \left(j_{\mathrm{cable}}\right)\right].Math.\exp \left(-j\left[\left(k\right)+{}_0^{\left(\mathrm{Open}\right)}+{}_{\mathrm{Ret}}\right]\right)\\ =a_{12dB}.Math.\exp \left(j\left[{}_{\mathrm{Meas}}-{}_{\mathrm{Ref}}\right]\right).Math.\left[1+a_{.Math.}.Math.\exp \left(j{}_{\mathrm{cable}}\right)\right]\end{array}& \left(8\right)\end{array}$

(33) For the short-measurement we get:

(34) $\begin{array}{cc}\begin{array}{c}{c}^{\left(\mathrm{Meas},\mathrm{Short}\right)}\left(k\right)=b^{\left(\mathrm{Meas},\mathrm{Open}\right)}\left(k\right).Math.\exp \left(-j\arg \left\{b^{\left(\mathrm{Ret},\mathrm{Short}\right)}\left(k\right)\right\}\right)\\ =\exp \left(j\left[\left(k\right)+{}_0^{\left(\mathrm{Short}\right)}+{}_{\mathrm{Meas}}\right]\right).Math.a_{12dB}.Math.\\ \left[1-a_{.Math.}.Math.\exp \left(j{}_{\mathrm{cable}}\right)\right].Math.\exp \left(-j\left[\left(k\right)+{}_0^{\left(\mathrm{Short}\right)}+{}_{\mathrm{Ret}}\right]\right)\\ =a_{12dB}.Math.\exp \left(j\left[{}_{\mathrm{Meas}}-{}_{\mathrm{Ref}}\right]\right).Math.\left[1-a_{.Math.}.Math.\exp \left(j{}_{\mathrm{cable}}\right)\right]\end{array}& \left(9\right)\end{array}$

(35) In FIG. 2, these vectors are shown graphically. From FIG. 2, it can easily be obtained that from both vectors the absolute value (magnitude) of the damping can be calculated. From the coefficient of these two estimated values, the damping in forward and backward direction can be obtained as follows:

(36) $\begin{array}{cc}{\hat{a}}_{.Math.}=.Math.\frac{c^{\left(\mathrm{Meas},\mathrm{Open}\right)}\left(k\right)-c^{\left(\mathrm{Meas},\mathrm{Short}\right)}\left(k\right)}{c^{\left(\mathrm{Meas},\mathrm{Open}\right)}\left(k\right)+c^{\left(\mathrm{Meas},\mathrm{Short}\right)}\left(k\right)}.Math.& \left(10\right)\end{array}$

(37) By inserting this result into formulas (3) and (2), we receive the cable damping as follows:

(38) $\begin{array}{cc}\hat{x}\left[\mathrm{dB}\right]=\frac{{\hat{a}}_{.Math.}\left[\mathrm{dB}\right]}{2}-3\mathrm{dB}& \left(11\right)\end{array}$

(39) In the embodiment of FIG. 1, all samples of the reference signal are measured first and then all samples of the measurement signal are measured or vice versa before the termination of the cable 5 is switched from short to open or vice versa. However, if this start phase shifts significantly in the meantime, there is a measurement error which can be significant. In the following, a second improved embodiment is described.

(40) In the improved embodiment shown in FIG. 3, the switch 3 are switched periodically so that the measurement of the samples of the measurement signal and of the reference signal is altered several times during the total measurement period. For receiver 8, a digital low pass 8a and storage device 8b are shown in FIG. 3. The other components are identical with the embodiment of FIG. 1. During the measurement, the switch 3 switch for a block length of K.sub.Block.Math.T.sub.a. After each switching, the low pass 8a of the receiver 8 with the impulse response h.sub.TP(K) need some time in order to stabilize (no transient oscillations anymore). As soon as the analog hardware is stabilized after switching, the acquisition of the measurement values b(k) can be started and can be stored into storage device 8b.

(41) FIG. 4 shows the timing of an open-measurement or a short-measurement at one single frequency point. The figure shows the magnitude |b(t)| of the signal received by the receiver 8. First of all, the analog hardware needs to stabilize on the new frequency point. Then the acquisition of the complex values b(k) starts, which are designated by respective dots in FIG. 4.

(42) In the example shown in FIG. 4, the measurement starts with a group of samples of the reference signal of the block length of the K.sub.Block. Then the measurement is switched in order to acquire a series of samples of the measuring signal of the same block length K.sub.Block. The block lengths are identical in the embodiment shown but this does not necessarily need to be the case. When switching, in needs to be waited for a specific number of samples K.sub.Alqu during which the receiving low pass 8a is stabilizing, before valid samples can be used for the estimation of the cable damping.

(43) The valid samples are designated by K.sub.Ref and K.sub.Meas in FIG. 4. These sample values are used in the following algorithm for estimating the magnitude of the cable damping. It can be possible that the analog hardware is not already stabilized when the samples of the measuring signal and the reference signal are already acquired. However, the stabilization time of magnitude is much longer than the stabilization time of the phase. Thus, the acquisition of values for the phase estimation can be started earlier than the acquisition of samples used for estimation of the magnitude. This will safe measurement time.

(44) In FIG. 4, the label 10 designates the start of the measurement of a new frequency. The label 11 designates the start of the analog/digital-converter (ADC). The label 12 designates the switching point between measurement of the reference signal Ref and of the measuring signal Meas. As already mentioned, an additional area 13 may be present, wherein the digital filter and the analog hardware is stabilized and which is used for measuring the magnitude of the measuring signal Meas. In the area 14, the analog hardware generally stabilizes on the new measuring frequency. However, it may happen that the accuracy is not already sufficient to measure the magnitude of a measuring signal Meas. Thus, it makes sense to wait to the time area 13 in order to make magnitude measurements. K.sub.|Meas| are the time indices of the stabilized reference signal.

(45) Now, the algorithm for the improved estimation of the cable damping is described. The variable x is used to distinguish between open and short. The input vector v_b comprises all samples b(k) of one measurement at one frequency. They are shown as dots in FIG. 4.

(46) FIG. 5 shows a block diagram of an embodiment putting the algorithm into practice. The vector v_b is submitted to first selection device 20 in order to select a first part V_b.sub.Meas of the samples v_b of the measuring signal. The first selection device 20 is followed by first phase averaging device 21 in order to evaluate the averaged phase of the measuring signal .sub.Meas. The receiver 8 also comprises second selection device 23 in order to select the samples v_b.sub.Ref of the reference signal. The second selection device 23 are followed by second phase averaging device 24. In order to evaluate the averaged phase of the reference signal .sub.Ref, the phase values can be estimated as follows:
.sub.Ref=arg{{circumflex over (b)}.sup.{Ref,x}}
.sub.Meas=arg{{circumflex over (b)}.sup.{Meas,x}}(12)
The phase difference .sub.Meas.sub.Ref is calculated in subtracting device 25. Exponential device 6 calculates an imaginary exponential value of the phase difference.

(47) Further, the receiver 8 comprise third selection device 27 in order to select the sample values in the area 13 shown in FIG. 4 used for estimation of the magnitude of the measuring signal. The third selection device 27 are followed by magnitude averaging device 28 in order to evaluate the averaged magnitude |{circumflex over (b)}.sup.{Meas,x}| of the measuring signal Meas. In the embodiment shown in FIG. 5, there is a switch 29 in order to select between the values submitted by the first selection device 20 or by the third selection device 27. Thus, the magnitude can be calculated on the basis of the regular Meas values or by the special Meas values in the area 13 shown in FIG. 4 depending on the switch 29.

(48) According to equations (8) and (9), the unknown start phase in the measuring signal Meas has to be eliminated by use of the reference-signal Ref using the equation:
.sup.{Meas,x}={circumflex over (b)}.sup.{Meas,x}.Math.exp(j arg{{circumflex over (b)}.sup.(Ref,x)})(13)

(49) By inserting equations (12) the following equation is achieved:

(50) $\begin{array}{cc}\begin{array}{c}{\hat{c}}^{\left(\mathrm{Meas},x\right)}=.Math.{\hat{b}}^{\left(\mathrm{Meas},x\right)}.Math..Math.\exp \left(j\arg \left\{{\hat{b}}^{\left(\mathrm{Measf},x\right)}\right\}\right).Math.\exp \left(-j\arg \left\{{\hat{b}}^{\left(\mathrm{Ref},x\right)}\right\}\right)\\ =.Math.{\hat{b}}^{\left(\mathrm{Meas},x\right)}.Math..Math.\exp \left(j{}_{\mathrm{Meas}}\right).Math.\exp \left(-j{}_{\mathrm{Ref}}\right)\\ =.Math.{\hat{b}}^{\left(\mathrm{Meas},x\right)}.Math..Math.\exp \left(j\left({}_{\mathrm{Meas}}-{}_{\mathrm{Ref}}\right)\right)\\ =.Math.{\hat{b}}^{\left(\mathrm{Meas},x\right)}.Math..Math.\exp \left(j\right)\end{array}& \left(14\right)\end{array}$

(51) In order to do the multiplication in this equation, multiplier device 30 are available as shown in FIG. 5. By use of equation (10), the forward and backward damping can be achieved as follows:

(52) 0$\begin{array}{cc}{\hat{a}}_{.Math.}=.Math.\frac{{\hat{c}}^{\left(\mathrm{Meas},\mathrm{Open}\right)}-{\hat{c}}^{\left(\mathrm{Meas},\mathrm{Short}\right)}}{{\hat{c}}^{\left(\mathrm{Meas},\mathrm{Open}\right)}+{\hat{c}}^{\left(\mathrm{Meas},\mathrm{Short}\right)}}.Math.& \left(15\right)\end{array}$

(53) By inserting the result into equation (11), finally the cable damping can be calculated as follows:

(54) $\begin{array}{cc}\hat{x}\left[\mathrm{dB}\right]=\frac{{\hat{a}}_{.Math.}\left[\mathrm{dB}\right]}{2}-3\mathrm{dB}& \left(16\right)\end{array}$

(55) FIG. 6A illustrates the measurement scenario of the first embodiment of the invention as shown in FIG. 1. In this basic embodiment, the measurement of the reference signal Ref, which has propagated through the reference path 9, and the measurement of the measuring signal Meas, which has propagated through the splitter 4, the port 6, the cable 5, has been reflected by the open or short and has propagated back through the cable 5, the port 6 and the splitter 4, is done in sequence. This means that all values of the reference signal Ref are measured first and then all values of the measuring signal Meas are acquired. If there is, however, a shift of the phase difference (t), which is a difference between the phase of the oscillator in the transmitter 2 and the phase of the oscillator of the receiver 8, then there is a significant measurement error as indicated in FIG. 6A.

(56) In FIG. 6A, it is assumed that this phase shift (t) is linearly depending on time t. This assumption is done for a simplification. Of course, also other phase shift can occur. The average values Ref of the reference signal Ref and Meas of the measuring signal Meas are shown in FIG. 6A and it is clear from the drawing that the difference .sub.0 is quite high.

(57) FIG. 6B shows the same situation but for the scenario of the improved embodiment of FIG. 3, FIG. 4 and FIG. 5. As explained previously, the main difference between the two embodiments is that in the improved embodiment, the measurement is always alternated between measuring of the reference signal Ref and measuring of the measuring signal Meas. The same linear phase shift is assumed. It is clear from FIG. 6B that the difference .sub.0 of the phase shift (t) is much smaller compared to the situation of FIG. 6A, because it is always switched between measuring of the reference signal Ref and of the measuring Meas.

(58) FIG. 7A shows a flow chart of a first part of the inventive method. In a first step S1, a first calibration element, such as a short, is connected to at least one port of the measuring device 1. The actual frequency f is set to the start frequency f.sub.start in step S2.

(59) In step S3, a signal with the actual frequency f is submitted from the transmitter 2 of the measuring device 1 to the first calibration element and the measuring signal Meas as a return signal reflected by the first calibration element is measured by the receiver 8 of the measuring device 1.

(60) In step S4, the signal of the actual frequency f is submitted from transmitter 2 to the receiver 8 through a reference path 9 of the measuring device 1 and the reference signal Ref is measured through the reference path 9. In step S5, it is checked, whether the actual frequency has reached the end frequency f.sub.end. If not the actual frequency f is incremented by the incremental f in step S6 and the steps S3 and S4 are repeated as long as the actual frequency f reaches the end frequency f.sub.end. If yes, the algorithm proceeds with the second part.

(61) FIG. 7B shows the second part of an example, embodiment of the inventive method. In a step S7, a second calibration element, such as an open, is connected to at least one port of the measuring device 1. The actual frequency is set to start frequency f.sub.start in step S8.

(62) In step S9, a signal with the actual frequency f is submitted from the transmitter 2 of the measuring device 1 to the second calibration element and the measuring signal Meas as a return signal reflected by the first calibration element is measured by the receiver 8 of the measuring device 1.

(63) In step S10, the signal of the actual frequency f is submitted from transmitter 2 to the receiver 8 through a reference path 9 of the measuring device 1 and the reference signal Ref is measured through the reference path 9. In step S11, it is checked, whether the actual frequency has reached the end frequency f.sub.end. If not the actual frequency f is incremented by the incremental f in step S12 and the steps S9 and S10 are repeated as long as the actual frequency f reaches the end frequency f.sub.end. If yes, the algorithm ends.

(64) There are several advantages of the inventive method and device. The cable damping can be obtained with very high accuracy. The cable damping can be obtained as a function of frequency. The damping values are directly available within the measuring device 1 and no external measurement such as with a vector analyzer needs to be done. Thus, the cable 5 does not need to be disconnected from the measuring device 1. No other measuring device such as a vector network analyzer, is necessary. Destroyed cables and connectors can be detected easily. When performing the calibration process, a circuit board comprising the short and open, and also the match, can be connected with a measuring device 1 instead of the device under test. The circuit board can have the same physical extensions and scalings as the device under test. Correction can be made at the transmission side. An approximation curve can be generated. Approximating values between the frequency values, for which the inventive measurement has been performed, can be created.

(65) All features described in the above description, claimed in the following claims or drawn in the attached drawings can be combined within the scope of the present invention.

(66) While various embodiments of the present invention have been described above, it should be understood that they have been presented by way of example only, and not limitation. Numerous changes to the disclosed embodiments can be made in accordance with the disclosure herein without departing from the spirit or scope of the invention. Thus, the breadth and scope of the present invention should not be limited by any of the above described embodiments. Rather, the scope of the invention should be defined in accordance with the following claims and their equivalents.

(67) Although the invention has been illustrated and described with respect to one or more implementations, equivalent alterations and modifications will occur to others skilled in the art upon the reading and understanding of this specification and the annexed drawings. In addition, while a particular feature of the invention may have been disclosed with respect to only one of several implementations, such feature may be combined with one or more other features of the other implementations as may be desired and advantageous for any given or particular application.