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<ep-patent-document id="EP17888019B1" file="EP17888019NWB1.xml" lang="en" country="EP" doc-number="3553320" kind="B1" date-publ="20230913" status="n" dtd-version="ep-patent-document-v1-6">
<SDOBI lang="en"><B000><eptags><B001EP>ATBECHDEDKESFRGBGRITLILUNLSEMCPTIESILTLVFIROMKCYALTRBGCZEEHUPLSK..HRIS..MTNORS..SM..................</B001EP><B005EP>J</B005EP><B007EP>2.0.21 -  2100000/0</B007EP></eptags></B000><B100><B110>3553320</B110><B120><B121>EUROPEAN PATENT SPECIFICATION</B121></B120><B130>B1</B130><B140><date>20230913</date></B140><B190>EP</B190></B100><B200><B210>17888019.1</B210><B220><date>20171208</date></B220><B240><B241><date>20190708</date></B241><B242><date>20211209</date></B242></B240><B250>ja</B250><B251EP>en</B251EP><B260>en</B260></B200><B300><B310>2016255373</B310><B320><date>20161228</date></B320><B330><ctry>JP</ctry></B330><B310>2017080267</B310><B320><date>20170414</date></B320><B330><ctry>JP</ctry></B330></B300><B400><B405><date>20230913</date><bnum>202337</bnum></B405><B430><date>20191016</date><bnum>201942</bnum></B430><B450><date>20230913</date><bnum>202337</bnum></B450><B452EP><date>20230413</date></B452EP></B400><B500><B510EP><classification-ipcr sequence="1"><text>F04D  29/38        20060101AFI20200616BHEP        </text></classification-ipcr><classification-ipcr sequence="2"><text>F04D  29/00        20060101ALI20200616BHEP        </text></classification-ipcr></B510EP><B520EP><classifications-cpc><classification-cpc sequence="1"><text>F04D  29/38        20130101 LI20180802BHEP        </text></classification-cpc><classification-cpc sequence="2"><text>F04D  29/00        20130101 LI20191018BHEP        </text></classification-cpc><classification-cpc sequence="3"><text>F04D  29/384       20130101 FI20200612BHEP        </text></classification-cpc></classifications-cpc></B520EP><B540><B541>de</B541><B542>PROPELLERLÜFTER</B542><B541>en</B541><B542>PROPELLER FAN</B542><B541>fr</B541><B542>VENTILATEUR HÉLICOÏDAL</B542></B540><B560><B561><text>CN-A- 102 341 603</text></B561><B561><text>JP-A- 2005 307 788</text></B561><B561><text>JP-A- 2010 275 986</text></B561><B561><text>JP-A- 2010 275 986</text></B561><B561><text>JP-A- 2012 052 443</text></B561><B565EP><date>20200622</date></B565EP></B560></B500><B700><B720><B721><snm>IWATA, Tooru</snm><adr><str>c/o DAIKIN INDUSTRIES, LTD.
Umeda Center Building
4-12 Nakazaki-Nishi 2-chome
Kita-ku</str><city>Osaka-shi
Osaka 530-8323</city><ctry>JP</ctry></adr></B721><B721><snm>TOMIOKA, Hirotaka</snm><adr><str>c/o DAIKIN INDUSTRIES, LTD.
Umeda Center Building
4-12 Nakazaki-Nishi 2-chome
Kita-ku</str><city>Osaka-shi
Osaka 530-8323</city><ctry>JP</ctry></adr></B721></B720><B730><B731><snm>Daikin Industries, Ltd.</snm><iid>101976536</iid><irf>215 831 a/fha</irf><adr><str>Osaka Umeda Twin Towers South, 1-13-1 
Umeda, Kita-ku</str><city>Osaka-shi, Osaka 530-0001</city><ctry>JP</ctry></adr></B731></B730><B740><B741><snm>Hoffmann Eitle</snm><iid>100061036</iid><adr><str>Patent- und Rechtsanwälte PartmbB 
Arabellastraße 30</str><city>81925 München</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><B860><B861><dnum><anum>JP2017044226</anum></dnum><date>20171208</date></B861><B862>ja</B862></B860><B870><B871><dnum><pnum>WO2018123519</pnum></dnum><date>20180705</date><bnum>201827</bnum></B871></B870></B800></SDOBI>
<description id="desc" lang="en"><!-- EPO <DP n="1"> -->
<heading id="h0001">TECHNICAL FIELD</heading>
<p id="p0001" num="0001">The present invention relates to a propeller fan for use in a blower or the like.</p>
<heading id="h0002">BACKGROUND ART</heading>
<p id="p0002" num="0002">Conventionally, a propeller fan is widely used for a blower or the like. For example, <patcit id="pcit0001" dnum="JP2012052443A"><text>JP 2012-052443</text></patcit> discloses a propeller fan having a hub and three blades.</p>
<p id="p0003" num="0003">The blade of a general propeller fan is formed to have a curved shape so as to bulge in the direction of the negative pressure surface side. That is, in the blade of the propeller fan, the camber, which is a distance from a chord line to a mean line in a blade cross section, becomes maximum between the leading edge and the trailing edge along the chord line of the blade. As can be seen from <figref idref="f0005 f0006">FIG. 6</figref> of <patcit id="pcit0002" dnum="JP2012052443A"><text>JP 2012-052443</text></patcit>, in each blade of the propeller fan, a position at which the camber becomes maximum in the blade cross section is set to be located gradually closer to the leading edge in the direction from the blade root toward the blade end.</p>
<p id="p0004" num="0004">Another example of the prior art is described in <patcit id="pcit0003" dnum="JP2010275986A"><text>JP 2010 275986 A</text></patcit>.</p>
<heading id="h0003">SUMMARY OF THE INVENTION</heading><!-- EPO <DP n="2"> -->
<heading id="h0004">TECHNICAL PROBLEM</heading>
<p id="p0005" num="0005">In a blade of a propeller fan, air flows back from the positive pressure surface side to the negative pressure surface side via the blade end of the blade, so that a blade end vortex is generated. This blade end vortex is generated in the vicinity of a position where a differential pressure between the positive pressure surface side and the negative pressure surface side of the blade becomes maximum. Therefore, in the blade of the propeller fan, the blade end vortex is generated in the vicinity of a position of the blade end where the camber becomes maximum.</p>
<p id="p0006" num="0006">The blade end vortex generated in the blade of the propeller fan develops larger in the direction to the trailing edge of the blade. Therefore, as the position of the blade end where the camber becomes maximum becomes farther away from the trailing edge of the blade, the blade end vortex develops longer. As described above, in each blade of the propeller fan of <patcit id="pcit0004" dnum="JP2012052443A"><text>JP 2012-052443</text></patcit>, the position where the camber becomes maximum in the blade cross section becomes relatively farther from the trailing edge in the direction from the blade root toward the blade end. Therefore, in the propeller fan of <patcit id="pcit0005" dnum="JP2012052443A"><text>JP 2012-052443</text></patcit>, the blade end vortex becomes longer and energy consumed for generation of the blade end vortex is increased. As a result, fan efficiency may not be sufficiently improved.</p>
<p id="p0007" num="0007">In view of the foregoing, it is therefore an object of the present invention to improve fan efficiency of a propeller fan.</p>
<heading id="h0005">SOLUTION TO THE PROBLEM</heading>
<p id="p0008" num="0008">A first aspect of the present disclosure is directed to a propeller fan comprising a<!-- EPO <DP n="3"> --> cylindrical hub (15) and a plurality of blades (20) extending outwardly from a side surface of the hub (15). Each of the blades (20) is configured such that a distance from a blade chord (31) to a mean line (32) in a blade cross section is set as a camber, that in the blade cross section, a position on the chord line (31) where the camber becomes maximum is set as a maximum camber position (A), that a ratio of a distance (d) between a leading edge (23) and the maximum camber position (A) in the blade cross section to a chord length (c) is set as a maximum camber position ratio (d/c), that an end portion at the hub (15) side of the blade (20) is set as a blade root (21), that an end portion of an outer circumferential side of the blade (20) is set as a blade end (22), and that the maximum camber position ratio (d/c) at the blade end (22) is larger than the maximum camber position ratio (d/c) at the blade root (21). Each of the blades (20) is configured such that the maximum camber position ratio (d/c) becomes maximum in an intermediate blade cross section (33a) located between the blade root (21) and the blade end (22).</p>
<p id="p0009" num="0009">A blade end vortex (90) is generated in the vicinity of a position where the camber becomes maximum at the blade end (22) of the blade (20) of the propeller fan (10). As the generation position of this blade end vortex (90) approaches to the leading edge (23) of the blade (20), the blade end vortex (90) becomes longer, and energy consumed for the generation of the blade end vortex (90) increases.</p>
<p id="p0010" num="0010">In contrast, in each blade (20) of the propeller fan (10) of the first aspect described above, the maximum camber position ratio (d/c) at the blade end (22) is larger than the maximum camber position ratio (d/c) at the blade root (21). That is, in each blade (20), the maximum camber position (A) at which the camber becomes maximum in the blade cross section becomes closer to the trailing edge (24) at the blade end (22) of the blade (20) than in the case of conventional propeller fans. Therefore, the development of the blade end vortex<!-- EPO <DP n="4"> --> maximum camber position (A) at which the camber becomes maximum in the blade cross section becomes closer to the trailing edge (24) at the blade end (22) of the blade (20) than in the case of conventional propeller fans. Therefore, the development of the blade end vortex (90) is suppressed and the blade end vortex (90) is shortened so that energy consumed for generation of the blade end vortex (90) is reduced and fan efficiency is improved.</p>
<p id="p0011" num="0011">The phrase "monotonically increase" described in this specification is "weakly increase". Accordingly, in each blade (20), the maximum camber position ratio (d/c) from the first reference blade cross section (33) toward the blade end (22) may continuously increase, or may be constant in some sections from the first reference blade section (33) to the blade end (22).</p>
<p id="p0012" num="0012">According to the first aspect of the present disclosure, each blade (20) of the first aspect is configured such that the maximum camber position ration (d/c) described above becomes maximum in the first reference blade cross section (33) located between the above blade root (21) and the above blade end (22).</p>
<p id="p0013" num="0013">In each blade (20) of the propeller fan (10) of the first aspect, the maximum camber position ratio (d/c) becomes maximum in the intermediate blade cross section (33a) located closer to the blade root (21) than to the blade end (22).</p>
<p id="p0014" num="0014">According to a second aspect of the present disclosure, each of the blades (20) of the first aspect is configured such that the maximum camber position ratio (d/c) becomes minimum at the blade root (21), and monotonously increases from the blade root (21) described above toward the intermediate blade cross section (33a).<!-- EPO <DP n="5"> --></p>
<p id="p0015" num="0015">In each blade (20) of the propeller fan (10) of the second aspect, the maximum camber position ratio (d/c) monotonically increases from minimum at the blade root (21) to maximum at the intermediate blade cross section (33a).</p>
<p id="p0016" num="0016">According to a third aspect of the present disclosure, in each of the blades (20) of the first or the second aspect, the distance from the blade root (21) to the intermediate blade cross section (33a) is longer than the distance from the blade end (22) to the intermediate blade cross section (33a).</p>
<p id="p0017" num="0017">In each blade (20) of the propeller fan (10) of the third aspect, the intermediate blade cross section (33a) is located closer to the blade end (22) than to the center between the blade root (21) and the blade end (22). In this intermediate reference blade cross section (33a), the maximum camber position ratio (d/c) becomes minimum.</p>
<p id="p0018" num="0018">According to a fourth aspect of the present disclosure, in any one of the first to third aspects, in each of the blades (20), the maximum value of the camber in the blade cross section is set as a maximum camber (f), a ratio of the maximum camber (f) to the chord length (c) in the blade cross section, the camber ratio (f/c) becomes maximum in the second reference blade cross section (33, 33b) between the blade root (21) and the blade end (22), monotonically decreases from the second reference blade cross section (33, 33b) toward the blade root (21), and monotonically decreases in the direction from the second reference blade cross section (33, 33b) toward the blade end (22)</p>
<p id="p0019" num="0019">In each of the blades (20) provided to the propeller fan (10) according to the fourth<!-- EPO <DP n="6"> --> aspect, the camber ratio (f/c) becomes maximum in the second reference blade cross section (33, 33b) separated from the blade root (21) by a predetermined distance. That is, in each blade (20), the camber ratio (f/c) monotonically decreases in the direction from the second reference blade cross section (33,33b) toward the blade root (21) and from the second reference blade cross section (33, 33b) toward the blade end (22).</p>
<p id="p0020" num="0020">The phrase "monotonically decrease" described in this specification means "weakly decrease". Accordingly, in each blade (20), the camber ratio (f/c) may continuously decrease from the second reference blade cross section (33, 33b) toward the blade end (22), or may be constant in some sections between the second reference blade cross section (33, 33b) and the blade end (22).</p>
<p id="p0021" num="0021">The area of the blade root (21) of the blade (20) is in the vicinity of the hub (15), so that turbulence of airflow tends to occur. On the other hand, in each blade (20) of the propeller fan (10) of the fourth aspect, the camber ratio (f/c) monotonically decreases in the direction from the second reference blade cross section (33, 33b) toward the blade root (21). That is, the camber ratio (f/c) is smaller in the vicinity of the blade root (21) of the blade (20) where turbulence of airflow tends to occur than in the second reference blade cross section (33, 33b). Therefore, turbulence of airflow in the vicinity of the blade root (21) of each blade (20) is suppressed, and energy consumed by the disturbance is reduced. As a result, fan efficiency is improved.</p>
<p id="p0022" num="0022">Further, in each blade (20) of the propeller fan (10) of the fourth aspect, the camber ratio (f/c) monotonically decreases in the direction from the second reference blade cross section (33, 33b) toward the blade end (22). That is, in each blade (20), the camber ratio (f/c) monotonically decreases in the direction from the second reference blade cross section<!-- EPO <DP n="7"> --> (33,33b) toward the blade end (22) where the circumferential speed is faster than that of the second reference blade cross section (33, 33b). Therefore, the work amount of the blade (20) (specifically, the lift force applied to the blades (20)) is averaged over the entire blade (20), so that the fan efficiency is improved.</p>
<p id="p0023" num="0023">In a fifth aspect of the present disclosure, each of the blades (20) according to the fourth aspect is configured such that the camber ratio (f/c) at the blade end (22) is smaller than the camber ratio (f/c) at the blade root (21).</p>
<p id="p0024" num="0024">Here, in each blade (20) of the propeller fan (10), the circumferential speed of the blade end (22) is higher than that of the blade root (21). Therefore, when the camber ratio (f/c) at the blade end (22) is approximately equal to the camber ratio (f/c) at the blade root (21), the air differential pressure between the positive pressure surface (25) side and the negative pressure surface (26) side near the blade end (22) of each blade (20) becomes too large, resulting in that the flow rate of air flowing from the positive pressure surface (25) side to the negative pressure surface (26) side via the blade end (22) of a blade (20) may increase, thereby causing decrease in fan efficiency.</p>
<p id="p0025" num="0025">In contrast, in each blade (20) of the propeller fan (10) of the fifth aspect, the camber ratio (f/c) at the blade end (22) is smaller than the camber ratio (f/c) at the blade root (21). Therefore, the air differential pressure between the positive pressure surface (25) side and the negative pressure surface (26) side in the vicinity of the blade end (22) of each blade (20) is suppressed to an extent which is not excessively large. As a result, the flow rate of air flowing back from the positive pressure side (25) side to the negative pressure surface (26) side via the blade end (22) of each blade (20) can be reduced, thereby improving fan efficiency. Further, the blade end vortex (90) generated in the vicinity of the blade end (22) is suppressed, so that<!-- EPO <DP n="8"> --> energy consumed to generate the blade end vortex (90) is reduced, which also results in that the fan efficiency is improved.</p>
<heading id="h0006">ADVANTAGES OF THE INVENTION</heading>
<p id="p0026" num="0026">In the first aspect described above, in each blade (20) of the propeller fan (10), the maximum camber position ratio (d/c) at the blade end (22) is larger than the maximum camber position ratio (d/c) at the blade root (21). Therefore, the development of the blade end vortex (90) is suppressed and the blade end vortex (90) is shortened so that energy consumed for the generation of the blade end vortex (90) is reduced. As a result, according to this aspect, the efficiency can be improved by reducing the loss of power of driving the propeller fan (10) to rotate.</p>
<p id="p0027" num="0027">According to the second aspect described above, in each blade (20) of the propeller fan (10), the maximum camber position ratio (d/c) monotonically increases from the first reference blade cross section (33) toward the blade end (22), and becomes maximum at the blade end (22). Therefore, the development of the blade end vortex (90) is suppressed and the blade end vortex (90) is shortened so that energy consumed for the generation of the blade end vortex (90) is reduced. As a result, according to this aspect, the efficiency can be improved by reducing the loss of power of driving the propeller fan (10) to rotate.</p>
<p id="p0028" num="0028">According to the fourth aspect described above, in each blade (20) of the propeller fan (10), the camber ratio (f/c) becomes maximum in the second reference blade cross section (33, 33b) located between the blade root (21) and the blade end (22), and monotonically decreases in the direction from the second reference blade cross section (33, 33b) toward the blade root (21) and monotonically decreases in the direction from the second reference blade cross section (33, 33b) toward the blade end (22). Therefore, turbulence of airflow in the<!-- EPO <DP n="9"> --> vicinity of the blade root (21) of each blade (20) can be suppressed, and the work amount of each blade (20) can be averaged over the entire blade (20). Therefore, according to this aspect, the loss of power of driving the fan to rotate can be further reduced, and fan efficiency can be further improved.</p>
<p id="p0029" num="0029">In each blade (20) of the propeller fan (10) of the fifth aspect described above, the camber ratio (f/c) at the blade end (22) is smaller than the camber ratio (f/c) at the blade root (21). Therefore, it is possible to reduce the flow rate of air flowing from the positive pressure surface (25) side to the negative pressure surface (26) side via the blade end (22) of the blade (20), and the blade end vortex (90) generated in the vicinity of the blade end (22) can be suppressed. Therefore, according to this aspect, the loss of power of driving the fan to rotate can be further reduced, and fan efficiency can be further improved.</p>
<heading id="h0007">BRIEF DESCRIPTION OF THE DRAWINGS</heading>
<p id="p0030" num="0030">
<ul id="ul0001" list-style="none" compact="compact">
<li>[<figref idref="f0001">FIG. 1] FIG. 1</figref> is a perspective view of a propeller fan of an example.</li>
<li>[<figref idref="f0002">FIG. 2] FIG. 2</figref> is a plan view of the propeller fan of the example.</li>
<li>[<figref idref="f0003">FIG. 3] FIG. 3</figref> is a cross-sectional view of a blade cross section of a blade of the propeller fan of the example.</li>
<li>[<figref idref="f0004">FIG. 4] FIG. 4</figref> is a graph showing a relationship between a distance r from the rotational center axis and the camber ratio (f/c) of the blade of the propeller fan of the example.</li>
<li>[<figref idref="f0004">FIG. 5] FIG. 5</figref> is a graph showing a relationship between the distance r from the rotational center axis and the maximum camber position ratio (d/c) of the blade of the propeller fan of the example.<!-- EPO <DP n="10"> --></li>
<li>[<figref idref="f0005">FIG. 6A] FIG. 6A</figref> is a cross-sectional view of the blade showing a blade cross section of a blade root of the blade of the propeller fan of the example.</li>
<li>[<figref idref="f0005">FIG. 6B] FIG. 6B</figref> is a cross-sectional view of the blade showing a reference blade cross section of the blade of the propeller fan of the example.</li>
<li>[<figref idref="f0006">FIG. 6C] FIG. 6C</figref> is a cross-sectional view of the blade showing a blade cross section of a blade end of the blade of the propeller fan the example.</li>
<li>[<figref idref="f0007">FIG.7] FIG. 7</figref> is a perspective view of a propeller fan showing an airflow on the propeller fan of the example</li>
<li>[<figref idref="f0008">FIG.8] FIG. 8</figref> is a perspective view of a conventional propeller fan showing an airflow on the conventional propeller fan</li>
<li>[<figref idref="f0009">FIG. 9] FIG. 9</figref> is a graph showing a relationship between the distance r from the rotational center axis and the camber ratio (f/c) of the blade of the propeller fan of a first variation of the example.</li>
<li>[<figref idref="f0009">FIG. 10] FIG. 10</figref> is a graph showing a relationship between the distance r from the rotational center axis and the maximum camber position ratio (d/c) of the blade of the propeller fan of a second variation of the example.</li>
<li>[<figref idref="f0010">FIG. 11] FIG. 11</figref> is a perspective view of a propeller fan of an embodiment.</li>
<li>[<figref idref="f0011">FIG. 12] FIG. 12</figref> is a plan view of the propeller fan of the embodiment.</li>
<li>[<figref idref="f0012">FIG. 13] FIG. 13</figref> is a graph showing a relationship between the distance r from the rotational center axis and the camber ratio (f/c) of the blade of the propeller fan of the embodiment.</li>
<li>[<figref idref="f0012">FIG. 14] FIG. 14</figref> is a graph showing a relationship between the distance r from the rotational center axis and the maximum camber position ratio (d/c) of the blade of the propeller fan of the embodiment.</li>
<li>[<figref idref="f0013">FIG. 15A] FIG. 15A</figref> is a cross-sectional view of the blade showing a blade cross<!-- EPO <DP n="11"> --> section of the blade root of the blade of the propeller fan of the embodiment.</li>
<li>[<figref idref="f0013">FIG. 15B] FIG. 15B</figref> is a cross-sectional view of the blade showing a second reference blade cross section of the blade of the propeller fan of the embodiment.</li>
<li>[<figref idref="f0013">FIG. 15C] FIG. 15C</figref> is a cross-sectional view of the blade showing a blade cross section of a blade end of the blade of the propeller fan of the embodiment.</li>
</ul></p>
<heading id="h0008">DESCRIPTION OF AN EMBODIMENT AND AN EXAMPLE</heading>
<p id="p0031" num="0031">An embodiment of the present invention and an example will be described in detail with reference to the drawings. Note that the following embodiments and variations are merely beneficial examples in nature, and are not intended to limit the scope, applications, or use of the invention.</p>
<heading id="h0009">«Example»</heading>
<p id="p0032" num="0032">The example will be described. A propeller fan (10) of this embodiment is configured as an axial fan. The propeller fan (10) is provided, for example, in a heat source unit of an air conditioner, and is used to supply outdoor air to a heat-source-side heat exchanger.</p>
<heading id="h0010">- Propeller Fan Configuration -</heading>
<p id="p0033" num="0033">As shown in <figref idref="f0001">FIG. 1</figref> and <figref idref="f0002">FIG. 2</figref>, the propeller fan (10) of this example includes one hub (15) and three blades (20). The hub (15) and the three blades (20) are integrally formed. The propeller fan (10) is made of a resin.</p>
<p id="p0034" num="0034">The hub (15) is formed into a shape of a cylinder whose tip end face (upper surface shown in <figref idref="f0001">FIG. 1</figref>) is closed. The hub (15) is attached to a drive shaft of a fan motor. The center<!-- EPO <DP n="12"> --> axis of the hub (15) is a rotational center axis (11) of the propeller fan (10).</p>
<p id="p0035" num="0035">Each blade (20) is arranged to project outwardly from the outer peripheral surface of the hub (15). The three blades (20) are arranged at regular angular intervals in the circumferential direction of the hub (15). Each blade (20) has a shape extending toward the outside in the radial direction of the propeller fan (10). The blades (20) have the identical shape.</p>
<p id="p0036" num="0036">The blade (20) is configured such that an end portion on a radial center side (i.e., a hub (15) side) of the propeller fan (10) is a blade root (21), and an outer end portion in a radial direction of the propeller fan (10) is a blade end (22). The blade root (21) of each blade (20) is joined to the hub (15). The distance r<sub>i</sub> from the rotational center axis (11) to the blade root (21) of the propeller fan (10) is substantially constant over the entire length of the blade root (21). The distance r<sub>o</sub> from the rotational center axis (11) to the blade end (22) of the propeller fan (10) is also substantially constant over the entire length of the blade end (22).</p>
<p id="p0037" num="0037">The blade (20) is configured such that a front edge in the rotation direction of the propeller fan (10) is a leading edge (23), and a rear edge in the rotation direction of the propeller fan (10) is a trailing edge (24). The leading edge (23) and the trailing edge (24) of the blade (20) extend from the blade root (21) toward the blade end (22) and thus extend toward the outer circumferential side of the propeller fan (10).</p>
<p id="p0038" num="0038">The blade (20) is inclined with respect to a plane orthogonal to the rotational center axis (11) of the propeller fan (10). Specifically, the blade (20) is arranged such that the leading edge (23) is located near a tip end (upper end shown in <figref idref="f0001">FIG. 1</figref>) of the hub (15), and the<!-- EPO <DP n="13"> --> trailing edge (24) is located near a base end (lower end shown in <figref idref="f0001">FIG. 1</figref>) of the hub (15). The blade (20) is configured such that a front surface (a downward face in <figref idref="f0001">FIG. 1</figref>) in the rotation direction of the propeller fan (10) is a positive pressure surface (25), and a rear surface (an upward face in <figref idref="f0001">FIG. 1</figref>) in the rotation direction of the propeller fan (10) is a negative pressure surface (26).</p>
<heading id="h0011">- Detailed Shape of Blades -</heading>
<p id="p0039" num="0039">Hereinafter, the shape of the blade (20) will be described in detail.</p>
<p id="p0040" num="0040">The blade cross section shown in <figref idref="f0003">FIG. 3</figref> is a planer view of a cross section, of a blade (20), located at a distance r from a rotational center axis (11) of a propeller fan (10). As shown in <figref idref="f0003">FIG. 3</figref>, the blade (20) is cambered so as to bulge toward the negative pressure surface (26) side.</p>
<p id="p0041" num="0041">In the blade cross section shown in <figref idref="f0003">FIG. 3</figref>, a line segment connecting the leading edge (23) and the trailing edge (24) is a chord line (31), and an angle formed by the chord line (31) with a "plane orthogonal to the rotational center axis (11) of the propeller fan (10)" is an attaching angle α. The chord length c is a value obtained through dividing the arc length rθ having an arc radius r and a central angle θ by a cosine cosα with respect to the attaching angle α (c = rθ/cosα). Note that θ is a central angle of the blade (20) at the position located with the distance r from the rotational center axis (11) of the propeller fan (10) (see <figref idref="f0002">FIG. 2</figref>), and the unit thereof is radian.</p>
<p id="p0042" num="0042">In the blade cross section shown in <figref idref="f0003">FIG. 3</figref>, a line connecting the midpoints of the positive pressure surface (25) and the negative pressure surface (26) is a mean line (32), and<!-- EPO <DP n="14"> --> the distance from the chord line (31) to the mean line (32) is a camber. The camber gradually increases in the direction from the leading edge (23) to the trailing edge (24) along the chord line (31), becomes maximum halfway between the leading edge (23) and the trailing edge (24), and gradually decreases in the direction from the position, at which the camber becomes maximum, toward the trailing edge (24). The maximum value of the camber is the maximum camber f, and the position on the chord line (31) where the camber reaches the maximum camber f is the maximum camber position A. Further, the distance from the leading edge (23) to the maximum camber position (A) is represented by d.</p>
<heading id="h0012">&lt;Camber Ratio&gt;</heading>
<p id="p0043" num="0043">As shown in <figref idref="f0004">FIG. 4</figref>, in the blade (20) of this example, the camber ratio (f/c), which is the ratio of the maximum camber f to the chord length c in the blade cross section, varies in accordance with the distance from the rotational center axis (11) of the propeller fan (10). This camber ratio (f/c) varies on a way from the blade root (21) to the blade end (22) such that the camber ratio becomes relative maximum only once and never becomes relative minimum.</p>
<p id="p0044" num="0044">Specifically, the camber ratio (f/c) becomes maximum value (f<sub>m</sub>/c<sub>m</sub>) in the reference blade cross section (33) located between the blade root (21) and the blade end (22). Note that f<sub>m</sub> is the maximum camber in the reference blade cross section (33), and c<sub>m</sub> is the chord length in the reference blade cross section (33) (see <figref idref="f0005">FIG. 6B</figref>).</p>
<p id="p0045" num="0045">The camber ratio (f/c) gradually decreases in the direction from the reference blade cross section (33) toward the blade root (21), and gradually decreases in the direction from the reference blade cross section (33) toward the blade end (22). That is, when r<sub>i</sub> ≦ r ≦ r<sub>m</sub>, the camber ratio (f/c) becomes smaller as the distance r becomes shorter, and when r<sub>m</sub> ≦ r ≦ r<sub>o</sub>, the<!-- EPO <DP n="15"> --> camber ratio (f/c) becomes smaller as the distance r becomes longer.</p>
<p id="p0046" num="0046">Here, the reference blade cross section (33) is a blade cross section at a position where the distance from the rotational center axis (11) of the propeller fan (10) is represented by r<sub>m</sub>. That is, the reference blade cross section (33) is a blade cross section which is separated from the blade root (21) by a distance (r<sub>m</sub>-r<sub>i</sub>). In this example, the distance (r<sub>m</sub> - r<sub>i</sub>) from the blade root (21) to the reference blade cross section (33) is about 10% (i.e., about 1/10) of the distance (r<sub>o</sub>-r<sub>i</sub>) from the blade root (21) to the blade end (22). That is, the reference blade cross section (33) is located closer to the blade root (21) than to the center between the blade root (21) and the blade end (22) in the radial direction of the propeller fan (10).</p>
<p id="p0047" num="0047">The distance (r<sub>m</sub>-r<sub>i</sub>) from the blade root (21) to the reference blade cross section (33) is preferably 5% to 30% of the distance (r<sub>o</sub>-r<sub>i</sub>) from the blade root (21) to the blade end (22), more preferably 5% to 20% of the distance (r<sub>o</sub>-r<sub>i</sub>) from the blade root (21) to the blade end (22), and yet more preferably 5% to 10% of the distance (r<sub>o</sub>-r<sub>i</sub>) from the blade root (21) to the blade end (22).</p>
<p id="p0048" num="0048">In the blade (20) of this example, the camber ratio (f<sub>o</sub>/c<sub>o</sub>) at the blade end (22) is smaller than the camber ratio (f<sub>i</sub>/c<sub>i</sub>) at the blade root (21). Specifically, the camber ratio (f<sub>o</sub>/c<sub>o</sub>) at the blade end (22) is substantially the half of the camber ratio (fi/ci) at the blade root (21). The camber ratio (f<sub>o</sub>/c<sub>o</sub>) at the blade end (22) is preferably set to be equal to or less than the half of the camber ratio (f<sub>i</sub>/c<sub>i</sub>) at the blade root (21) and greater than or zero. Note that fi is the maximum camber at the blade root (21), and ci is the chord length at the blade root (21) (see <figref idref="f0005">FIG. 6A</figref>). Further, f<sub>o</sub> is the maximum camber at the blade end (22), and c<sub>o</sub> is the chord length at the blade end (22) (see <figref idref="f0006">FIG. 6C</figref>).<!-- EPO <DP n="16"> --></p>
<heading id="h0013">&lt;Maximum Camber Position Ratio&gt;</heading>
<p id="p0049" num="0049">As shown in <figref idref="f0004">FIG. 5</figref>, in the blade (20) of this example, the maximum camber position ratio (d/c), which is the ratio of the distance d between the leading edge (23) and the maximum camber position A to the chord length c, varies in accordance with the distance from the rotational center axis (11) of the propeller fan (10). The maximum camber position ratio (d/c) varies on a way from the blade root (21) to the blade end (22) such that the maximum camber position ratio becomes relative minimum only once and never becomes relative maximum.</p>
<p id="p0050" num="0050">Specifically, the maximum camber position ratio (d/c) reaches the minimum value (d<sub>m</sub>/c<sub>m</sub>) in the reference blade cross section (33) located between the blade root (21) and the blade end (22). Note that d<sub>m</sub> is the distance from the leading edge (23) to the maximum camber position A in the reference blade cross section (33) (see <figref idref="f0005">FIG. 6B</figref>).</p>
<p id="p0051" num="0051">Further, the maximum camber position ratio (d/c) gradually increases in the direction from the reference blade cross section (33) toward the blade root (21), and gradually increases in the direction from the reference blade cross section (33) toward the blade end (22). That is, when r<sub>i</sub> ≦ r ≦ r<sub>m</sub>, the maximum camber position ratio (d/c) becomes larger as the distance r becomes shorter, and when r<sub>m</sub> I r ≦ r<sub>o</sub>, the maximum camber position ratio (d/c) becomes larger as the distance r becomes longer. As the maximum camber position ratio (d/c) increases, the maximum camber position A moves relatively farther away from the leading edge (23), and the maximum camber position A becomes relatively closer to the trailing edge (24). A maximum camber position line (35) connecting the maximum camber positions Ain the blade cross section, which are respectively positioned at certain distances from the rotational center axis (11) of the propeller fan (10), is indicated by a long dashed double-short dashed line in <figref idref="f0002">FIG.<!-- EPO <DP n="17"> --> 2</figref>.</p>
<p id="p0052" num="0052">In this example, the maximum camber position ratio (d/c) reaches the minimum value and the camber ratio (f/c) reaches the maximum value in the reference blade cross section (33). In other words, in this example, the first reference blade cross section at which the maximum camber position ratio (d/c) reaches the minimum value coincides with the second reference blade cross section at which the camber ratio (f/c) reaches the maximum value.</p>
<p id="p0053" num="0053">In the blade (20) of this example, the maximum camber position ratio (d/c) reaches the maximum value (d<sub>o</sub>/c<sub>o</sub>) at the blade end (22). That is, in the blade (20) of this example, the maximum camber position ratio (d<sub>o</sub>/c<sub>o</sub>) at the blade end (22) is larger than the maximum camber position ratio (d<sub>i</sub>/c<sub>i</sub>) at the blade root (21). Note that di is a distance from the leading edge (23) to the maximum camber position A in the blade root (21) (see <figref idref="f0005">FIG. 6A</figref>), and d<sub>o</sub> is a distance from the leading edge (23) to the maximum camber position A in the blade end (22) (see <figref idref="f0006">FIG. 6C</figref>).</p>
<p id="p0054" num="0054">In the blade (20) of this example, the maximum camber position ratio (d/c) is set to a value equal to or greater than 0.6 and equal to or smaller than 0.7 in all the blade cross sections. It is preferable that the maximum camber position ratio (d/c) is set to a value equal to or greater than 0.5 and equal to or smaller than 0.8.</p>
<heading id="h0014">&lt;Attaching Angle&gt;</heading>
<p id="p0055" num="0055">As shown in <figref idref="f0005 f0006">FIG. 6A to FIG. 6C</figref>, in the blade (20) of this example, the attaching angle α gradually decreases in the direction from the blade root (21) toward the blade end (22). That is,<!-- EPO <DP n="18"> --> the attaching angle α becomes smaller as the blade cross section is farther away from the rotational center axis (11) of the propeller fan (10). Therefore, in the blade (20) of this example, the attaching angle α<sub>i</sub> at the blade root (21) reaches the maximum value, and the attaching angle α<sub>o</sub> at the blade end (22) reaches the minimum value.</p>
<heading id="h0015">- Blowing Effect of Propeller Fan -</heading>
<p id="p0056" num="0056">The propeller fan (10) of this example is driven by a fan motor connected to a hub (15), and rotates in the clockwise direction of <figref idref="f0002">FIG. 2</figref>. When the propeller fan (10) rotates, air is pushed out in the direction of the rotational center axis (11) of the propeller fan (10) by the blades (20).</p>
<p id="p0057" num="0057">In each blade (20) of the propeller fan (10), the air pressure on the positive pressure surface (25) side becomes higher than the atmospheric pressure, and the air pressure on the negative pressure surface (26) side becomes lower than the atmospheric pressure. Therefore, lift force is applied to each of the blades (20) of the propeller fan (10). The lift force pushes the blades (20) in the direction from the positive pressure surface (25) toward the negative pressure surface (26). The lift force is a reaction force for the force with which each of the blades (20) of the propeller fan (10) pushes out air. Accordingly, the larger the lift force applied to the blades (20), the larger the work amount of the blades (20) pushing out air.</p>
<heading id="h0016">&lt;Relationship of the Camber Ratio to Airflow&gt;</heading>
<p id="p0058" num="0058">The region in the vicinity of the blade root (21) of the blade (20) in the propeller fan (10) is the vicinity of the hub (15), so that turbulence of airflow tends to occur. On the other hand, in each blade (20) of the propeller fan (10) of this example, the camber ratio (f/c) gradually decreases in the direction from the reference blade cross section (33) toward the blade root<!-- EPO <DP n="19"> --> (21). That is, the camber ratio (f/c) is smaller in a region in the vicinity of the blade root (21) of the blade (20) where turbulence of airflow tends to occur than in the reference blade cross section (33). Therefore, turbulence of airflow in the vicinity of the blade root (21) of each blade (20) is suppressed, and energy consumed by the disturbance is reduced. As a result, fan efficiency is improved, and power consumption of the fan motor driving the propeller fan (10) is reduced.</p>
<p id="p0059" num="0059">In addition, in each blade (20) of the propeller fan (10) of this example, the camber ratio (f/c) gradually decreases in the direction from the reference blade cross section (33) toward the blade end (22). That is, in each blade (20), the camber ratio (f/c) gradually decreases in the direction from the reference blade cross section (33) toward the blade end (22) where the circumferential speed is faster than that of the reference blade cross section (33). Therefore, the work amount of the blade (20) (specifically, the lift force applied to the blades (20)) is averaged over the entire blade (20), so that the fan efficiency is improved.</p>
<p id="p0060" num="0060">Here, in each blade (20) of the propeller fan (10), the circumferential speed of the blade end (22) is higher than that of the blade root (21). Therefore, when the camber ratio (f<sub>o</sub>/c<sub>o</sub>) at the blade end (22) is approximately equal to the camber ratio (f<sub>i</sub>/c<sub>i</sub>) at the blade root (21), the air differential pressure between the positive pressure surface (25) side and the negative pressure surface (26) side near the blade end (22) of each blade (20) becomes too large, resulting in that the flow rate of air flowing from the positive pressure surface (25) side to the negative pressure surface (26) side via the blade end (22) of a blade (20) may increase, thereby causing decrease in fan efficiency.</p>
<p id="p0061" num="0061">On the other hand, in each blade (20) of the propeller fan (10) of this example, the<!-- EPO <DP n="20"> --> camber ratio (f<sub>o</sub>/c<sub>o</sub>) at the blade end (22) is approximately the half of the camber ratio (f<sub>i</sub>/c<sub>i</sub>) at the blade root (21). Therefore, the air differential pressure between the positive pressure surface (25) side and the negative pressure surface (26) side in the vicinity of the blade end (22) of each blade (20) is suppressed to an extent which is not excessively large. As a result, the flow rate of air flowing back from the positive pressure side (25) side to the negative pressure surface (26) side via the blade end (22) of each blade (20) can be reduced, thereby improving fan efficiency. Further, the blade end vortex (90) generated in the vicinity of the blade end (22) is suppressed, so that energy consumed to generate the blade end vortex (90) is reduced, which also results in that the fan efficiency is improved.</p>
<heading id="h0017">&lt;Relationship between Maximum Camber Position Ratio to Airflow&gt;</heading>
<p id="p0062" num="0062">In the blade (20) of the propeller fan (10), a blade end vortex (90) is generated in the vicinity of a position where the camber becomes maximum at the blade end (22). As shown in <figref idref="f0008">FIG. 8</figref>, as the generation position of the blade end vortex (90) approaches to the leading edge (23) of the blade (80), the blade end vortex (90) becomes longer, and energy consumed for the generation of the blade end vortex (90) increases.</p>
<p id="p0063" num="0063">On the other hand, in each blade (20) of the propeller fan (10) of this example, the maximum camber position ratio (d/c) gradually increases in the direction from the reference blade cross section (33) toward the blade end (22). That is, in each blade (20), the maximum camber position A at which the camber becomes maximum in the blade cross section becomes relatively closer to the trailing edge (24) of the blade (20) in the direction from the reference blade cross section (33) toward the blade end (22). As shown in <figref idref="f0007">FIG. 7</figref>, the position where the blade end vortex (90) is generated in the blade (20) of this example is closer to the trailing edge (24) of the blade (20) than that in the conventional blade (80) shown in <figref idref="f0008">FIG. 8</figref>.<!-- EPO <DP n="21"> --> Therefore, the development of the blade end vortex (90) is suppressed and the blade end vortex (90) is shortened so that energy consumed for the generation of the blade end vortex (90) is reduced. As a result, fan efficiency is improved, and power consumption of the fan motor driving the propeller fan (10) is reduced.</p>
<p id="p0064" num="0064">Here, there is a case where the airflow flowing from the leading edge (23) to the trailing edge (24) along the negative pressure surface (26) of the blade (20) separates from the negative pressure surface (26) of the blade (20) in the vicinity of the region where the airflow just passes by the maximum camber position A. Therefore, if the maximum camber position A is too close to the leading edge (23), the region where the airflow separates from the negative pressure surface (26) of the blade (20) is enlarged, which may lead to increase in blowing sound and decrease in fan efficiency. In order to avoid this problem, it is desirable to set the maximum camber position ratio (d/c) to a value equal to or greater than 0.5. In view of the above, in the blade (20) of this example, the maximum camber position ratio (d/c) is set to equal to or greater than 0.6.</p>
<p id="p0065" num="0065">When the maximum camber position A is too close to the trailing edge (24), the shape of the blade cross section is sharply bent at a position near the trailing edge (24). Therefore, when the maximum camber position A is too close to the trailing edge (24), the airflow flowing along the negative pressure surface (26) of the blade (20) tends to separate from the negative pressure surface (26). When the airflow separates from the negative pressure surface (26) of the blade (20), there arises a possibility of increased blowing sound and decreased fan efficiency. In order to avoid this problem, it is desirable to set the maximum camber position ratio (d/c) to a value equal to or less than 0.8. In view of the above, in the blade (20) of this example, the maximum camber position ratio (d/c) is set to equal to or less<!-- EPO <DP n="22"> --> than 0.7.</p>
<p id="p0066" num="0066">As described above, in the blade (20) of this example, the attaching angle α becomes larger in the blade cross section located closer to the blade root (21). The larger the attaching angle α is, the more easily airflow flowing along the negative pressure surface (26) of the blade (20) separates from the negative pressure surface (26). On the other hand, when the maximum camber position ratio (d/c) is substantially equal to or greater than 0.5, the smaller the maximum camber position ratio (d/c) is (i. e., the closer the maximum camber position A is to the leading edge (23)), the less likely airflow flowing along the negative pressure surface (26) of the blade (20) separates from the negative pressure surface (26). Therefore, in the blade (20) of this example, in the region between the blade end (22) and the reference blade cross section (33), the maximum camber position ratio (d/c) gradually decreases as the reference blade cross section gets closer to the blade root (21) (i. e., as the attaching angle α increases), thereby making it difficult for the airflow from separating from the negative pressure surface (26) of the blade (20).</p>
<heading id="h0018">- Advantages of Example -</heading>
<p id="p0067" num="0067">In each blade (20) of the propeller fan (10) of this example, the maximum camber position ratio (d/c) gradually increases from the reference blade cross section (33) to the blade end (22), and becomes maximum at the blade end (22). Therefore, the development of the blade end vortex (90) is suppressed and the blade end vortex (90) is shortened so that energy consumed for the generation of the blade end vortex (90) is reduced. As a result, according to this example, fan efficiency can be improved by reducing the loss of power of driving the fan to rotate, and the power consumption of the fan motor driving the propeller fan (10) can be reduced.<!-- EPO <DP n="23"> --></p>
<p id="p0068" num="0068">In each blade (20) of the propeller fan (10) of this example, the maximum camber position ratio (d/c) is set to equal to or greater than 0.5 to equal to or less than 0.8. Therefore, the airflow is less likely to separate from the negative pressure surface (26) of the blade (20), so that the increase in air blowing sound caused by the airflow detached and the reduction in fan efficiency can be avoided.</p>
<p id="p0069" num="0069">In each blade (20) of the propeller fan (10) of this example, the camber ratio (f/c) becomes maximum in the reference blade cross section (33), gradually decreases in the direction from the reference blade cross section (33) toward the blade root (21), and gradually decreases in the direction from the reference blade cross section (33) toward the blade end (22). Therefore, turbulence of airflow in the vicinity of the blade root (21) of each blade (20) can be suppressed, and the work amount of each blade (20) can be averaged over the entire blade (20). Therefore, according to this example, it is possible to further reduce the loss of power of driving the fan to rotate, and to further improve the fan efficiency.</p>
<p id="p0070" num="0070">Moreover, in each blade (20) of the propeller fan (10) of this example, the camber ratio (f/c) at the blade end (22) is smaller than the camber ratio (f/c) at the blade root (21). Therefore, it is possible to reduce the flow rate of air flowing from the positive pressure surface (25) side to the negative pressure surface (26) side via the blade end (22) of the blade (20), and the blade end vortex (90) generated in the vicinity of the blade end (22) can be suppressed. Therefore, according to this example, it is possible to further reduce the loss of power of driving the fan to rotate, and to further improve the fan efficiency.</p>
<heading id="h0019">-First Variation of Example-</heading><!-- EPO <DP n="24"> -->
<p id="p0071" num="0071">In each blade (20) of the propeller fan (10) of this example, there may be a section in which the camber ratio (f/c) is constant in one or both of: the region from the blade root (21) to the reference blade cross section (33); and the region from the reference blade cross section (33) to the blade end (22). For example, as shown in <figref idref="f0009">FIG. 9</figref>, the camber ratio (f/c) may be constant in a region extending from a position near the blade end (22) to the blade end (22) in the blade (20).</p>
<heading id="h0020">- Second Variation of Example -</heading>
<p id="p0072" num="0072">In each blade (20) of the propeller fan (10) of this example, there may be a section in which the maximum camber position ratio (d/c) is constant in one or both of: the region from the blade root (21) to the reference blade cross section (33); and the region from the reference blade cross section (33) to the blade end (22). Further, as shown in <figref idref="f0009">FIG. 10</figref>, the maximum camber position ratio (d/c) may be constant in a region extending from the blade root (21) to the reference blade cross section (33) in the blade (20). In this case, the maximum camber position ratio (d/c) has a minimum value in a region extending from the blade root (21) to the reference blade cross section (33) in the blade (20).</p>
<heading id="h0021">&lt;&lt;Embodiment&gt;&gt;</heading>
<p id="p0073" num="0073">An embodiment will be described. A propeller fan (10) of this embodiment is obtained by changing the shape of blades (20) of the propeller fan (10) of the example. The propeller fan (10) of this embodiment will be described mainly through explaining a difference between the propeller fan (10) of this embodiment and the propeller fan (10) of the example.</p>
<p id="p0074" num="0074">As shown in <figref idref="f0010">FIG. 11</figref> and <figref idref="f0011">FIG. 12</figref>, the propeller fan (10) of this embodiment includes one hub (15) and three blades (20), as is the case with the propeller fan (10) of the example.<!-- EPO <DP n="25"> --></p>
<heading id="h0022">- Detailed Shape of Blades -</heading>
<p id="p0075" num="0075">The shape of the blade (20) will be described in detail. The blade (20) of this embodiment is formed to have a curved shape so as to bulge in the direction of the negative pressure surface (26) side. In this point, the embodiment has in common with the blades (20) of the example.</p>
<heading id="h0023">&lt;Camber Ratio&gt;</heading>
<p id="p0076" num="0076">As shown in <figref idref="f0012">FIG. 13</figref>, in the blade (20) of this embodiment, the camber ratio (f/c), which is the ratio of the maximum camber f to the chord length c in the blade cross section, varies in accordance with the distance from the rotational center axis (11) of the propeller fan (10). This camber ratio (f/c) varies on a way from the blade root (21) to the blade end (22) such that the camber ratio becomes relative maximum only once and never becomes relative minimum.</p>
<p id="p0077" num="0077">Specifically, the camber ratio (f/c) reaches the maximum value (f<sub>m2</sub>/c<sub>m2</sub>) in the second reference blade cross section (33b) located between the blade root (21) and the blade end (22). Note that f<sub>m2</sub> is the maximum camber in the second reference blade cross section (33b), and c<sub>m2</sub> is the chord length in the second reference blade cross section (33b) (see <figref idref="f0013">FIG. 15B</figref>).</p>
<p id="p0078" num="0078">The camber ratio (f/c) decreases gradually in the direction from the second reference blade cross section (33b) toward the blade root (21), and gradually decreases in the direction from the second reference blade cross section (33b) toward the blade end (22). That is, when r<sub>i</sub> ≦ r ≦ r<sub>m2</sub>, the camber ratio (f/c) becomes larger as the distance r becomes larger, and when r<sub>m2</sub> ≦ r ≦ r<sub>o</sub>, the camber ratio (f/c) becomes smaller as the distance r becomes larger.</p>
<p id="p0079" num="0079"><!-- EPO <DP n="26"> --> Here, the second reference blade cross section (33b) is a blade cross section at a position at which the distance from the rotational center axis (11) of the propeller fan (10) is represented by r<sub>m2</sub>. That is, the second reference blade cross section (33b) is a blade cross section which is separated from the blade root (21) by a distance (r<sub>m2</sub>-r<sub>i</sub>). In this embodiment, the distance (r<sub>m2</sub>-r<sub>i</sub>) from the blade root (21) to the second reference blade cross section (33b) is about 15% of the distance (r<sub>o</sub>-r<sub>i</sub>) from the blade root (21) to the blade end (22). That is, the second reference blade cross section (33b) is located closer to the blade root (21) than to the center of the blade root (21) and the blade end (22) in the radial direction of the propeller fan (10).</p>
<p id="p0080" num="0080">In the blade (20) of this embodiment, the camber ratio (f<sub>o</sub>/c<sub>o</sub>) at the blade end (22) is smaller than the camber ratio (f<sub>i</sub>/c<sub>i</sub>) at the blade root (21). Specifically, the camber ratio (f<sub>o</sub>/c<sub>o</sub>) at the blade end (22) is about 55% of the camber ratio (f<sub>i</sub>/c<sub>i</sub>) at the blade root (21). Note that fi is the maximum camber in the blade root (21), and ci is the chord length in the blade root (21) (see <figref idref="f0013">FIG. 15A</figref>). Further, f<sub>o</sub> is the maximum camber at the blade end (22), and c<sub>o</sub> is the chord length at the blade end (22) (see <figref idref="f0013">FIG. 15C</figref>).</p>
<heading id="h0024">&lt;Maximum Camber Position Ratio&gt;</heading>
<p id="p0081" num="0081">As shown in <figref idref="f0012">FIG. 14</figref>, in the blade (20) of this embodiment, the maximum camber position ratio (d/c), which is the ratio of the distance d between the leading edge (23) and the maximum camber position A to the chord length c, varies in accordance with the distance from the rotational center axis (11) of the propeller fan (10). The maximum camber position ratio (d/c) varies on a way from the blade root (21) to the blade end (22) such that the maximum camber position ratio becomes relative maximum only once and never becomes relative minimum.<!-- EPO <DP n="27"> --></p>
<p id="p0082" num="0082">Specifically, the maximum camber position ratio (d/c) has a maximum value (d<sub>m1</sub>/c<sub>m1</sub>) in the intermediate blade cross section (33a) located between the blade root (21) and the blade end (22). Note that d<sub>m1</sub> is the distance from the leading edge (23) to the maximum camber position A in the intermediate blade cross section (33).</p>
<p id="p0083" num="0083">The maximum camber position ratio (d/c) gradually increases in the direction from the intermediate blade cross section (33a) toward the blade root (21), and gradually decreases in the direction from the intermediate blade cross section (33a) toward the blade end (22). That is, when r<sub>i</sub> ≦ r ≦ r<sub>m1</sub>, the maximum camber position ratio (d/c) becomes larger as the distance r becomes larger, and when r<sub>m1</sub> ≦ r ≦ r<sub>o</sub>, the maximum camber position ratio (d/c) becomes smaller as the distance r becomes larger. As the maximum camber position ratio (d/c) increases, the maximum camber position A moves relatively farther away from the leading edge (23), and the maximum camber position A becomes relatively closer to the trailing edge (24). A maximum camber position line (35) connecting the maximum camber positions Ain the blade cross section, which are positioned at certain distances from the rotational center axis (11) of the propeller fan (10), is indicated by a long dashed double-short dashed line in <figref idref="f0011">FIG. 12</figref>.</p>
<p id="p0084" num="0084">Here, the intermediate blade cross section (33a) is a blade cross section at a position at which the distance from the rotational center axis (11) of the propeller fan (10) is represented by r<sub>m1</sub>. That is, the intermediate blade cross section (33a) is a blade cross section which is separated from the blade root (21) by a distance (r<sub>m1</sub>-r<sub>i</sub>). In this embodiment, the distance (r<sub>m1</sub> - r<sub>i</sub>) from the blade root (21) to the intermediate blade cross section (33a) is about 90% of the distance (r<sub>o</sub>-r<sub>i</sub>) from the blade root (21) to the blade end (22). That is, intermediate blade cross section (33a) is located closer to the blade end (22) than to the center<!-- EPO <DP n="28"> --> of the blade root (21) and the blade end (22) in the radial direction of the propeller fan (10).</p>
<p id="p0085" num="0085">In the blade (20) of this embodiment, the maximum camber position ratio (d<sub>o</sub>/c<sub>o</sub>) at the blade end (22) is larger than the maximum camber position ratio (d<sub>i</sub>/c<sub>i</sub>) at the blade root (21). Note that di is a distance from the leading edge (23) to the maximum camber position A in the blade root (21) (see <figref idref="f0013">FIG. 15A</figref>), and d<sub>o</sub> is a distance from the leading edge (23) to the maximum camber position A in the blade end (22) (see <figref idref="f0013">FIG. 15C</figref>).</p>
<p id="p0086" num="0086">In the blade (20) of this embodiment, the maximum camber position ratio (d/c) is set to a value equal to or greater than 0.55 and equal to or smaller than 0.65 in all the blade cross sections. As is the case with the blade (20) of the example, it is preferable in the blade (20) of this embodiment that the maximum camber position ratio (d/c) is set to a value equal to or greater than 0.5 and equal to or smaller than 0.8.</p>
<heading id="h0025">&lt;Attaching Angle&gt;</heading>
<p id="p0087" num="0087">As shown in <figref idref="f0013">FIG. 15A to FIG. 15C</figref>, in the blade (20) of this embodiment, the attaching angle α gradually decreases in the direction from the blade root (21) to the blade end (22) as is the case with the blade (20) of the example. That is, the attaching angle α becomes smaller in the blade cross section farther away from the rotational center axis (11) of the propeller fan (10). Therefore, in the blade (20) of this embodiment, the attaching angle α<sub>i</sub> at the blade root (21) reaches the maximum value, and the attaching angle α<sub>o</sub> at the blade end (22) reaches the minimum value.</p>
<heading id="h0026">- Blowing Effect of Propeller Fan -</heading>
<p id="p0088" num="0088">The propeller fan (10) of this embodiment is driven by a fan motor connected to the hub (15),<!-- EPO <DP n="29"> --> and rotates in the clockwise direction of <figref idref="f0011">FIG. 12</figref>. When the propeller fan (10) rotates, air is pushed out in the direction of the rotational center axis (11) of the propeller fan (10) by the blades (20). Further, in each blade (20) of the propeller fan (10), the air pressure on the positive pressure (25) side becomes higher than the atmospheric pressure, and the air pressure on the negative pressure surface (26) side becomes lower than the atmospheric pressure.</p>
<heading id="h0027">&lt;Relationship of Camber ratio to Airflow&gt;</heading>
<p id="p0089" num="0089">In the propeller fan (10) of this embodiment, the camber ratio (f/c) is smaller in the vicinity of the blade root (21) of the blade (20) where turbulence of airflow is likely to occur than in the second reference blade cross section (33b). Therefore, as is the case with the propeller fan (10) of the example, turbulence of airflow in the vicinity of the blade root (21) of each blade (20) is suppressed, and energy consumed by the disturbance is reduced. As a result, fan efficiency is improved, and power consumption of the fan motor driving the propeller fan (10) is reduced.</p>
<p id="p0090" num="0090">Further, in each blade (20) of the propeller fan (10) of this embodiment, the camber ratio (f/c) gradually decreases in the direction from the second reference blade cross section (33b) toward the blade end (22) where the circumferential speed is faster than that of the second reference blade cross section (33b). Therefore, the work amount of the blade (20) (specifically, the lift force applied to the blades (20)) is averaged over the entire blade (20), so that the fan efficiency is improved.</p>
<p id="p0091" num="0091">Moreover, in each blade (20) of the propeller fan (10) of this embodiment, the camber ratio (f<sub>o</sub>/c<sub>o</sub>) at the blade end (22) is approximately 56% of the camber ratio (f<sub>i</sub>/c<sub>i</sub>) at the blade root (21). Therefore, similar to the propeller fan (10) of the example, the air differential<!-- EPO <DP n="30"> --> pressure between the positive pressure surface (25) side and the negative pressure surface (26) side in the vicinity of the blade end (22) of each blade (20) is suppressed to an extent which is not excessively large. Therefore, the flow rate of air flowing from the positive pressure side (25) side to the negative pressure surface (26) side of the blade (20) can be reduced, and the blade end vortex (90) generated in the vicinity of the blade end (22) can be suppressed, so that fan efficiency can be improved.</p>
<heading id="h0028">&lt;Relationship between Maximum Camber Position Ratio to Airflow&gt;</heading>
<p id="p0092" num="0092">In each blade (20) of the propeller fan (10) of this embodiment, the maximum camber position ratio (d<sub>o</sub>/c<sub>o</sub>) at the blade end (22) is larger than the maximum camber position ratio (d<sub>i</sub>/c<sub>i</sub>) at the blade root (21). That is, at the blade end (22) of each blade (20), the maximum camber position A at which the camber becomes maximum in the blade cross section becomes relatively closer to the trailing edge (24) of the blade (20). In the blade (20) of this embodiment, similar to the blade (20) of the example, the position where the blade end vortex (90) is generated in the blade (20) of this embodiment is close to the trailing edge (24) of the blade (20). Therefore, the blade end vortex (90) is shortened so that energy consumed for the generation of the blade end vortex (90) is reduced, so that the energy consumption of the fan motor driving the propeller fan (10) is reduced.</p>
<p id="p0093" num="0093">Further, as described in connection with the example, it is preferable in each blade (20) of the propeller fan (10) that the maximum camber position ratio (d/c) is set to a value equal to or greater than 0.5 and equal to or smaller than 0.8. In the propeller fan (10) of this embodiment, the maximum camber position ratio (d/c) of each blade (20) is set to a value equal to or greater than 0.55 and equal to or smaller than 0.65. As a result, a region where the airflow separates from the negative pressure surface (26) of the blade (20) is reduced, so that<!-- EPO <DP n="31"> --> the blowing sound is reduced and the fan efficiency is improved.</p>
<p id="p0094" num="0094">In each blade (20) of the propeller fan (10) of this embodiment, the maximum camber position ratio (d/c) gradually decreases as approaching the blade root (21) in a region between the intermediate blade cross section (33a) and the blade root (21) (i. e., as the attaching angle α increases). Therefore, as is the case with the propeller fan (10) of the example, the airflow is less likely to separate from the negative pressure surface (26) of the blade (20).</p>
<heading id="h0029">- Advantages of the Embodiment -</heading>
<p id="p0095" num="0095">According to the propeller fan (10) of this embodiment, effects similar to those obtained by the propeller fan (10) of the example can be obtained.</p>
<heading id="h0030">INDUSTRIAL APPLICABILITY</heading>
<p id="p0096" num="0096">As described above, the present invention is usable as a propeller fan for use in a blower or the like.</p>
<heading id="h0031">DESCRIPTION OF REFERENCE CHARACTERS</heading>
<p id="p0097" num="0097">
<ul id="ul0002" list-style="none" compact="compact">
<li>10 Propeller Fan</li>
<li>15 Hub</li>
<li>20 Blade</li>
<li>21 Blade Root</li>
<li>22 Blade End<!-- EPO <DP n="32"> --></li>
<li>31 Chord line</li>
<li>32 Mean line</li>
<li>33 Reference Blade Cross Section (First Reference Blade Cross Section, Second Reference Blade Cross Section)</li>
<li>33a Intermediate Blade Cross Section</li>
<li>33b Second Reference Blade Cross Section</li>
</ul></p>
</description>
<claims id="claims01" lang="en"><!-- EPO <DP n="33"> -->
<claim id="c-en-01-0001" num="0001">
<claim-text>A propeller fan, comprising a hub (15) formed into a cylindrical shape, and a plurality of blades (20) extending outwardly from a side surface of the hub (15), wherein
<claim-text>each of the blades (20) is configured such that</claim-text>
<claim-text>a distance from a chord line (31) to a mean line (32) in a blade cross section is set as a camber, that in the blade cross section,</claim-text>
<claim-text>a position on the chord line (31) where the camber becomes maximum is set as a maximum camber position (A), that</claim-text>
<claim-text>a ratio of a distance (d) between a leading edge (23) and the maximum camber position (A) in the blade cross section to a chord length (c) is set as a maximum camber position ratio (d/c), that</claim-text>
<claim-text>an end portion at the hub (15) side of the blade (20) is set as a blade root (21), that</claim-text>
<claim-text>an end portion of an outer circumferential side of the blade (20) is set as a blade end (22),</claim-text>
<claim-text><b>characterized in that</b></claim-text>
<claim-text>the maximum camber position ratio (d/c) at the blade end (22) is larger than the maximum camber position ratio (d/c) at the blade root (21), wherein each of the blades (20) is configured such that the maximum camber position ratio (d/c) becomes maximum in an intermediate blade cross section (33a) located between the blade root (21) and the blade end (22).</claim-text></claim-text></claim>
<claim id="c-en-01-0002" num="0002">
<claim-text>The propeller fan of claim 1, wherein<br/>
<!-- EPO <DP n="34"> -->each of the blades (20) is configured such that the maximum camber position ratio (d/c) becomes minimum at the blade root (21) and monotonically increases in the direction from the blade root (21) toward the intermediate blade cross section (33a).</claim-text></claim>
<claim id="c-en-01-0003" num="0003">
<claim-text>The propeller fan of claim 1 or 2, wherein<br/>
each of the blades (20) is configured such that a distance from the blade root (21) to the intermediate reference blade cross section (33a) is longer than a distance from the blade end (22) to the intermediate reference blade cross section (33a).</claim-text></claim>
<claim id="c-en-01-0004" num="0004">
<claim-text>The propeller fan of any one of claims 1 to 3, wherein
<claim-text>each of the blades (20) is configured such that</claim-text>
<claim-text>a maximum value of the camber in the blade cross section is set as a maximum camber (f), that</claim-text>
<claim-text>a ratio of the maximum camber (f) to the chord length (c) in the blade cross section is set as a camber ratio (f/c), and that</claim-text>
<claim-text>the camber ratio (f/c) becomes maximum in the second reference blade cross section (33, 33b) located between the blade root (21) and the blade end (22), monotonically decreases in the direction from the second reference blade cross section (33, 33b) toward the blade root (21), and monotonically decreases in the direction from the second reference blade cross section (33, 33b) toward the blade end (22).</claim-text></claim-text></claim>
<claim id="c-en-01-0005" num="0005">
<claim-text>The propeller fan of claim 4, wherein<br/>
each of the blades (20) is configured such that the camber ratio (f/c) at the blade end (22) is smaller than the camber ratio (f/c) at the blade root (21).</claim-text></claim>
</claims>
<claims id="claims02" lang="de"><!-- EPO <DP n="35"> -->
<claim id="c-de-01-0001" num="0001">
<claim-text>Propellerlüfter, der eine Nabe (15), die in einer zylindrischen Form gebildet ist, und eine Vielzahl von Blättern (20), die sich von einer Seitenoberfläche der Nabe (15) nach außen erstrecken, umfasst, wobei
<claim-text>jedes der Blätter (20) derart konfiguriert ist, dass</claim-text>
<claim-text>ein Abstand von einer Sehnenlinie (31) zu einer Mittellinie (32) in einem Blattquerschnitt als eine Wölbung festgelegt ist, dass in dem Blattquerschnitt</claim-text>
<claim-text>eine Position auf der Sehnenlinie (31), an der die Wölbung maximal wird, als eine maximale Wölbungsposition (A) festgelegt ist, dass</claim-text>
<claim-text>ein Verhältnis eines Abstands (d) zwischen einer Vorderkante (23) und der maximalen Wölbungsposition (A) in dem Blattquerschnitt zu einer Sehnenlänge (c) als ein maximales Wölbungspositionsverhältnis (d/c) festgelegt ist, dass</claim-text>
<claim-text>ein Endabschnitt an der Seite der Nabe (15) des Blattes (20) als eine Blattwurzel (21) festgelegt ist, dass ein Endabschnitt einer äußeren Umfangsseite des Blattes (20) als ein Blattende (22) festgelegt ist,</claim-text>
<claim-text><b>dadurch gekennzeichnet, dass</b></claim-text>
<claim-text>das maximale Wölbungspositionsverhältnis (d/c) an dem Blattende (22) größer als das maximale Wölbungspositionsverhältnis (d/c) an der Blattwurzel (21) ist, wobei jedes der Blätter (20) derart konfiguriert ist, dass das maximale Wölbungspositionsverhältnis (d/c) in einem Zwischenblattquerschnitt (33a), der sich zwischen der Blattwurzel (21) und dem Blattende (22) befindet, maximal wird.</claim-text></claim-text></claim>
<claim id="c-de-01-0002" num="0002">
<claim-text>Propellerlüfter nach Anspruch 1, wobei<br/>
jedes der Blätter (20) derart konfiguriert ist, dass das maximale Wölbungspositionsverhältnis (d/c) an der Blattwurzel (21) minimal wird und in der Richtung von der Blattwurzel (21) hin zu dem Zwischenblattquerschnitt (33a) monoton zunimmt.</claim-text></claim>
<claim id="c-de-01-0003" num="0003">
<claim-text>Propellerlüfter nach Anspruch 1 oder 2, wobei<br/>
jedes der Blätter (20) derart konfiguriert ist, dass ein Abstand von der Blattwurzel (21) zu dem Zwischenreferenzblattquerschnitt (33a) länger als ein Abstand von dem Blattende (22) zu dem Zwischenreferenzblattquerschnitt (33a) ist.<!-- EPO <DP n="36"> --></claim-text></claim>
<claim id="c-de-01-0004" num="0004">
<claim-text>Propellerlüfter nach einem der Ansprüche 1 bis 3, wobei
<claim-text>jedes der Blätter (20) derart konfiguriert ist, dass</claim-text>
<claim-text>ein Maximalwert der Wölbung in dem Blattquerschnitt als eine maximale Wölbung (f) festgelegt ist, dass</claim-text>
<claim-text>ein Verhältnis der maximalen Wölbung (f) zu der Sehnenlänge (c) in dem Blattquerschnitt als ein Wölbungsverhältnis (f/c) festgelegt ist, und dass</claim-text>
<claim-text>das Wölbungsverhältnis (f/c) in dem zweiten Referenzblattquerschnitt (33, 33b), der sich zwischen der Blattwurzel (21) und dem Blattende (22) befindet, maximal wird, in der Richtung von dem zweiten Referenzblattquerschnitt (33, 33b) hin zu der Blattwurzel (21) monoton abnimmt, und in der Richtung von dem zweiten Referenzblattquerschnitt (33, 33b) hin zu dem Blattende (22) monoton abnimmt.</claim-text></claim-text></claim>
<claim id="c-de-01-0005" num="0005">
<claim-text>Propellerlüfter nach Anspruch 4, wobei<br/>
jedes der Blätter (20) derart konfiguriert ist, dass das Wölbungsverhältnis (f/c) an dem Blattende (22) kleiner als das Wölbungsverhältnis (f/c) an der Blattwurzel (21) ist.</claim-text></claim>
</claims>
<claims id="claims03" lang="fr"><!-- EPO <DP n="37"> -->
<claim id="c-fr-01-0001" num="0001">
<claim-text>Ventilateur hélicoïdal, comprenant un moyeu (15) formé selon une forme cylindrique, et une pluralité de pales (20) s'étendant vers l'extérieur depuis une surface latérale du moyeu (15), dans lequel
<claim-text>chacune des pales (20) est configurée de telle sorte que</claim-text>
<claim-text>une distance depuis une ligne de corde (31) jusqu'à une ligne médiane (32) dans une section transversale de pale est définie comme étant une cambrure, que dans la section transversale de pale,</claim-text>
<claim-text>une position sur la ligne de corde (31) où la cambrure devient maximale est définie comme étant une position de cambrure maximale (A), que</claim-text>
<claim-text>un rapport d'une distance (d) entre un bord d'attaque (23) et la position de cambrure maximale (A) dans la section transversale de pale et d'une longueur de corde (c) est défini comme étant un rapport de position de cambrure maximale (d/c), que</claim-text>
<claim-text>une partie d'extrémité au niveau du côté moyeu (15) de la pale (20) est définie comme étant une emplanture (21) de pale, qu'une partie d'extrémité d'un côté circonférentiel extérieur de la pale (20) est définie comme étant une extrémité (22) de pale,</claim-text>
<claim-text><b>caractérisé en ce que</b></claim-text>
<claim-text>le rapport de position de cambrure maximale (d/c) au niveau de l'extrémité (22) de pale est supérieur au rapport de position de cambrure maximale (d/c) au niveau de l'emplanture (21) de pale, dans lequel chacune des pales (20) est configurée de telle sorte que le rapport de position de cambrure maximale (d/c) devient maximal dans une section transversale de pale intermédiaire (33a) située entre l'emplanture (21) de pale et l'extrémité (22) de pale.</claim-text></claim-text></claim>
<claim id="c-fr-01-0002" num="0002">
<claim-text>Ventilateur hélicoïdal selon la revendication 1, dans lequel<br/>
chacune des pales (20) est configurée de telle sorte que le rapport de position de cambrure maximale (d/c) devient minimal au niveau de l'emplanture (21) de pale et augmente de manière monotone dans la direction de l'emplanture (21) de pale vers la section transversale de pale intermédiaire (33a).<!-- EPO <DP n="38"> --></claim-text></claim>
<claim id="c-fr-01-0003" num="0003">
<claim-text>Ventilateur hélicoïdal selon la revendication 1 ou la revendication 2, dans lequel<br/>
chacune des pales (20) est configurée de telle sorte qu'une distance de l'emplanture (21) de pale à la section transversale de pale de référence intermédiaire (33a) est plus longue qu'une distance de l'extrémité (22) de pale à la section transversale de pale de référence intermédiaire (33a).</claim-text></claim>
<claim id="c-fr-01-0004" num="0004">
<claim-text>Procédé selon l'une quelconque des revendications 1 à 3, dans lequel
<claim-text>chacune des pales (20) est configurée de telle sorte que</claim-text>
<claim-text>une valeur maximale de la cambrure dans la section transversale de pale est définie comme étant une cambrure maximale (f), que</claim-text>
<claim-text>un rapport de la cambrure maximale (f) et de la longueur de corde (c) dans la section transversale de pale est défini comme étant un rapport de cambrure (f/c), et que</claim-text>
<claim-text>le rapport de cambrure (f/c) devient maximal dans la deuxième section transversale de pale de référence (33, 33b) située entre l'emplanture (21) de pale et l'extrémité (22) de pale, diminue de manière monotone dans la direction de la deuxième section transversale de pale de référence (33, 33b) vers l'emplanture (21) de pale et diminue de manière monotone dans la direction de la deuxième section transversale de pale de référence (33, 33b) vers l'extrémité (22) de pale.</claim-text></claim-text></claim>
<claim id="c-fr-01-0005" num="0005">
<claim-text>Ventilateur hélicoïdal selon la revendication 4, dans lequel<br/>
chacune des pales (20) est configurée de telle sorte que le rapport de cambrure (f/c) au niveau de l'extrémité (22) de pale est inférieur au rapport de cambrure (f/c) au niveau de l'emplanture (21) de pale.</claim-text></claim>
</claims>
<drawings id="draw" lang="en"><!-- EPO <DP n="39"> -->
<figure id="f0001" num="1"><img id="if0001" file="imgf0001.tif" wi="151" he="151" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="40"> -->
<figure id="f0002" num="2"><img id="if0002" file="imgf0002.tif" wi="156" he="200" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="41"> -->
<figure id="f0003" num="3"><img id="if0003" file="imgf0003.tif" wi="132" he="158" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="42"> -->
<figure id="f0004" num="4,5"><img id="if0004" file="imgf0004.tif" wi="136" he="227" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="43"> -->
<figure id="f0005" num="6A,6B"><img id="if0005" file="imgf0005.tif" wi="68" he="199" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="44"> -->
<figure id="f0006" num="6C"><img id="if0006" file="imgf0006.tif" wi="165" he="124" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="45"> -->
<figure id="f0007" num="7"><img id="if0007" file="imgf0007.tif" wi="143" he="156" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="46"> -->
<figure id="f0008" num="8"><img id="if0008" file="imgf0008.tif" wi="143" he="156" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="47"> -->
<figure id="f0009" num="9,10"><img id="if0009" file="imgf0009.tif" wi="137" he="227" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="48"> -->
<figure id="f0010" num="11"><img id="if0010" file="imgf0010.tif" wi="143" he="155" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="49"> -->
<figure id="f0011" num="12"><img id="if0011" file="imgf0011.tif" wi="162" he="197" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="50"> -->
<figure id="f0012" num="13,14"><img id="if0012" file="imgf0012.tif" wi="145" he="219" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="51"> -->
<figure id="f0013" num="15A,15B,15C"><img id="if0013" file="imgf0013.tif" wi="165" he="230" 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="JP2012052443A"><document-id><country>JP</country><doc-number>2012052443</doc-number><kind>A</kind></document-id></patcit><crossref idref="pcit0001">[0002]</crossref><crossref idref="pcit0002">[0003]</crossref><crossref idref="pcit0004">[0006]</crossref><crossref idref="pcit0005">[0006]</crossref></li>
<li><patcit id="ref-pcit0002" dnum="JP2010275986A"><document-id><country>JP</country><doc-number>2010275986</doc-number><kind>A</kind></document-id></patcit><crossref idref="pcit0003">[0004]</crossref></li>
</ul></p>
</ep-reference-list>
</ep-patent-document>
