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<ep-patent-document id="EP22164092B1" file="EP22164092NWB1.xml" lang="en" country="EP" doc-number="4036300" kind="B1" date-publ="20260121" status="n" dtd-version="ep-patent-document-v1-7-1">
<SDOBI lang="en"><B000><eptags><B001EP>ATBECHDEDKESFRGBGRITLILUNLSEMCPTIESILTLVFIROMKCYALTRBGCZEEHUPLSK..HRIS..MTNORS..SM..................</B001EP><B005EP>J</B005EP><B007EP>0009210-RPUB02</B007EP></eptags></B000><B100><B110>4036300</B110><B120><B121>EUROPEAN PATENT SPECIFICATION</B121></B120><B130>B1</B130><B140><date>20260121</date></B140><B190>EP</B190></B100><B200><B210>22164092.3</B210><B220><date>20200302</date></B220><B240><B241><date>20230127</date></B241><B242><date>20240202</date></B242></B240><B250>en</B250><B251EP>en</B251EP><B260>en</B260></B200><B400><B405><date>20260121</date><bnum>202604</bnum></B405><B430><date>20220803</date><bnum>202231</bnum></B430><B450><date>20260121</date><bnum>202604</bnum></B450><B452EP><date>20250829</date></B452EP></B400><B500><B510EP><classification-ipcr sequence="1"><text>D06F  33/76        20200101AFI20250728BHEP        </text></classification-ipcr><classification-ipcr sequence="2"><text>D06F  34/16        20200101ALI20250728BHEP        </text></classification-ipcr><classification-ipcr sequence="3"><text>D06F  58/52        20200101ALI20250728BHEP        </text></classification-ipcr><classification-ipcr sequence="4"><text>D06F 103/24        20200101ALN20250728BHEP        </text></classification-ipcr><classification-ipcr sequence="5"><text>D06F 103/46        20200101ALN20250728BHEP        </text></classification-ipcr><classification-ipcr sequence="6"><text>D06F 105/62        20200101ALN20250728BHEP        </text></classification-ipcr><classification-ipcr sequence="7"><text>D06F 105/48        20200101ALN20250728BHEP        </text></classification-ipcr><classification-ipcr sequence="8"><text>D06F 105/52        20200101ALN20250728BHEP        </text></classification-ipcr></B510EP><B520EP><classifications-cpc><classification-cpc sequence="1"><text>D06F  33/76        20200201 FI20200629BHEP        </text></classification-cpc><classification-cpc sequence="2"><text>D06F  34/16        20200201 LI20200629BHEP        </text></classification-cpc><classification-cpc sequence="3"><text>D06F2103/24        20200201 LA20200629BHEP        </text></classification-cpc><classification-cpc sequence="4"><text>D06F2103/46        20200201 LA20200629BHEP        </text></classification-cpc><classification-cpc sequence="5"><text>D06F2105/62        20200201 LA20200629BHEP        </text></classification-cpc><classification-cpc sequence="6"><text>D06F  58/52        20200201 LI20200629BHEP        </text></classification-cpc><classification-cpc sequence="7"><text>D06F2105/52        20200201 LA20200629BHEP        </text></classification-cpc><classification-cpc sequence="8"><text>D06F2105/48        20200201 LA20200629BHEP        </text></classification-cpc></classifications-cpc></B520EP><B540><B541>de</B541><B542>VERFAHREN ZUR SCHÄTZUNG EINES LASTVERHALTENS IN EINER WÄSCHEBEHANDLUNGSMASCHINE UND WÄSCHEBEHANDLUNGSMASCHINE</B542><B541>en</B541><B542>METHOD TO ESTIMATE A LOAD BEHAVIOR IN A LAUNDRY TREATMENT MACHINE AND LAUNDRY TREATMENT MACHINE</B542><B541>fr</B541><B542>PROCÉDÉ D'ESTIMATION DE COMPORTEMENT D'UNE CHARGE DANS UNE MACHINE DE TRAITEMENT DE LINGE ET MACHINE DE TRAITEMENT DE LINGE</B542></B540><B560><B561><text>EP-A2- 2 607 535</text></B561><B561><text>DE-A1- 102008 055 091</text></B561><B561><text>US-A1- 2019 112 745</text></B561></B560></B500><B600><B620><parent><pdoc><dnum><anum>20160332.1</anum><pnum>3875661</pnum></dnum><date>20200302</date></pdoc></parent></B620></B600><B700><B720><B721><snm>Martinello, Daniele</snm><adr><city>90411 Nürnberg</city><ctry>DE</ctry></adr></B721><B721><snm>Bobek, Viktor</snm><adr><city>90491 Nürnberg</city><ctry>DE</ctry></adr></B721><B721><snm>Petracek, Pavol</snm><adr><city>90482 Nürnberg</city><ctry>DE</ctry></adr></B721></B720><B730><B731><snm>HAIER Germany GmbH</snm><iid>101938748</iid><irf>P201711EP</irf><adr><str>Konrad-Zuse-Platz 6</str><city>81829 München</city><ctry>DE</ctry></adr></B731></B730><B740><B741><snm>Rau, Schneck &amp; Hübner
Patentanwälte Rechtsanwälte PartGmbB</snm><iid>101189752</iid><adr><str>Königstraße 2</str><city>90402 Nürnberg</city><ctry>DE</ctry></adr></B741></B740></B700><B800><B840><ctry>AL</ctry><ctry>AT</ctry><ctry>BE</ctry><ctry>BG</ctry><ctry>CH</ctry><ctry>CY</ctry><ctry>CZ</ctry><ctry>DE</ctry><ctry>DK</ctry><ctry>EE</ctry><ctry>ES</ctry><ctry>FI</ctry><ctry>FR</ctry><ctry>GB</ctry><ctry>GR</ctry><ctry>HR</ctry><ctry>HU</ctry><ctry>IE</ctry><ctry>IS</ctry><ctry>IT</ctry><ctry>LI</ctry><ctry>LT</ctry><ctry>LU</ctry><ctry>LV</ctry><ctry>MC</ctry><ctry>MK</ctry><ctry>MT</ctry><ctry>NL</ctry><ctry>NO</ctry><ctry>PL</ctry><ctry>PT</ctry><ctry>RO</ctry><ctry>RS</ctry><ctry>SE</ctry><ctry>SI</ctry><ctry>SK</ctry><ctry>SM</ctry><ctry>TR</ctry></B840></B800></SDOBI>
<description id="desc" lang="en"><!-- EPO <DP n="1"> -->
<p id="p0001" num="0001">The invention relates to a method to estimate a load behavior in a laundry treatment machine. Furthermore, the invention relates to a laundry treatment machine with a control unit to estimate a load behavior. For example, the laundry treatment machine is a washing machine or a drying machine or a combined washing and drying machine.</p>
<p id="p0002" num="0002">The estimation of a load inertia at the beginning of a washing cycle has a key role to set the amount of resources such as water, detergent, bleach and softener and the amount of energy in order to achieve a good washing performance without wasting resources and energy. The load inertia is caused by the laundry within the drum of the laundry treatment machine and varies in a wide range.</p>
<p id="p0003" num="0003">The washing unit is suspended to the cabinet by a set of springs and dampers. This mechanical system is adjusted to have a resonance frequency at a relatively low angular speed between 150 rpm and 300 rpm. During the spinning phase, the angular speed of the drum has to cross this resonance region without interference between the tub and the cabinet. Due to an increase of the drum size and a loading capacity of the laundry treatment machine the available space between the tub and the cabinet decreased. As a consequence, a precise estimation of a load unbalance is required in order to avoid a mechanical impact between the tub and the cabinet when the resonance region is crossed.</p>
<p id="p0004" num="0004"><patcit id="pcit0001" dnum="US2005204482A1"><text>US 2005/204482 A1</text></patcit> discloses a method to estimate a load inertia and a load unbalance. The estimation is based on an angular speed signal and a torque signal during an acceleration of the drum or during superimposition<!-- EPO <DP n="2"> --> of a dither signal to a substantially constant angular speed in order to excite the mechanical system of the laundry treatment machine.</p>
<p id="p0005" num="0005"><patcit id="pcit0002" dnum="EP2607535A2"><text>EP 2 607 535 A2</text></patcit> discloses a method of operating a laundry treating appliance comprising at least one cycle of operation controlling the extraction of liquid from the laundry load on the basis of the inertia of the laundry load. <patcit id="pcit0003" dnum="US20190112745A1"><text>US 2019/0112745 A1</text></patcit> discloses a method of operating a laundry washing machine.</p>
<p id="p0006" num="0006">It is an object of the present invention to provide a method to estimate a load behavior in a laundry treatment machine in an easy, reliable and accurate manner.</p>
<p id="p0007" num="0007">This object is achieved by a method comprising the steps of claim 1. According to the inventive method the inertia and the load torque is determined based on two operations of the laundry treatment machine with two different speed controller parameters and bandwidths of the speed controller. The speed controller regulates the angular speed of the drive motor an is part of the speed control loop. The first operation can be described by <maths id="math0001" num="(1)"><math display="block"><mo>−</mo><msub><mover accent="true"><mi>T</mi><mo>^</mo></mover><mi>L</mi></msub><mo>+</mo><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup><mo>=</mo><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>t</mi></msub><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0001" file="imgb0001.tif" wi="133" he="6" img-content="math" img-format="tif"/></maths> and the second operation can be described by <maths id="math0002" num="(2),"><math display="block"><mo>−</mo><msub><mover accent="true"><mi>T</mi><mo>^</mo></mover><mi>L</mi></msub><mo>+</mo><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup><mo>=</mo><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>t</mi></msub><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0002" file="imgb0002.tif" wi="134" he="6" img-content="math" img-format="tif"/></maths> wherein<!-- EPO <DP n="3"> -->
<br/>
<maths id="math0003" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0003" file="imgb0003.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths>  denotes the first torque signal,<br/>
<maths id="math0004" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0004" file="imgb0004.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths>  denotes the derivative of the first angular speed signal,<br/>
<maths id="math0005" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0005" file="imgb0005.tif" wi="9" he="6" img-content="math" img-format="tif" inline="yes"/></maths>  denotes the second torque signal,<br/>
<maths id="math0006" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0006" file="imgb0006.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths>  denotes the derivative of the second angular speed signal,<br/>
<i>T̂<sub>L</sub></i>  denotes the load torque and<!-- EPO <DP n="4"> --><br/>
<i>Ĵ<sub>t</sub></i>  denotes the total inertia of the laundry treatment machine with regard to a rotation around the rotational axis.</p>
<p id="p0008" num="0008">Based on equations (1) and (2) the total inertia can be evaluated by <maths id="math0007" num="(3)."><math display="block"><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>t</mi></msub><mo>=</mo><mfrac><mrow><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup><mo>−</mo><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></mrow><mrow><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover><mo>−</mo><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></mrow></mfrac></math><img id="ib0007" file="imgb0007.tif" wi="135" he="9" img-content="math" img-format="tif"/></maths></p>
<p id="p0009" num="0009">The load inertia can be evaluated by <maths id="math0008" num="(4),"><math display="block"><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>L</mi></msub><mo>=</mo><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>t</mi></msub><mo>−</mo><msub><mi>J</mi><mi>m</mi></msub></math><img id="ib0008" file="imgb0008.tif" wi="135" he="6" img-content="math" img-format="tif"/></maths> wherein
<dl id="dl0001" compact="compact">
<dt><i>Ĵ<sub>L</sub></i></dt><dd>denotes the load inertia and</dd>
<dt><i>J<sub>m</sub></i></dt><dd>denotes the inertia of the laundry treatment machine.</dd>
</dl></p>
<p id="p0010" num="0010">The inertia <i>J<sub>m</sub></i> of the laundry treatment machine is known from construction data or can be measured by running a test without a distributed load inside the drum.</p>
<p id="p0011" num="0011">Furthermore, in case that the load inertia is evaluated according to equation (4), the load torque can be determined, for example according to equation (1) and/or equation (2) and/or by means of a load observer as soon as the total inertia <i>Ĵ<sub>t</sub></i> is estimated according to equation (3) and the load torque observer is parametrized accordingly.</p>
<p id="p0012" num="0012">The load torque observer enables an accurate and continuous estimation of the load torque. The load torque observer can be easily implemented into a<!-- EPO <DP n="5"> --> control unit of a laundry treatment machine. Additional hardware components, like sensors, are not required.</p>
<p id="p0013" num="0013">The advantages of the inventive method are as follows:<br/>
The load inertia and the total inertia can be evaluated at a constant angular speed, for example at 100 rpm, in order to avoid the use of an acceleration ramp and to avoid the risk of a mechanical impact between the tub and the cabinet. The same applies for the estimation of a load unbalance based on the load torque. The method can be used to estimate the dry load at the beginning of the washing cycle without using an acceleration ramp in order to set the amount of resources and energy. In case of a combined washing and drying machine or a drying machine the inertia estimation can be used to stop the drying cycle at a desired moisture retention. Furthermore, the inventive method can be used to estimate the wet load at the end of the washing cycle without using an acceleration ramp. The estimated load torque and an estimation of the load unbalance based thereon can be automatically adapted with the estimated total inertia. The inventive method can be used in a laundry treatment machine with a large drum and can be easily implemented in existing control units. The estimation of the inertia and/or the load torque is not affected by friction or by the speed controller setting. Furthermore, the estimation of the inertia and/or the load torque just requires an operation of the laundry treatment machine at a constant angular speed without the need of an acceleration ramp such that the inertia and/or the load torque can be estimated in an easy and quick manner.</p>
<p id="p0014" num="0014">A method according to claim 2 ensures an easy, reliable and accurate estimation of the load behavior. The desired angular speed or the target speed is constant. The resulting speed fluctuations or speed oscillations depend<!-- EPO <DP n="6"> --> on the bandwidth of the speed controller and/or on the controller parameters of the speed controller, on the mass of the load and on the total inertia. A change of the speed controller parameters that changes the bandwidth of the speed controller at a constant desired angular speed results in a change of the speed oscillations and of the drive torque. The angular speed oscillations about the constant desired angular speed could be, as example, within +- 10 rpm, or within +- 5 rpm, or within +- 2 rpm.</p>
<p id="p0015" num="0015">A method according to claim 3 ensures an easy, reliable and accurate estimation of the load behavior. The mass of the load can be estimated in an easy and accurate manner depending on the load torque. The unbalance mass can be estimated by <maths id="math0009" num="(5),"><math display="block"><mover accent="true"><mi>m</mi><mo>^</mo></mover><mo>=</mo><mfrac><mrow><mi>max</mi><mfenced><msub><mover accent="true"><mi>T</mi><mo>^</mo></mover><mi>L</mi></msub></mfenced></mrow><mrow><mi>g</mi><mo>⋅</mo><mi>r</mi></mrow></mfrac></math><img id="ib0009" file="imgb0009.tif" wi="134" he="9" img-content="math" img-format="tif"/></maths> wherein
<dl id="dl0002" compact="compact">
<dt><i>m̂</i></dt><dd>denotes the mass of the load which corresponds to the unbalance mass,</dd>
<dt>max(<i>T̂<sub>L</sub></i>)</dt><dd>denotes the maximum of the load torque,</dd>
<dt><i>g</i></dt><dd>denotes the gravitational acceleration and</dd>
<dt>r</dt><dd>denotes the drum radius.</dd>
</dl></p>
<p id="p0016" num="0016">A method according to claim 4 ensures an easy, reliable and accurate estimation of the load behavior. The angular load position can be estimated by solving <maths id="math0010" num="(6),"><math display="block"><msub><mover accent="true"><mi>T</mi><mo>^</mo></mover><mi>L</mi></msub><mo>=</mo><mo>−</mo><mover accent="true"><mi>m</mi><mo>^</mo></mover><mspace width="1ex"/><mi>g</mi><mspace width="1ex"/><mi>r</mi><mspace width="1ex"/><mi>sin</mi><mfenced separators=""><mover accent="true"><mi>Θ</mi><mo>^</mo></mover><mo>+</mo><mover accent="true"><mi>σ</mi><mo>^</mo></mover></mfenced></math><img id="ib0010" file="imgb0010.tif" wi="134" he="6" img-content="math" img-format="tif"/></maths><!-- EPO <DP n="7"> --> wherein
<dl id="dl0003" compact="compact">
<dt><i>Θ̂</i></dt><dd>denotes the angular drum position in relation to a reference position,</dd>
<dt><i>σ̂</i></dt><dd>denotes the angular relative load position inside the drum,</dd>
<dt><i>T̂<sub>L</sub></i></dt><dd>denotes the load torque,</dd>
<dt><i>m̂</i></dt><dd>denotes the mass of the load which corresponds to the unbalance mass,</dd>
<dt><i>g</i></dt><dd>denotes the gravitational acceleration and</dd>
<dt>r</dt><dd>denotes the drum radius.</dd>
</dl></p>
<p id="p0017" num="0017">The angular load position can be described by <maths id="math0011" num=""><math display="block"><mover accent="true"><mi>α</mi><mo>^</mo></mover><mo>=</mo><mover accent="true"><mi>θ</mi><mo>^</mo></mover><mo>+</mo><mover accent="true"><mi>σ</mi><mo>^</mo></mover><mo>,</mo></math><img id="ib0011" file="imgb0011.tif" wi="24" he="6" img-content="math" img-format="tif"/></maths> wherein
<ul id="ul0001" list-style="none" compact="compact">
<li><i>α̂</i> denotes the angular position of the load in relation to the reference position</li>
<li>such that <maths id="math0012" num=""><math display="block"><msub><mover accent="true"><mi>T</mi><mo>^</mo></mover><mi>L</mi></msub><mo>=</mo><mo>−</mo><mover accent="true"><mi>m</mi><mo>^</mo></mover><mspace width="1ex"/><mi>g</mi><mspace width="1ex"/><mi>r</mi><mspace width="1ex"/><mi>cos</mi><mfenced><mover accent="true"><mi>α</mi><mo>^</mo></mover></mfenced></math><img id="ib0012" file="imgb0012.tif" wi="40" he="6" img-content="math" img-format="tif"/></maths></li>
<li>since the load torque has a maximum value, if <i>α̂</i> = 90°.</li>
</ul><!-- EPO <DP n="8"> --></p>
<p id="p0018" num="0018">A method according to claim 5 ensures an easy, reliable and accurate estimation of the load behavior. The total inertia can be easily estimated according to equation (3). Furthermore, the load inertia can be easily estimated according to equation (4).</p>
<p id="p0019" num="0019">A method according to claim 6 ensures an easy, reliable and accurate estimation of the load behavior. The signals are transformed into a frequency domain, in particular by computing a Fourier Transformation (FT). This transformation enables to determine respective first harmonics of the signals. The first harmonics are used for the subsequent determination of the inertia and/or the load torque. The determination of the inertia and/or the load torque is not affected by noise signals. The first harmonics comprise information about the frequency, the amplitude and the phase of the signals. At least one of the frequency, the amplitude and the phase are used for the subsequent estimation of the inertia and/or the load torque.</p>
<p id="p0020" num="0020">A method according to claim 7 ensures an easy, reliable an accurate estimation of the load behavior. By using the first harmonics of the signals the estimation of the inertia and/or the load torque is not affected by noise signals. The first harmonics of the signals are calculated for example by a Fourier Transformation (FT). The first harmonics comprise information about the frequency, the amplitude and the phase of the signals. At least one of the frequency, the amplitude and the phase are used for the subsequent estimation of the inertia and/or the load torque.</p>
<p id="p0021" num="0021">A method according to claim 8 ensures an easy, reliable and accurate estimation of the load behavior. The angular position and/or the drive torque of the drive motor can either be measured or estimated. The angular position is used to calculate an observer error.<!-- EPO <DP n="9"> --></p>
<p id="p0022" num="0022">A method according to claim 9 ensures an easy, reliable and accurate estimation of the load behavior. The observer error is used to estimate and/or correct internal states of the load torque observer. The internal states of the load torque observer are in particular the observed angular position, an observed angular acceleration and the load torque. The observer error is multiplied with observer coefficients or observer gains. The observer coefficients are used to adapt the accuracy and the behavior of the load torque observer.</p>
<p id="p0023" num="0023">A method according to claim 10 ensures an easy, reliable and accurate estimation of the load behavior. The observer error is multiplied with observer coefficients or observer gains in order to calculate observer signals. These observer signals are used to estimate and/or correct the internal states of the observer. A first observer signal is calculated by multiplying a derivative of the observer error with a first observer coefficient. A second observer signal is calculated by multiplying the observer error with a second observer coefficient. Furthermore, a third observer signal is calculated by multiplying the observer error with a third observer coefficient and by integrating the resulting signal. The load torque depends on the sum of the first observer signal, the second observer signal and the third observer signal.</p>
<p id="p0024" num="0024">A method according to claim 11 ensures an easy, reliable and accurate estimation of the load behavior. An observed angular acceleration and in consequence the observed angular position depends on the total inertia of the laundry treatment machine and the load. The total inertia is estimated according to equation (3). The total inertia can be adapted during the operation of the laundry treatment machine, if necessary. For example, the total inertia increases depending on the wetness of the laundry.<!-- EPO <DP n="10"> --></p>
<p id="p0025" num="0025">A method according to claim 12 ensures an easy, reliable and accurate estimation of the load behavior. Sensorless drive motors are well known and do not comprise an angular position sensor and an angular speed sensor. Hence, the angular position of the drive motor is estimated, for example by means of a position and/or speed estimator or a position and/or speed observer. The load torque observer is preferably provided with an estimated angular position of the drive motor.</p>
<p id="p0026" num="0026">A method according to claim 13 ensures an easy, reliable and accurate estimation of the load behavior. The load torque observer is provided with the desired drive torque of the drive motor. An output signal of the speed controller is used to estimate the drive torque. This output signal characterizes the desired electromagnetic drive torque of the drive motor and can be used to estimate the drive torque and/or the load torque which acts on the drum.</p>
<p id="p0027" num="0027">Furthermore, it is an object of the present invention to provide a laundry treatment machine which enables to estimate a load behavior in an easy, reliable and accurate manner.</p>
<p id="p0028" num="0028">This object is achieved by a laundry treatment machine with the features of claim 14. The advantages of the laundry treatment machine according to the invention correspond to the advantages already described in connection with the method according to the invention.</p>
<p id="p0029" num="0029">Further features, advantages and details of the invention will be apparent from the following description of an embodiment which refers to the accompanying drawings.<!-- EPO <DP n="11"> -->
<dl id="dl0004">
<dt>Fig. 1</dt><dd>shows a schematic view of a laundry treatment machine with a drum, a drive motor and a control unit,</dd>
<dt>Fig. 2</dt><dd>shows a schematic cross sectional view of the drum with a load located inside the drum,</dd>
<dt>Fig. 3</dt><dd>shows a block diagram of a controller and a load torque observer implemented in the control unit,</dd>
<dt>Fig. 4</dt><dd>shows a block diagram of the load torque observer in <figref idref="f0003">Fig. 3</figref>,</dd>
<dt>Fig. 5</dt><dd>shows a flow chart of a method to estimate a total inertia of the laundry treatment machine and the load with respect to a rotation of the drum around a rotational axis,</dd>
<dt>Fig. 6</dt><dd>shows a time diagram of an angular speed and a drive torque of the drive motor during a first operation and a second operation of the laundry treatment machine in order to estimate the total inertia according to the flow chart in <figref idref="f0005">Fig. 5</figref>,</dd>
<dt>Fig. 7</dt><dd>shows a first torque signal and a first angular acceleration signal during a first operation and a second torque signal and a second angular acceleration signal during a second operation of the laundry treatment machine as well as a torque difference signal and an acceleration difference signal depending on the angular position of the drum in order to estimate the total inertia, and<!-- EPO <DP n="12"> --></dd>
<dt>Fig. 8</dt><dd>shows an estimated load torque depending on an angular position of the drum.</dd>
</dl></p>
<p id="p0030" num="0030"><figref idref="f0001">Fig. 1</figref> shows a laundry treatment machine, namely a washing machine 1 with a cabinet 2 and a washing unit 3. The washing unit 3 comprises a tub 4 and a drum 5. The tub 4 is mounted to the cabinet 2 via dampers 6 and springs 7.</p>
<p id="p0031" num="0031">The drum 5 is mounted in a rotatable manner to the tub 4. The drum 5 is connected via a drive shaft 8 with a drive motor 9. The drive motor 9 is mounted at a backside of the tub 4. The drive motor 9 rotates the drum 5 around a horizontal rotational axis 10.</p>
<p id="p0032" num="0032">The washing machine 1 comprises several lifters 11 to move the laundry. The lifters 11 are mounted in equal angular distances to an inner side of the drum 5.</p>
<p id="p0033" num="0033">Furthermore, the washing machine 1 comprises a control unit 12 to control the operation of the washing machine 1. The drive motor 9 has an angular position Θ, an angular speed ω and an angular acceleration ω̇. Due to the stiff drive shaft 8 the angular position, the angular speed and the angular acceleration of the drum 5 corresponds to the angular position Θ, the angular speed ω and the angular acceleration ω̇. In case of belt driven motor, the pulley ratio will be used to evaluate the angular position, the angular speed and the angular acceleration of the drum starting from the angular position, the angular speed and the angular acceleration of the motor.<!-- EPO <DP n="13"> --></p>
<p id="p0034" num="0034">The load L, namely the laundry inside the drum 5 produces a load torque T<sub>L</sub>. In case that the angular speed of the drum 5 is higher than a satelization speed the load torque T<sub>L</sub> can be described by <maths id="math0013" num="(7),"><math display="block"><msub><mi>T</mi><mi>L</mi></msub><mo>=</mo><mo>−</mo><mi mathvariant="italic">mgr</mi><mspace width="1ex"/><mi>sin</mi><mfenced separators=""><mi mathvariant="normal">θ</mi><mo>+</mo><mi mathvariant="normal">σ</mi></mfenced></math><img id="ib0013" file="imgb0013.tif" wi="134" he="5" img-content="math" img-format="tif"/></maths> wherein
<dl id="dl0005" compact="compact">
<dt>m</dt><dd>denotes the real mass of the load L,</dd>
<dt>g</dt><dd>denotes the gravitational acceleration,</dd>
<dt>r</dt><dd>denotes the drum radius,</dd>
<dt>Θ</dt><dd>denotes the angular position of the drum in relation to a reference position Θ<sub>0</sub>, and</dd>
<dt>σ</dt><dd>denotes the angular relative position of the load L inside the drum, namely an angle between the position of the load L and a drum reference position.</dd>
</dl></p>
<p id="p0035" num="0035">The angular position α of the load L can be described by <maths id="math0014" num="(8),"><math display="block"><mi mathvariant="normal">α</mi><mo>=</mo><mi mathvariant="normal">Θ</mi><mo>+</mo><mi mathvariant="normal">σ</mi></math><img id="ib0014" file="imgb0014.tif" wi="134" he="5" img-content="math" img-format="tif"/></maths> wherein
<dl id="dl0006" compact="compact">
<dt>α</dt><dd>denotes the angular position of the load L in relation to the reference position θ<sub>0</sub>.</dd>
</dl><!-- EPO <DP n="14"> --></p>
<p id="p0036" num="0036">The angular positions σ and α and the mass m are unknown. The gravitational acceleration g and the drum radius r are known. The load torque T<sub>L</sub> has a maximum value if α = 90° such that <maths id="math0015" num=""><math display="block"><msub><mi>T</mi><mi>L</mi></msub><mo>=</mo><mo>−</mo><mi mathvariant="italic">mgr</mi><mspace width="1ex"/><mi>cos</mi><mfenced><mi>α</mi></mfenced><mo>.</mo></math><img id="ib0015" file="imgb0015.tif" wi="38" he="5" img-content="math" img-format="tif"/></maths></p>
<p id="p0037" num="0037">The drive motor 9 creates a drive torque <i>T<sub>em</sub></i> which accelerates the drum 5.</p>
<p id="p0038" num="0038">The drive torque T<sub>em</sub> is superimposed by the load torque T<sub>L</sub>.</p>
<p id="p0039" num="0039">The control unit 12 comprises a speed controller 13, a torque controller 14, a first coordinate transformation 15, a pulse width modulator 16, a position and speed observer 17, a second coordinate transformation 18 and a load torque observer 19.</p>
<p id="p0040" num="0040">The torque controller 14 is part of an inner control loop or a torque control loop to control the drive torque <i>T<sub>em</sub></i> of the drive motor 9. For example, the torque controller 14 is a PI controller. The torque controller 14 is provided with a desired drive torque <maths id="math0016" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>∗</mo></msubsup></math><img id="ib0016" file="imgb0016.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths> and the drive motor currents which are denoted in common with i<sub>abc</sub>. The drive motor currents i<sub>abc</sub> are transformed by means of the second coordinate transformation 18 into a dq coordinate system. The corresponding currents are denoted in common with i<sub>dq</sub>. The torque controller 14 creates in the dq coordinate system desired voltages which are denoted in common with v*<sub>dq</sub>. The voltages v*<sub>aq</sub> are transformed by means of the first coordinate transformation 15 into desired voltages in an abc coordinate system which are denoted in common with v<sub>abc</sub>. The voltages v<sub>abc</sub> are provided to the pulse width modulator 16 which creates via a switch circuit currents i<sub>a</sub>, i<sub>b</sub>, i<sub>c</sub> to operate the drive motor 9 with a torque <i>T<sub>em</sub></i> which corresponds to the desired torque <maths id="math0017" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>∗</mo></msubsup></math><img id="ib0017" file="imgb0017.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths><i>.</i><!-- EPO <DP n="15"> --></p>
<p id="p0041" num="0041">The drive motor 9 is designed sensorless, namely without a speed sensor and a torque sensor. Therefore, the position and speed observer 17 is used to produce an estimated angular position <i>Θ̂</i> and an estimated angular speed ω̂. The position and speed observer 17 is provided with the voltages v<sub>abc</sub> and the currents i<sub>abc</sub>. The estimated angular position <i>Θ̂</i> is provided to the first coordinate transformation 15 and the second coordinate transformation 18.</p>
<p id="p0042" num="0042">The speed controller 13 is part of an outer control loop or a speed control loop. The speed controller 13 is provided with the difference of a desired angular speed ω* and the estimated angular speed ω̂. The output signal of the speed controller 13 is the desired drive torque <maths id="math0018" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>∗</mo></msubsup></math><img id="ib0018" file="imgb0018.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths><i>.</i></p>
<p id="p0043" num="0043">The load torque observer 19 evaluates an estimated load torque <i>T̂<sub>L</sub>.</i> The load torque observer 19 is provided with the desired drive torque <maths id="math0019" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>∗</mo></msubsup></math><img id="ib0019" file="imgb0019.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths> and the estimated angular position <i>Θ̂</i> as input signals. The load torque observer 19 calculates an observer error <i>e<sub>obs</sub></i> which is the difference of the estimated angular position <i>Θ̂</i> and an observed angular position <i>Θ<sub>obs</sub>.</i></p>
<p id="p0044" num="0044">The load torque observer 19 calculates three observer signals k<sub>1</sub>, k<sub>2</sub> and k<sub>3</sub>. These observer signals can be described by: <maths id="math0020" num="(9),"><math display="block"><msub><mi mathvariant="normal">k</mi><mn>1</mn></msub><mo>=</mo><mi mathvariant="normal">K</mi><mn>1</mn><mo>⋅</mo><mi mathvariant="normal">s</mi><mo>⋅</mo><msub><mi>e</mi><mi mathvariant="italic">obs</mi></msub></math><img id="ib0020" file="imgb0020.tif" wi="134" he="5" img-content="math" img-format="tif"/></maths> <maths id="math0021" num="(10),"><math display="block"><msub><mi mathvariant="normal">k</mi><mn>2</mn></msub><mo>=</mo><mi mathvariant="normal">K</mi><mn>2</mn><mo>⋅</mo><msub><mi>e</mi><mi mathvariant="italic">obs</mi></msub></math><img id="ib0021" file="imgb0021.tif" wi="135" he="5" img-content="math" img-format="tif"/></maths> <maths id="math0022" num="(11),"><math display="block"><msub><mi mathvariant="normal">k</mi><mn>3</mn></msub><mo>=</mo><mi mathvariant="normal">K</mi><mn>3</mn><mo>/</mo><mi mathvariant="normal">s</mi><mo>⋅</mo><msub><mi>e</mi><mi mathvariant="italic">obs</mi></msub></math><img id="ib0022" file="imgb0022.tif" wi="135" he="5" img-content="math" img-format="tif"/></maths><!-- EPO <DP n="16"> --> wherein
<ul id="ul0002" list-style="none" compact="compact">
<li>k<sub>1</sub> denotes a first observer coefficient,</li>
<li>k<sub>2</sub> denotes a second observer coefficient,</li>
<li>k<sub>3</sub> denotes a third observer coefficient,</li>
<li>s denotes a derivator, and</li>
<li>1/s denotes an integrator.</li>
</ul></p>
<p id="p0045" num="0045">The observer coefficients are for example set to <maths id="math0023" num=""><math display="block"><mi mathvariant="normal">K</mi><mn>1</mn><mo>=</mo><mn>64</mn><mo>,</mo></math><img id="ib0023" file="imgb0023.tif" wi="17" he="5" img-content="math" img-format="tif"/></maths> <maths id="math0024" num=""><math display="block"><mi mathvariant="normal">K</mi><mn>2</mn><mo>=</mo><mn>13</mn><mo>,</mo></math><img id="ib0024" file="imgb0024.tif" wi="17" he="5" img-content="math" img-format="tif"/></maths> and <maths id="math0025" num=""><math display="block"><mi mathvariant="normal">K</mi><mn>3</mn><mo>=</mo><mn>5</mn><mo>.</mo></math><img id="ib0025" file="imgb0025.tif" wi="15" he="4" img-content="math" img-format="tif"/></maths></p>
<p id="p0046" num="0046">The estimated load torque <i>T<sub>L</sub></i> can be calculated by <maths id="math0026" num="(12)."><math display="block"><msub><mover accent="true"><mi>T</mi><mo>^</mo></mover><mi>L</mi></msub><mo>=</mo><mo>−</mo><mfenced separators=""><msub><mi>k</mi><mn>1</mn></msub><mo>+</mo><msub><mi>k</mi><mn>2</mn></msub><mo>+</mo><msub><mi>k</mi><mn>3</mn></msub></mfenced></math><img id="ib0026" file="imgb0026.tif" wi="135" he="6" img-content="math" img-format="tif"/></maths></p>
<p id="p0047" num="0047">The load torque observer 19 calculates an observed angular acceleration ω̇<i><sub>obs</sub></i> by <maths id="math0027" num="(13),"><math display="block"><msub><mover accent="true"><mi mathvariant="normal">ω</mi><mo>˙</mo></mover><mi mathvariant="italic">obs</mi></msub><mo>=</mo><mfrac><mn>1</mn><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>t</mi></msub></mfrac><mo>⋅</mo><mfenced separators=""><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>*</mo></msubsup><mo>−</mo><msub><mover accent="true"><mi>T</mi><mo>^</mo></mover><mi>L</mi></msub></mfenced></math><img id="ib0027" file="imgb0027.tif" wi="135" he="9" img-content="math" img-format="tif"/></maths> wherein<br/>
<i>Ĵ<sub>t</sub></i> is the total inertia of those parts of the washing machine 1 which rotate around the rotational axis 10, in particular of the drum 5 with the balancers<!-- EPO <DP n="17"> --> 11, of the drive shaft 8, of the drive motor 9, and of the load L. The total inertia can be described by<maths id="math0028" num="(14),"><math display="block"><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>t</mi></msub><mo>=</mo><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>L</mi></msub><mo>+</mo><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>m</mi></msub></math><img id="ib0028" file="imgb0028.tif" wi="140" he="12" img-content="math" img-format="tif"/></maths> wherein<br/>
<i>Ĵ<sub>L</sub></i> denotes the load inertia and <i>J<sub>m</sub></i> denotes the inertia of the washing machine 1. The inertia of the washing machine 1 is known from construction data.</p>
<p id="p0048" num="0048">The load torque observer 19 calculates an observed angular speed ω<i><sub>obs</sub></i> by integrating the observed angular acceleration ω̇<i><sub>obs</sub></i>. Furthermore, the load torque observer 19 calculates the observed angular position <i>Θ<sub>obs</sub></i> by integrating the observed angular speed <i>ω<sub>obs</sub></i>.</p>
<p id="p0049" num="0049">In the following the estimation of the total inertia <i>Ĵ<sub>t</sub></i> is described in detail:<br/>
In step S<sub>1</sub> the speed controller 13 is parametrized with first controller parameters P<sub>1</sub>. For example, the speed controller 13 is a PI controller.</p>
<p id="p0050" num="0050">In a second step S<sub>2</sub> the drum 5 is accelerated by means of the drive motor 9 as example from 0 rpm to 100 rpm.</p>
<p id="p0051" num="0051">Afterwards, in a third step S<sub>3</sub> the drum 5 is rotated with an essentially constant drum speed ω. During the third step S<sub>3</sub> the control unit 12 transforms the desired drive torque <maths id="math0029" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>*</mo></msubsup></math><img id="ib0029" file="imgb0029.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths> and the estimated angular speed ω̂ into the frequency<!-- EPO <DP n="18"> --> domain by calculating a Fourier Transformation. The first harmonic of the desired drive torque <maths id="math0030" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>*</mo></msubsup></math><img id="ib0030" file="imgb0030.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths> is stored in the control unit 12 and is denoted <maths id="math0031" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0031" file="imgb0031.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths><i>.</i> Furthermore, the first harmonic information, for example the frequency, the amplitude and the phase, of the estimated angular speed ω̂ are used to get an estimated angular acceleration which is denoted <maths id="math0032" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0032" file="imgb0032.tif" wi="6" he="5" img-content="math" img-format="tif" inline="yes"/></maths>. The estimated angular acceleration <maths id="math0033" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0033" file="imgb0033.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> is stored in the control unit 12.</p>
<p id="p0052" num="0052">Afterwards, in a step S<sub>4</sub> the speed controller 13 is parametrized with second controller parameters P<sub>2</sub>.</p>
<p id="p0053" num="0053">Afterwards, in a fifth step S<sub>5</sub> the drum 5 is rotated with an essentially constant drum speed ω. During the step S<sub>5</sub> the control unit 12 transforms the desired drive torque <maths id="math0034" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>*</mo></msubsup></math><img id="ib0034" file="imgb0034.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths> and the estimated angular speed ω̂ into the frequency domain by calculating a Fourier Transformation. The first harmonic of the desired drive torque <maths id="math0035" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>*</mo></msubsup></math><img id="ib0035" file="imgb0035.tif" wi="8" he="5" img-content="math" img-format="tif" inline="yes"/></maths> is stored in the control unit 12 and is denoted <maths id="math0036" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0036" file="imgb0036.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths><i>.</i> Furthermore, the first harmonic information, for example the frequency, the amplitude and the phase, of the estimated angular speed ω̂ are used to get an estimated angular acceleration which is denoted <maths id="math0037" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0037" file="imgb0037.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths>. The estimated angular acceleration <maths id="math0038" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0038" file="imgb0038.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> is stored in the control unit 12.</p>
<p id="p0054" num="0054">In a subsequent sixth step S6 the total inertia can be calculated by <maths id="math0039" num="(15)."><math display="block"><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>t</mi></msub><mo>=</mo><mfrac><mrow><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup><mo>−</mo><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></mrow><mrow><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover><mo>−</mo><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></mrow></mfrac></math><img id="ib0039" file="imgb0039.tif" wi="136" he="9" img-content="math" img-format="tif"/></maths></p>
<p id="p0055" num="0055">The estimated total inertia <i>Ĵ<sub>t</sub></i> is used to parametrize the load torque observer 19. Equation (15) is illustrated in <figref idref="f0007">fig. 7</figref>.<!-- EPO <DP n="19"> --></p>
<p id="p0056" num="0056">After parameterization the load torque observer 19 can be used in a seventh step to observe and estimate the load torque <i>T̂<sub>L</sub>.</i> Furthermore, the load inertia can be calculated by <maths id="math0040" num="(16),"><math display="block"><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>L</mi></msub><mo>=</mo><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>t</mi></msub><mo>−</mo><msub><mi>J</mi><mi>m</mi></msub></math><img id="ib0040" file="imgb0040.tif" wi="136" he="6" img-content="math" img-format="tif"/></maths> and the estimated mass <i>m̂</i> of the load or the unbalance mass can be calculated by <maths id="math0041" num="(17)."><math display="block"><mover accent="true"><mi>m</mi><mo>^</mo></mover><mo>=</mo><mfrac><mrow><mi>max</mi><mfenced><msub><mover accent="true"><mi>T</mi><mo>^</mo></mover><mi>L</mi></msub></mfenced></mrow><mi mathvariant="italic">gr</mi></mfrac></math><img id="ib0041" file="imgb0041.tif" wi="135" he="9" img-content="math" img-format="tif"/></maths></p>
<p id="p0057" num="0057">The angular position <i>Θ̂</i> of the load L is already known. <figref idref="f0008">Fig. 8</figref> illustrates the estimated load torque <i>T̂<sub>L</sub>.</i></p>
<p id="p0058" num="0058">The load inertia <i>Ĵ<sub>L</sub>,</i> the load torque <i>T̂<sub>L</sub>,</i> the mass <i>m̂</i> and the angular load position <i>Θ̂</i> characterize the behavior of the load L and can be used for several purposes, for example to adapt the maximum spinning speed, to compensate the load L by filling the balancers 11 with water, to estimate the dry load at the beginning of the washing cycle and to set properly the required amount of water and/or detergent, to estimate the wet load at the beginning of the spinning cycle and to estimate the remaining moisture retention during a drying process.</p>
</description>
<claims id="claims01" lang="en"><!-- EPO <DP n="20"> -->
<claim id="c-en-01-0001" num="0001">
<claim-text>Method to estimate a load behavior in a laundry treatment machine with the steps of:
<claim-text>- providing a laundry treatment machine (1) with a drum (5), a drive motor (9) to rotate the drum (5) around a rotational axis (10) and a controller (13) to regulate an angular speed of the drive motor (9),</claim-text>
<claim-text>- performing a first operation of the laundry treatment machine (1) with a load (L) inside the drum (5), wherein the controller (13) is operated with first controller parameters (P<sub>1</sub>),</claim-text>
<claim-text>- determining a first torque signal <maths id="math0042" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0042" file="imgb0042.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths> and a derivative <maths id="math0043" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0043" file="imgb0043.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> of a first angular speed signal of the drive motor (9) based on the first operation,</claim-text>
<claim-text>- performing a second operation of the laundry treatment machine (1) with the load (L) inside the drum (5), wherein the controller (13) is operated with second controller parameters (P<sub>2</sub>),</claim-text>
<claim-text>- determining a second torque signal <maths id="math0044" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0044" file="imgb0044.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths> and a derivative <maths id="math0045" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0045" file="imgb0045.tif" wi="5" he="6" img-content="math" img-format="tif" inline="yes"/></maths> of a second angular speed signal of the drive motor (9) based on the second operation, and</claim-text>
<claim-text>- determining an inertia <i>Ĵ<sub>t</sub></i> with the equation <maths id="math0046" num=""><math display="block"><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>t</mi></msub><mo>=</mo><mfrac><mrow><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup><mo>−</mo><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></mrow><mrow><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover><mo>−</mo><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></mrow></mfrac></math><img id="ib0046" file="imgb0046.tif" wi="30" he="12" img-content="math" img-format="tif"/></maths> and <b>characterized by</b>:<br/>
determining a load torque (<i>T̂<sub>L</sub></i>) caused by the load (L) depending on the first torque signal <maths id="math0047" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0047" file="imgb0047.tif" wi="8" he="7" img-content="math" img-format="tif" inline="yes"/></maths>, the second torque signal <maths id="math0048" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0048" file="imgb0048.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths><i>,</i> the derivative <maths id="math0049" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0049" file="imgb0049.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> of the first angular speed signal and the derivative <maths id="math0050" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0050" file="imgb0050.tif" wi="6" he="7" img-content="math" img-format="tif" inline="yes"/></maths> of the second angular speed signal, wherein the load torque (<i>T̂<sub>L</sub></i>) is determined by means of a load torque observer (19).</claim-text><!-- EPO <DP n="21"> --></claim-text></claim>
<claim id="c-en-01-0002" num="0002">
<claim-text>Method according to claim 1, <b>characterized in</b><br/>
<b>that</b> at least one of the first operation and the second operation is performed at a constant desired target angular speed (ω*), while in particular a real speed (ω) oscillates according to the controller parameters (P<sub>1</sub>, P<sub>2</sub>) and the load (L).</claim-text></claim>
<claim id="c-en-01-0003" num="0003">
<claim-text>Method according to claim 1 or 2, <b>characterized</b><br/>
<b>by</b> the step of determining a mass (<i>m̂</i>) of the load (L) depending on the load torque (<i>T̂<sub>L</sub></i>)<i>.</i></claim-text></claim>
<claim id="c-en-01-0004" num="0004">
<claim-text>Method according to at least one of the preceding claims, <b>characterized</b><br/>
<b>by</b> the step of determining an angular load position (<i>α̂</i>) of the load (L) depending on the load torque (<i>T̂<sub>L</sub></i>).</claim-text></claim>
<claim id="c-en-01-0005" num="0005">
<claim-text>Method according to at least one of the preceding claims, <b>characterized</b><br/>
<b>by</b> the step of determining a total inertia <i>(J<sub>t</sub>)</i> of the laundry treatment machine (1) and the load (L), wherein in particular a load inertia <i>(J<sub>L</sub></i>) is the difference between the total inertia (<i>Ĵ<sub>t</sub></i>) and a machine inertia (<i>J<sub>m</sub></i>).</claim-text></claim>
<claim id="c-en-01-0006" num="0006">
<claim-text>Method according to at least one of the preceding claims, <b>characterized in</b><br/>
<b>that</b> the first torque signal ( <maths id="math0051" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0051" file="imgb0051.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths>), the second torque signal ( <maths id="math0052" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0052" file="imgb0052.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths>), the first angular speed signal and the second angular speed signal are transformed into a frequency domain.<!-- EPO <DP n="22"> --></claim-text></claim>
<claim id="c-en-01-0007" num="0007">
<claim-text>Method according to at least one of the preceding claims, <b>characterized in</b><br/>
<b>that</b> a respective first harmonic of the first torque signal ( <maths id="math0053" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0053" file="imgb0053.tif" wi="7" he="7" img-content="math" img-format="tif" inline="yes"/></maths>), of the second torque signal ( <maths id="math0054" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0054" file="imgb0054.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths>), of the first angular speed signal and of the second angular speed signal are used to determine the inertia (<i>Ĵ<sub>t</sub>, Ĵ<sub>L</sub></i>) and/or the load torque (<i>T̂<sub>L</sub></i>).</claim-text></claim>
<claim id="c-en-01-0008" num="0008">
<claim-text>Method according to at least one of the preceding claims, <b>characterized in</b><br/>
<b>that</b> the load torque observer (19) is provided with an angular position (<i>Θ̂</i>) of the drive motor (9) and/or a drive torque ( <maths id="math0055" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>∗</mo></msubsup></math><img id="ib0055" file="imgb0055.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths>) of the drive motor (9).</claim-text></claim>
<claim id="c-en-01-0009" num="0009">
<claim-text>Method according to at least one of the preceding claims, <b>characterized in</b><br/>
<b>that</b> the load torque observer (19) determines an observer error (<i>e<sub>obs</sub></i>) depending on an angular position (<i>Θ̂</i>) of the drive motor (9) and an observed angular position (<i>Θ<sub>obs</sub></i>).</claim-text></claim>
<claim id="c-en-01-0010" num="0010">
<claim-text>Method according to at least one of the preceding claims, <b>characterized in</b><br/>
<b>that</b> the load torque observer (19) determines observer signals (k<sub>1</sub>, k<sub>2</sub>, k<sub>3</sub>) depending on an observer error (<i>e<sub>obs</sub></i>) and observer coefficients (K1, K2, K3) to determine the load torque (<i>T̂<sub>L</sub></i>) and/or an observed angular position (<i>Θ<sub>obs</sub></i>).</claim-text></claim>
<claim id="c-en-01-0011" num="0011">
<claim-text>Method according to at least one of the preceding claims, <b>characterized in</b><br/>
<b><!-- EPO <DP n="23"> -->that</b> the load torque observer (19) determines an observed angular position (<i>Θ<sub>obs</sub></i>) depending on a total inertia <i>(J<sub>t</sub>)</i> of the laundry treatment machine (1) and the load (L).</claim-text></claim>
<claim id="c-en-01-0012" num="0012">
<claim-text>Method according to at least one of claims 8 to 11, <b>characterized in that</b> the drive motor (9) is designed sensorless and the angular position (<i>Θ̂</i>) of the drive motor (9) is estimated, in particular by means of a position observer (17).</claim-text></claim>
<claim id="c-en-01-0013" num="0013">
<claim-text>Method according to at least one of claims 8, <b>characterized in that</b> the drive torque ( <maths id="math0056" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>∗</mo></msubsup></math><img id="ib0056" file="imgb0056.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths>) of the drive motor (9) is estimated or is the desired drive torque ( <maths id="math0057" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>∗</mo></msubsup></math><img id="ib0057" file="imgb0057.tif" wi="7" he="5" img-content="math" img-format="tif" inline="yes"/></maths>) and the output of the controller (13).</claim-text></claim>
<claim id="c-en-01-0014" num="0014">
<claim-text>Laundry treatment machine with
<claim-text>- a drum (5),</claim-text>
<claim-text>- a drive motor (9) to rotate the drum (5) around a rotational axis (10), and</claim-text>
<claim-text>- a control unit (12) configured to estimate a load behavior with a controller (13) to regulate an angular speed of the drive motor (9), wherein the control unit (12) is designed such that
<claim-text>-- a first operation of the laundry treatment machine (1) with a load (L) inside the drum (5) is performed, wherein the controller (13) is operated with first controller parameters (P<sub>1</sub>),</claim-text>
<claim-text>-- a first torque signal <maths id="math0058" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0058" file="imgb0058.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths> and a derivative <maths id="math0059" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0059" file="imgb0059.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> of a first angular speed signal of the drive motor (9) are determined based on the first operation,<!-- EPO <DP n="24"> --></claim-text>
<claim-text>-- a second operation of the laundry treatment machine (1) with the load (L) inside the drum (5) is performed, wherein the controller (13) is operated with second controller parameters (P<sub>2</sub>),</claim-text>
<claim-text>-- a second torque signal <maths id="math0060" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0060" file="imgb0060.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths> and a derivative <maths id="math0061" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0061" file="imgb0061.tif" wi="6" he="7" img-content="math" img-format="tif" inline="yes"/></maths> of a second angular speed signal of the drive motor (9) are determined based on the second operation, and</claim-text>
<claim-text>-- an inertia <i>Ĵ<sub>t</sub></i> using the equation <maths id="math0062" num=""><math display="block"><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>t</mi></msub><mo>=</mo><mfrac><mrow><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup><mo>−</mo><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></mrow><mrow><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover><mo>−</mo><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></mrow></mfrac></math><img id="ib0062" file="imgb0062.tif" wi="30" he="12" img-content="math" img-format="tif"/></maths> and <b>characterized in that</b>:<br/>
a load torque (<i>T̂<sub>L</sub></i>) caused by the load (L) is determined depending on the first torque signal <maths id="math0063" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0063" file="imgb0063.tif" wi="7" he="7" img-content="math" img-format="tif" inline="yes"/></maths>, the second torque signal <maths id="math0064" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0064" file="imgb0064.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths><i>,</i> the derivative <maths id="math0065" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0065" file="imgb0065.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> of the first angular speed signal and the derivative <maths id="math0066" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0066" file="imgb0066.tif" wi="6" he="7" img-content="math" img-format="tif" inline="yes"/></maths> of the second angular speed signal, wherein the load torque (<i>T̂<sub>L</sub></i>) is determined by means of a load torque observer (19).</claim-text></claim-text></claim-text></claim>
</claims>
<claims id="claims02" lang="de"><!-- EPO <DP n="25"> -->
<claim id="c-de-01-0001" num="0001">
<claim-text>Verfahren zum Schätzen eines Lastverhaltens in einer Wäschebehandlungsmaschine mit den Schritten:
<claim-text>- Bereitstellen einer Wäschebehandlungsmaschine (1) mit einer Trommel (5), einem Antriebsmotor (9) zum Drehantreiben der Trommel (5) um eine Drehachse (10) und einer Steuerung (13) zum Regeln einer Winkelgeschwindigkeit des Antriebsmotors (9),</claim-text>
<claim-text>- Durchführen eines ersten Arbeitsganges der Wäschebehandlungsmaschine (1) mit einer Beladung (L) in der Trommel (5), wobei die Steuerung (13) mit ersten Steuerungsparametern (P<sub>1</sub>) betrieben wird,</claim-text>
<claim-text>- Bestimmen eines ersten Drehmomentsignals <maths id="math0067" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0067" file="imgb0067.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths> und einer Ableitung <maths id="math0068" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0068" file="imgb0068.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> eines ersten Winkelgeschwindigkeitssignals des Antriebsmotors (9) auf der Grundlage des ersten Arbeitsganges,</claim-text>
<claim-text>- Durchführen eines zweiten Arbeitsganges der Wäschebehandlungsmaschine (1) mit der Beladung (L) in der Trommel (5), wobei die Steuerung (13) mit zweiten Steuerungsparametern (P<sub>2</sub>) betrieben wird,</claim-text>
<claim-text>- Bestimmen eines zweiten Drehmomentsignals <maths id="math0069" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0069" file="imgb0069.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths> und einer Ableitung <maths id="math0070" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0070" file="imgb0070.tif" wi="6" he="5" img-content="math" img-format="tif" inline="yes"/></maths> eines zweiten Winkelgeschwindigkeitssignals des Antriebsmotors (9) auf der Grundlage des zweiten Arbeitsganges, und</claim-text>
<claim-text>- Bestimmen einer Trägheit <i>Ĵ<sub>t</sub></i> mit der Gleichung <maths id="math0071" num=""><math display="block"><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>t</mi></msub><mo>=</mo><mfrac><mrow><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup><mo>−</mo><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></mrow><mrow><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover><mo>−</mo><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></mrow></mfrac></math><img id="ib0071" file="imgb0071.tif" wi="30" he="12" img-content="math" img-format="tif"/></maths> und <b>gekennzeichnet durch:</b><br/>
<!-- EPO <DP n="26"> -->Bestimmen eines Lastmoments (<i>T̂<sub>L</sub></i>), welches von der Beladung (L) verursacht wird, in Abhängigkeit von dem ersten Drehmomentsignal <maths id="math0072" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0072" file="imgb0072.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths><i>,</i> dem zweiten Drehmomentsignal <maths id="math0073" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0073" file="imgb0073.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths>, der Ableitung <maths id="math0074" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0074" file="imgb0074.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> des ersten Winkelgeschwindigkeitssignals und der Ableitung <maths id="math0075" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0075" file="imgb0075.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> des zweiten Winkelgeschwindigkeitssignals, wobei das Lastmoment (<i>T̂<sub>L</sub></i>) mithilfe eines Lastmomentbeobachters (19) bestimmt wird.</claim-text></claim-text></claim>
<claim id="c-de-01-0002" num="0002">
<claim-text>Verfahren nach Anspruch 1, <b>dadurch gekennzeichnet,</b><br/>
<b>dass</b> mindestens einer von dem ersten Arbeitsgang und dem zweiten Arbeitsgang bei einer konstanten Soll-Winkelgeschwindigkeit (ω*) durchgeführt wird, während insbesondere eine reale Geschwindigkeit (ω) entsprechend den Steuerungsparametern (P<sub>1</sub>, P<sub>2</sub>) und der Beladung (L) schwankt.</claim-text></claim>
<claim id="c-de-01-0003" num="0003">
<claim-text>Verfahren nach der Ansprüche 1 oder 2, <b>gekennzeichnet durch</b> den Schritt des Bestimmens einer Masse (<i>m̂</i>) der Beladung (L) in Abhängigkeit von dem Lastmoment (<i>T̂<sub>L</sub></i>).</claim-text></claim>
<claim id="c-de-01-0004" num="0004">
<claim-text>Verfahren nach mindestens einem der vorhergehenden Ansprüche, <b>gekennzeichnet</b><br/>
<b>durch</b> den Schritt des Bestimmens einer Lastwinkelposition (<i>α̂</i>) der Beladung (L) in Abhängigkeit von dem Lastmoment (<i>T̂<sub>L</sub></i>).</claim-text></claim>
<claim id="c-de-01-0005" num="0005">
<claim-text>Verfahren nach mindestens einem der vorhergehenden Ansprüche, <b>gekennzeichnet</b><br/>
<b><!-- EPO <DP n="27"> -->durch</b> den Schritt des Bestimmens einer Gesamtträgheit (<i>Ĵ<sub>t</sub></i>) der Wäschebehandlungsmaschine (1) und der Beladung (L), wobei insbesondere eine Ladungsträgheit (<i>Ĵ<sub>L</sub></i>) die Differenz zwischen der Gesamtträgheit (<i>Ĵ<sub>t</sub></i>) und einer Maschinenträgheit (<i>J<sub>m</sub></i>) beträgt.</claim-text></claim>
<claim id="c-de-01-0006" num="0006">
<claim-text>Verfahren nach mindestens einem der vorhergehenden Ansprüche,<br/>
<b>dadurch gekennzeichnet,</b><br/>
<b>dass</b> das erste Drehmomentsignal ( <maths id="math0076" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0076" file="imgb0076.tif" wi="7" he="5" img-content="math" img-format="tif" inline="yes"/></maths>), das zweite Drehmomentsignal ( <maths id="math0077" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0077" file="imgb0077.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths>), das erste Winkelgeschwindigkeitssignal und das zweite Winkelgeschwindigkeitssignal in einen Frequenzbereich transformiert werden.</claim-text></claim>
<claim id="c-de-01-0007" num="0007">
<claim-text>Verfahren nach mindestens einem der vorhergehenden Ansprüche,<br/>
<b>dadurch gekennzeichnet,</b><br/>
<b>dass</b> eine jeweilige erste Harmonische des ersten Drehmomentsignals ( <maths id="math0078" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0078" file="imgb0078.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths>), des zweiten Drehmomentsignals ( <maths id="math0079" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0079" file="imgb0079.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths>), des ersten Winkelgeschwindigkeitssignals und des zweiten Winkelgeschwindigkeitssignals zum Bestimmen der Trägheit (<i>Ĵ<sub>t</sub>, Ĵ<sub>L</sub></i>) und/oder des Lastmoments (<i>T̂<sub>L</sub></i>) verwendet werden.</claim-text></claim>
<claim id="c-de-01-0008" num="0008">
<claim-text>Verfahren nach mindestens einem der vorhergehenden Ansprüche,<br/>
<b>dadurch gekennzeichnet,</b><br/>
<b>dass</b> der Lastmomentbeobachter (19) eine Winkelposition (<i>Θ̂</i>) des Antriebsmotors (9) und/oder ein Antriebsmoment ( <maths id="math0080" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>∗</mo></msubsup></math><img id="ib0080" file="imgb0080.tif" wi="7" he="5" img-content="math" img-format="tif" inline="yes"/></maths>) des Antriebsmotors (9) erhält.</claim-text></claim>
<claim id="c-de-01-0009" num="0009">
<claim-text>Verfahren nach mindestens einem der vorhergehenden Ansprüche,<br/>
<b>dadurch gekennzeichnet,</b><br/>
<b><!-- EPO <DP n="28"> -->dass</b> der Lastmomentbeobachter (19) einen Beobachterfehler (<i>e<sub>obs</sub></i>) in Abhängigkeit von einer Winkelposition (<i>Θ̂</i>) des Antriebsmotors (9) und einer beobachteten Winkelposition (<i>Θ<sub>obs</sub></i>) bestimmt.</claim-text></claim>
<claim id="c-de-01-0010" num="0010">
<claim-text>Verfahren nach mindestens einem der vorhergehenden Ansprüche,<br/>
<b>dadurch gekennzeichnet,</b><br/>
<b>dass</b> der Lastmomentbeobachter (19) Beobachtersignale (k<sub>1</sub>, k<sub>2</sub>, k<sub>3</sub>) in Abhängigkeit von einem Beobachterfehler (<i>e<sub>obs</sub></i>) und Beobachterkoeffizienten (K1, K2, K3) zum Bestimmen des Lastmoments (<i>T̂<sub>L</sub></i>) und/oder einer beobachteten Winkelposition (<i>Θ<sub>obs</sub></i>) bestimmt.</claim-text></claim>
<claim id="c-de-01-0011" num="0011">
<claim-text>Verfahren nach mindestens einem der vorhergehenden Ansprüche,<br/>
<b>dadurch gekennzeichnet,</b><br/>
<b>dass</b> der Lastmomentbeobachter (19) eine beobachtete Winkelposition (<i>Θ<sub>obs</sub></i>) in Abhängigkeit von einer Gesamtträgheit (<i>Ĵ<sub>t</sub></i>) der Wäschebehandlungsmaschine (1) und der Beladung (L) bestimmt.</claim-text></claim>
<claim id="c-de-01-0012" num="0012">
<claim-text>Verfahren nach mindestens einem der Ansprüche 8 bis 11, <b>dadurch gekennzeichnet, dass</b> der Antriebsmotor (9) sensorlos ausgeführt ist und die Winkelposition (<i>Θ̂</i>) des Antriebsmotors (9) geschätzt wird, insbesondere mithilfe eines Positionsbeobachters (17).</claim-text></claim>
<claim id="c-de-01-0013" num="0013">
<claim-text>Verfahren nach mindestens einem der Ansprüche 8, <b>dadurch gekennzeichnet,</b><br/>
<b>dass</b> das Antriebsmoment ( <maths id="math0081" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>∗</mo></msubsup></math><img id="ib0081" file="imgb0081.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths>) des Antriebsmotors (9) geschätzt wird oder das gewünschte Antriebsmoment ( <maths id="math0082" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>∗</mo></msubsup></math><img id="ib0082" file="imgb0082.tif" wi="7" he="5" img-content="math" img-format="tif" inline="yes"/></maths>) und die Ausgabe der Steuerung (13) beträgt.<!-- EPO <DP n="29"> --></claim-text></claim>
<claim id="c-de-01-0014" num="0014">
<claim-text>Wäschebehandlungsmaschine mit
<claim-text>- einer Trommel (5),</claim-text>
<claim-text>- einem Antriebsmotor (9) zum Drehantreiben der Trommel (5) um eine Drehachse (10), und</claim-text>
<claim-text>- einer Steuereinheit (12), welche dazu ausgebildet ist, mit einer Steuerung (13) ein Lastverhalten abzuschätzen, um eine Winkelgeschwindigkeit des Antriebsmotors (9) zu steuern, wobei die Steuereinheit (12) so ausgebildet ist, dass
<claim-text>-- ein erster Arbeitsgang der Wäschebehandlungsmaschine (1) mit einer Beladung (L) in der Trommel (5) durchgeführt wird, wobei die Steuerung (13) mit ersten Steuerungsparametern (P<sub>1</sub>) betrieben wird,</claim-text>
<claim-text>-- ein erstes Drehmomentsignal <maths id="math0083" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0083" file="imgb0083.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths> und eine Ableitung <maths id="math0084" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0084" file="imgb0084.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> eines ersten Winkelgeschwindigkeitssignals des Antriebsmotors (9) auf der Grundlage des ersten Arbeitsgangs bestimmt werden,</claim-text>
<claim-text>-- ein zweiter Arbeitsgang der Wäschebehandlungsmaschine (1) mit der Beladung (L) in der Trommel (5) durchgeführt wird, wobei die Steuerung (13) mit zweiten Steuerungsparametern (P<sub>2</sub>) betrieben wird,</claim-text>
<claim-text>-- ein zweites Drehmomentsignal <maths id="math0085" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0085" file="imgb0085.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths> und eine Ableitung <maths id="math0086" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0086" file="imgb0086.tif" wi="6" he="5" img-content="math" img-format="tif" inline="yes"/></maths> eines zweiten Winkelgeschwindigkeitssignals des Antriebsmotors (9) auf der Grundlage des zweiten Arbeitsganges bestimmt werden, und</claim-text>
<claim-text>-- eine Trägheit <i>Ĵ<sub>t</sub></i> unter Verwendung der Gleichung <maths id="math0087" num=""><math display="block"><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>t</mi></msub><mo>=</mo><mfrac><mrow><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup><mo>−</mo><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></mrow><mrow><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover><mo>−</mo><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></mrow></mfrac></math><img id="ib0087" file="imgb0087.tif" wi="30" he="12" img-content="math" img-format="tif"/></maths> und<br/>
<b>dadurch gekennzeichnet,<!-- EPO <DP n="30"> --> dass:</b><br/>
ein Lastmoment (<i>T̂<sub>L</sub></i>), welches von der Beladung (L) verursacht wird, in Abhängigkeit von dem ersten Drehmomentsignal <maths id="math0088" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0088" file="imgb0088.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths>, dem zweiten Drehmomentsignal <maths id="math0089" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0089" file="imgb0089.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths>, der Ableitung <maths id="math0090" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0090" file="imgb0090.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> des ersten Winkelgeschwindigkeitssignals und der Ableitung <maths id="math0091" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0091" file="imgb0091.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> des zweiten Winkelgeschwindigkeitssignals bestimmt wird, wobei das Lastmoment <maths id="math0092" num=""><math display="inline"><mover accent="true"><mfenced><msub><mi>T</mi><mi>L</mi></msub></mfenced><mo>^</mo></mover></math><img id="ib0092" file="imgb0092.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths> mithilfe eines Lastmomentbeobachters (19) bestimmt wird.</claim-text></claim-text></claim-text></claim>
</claims>
<claims id="claims03" lang="fr"><!-- EPO <DP n="31"> -->
<claim id="c-fr-01-0001" num="0001">
<claim-text>Procédé pour estimer le comportement d'une charge dans une machine de traitement de linge avec les étapes suivantes :
<claim-text>- mise à disposition d'une machine de traitement du linge (1) avec un tambour (5), un moteur d'entraînement (9) pour faire tourner le tambour (5) autour d'un axe de rotation (10) et un contrôleur (13) pour réguler une vitesse angulaire du moteur d'entraînement (9),</claim-text>
<claim-text>- mise en œuvre d'une première opération de la machine de traitement de linge (1) avec une charge (L) à l'intérieur du tambour (5), le contrôleur (13) étant actionné avec des premiers paramètres de contrôleur (P<sub>1</sub>),</claim-text>
<claim-text>- détermination d'un premier signal de couple <maths id="math0093" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0093" file="imgb0093.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths> et d'une dérivée <maths id="math0094" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0094" file="imgb0094.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> d'un premier signal de vitesse angulaire du moteur d'entraînement (9) sur la base de la première opération,</claim-text>
<claim-text>- mise en œuvre d'une deuxième opération de la machine de traitement de linge (1) avec la charge (L) à l'intérieur du tambour (5), le contrôleur (13) étant actionné avec des deuxièmes paramètres de contrôleur (P<sub>2</sub>),</claim-text>
<claim-text>- détermination d'un deuxième signal de couple <maths id="math0095" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0095" file="imgb0095.tif" wi="8" he="7" img-content="math" img-format="tif" inline="yes"/></maths> et d'une dérivée <maths id="math0096" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0096" file="imgb0096.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> d'un deuxième signal de vitesse angulaire du moteur d'entraînement (9) sur la base de la deuxième opération, et</claim-text>
<claim-text>- détermination d'une inertie <i>Ĵ<sub>t</sub></i> avec l'équation <maths id="math0097" num=""><math display="block"><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>t</mi></msub><mo>=</mo><mfrac><mrow><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup><mo>−</mo><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></mrow><mrow><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover><mo>−</mo><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></mrow></mfrac></math><img id="ib0097" file="imgb0097.tif" wi="30" he="12" img-content="math" img-format="tif"/></maths> et <b>caractérisé par :</b><br/>
<!-- EPO <DP n="32"> -->la détermination d'un couple de charge (<i>T̂<sub>L</sub></i>) provoqué par la charge (L) en fonction du premier signal de couple <maths id="math0098" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0098" file="imgb0098.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths>, du deuxième signal de couple <maths id="math0099" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0099" file="imgb0099.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths>, de la dérivée <maths id="math0100" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0100" file="imgb0100.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> du premier signal de vitesse angulaire et de la dérivée <maths id="math0101" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0101" file="imgb0101.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths> du deuxième signal de vitesse angulaire, le couple de charge (<i>T̂<sub>L</sub></i>) étant déterminé au moyen d'un observateur de couple de charge (19).</claim-text></claim-text></claim>
<claim id="c-fr-01-0002" num="0002">
<claim-text>Procédé selon la revendication 1, <b>caractérisé en ce</b><br/>
<b>que</b> la première opération et/ou la deuxième opération sont effectuées à une vitesse angulaire cible désirée constante (ω*), tandis que, en particulier, une vitesse réelle (ω) oscille en fonction des paramètres du contrôleur (P<sub>1</sub>, P<sub>2</sub>) et de la charge (L).</claim-text></claim>
<claim id="c-fr-01-0003" num="0003">
<claim-text>Procédé selon la revendication 1 ou 2, <b>caractérisé</b><br/>
<b>par</b> l'étape de détermination d'une masse (<i>m̂</i>) de la charge (L) en fonction du couple de charge (<i>T̂<sub>L</sub></i>).</claim-text></claim>
<claim id="c-fr-01-0004" num="0004">
<claim-text>Procédé selon au moins l'une quelconque des revendications précédentes, <b>caractérisé</b><br/>
<b>par</b> l'étape de détermination d'une position angulaire de charge (<i>α̂</i>) de la charge (L) en fonction du couple de charge (<i>T̂<sub>L</sub></i>).</claim-text></claim>
<claim id="c-fr-01-0005" num="0005">
<claim-text>Procédé selon au moins l'une quelconque des revendications précédentes, <b>caractérisé</b><br/>
<b>par</b> l'étape de détermination d'une inertie totale (<i>Ĵ<sub>t</sub></i>) de la machine de traitement de linge (1) et de la charge (L), dans laquelle en particulier une inertie de charge (<i>Ĵ<sub>L</sub></i>) est la différence entre l'inertie totale (<i>Ĵ<sub>t</sub></i>) et l'inertie de la machine (<i>J<sub>m</sub></i>).<!-- EPO <DP n="33"> --></claim-text></claim>
<claim id="c-fr-01-0006" num="0006">
<claim-text>Procédé selon au moins l'une quelconque des revendications précédentes, <b>caractérisé en ce</b><br/>
<b>que</b> le premier signal de couple ( <maths id="math0102" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0102" file="imgb0102.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths>), le deuxième signal de couple ( <maths id="math0103" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0103" file="imgb0103.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths>), le premier signal de vitesse angulaire et le deuxième signal de vitesse angulaire sont transformés dans un domaine de fréquence.</claim-text></claim>
<claim id="c-fr-01-0007" num="0007">
<claim-text>Procédé selon au moins l'une quelconque des revendications précédentes, <b>caractérisé en ce</b><br/>
<b>qu</b>'une première harmonique respective du premier signal de couple ( <maths id="math0104" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0104" file="imgb0104.tif" wi="7" he="5" img-content="math" img-format="tif" inline="yes"/></maths>), du deuxième signal de couple ( <maths id="math0105" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0105" file="imgb0105.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths>), du premier signal de vitesse angulaire et du deuxième signal de vitesse angulaire sont utilisées pour déterminer l'inertie (<i>Ĵ<sub>t</sub>, Ĵ<sub>L</sub></i>) et/ou le couple de charge (<i>T̂<sub>L</sub></i>).</claim-text></claim>
<claim id="c-fr-01-0008" num="0008">
<claim-text>Procédé selon au moins l'une quelconque des revendications précédentes, <b>caractérisé en ce</b><br/>
<b>que</b> l'observateur de couple de charge (19) reçoit une position angulaire (<i>Θ̂</i>) du moteur d'entraînement (9) et/ou un couple d'entraînement ( <maths id="math0106" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>∗</mo></msubsup></math><img id="ib0106" file="imgb0106.tif" wi="7" he="5" img-content="math" img-format="tif" inline="yes"/></maths>) du moteur d'entraînement (9).</claim-text></claim>
<claim id="c-fr-01-0009" num="0009">
<claim-text>Procédé selon au moins l'une quelconque des revendications précédentes, <b>caractérisé en ce</b><br/>
<b>que</b> l'observateur de couple de charge (19) détermine une erreur d'observateur (<i>e<sub>obs</sub></i>) en fonction d'une position angulaire (<i>Θ̂</i>) du moteur d'entraînement (9) et d'une position angulaire observée (<i>Θ<sub>obs</sub></i>).</claim-text></claim>
<claim id="c-fr-01-0010" num="0010">
<claim-text>Procédé selon au moins l'une quelconque des revendications précédentes, <b>caractérisé en ce</b><br/>
<b><!-- EPO <DP n="34"> -->que</b> l'observateur de couple de charge (19) détermine des signaux d'observateur (k<sub>1</sub>, k<sub>2</sub>, k<sub>3</sub>) en fonction d'une erreur d'observateur (<i>e<sub>obs</sub></i>) et des coefficients d'observateur (K1, K2, K3) pour déterminer le couple de charge (<i>T̂<sub>L</sub></i>) et/ou une position angulaire observée (<i>Θ<sub>obs</sub></i>).</claim-text></claim>
<claim id="c-fr-01-0011" num="0011">
<claim-text>Procédé selon au moins l'une quelconque des revendications précédentes, <b>caractérisé en ce</b><br/>
<b>que</b> l'observateur de couple de charge (19) détermine une position angulaire observée (<i>Θ<sub>obs</sub></i>) en fonction d'une inertie totale (<i>Ĵ<sub>t</sub></i>) de la machine de traitement de linge (1) et de la charge (L).</claim-text></claim>
<claim id="c-fr-01-0012" num="0012">
<claim-text>Procédé selon au moins l'une quelconque des revendications 8 à 11,<br/>
<b>caractérisé en ce</b><br/>
<b>que</b> le moteur d'entraînement (9) est conçu sans capteur et que la position angulaire (<i>Θ̂</i>) du moteur d'entraînement (9) est estimée, en particulier au moyen d'un observateur de position (17).</claim-text></claim>
<claim id="c-fr-01-0013" num="0013">
<claim-text>Procédé selon selon au moins l'une quelconque de la revendication 8,<br/>
<b>caractérisé en ce</b><br/>
<b>que</b> le couple d'entraînement ( <maths id="math0107" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>∗</mo></msubsup></math><img id="ib0107" file="imgb0107.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths>) du moteur d'entraînement (9) est estimé ou est le couple d'entraînement souhaité ( <maths id="math0108" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mo>∗</mo></msubsup></math><img id="ib0108" file="imgb0108.tif" wi="7" he="5" img-content="math" img-format="tif" inline="yes"/></maths>) et la sortie du contrôleur (13).</claim-text></claim>
<claim id="c-fr-01-0014" num="0014">
<claim-text>Machine de traitement de linge avec
<claim-text>- un tambour (5),</claim-text>
<claim-text>- un moteur d'entraînement (9) pour faire tourner le tambour (5) autour d'un axe de rotation (10), et<!-- EPO <DP n="35"> --></claim-text>
<claim-text>- une unité de commande (12) configurée pour estimer un comportement de charge avec un contrôleur (13) pour réguler une vitesse angulaire du moteur d'entraînement (9), l'unité de commande (12) étant conçue de sorte que
<claim-text>-- une première opération de la machine de traitement de linge (1) avec une charge (L) à l'intérieur du tambour (5) est effectuée, le contrôleur (13) étant actionné avec des premiers paramètres de contrôleur (P<sub>1</sub>),</claim-text>
<claim-text>-- un premier signal de couple <maths id="math0109" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0109" file="imgb0109.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths> et une dérivée <maths id="math0110" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0110" file="imgb0110.tif" wi="7" he="6" img-content="math" img-format="tif" inline="yes"/></maths> d'un premier signal de vitesse angulaire du moteur d'entraînement (9) sont déterminés sur la base de la première opération,</claim-text>
<claim-text>-- une deuxième opération de la machine de traitement de linge (1) avec la charge (L) à l'intérieur du tambour (5) est effectuée, le contrôleur (13) étant actionné avec des deuxièmes paramètres de contrôleur (P<sub>2</sub>),</claim-text>
<claim-text>-- un deuxième signal de couple <maths id="math0111" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0111" file="imgb0111.tif" wi="9" he="6" img-content="math" img-format="tif" inline="yes"/></maths> et une dérivée <maths id="math0112" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0112" file="imgb0112.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> d'un deuxième signal de vitesse angulaire du moteur d'entraînement (9) sont déterminés sur la base de la deuxième opération, et</claim-text>
<claim-text>-- une inertie <i>Ĵ<sub>t</sub></i> en utilisant l'équation <maths id="math0113" num=""><math display="block"><msub><mover accent="true"><mi>J</mi><mo>^</mo></mover><mi>t</mi></msub><mo>=</mo><mfrac><mrow><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup><mo>−</mo><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></mrow><mrow><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover><mo>−</mo><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></mrow></mfrac></math><img id="ib0113" file="imgb0113.tif" wi="30" he="12" img-content="math" img-format="tif"/></maths> et<br/>
<b>caractérisée en ce</b><br/>
<b>que :</b><br/>
un couple de charge (<i>T̂<sub>L</sub></i>) provoqué par la charge (L) est déterminé en fonction du premier signal de couple <maths id="math0114" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>1</mn></mrow></msubsup></math><img id="ib0114" file="imgb0114.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths>, du deuxième signal de couple <maths id="math0115" num=""><math display="inline"><msubsup><mi>T</mi><mi mathvariant="italic">em</mi><mrow><mo>∗</mo><mn>2</mn></mrow></msubsup></math><img id="ib0115" file="imgb0115.tif" wi="8" he="6" img-content="math" img-format="tif" inline="yes"/></maths>, de la dérivée <maths id="math0116" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>1</mn></msup><mo>^</mo></mover></math><img id="ib0116" file="imgb0116.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> du premier signal de vitesse angulaire et de la dérivée <maths id="math0117" num=""><math display="inline"><mover accent="true"><msup><mover accent="true"><mi>ω</mi><mo>˙</mo></mover><mn>2</mn></msup><mo>^</mo></mover></math><img id="ib0117" file="imgb0117.tif" wi="6" he="6" img-content="math" img-format="tif" inline="yes"/></maths> du deuxième signal de vitesse angulaire, le couple de<!-- EPO <DP n="36"> --> charge (<i>T̂<sub>L</sub></i>) étant déterminé au moyen d'un observateur de couple de charge (19).</claim-text></claim-text></claim-text></claim>
</claims>
<drawings id="draw" lang="en"><!-- EPO <DP n="37"> -->
<figure id="f0001" num="1"><img id="if0001" file="imgf0001.tif" wi="151" he="187" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="38"> -->
<figure id="f0002" num="2"><img id="if0002" file="imgf0002.tif" wi="88" he="133" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="39"> -->
<figure id="f0003" num="3"><img id="if0003" file="imgf0003.tif" wi="124" he="240" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="40"> -->
<figure id="f0004" num="4"><img id="if0004" file="imgf0004.tif" wi="111" he="188" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="41"> -->
<figure id="f0005" num="5"><img id="if0005" file="imgf0005.tif" wi="123" he="230" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="42"> -->
<figure id="f0006" num="6"><img id="if0006" file="imgf0006.tif" wi="160" he="174" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="43"> -->
<figure id="f0007" num="7"><img id="if0007" file="imgf0007.tif" wi="151" he="201" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="44"> -->
<figure id="f0008" num="8"><img id="if0008" file="imgf0008.tif" wi="155" he="193" img-content="drawing" img-format="tif"/></figure>
</drawings>
<ep-reference-list id="ref-list">
<heading id="ref-h0001"><b>REFERENCES CITED IN THE DESCRIPTION</b></heading>
<p id="ref-p0001" num=""><i>This list of references cited by the applicant is for the reader's convenience only. It does not form part of the European patent document. Even though great care has been taken in compiling the references, errors or omissions cannot be excluded and the EPO disclaims all liability in this regard.</i></p>
<heading id="ref-h0002"><b>Patent documents cited in the description</b></heading>
<p id="ref-p0002" num="">
<ul id="ref-ul0001" list-style="bullet">
<li><patcit id="ref-pcit0001" dnum="US2005204482A1"><document-id><country>US</country><doc-number>2005204482</doc-number><kind>A1</kind></document-id></patcit><crossref idref="pcit0001">[0004]</crossref></li>
<li><patcit id="ref-pcit0002" dnum="EP2607535A2"><document-id><country>EP</country><doc-number>2607535</doc-number><kind>A2</kind></document-id></patcit><crossref idref="pcit0002">[0005]</crossref></li>
<li><patcit id="ref-pcit0003" dnum="US20190112745A1"><document-id><country>US</country><doc-number>20190112745</doc-number><kind>A1</kind></document-id></patcit><crossref idref="pcit0003">[0005]</crossref></li>
</ul></p>
</ep-reference-list>
</ep-patent-document>
