Patent Description:
Machines that perform mutual conversion between mechanical and electrical energy and have a rotating part, such as motors and generators, are collectively called rotating electric machines and are installed in a variety of equipment.

A rotating electric machine is equipped with a rotor and a stator. At least one of them is provided with a plurality of teeth arranged in a circumferential direction, and the rotor rotates when electric power is supplied to a coil in which a coil conductor is wound around the teeth. Such a rotating electric machine is known from, for example, <CIT>, <CIT>, <CIT>, <CIT>, <CIT>, and <CIT>.

In general, a cooling structure is provided in a rotating electric machine to release the heat generated by the power supply to the outside. For example, in the cooling structure disclosed in <CIT>, a housing is provided to house a coil conductor wound around each of teeth, and a cooling fluid flows into the housing to directly cool the coil conductor. <CIT> discloses a rotating electric machine having radiator plates inserted between turns of a copper wire to separate the turns. <CIT> discloses a rotating electric machine as specified in the preamble of claim <NUM>. In the rotating electric machine of <CIT>, two sets of windings wound around a salient pole of a rotor body are held apart using a hollow spacer that creates air gaps between the two sets of windings.

For example, in fan motors for propulsion of aircraft (electric aircraft), a high power density of approximately <NUM> to <NUM> kW/kg is required, and to achieve this, downsizing as much as possible is promoted. However, as the size of the rotating electric machine decreases, the surface area decreases with the decrease in volume, making it difficult for the generated heat to escape to the outside. Therefore, a cooling structure that can achieve especially high cooling performance is required for a rotating electric machine that achieves such a high power density.

The present invention has been made to solve the above issue, and it is intended to provide a cooling structure of a rotating electric machine that can achieve high cooling performance.

The present invention has implemented the following means in order to achieve the above object.

That is, the present invention is a rotating electric machine having a configuration as specified in claim <NUM>.

According to this configuration, a gap is formed between the turns of the coil conductor, and the cooling medium is distributed therein, and thus the contact area between the coil conductor and the cooling medium is sufficiently secured, and the coil is effectively cooled. In addition, the notched section is provided in the middle of the extension of the spacer section to form a locally wide region in the middle portion of the gap that is a flow channel of the cooling medium. The turbulence in the flow of the cooling medium and the stirring of the cooling medium as it passes through the non-straight shaped flow channel improves the heat transfer coefficient. In addition, the notched section provided in the spacer section reduces the contact area between the coil conductor and the spacer section, which increases the contact area (that is, the heat dissipation area) between the coil conductor and the cooling medium. The improvement in the heat transfer coefficient and the increase in the heat dissipation area both lead to the improvement in the heat dissipation capability, thus achieving high cooling performance.

Preferably, in the rotating electric machine, a plurality of the notched sections are provided in the middle of the extension of the spacer section.

According to this configuration, a plurality of locally wide regions are formed in the middle portion of the gap that is a flow channel of the cooling medium. Therefore, the stirring action of the cooling medium is enhanced, and the heat transfer coefficient (and thus the heat dissipation capability) is greatly improved. This allows for particularly high cooling performance.

Preferably, in the rotating electric machine, the plurality of the notched sections are disposed at a fixed pitch.

According to this configuration, the heat dissipation capability is less likely to be biased depending on the location, and the coil is uniformly cooled.

Preferably, in the rotating electric machine, at least one of corner portions of the notched section has a round shape.

At least one of the corner portions of the notched section is made into a round shape, and thus the stagnation of the cooling medium is less likely to occur in the vicinity of the corner portion. The formation of stagnation of the cooling medium may reduce the heat transfer coefficient (and thus the heat dissipation capability), but the suppression of the occurrence of stagnation suppresses the resulting reduction in heat dissipation capability.

Preferably, in the rotating electric machine, at least one of the corner portions of the notched section has a taper shape.

At least one of the corner portions of the notched section is made into a taper shape to suppress the occurrence of stagnation of the cooling medium in the vicinity of the corner portions, while also ensuring the stirring effect of the cooling medium at the corner portions. Therefore, it is possible to improve the heat transfer coefficient by stirring the cooling medium while suppressing the decrease in the heat transfer coefficient derived from the stagnation, and the heat dissipation capability can be increased in a balanced manner.

Preferably, in the rotating electric machine, the lengthwise dimension of the notched section is specified within a range such that a pressure loss when the cooling medium is distributed in the gap is equal to or less than a predetermined value.

According to this configuration, since the pressure loss when distributing the cooling medium in the gap is equal to or less than a predetermined value, the load on the mechanism (e.g., a pump) for distributing the cooling medium can be reduced.

According to the present invention, a high cooling performance is achieved, and thus the rotating electric machine can be sufficiently cooled.

Hereinafter, an embodiment of the present invention is described with reference to the drawings.

A configuration of a rotating electric machine according to an embodiment will be described with reference to <FIG>. <FIG> is a longitudinal cross-sectional view of a rotating electric machine <NUM> according to an embodiment, cut in a plane perpendicular to the axial direction of a rotary shaft <NUM>. <FIG> is a cross-sectional view of the rotating electric machine <NUM> viewed from the direction of arrow A in <FIG>. <FIG> are both longitudinal cross-sectional views of a part of the rotating electric machine <NUM>. <FIG> is a view of the rotating electric machine <NUM> cut at a position where a notched section <NUM> is not provided in a spacer section <NUM>, and <FIG> is a view of the rotating electric machine <NUM> cut at a position where the notched section <NUM> is provided in the spacer section <NUM>.

The rotating electric machine <NUM> is used, for example, as a fan motor for propulsion of an aircraft (electric aircraft), and includes a rotor <NUM>, a stator <NUM>, a coil <NUM>, a coil holding member <NUM>, a space forming member <NUM>, a cooling medium supply section <NUM>, and the like.

The rotor <NUM> includes a columnar rotor core <NUM>. The outer peripheral surface of the rotor core <NUM> is provided with a permanent magnet <NUM> divided into a cylindrical or arched shape. In addition, in the center of the rotor core <NUM> in the radial direction, a columnar penetrating portion is provided through the axial direction, into which the rotary shaft <NUM> is inserted. The rotary shaft <NUM> is longer than the rotor <NUM> in the axial direction and is provided with the vicinity of both ends protruding from the both ends of the rotor <NUM>.

The stator <NUM> is a substantially cylindrical member and is disposed to surround the outer peripheral surface of the rotor <NUM>. The stator <NUM> includes a stator core <NUM>. The stator core <NUM> is integrally composed of a cylindrical yoke 21a and a plurality of teeth 21b protruding inwardly in the radial direction from the inner peripheral surface thereof. Each of the teeth 21b is formed over the entire axial direction from one end to the other end of the stator <NUM>. The plurality of teeth 21b are arranged at intervals along the circumferential direction, and a gap called a slot S is formed between adjacent teeth 21b.

The coil <NUM> includes a conductor (coil conductor) <NUM> that is wound around each of the teeth 21b and disposed in the slot S. However, as will be described below, in this rotating electric machine <NUM>, the coil conductor <NUM> is not wound directly around the teeth 21b, but is wound around the teeth 21b via the coil holding member <NUM> described below.

The coil <NUM> is a three-phase coil including a U-phase coil, a V-phase coil, and a W-phase coil, each end of which is drawn outward in the radial direction from one end side in the axial direction of the stator <NUM> and connected to one end of a power line (not illustrated in the figure) of each phase, respectively. The other end of the power line of each phase is connected to a drive unit, and when a three-phase alternating current voltage is applied to the coil <NUM> from the drive unit, the rotor <NUM> rotates and the rotational driving force is output from the rotary shaft <NUM>.

The coil holding member <NUM> is a member that holds the coil <NUM>. The coil conductor <NUM> is wound around the coil holding member <NUM> in advance, and the coil holding member <NUM> around which the coil conductor <NUM> is wound is attached to the teeth 21b, and thus the coil conductor <NUM> is wound around the teeth 21b and disposed in the slot S. The configuration of the coil holding member <NUM> will be described below.

The space forming member <NUM> is a member that forms a space (coil housing space) <NUM> for housing the coil <NUM> disposed in the slot S, and includes a division wall <NUM>, a plurality of partition walls <NUM>, a pair of lid sections 53a and 53b, and the like.

The division wall <NUM> is a thin-walled cylindrical member and is disposed in the space between the rotor <NUM> and the stator <NUM>. The division wall <NUM> has an axial length that is approximately the same as that of the stator <NUM>, and is provided in overall contact with the tip of each of the teeth 21b on the outer peripheral surface. This makes each slot S a space that is separated from the space on the rotor <NUM> side.

The partition wall <NUM> is a long, substantially plate-shaped member and is disposed at the substantially center of the adjacent teeth 21b in each slot S. The longitudinal dimension of the partition wall <NUM> is approximately the same as the axial dimension of the stator <NUM>, and the partition wall <NUM> extends from one end of the slot S to the other end. In addition, the partition wall <NUM> is provided in contact with the inner peripheral surface of the yoke 21a at one end in the radial direction of the stator <NUM> and in contact with the outer peripheral surface of the division wall <NUM> at the other end. As a result, each slot S is divided into approximately two equal parts in the circumferential direction of the stator <NUM>.

Each of the pair of lid sections 53a and 53b is a circular or discshaped member, and is disposed at each end of the stator <NUM> in the axial direction to block the opening end of each slot S facing the end.

The division wall <NUM>, the partition wall <NUM>, and the pair of lid sections 53a and 53b form the coil housing space <NUM>. That is, the coil conductor <NUM> disposed in each slot S is housed in the coil housing space <NUM> surrounded by the teeth 21b, the partition wall <NUM>, the division wall <NUM>, and the pair of lid sections 53a and 53b.

The cooling medium supply section <NUM> is an element that supplies a cooling medium to the coil housing space <NUM> formed in each slot S, and includes a circulation flow channel <NUM>, a pump <NUM>, a cooler <NUM>, and the like. Various fluids can be used as the cooling medium, but here, for example, oil (cooling oil) is used.

The circulation flow channel <NUM> is a flow channel for distributing the cooling medium, one end of which is connected with an introduction port 531a provided on one lid section 53a, and the other end of which is connected with an outlet port 531b provided on the other lid section 53b. Each of the lid sections 53a and 53b has a branch flow channel 532a (532b) that is connected at one end to the introduction port 531a (or the outlet port 531b) and branches off in the middle to connect with each coil housing space <NUM>. That is, the circulation flow channel <NUM> is connected to each coil housing space <NUM> via the branch flow channels 532a and 532b, and the cooling medium introduced from the circulation flow channel <NUM> via the introduction port 531a flows into each coil housing space <NUM> via the branch flow channel 532a. The cooling medium flowing out from each coil housing space <NUM> is led through the branch flow channel 532b and through the outlet port 531b to the circulation flow channel <NUM>.

The pump <NUM> and the cooler <NUM> are both inserted in the middle of the circulation flow channel <NUM>. When the pump <NUM> is driven, the cooling medium circulates through the circulation flow channel <NUM>, and the cooling medium is distributed in each coil housing space <NUM>. Then, the cooling medium circulating in the circulation flow channel <NUM> is cooled by the cooler <NUM> installed in the middle of the channel, which takes away heat from the cooling medium.

As the cooling medium is distributed in the coil housing space <NUM>, the coil <NUM> disposed therein is directly cooled by the cooling medium.

A configuration of the coil holding member <NUM> will be described with reference to <FIG> in addition to <FIG>. <FIG> and <FIG> are both perspective views illustrating an example configuration of the coil holding member <NUM>.

The coil holding member <NUM> is a member that holds the coil <NUM>, and includes a base section <NUM> and the spacer section <NUM>.

The base section <NUM> is a member including a thin-walled band-shaped member formed into a frame corresponding to the teeth 21b. Specifically, the base section <NUM> includes a pair of long portions 41a and 41a, each end of which is connected via a pair of short portions 41b, and has a flat, substantially rectangular shape as a whole. The dimension of each long portion 41a is approximately the same as the dimension in the extending direction of the teeth 21b, and the dimension of each short portion 41b is approximately the same as the widthwise dimension of the teeth 21b.

The coil conductor <NUM> is wound around the base section <NUM> (<FIG> and <FIG>). The coil conductor <NUM> specifically includes, for example, a flat band-shaped conductor whose cross section is smaller in the thickness direction than in the width direction, and is wound around the base section <NUM> with the width direction being oriented to match the normal direction of the outer peripheral surface of the base section <NUM>. Here, the portion of the coil conductor <NUM> that circles around the base section <NUM> (and thus the teeth 21b) is referred to as "one turn". Each turn may be continuous or discontinuous. For example, in a case where a continuous coil conductor <NUM> is wound around, each turn is a continuous one. In addition, in a case where the coil conductor <NUM> is a stacked frame of conductor portions corresponding to one turn, each turn is discontinuous.

The spacer section <NUM> is a long plate-shaped member and is protruded on the outer surface of the long portion 41a in such a posture that the long direction is along the extending direction of the long portion 41a of the base section <NUM> and the width direction is along the normal direction of the outer surface of the base section <NUM>. The dimension in the extending direction of the spacer section <NUM> is approximately the same as the dimension of the long portion 41a of the base section <NUM>, and the spacer section <NUM> extends from one end of the long portion 41a to the other end. Although the widthwise dimension (i.e., the protruding dimension from the base section <NUM>) L0 of the spacer section <NUM> can be specified as appropriate, it is also preferable that it be approximately <NUM>/<NUM> to <NUM>/<NUM> of the widthwise dimension of the coil conductor <NUM>.

On each of the pair of long portions 41a and 41a of the base section <NUM>, a number of spacer sections <NUM> corresponding to the number of turns of the coil conductor <NUM> are provided in multiple stages. In the example illustrated in the figure, the number of turns of the coil conductor <NUM> is three, and four spacer sections <NUM>, for which one is added to this number of turns, are arranged at a fixed interval (pitch) in each long portion 41a. The pitch at this time is approximately the same as the thickness of the coil conductor <NUM>.

The coil conductor <NUM> is wound around the base section <NUM> in such a manner the end in the width direction is inserted between the spacer sections <NUM> of adjacent stages, and is held between the spacer sections <NUM> of the adjacent stages. Accordingly, the spacer section <NUM> is inserted between turns of the coil conductor <NUM> wound around the base section <NUM>. By inserting the spacer section <NUM> between the turns, a gap G corresponding to the thickness of the spacer section <NUM> is defined between the turns (<FIG> and <FIG>). That is, the spacer section <NUM> is a member that holds the coil conductor <NUM> and defines the gap G between the turns.

For example, when a continuous coil conductor <NUM> is wound around the base section <NUM> (i.e., when each turn is continuous), the coil conductor <NUM> is wound around the base section <NUM> while alternately passing through the long portion 41a and the short portion 41b. However, as described above, in the long portion 41a, the coil conductor <NUM> is wound in such a manner that the end in the width direction is inserted between the spacer sections <NUM> of the adjacent stages. Here, each spacer section <NUM> is provided in a horizontal posture (i.e., in such a posture that the position in the height direction is constant over the entire extending direction), and the coil conductor <NUM> is wound in a substantially horizontal posture by being guided by the spacer section <NUM> in the long portion 41a. Then, the coil conductor <NUM>, which has reached the other long portion 41a via the one short portion 41b, is guided by the spacer section <NUM> of the same height as the previous one in the long portion 41a, and is continuously wound in the substantially horizontal posture. Then, the coil conductor <NUM> which has reached the other short portion 41b is bent diagonally downward (or upward) here and led downward (or upward) by the thickness of the spacer section <NUM> and the coil conductor per se <NUM> than the coil conductor <NUM> being wound previously. Then, the coil conductor <NUM> is again wound in the substantially horizontal posture by being guided by the spacer section <NUM> of the same stage in the pair of long portions 41a and one short portion 41b sandwiched between them. Thus, the coil conductor <NUM> is wound around the base section <NUM> in a substantially horizontal posture, at least in each long portion 41a. Therefore, the gap G defined between the turns will extend substantially horizontally.

Each spacer section <NUM> has a notched section <NUM>, which is a portion cut out in such a manner that the widthwise dimension of the spacer section <NUM> is relatively short, in the middle of its extension (i.e., in the middle of the extending direction of the long portion 41a).

The number, disposition (interval (pitch) of adjacent notched sections <NUM>), shape, dimension (lengthwise dimension L1, widthwise dimension L2), and the like of the notched section <NUM> provided in the spacer section <NUM> can be specified as appropriate as long as the function of the spacer section <NUM> (i.e., the function of holding the coil conductor <NUM> between the spacer sections <NUM> of adjacent stages and the function of defining a gap G between the turns) is not impaired. However, the "lengthwise" here refers to the extending direction of the spacer section <NUM> (i.e., the extending direction of the long portion 41a), and the "widthwise" refers to the protruding direction of the spacer section <NUM> from the base section <NUM>.

For example, in the coil holding member <NUM> (4A) illustrated in <FIG>, the number of the notched sections <NUM> provided in the spacer section <NUM> is five. In addition, the five notched sections <NUM> are disposed at a fixed pitch. Moreover, each notched section <NUM> has a right-angled corner portion. That is, each notched section <NUM> has a rectangular shape in plan view. Further, the lengthwise dimension L1 (4A) of each notched section <NUM> is approximately <NUM>/<NUM> of the lengthwise dimension of the unnotched section (the uncut portion in the spacer section <NUM>). Furthermore, the widthwise dimension L2 (4A) of each notched section <NUM> is approximately the same as widthwise dimension L0 (4A) of the spacer section <NUM>. That is, the notched section <NUM> is formed by cutting a portion of the spacer section <NUM> over the entire width direction, and the widthwise dimension of the spacer section <NUM> is zero at the formation position of the notched section <NUM>.

In addition, for example, in the coil holding member <NUM> (4B) illustrated in <FIG>, the number of the notched sections <NUM> provided in the spacer section <NUM> is <NUM>. Other points are the same as the notched section <NUM> provided in the coil holding member 4A illustrated in <FIG>. That is, <NUM> notched sections <NUM> are disposed at a fixed pitch. Moreover, each notched section <NUM> has a right-angled corner portion. Moreover, the lengthwise dimension L1 (4B) of each notched section <NUM> is approximately <NUM>/<NUM> of the lengthwise dimension of the unnotched section. Further, the widthwise dimension L2 (4B) of each notched section <NUM> is approximately the same as widthwise dimension L0 (4B) of the spacer section <NUM>. However, the widthwise dimension L0 (4B) of the spacer section <NUM> of this coil holding member <NUM> (4B) is smaller than the widthwise dimension L0 (4A) of the spacer section <NUM> of the coil holding member 4A illustrated in <FIG>.

In the assembly process of the rotating electric machine <NUM>, first, the coil conductor <NUM> is wound around the coil holding member <NUM> (<FIG> and <FIG>). Specifically, the coil conductor <NUM> is wound around the base section <NUM> in such a manner the end in the width direction is inserted between the spacer sections <NUM> of adjacent stages. As a result, the spacer section <NUM> is inserted between the turns of the coil conductor <NUM> wound around the base section <NUM>, and the gap G corresponding to the thickness of the spacer section <NUM> extending in the extending direction of the base section <NUM> is defined between the turns (<FIG> and <FIG>).

Then, the coil holding member <NUM> around which the coil conductor <NUM> is wound is attached to the teeth 21b. The base section <NUM> is frame-shaped corresponding to the teeth 21b, and in a state where the base section <NUM> is mounted here so as to surround the periphery of the teeth 21b, the inner peripheral surface of the base section <NUM> contacts, as a whole, the outer peripheral surface of the teeth 21b without a gap. In addition, in this state, the spacer section <NUM> on each long portion 41a of the base section <NUM> extends along the slot S.

In this manner, the coil holding member <NUM> around which the coil conductor <NUM> is wound is attached to the teeth 21b, and thus the coil conductor <NUM> is wound around the teeth 21b via the coil holding member <NUM> and disposed in the slot S. Then, in this state, the gap G extending in the extending direction of the slot S is defined between the turns of the coil conductor <NUM>.

The cooling manner of the coil <NUM> in the rotating electric machine <NUM> will be described with continued reference to <FIG>.

In the rotating electric machine <NUM>, as described above, the space forming member <NUM> forms the coil housing space <NUM> that houses the coil <NUM> (specifically, the coil conductor <NUM>) disposed in each slot S, and the cooling medium supply section <NUM> supplies a cooling medium to the coil housing space <NUM> formed in each slot S. Consequently, the coil conductor <NUM> disposed in the coil housing space <NUM> is directly cooled by the cooling medium.

Here, the gap G extending in the extending direction of the slot S is defined between the turns of the coil conductor <NUM> disposed in the slot S. Therefore, a portion of the cooling medium supplied to the coil housing space <NUM> is distributed in this gap G. That is, a portion of the cooling medium flowing from the circulation flow channel <NUM> into each coil housing space <NUM> via the introduction port 531a and the branch flow channel 532a flows into the gap G from one end in the extending direction of the gap G, flows into the gap G, flows out from the other end in the extending direction of the gap G, and flows into the circulation flow channel <NUM> via the branch flow channel 523b and the outlet port 531b. By the cooling medium flowing through the gap G formed between the turns of the coil conductor <NUM>, the contact area between the coil conductor <NUM> and the cooling medium is sufficiently secured, and the coil <NUM> is effectively cooled.

In particular, here, the notched section <NUM> is provided in the middle of the extension of the spacer section <NUM> defining the gap G, thereby effectively enhancing the capability to dissipate heat from the coil <NUM> (heat dissipation capability). This point will be described with reference to <FIG>. <FIG> illustrates the results of a simulation calculation (thermo-fluid analysis) of the heat dissipation capability achieved by each of the coil holding member (first coil holding member) 4A according to a first form illustrated in <FIG> and the coil holding member (second coil holding member) 4B according to a second form illustrated in <FIG>.

However, here, the coil holding member <NUM> that differs from the first coil holding member 4A only in the fact that the notched section <NUM> is not provided in the spacer section <NUM> is considered to be a "comparative example", and the heat dissipation capability of the respective coil holding members 4A and 4B is indicated in a ratio when the heat dissipation capability achieved by the coil holding member <NUM> according to the comparative example is set to "<NUM>". <FIG> schematically illustrate the shapes of gaps G(<NUM>), G(4A), and G(4B) (i.e., the shapes of the flow channels through which the cooling medium is distributed) formed by the coil holding member <NUM> according to the comparative example and the first and second coil holding members 4A and 4B, respectively.

As illustrated in <FIG>, in the present simulation, the heat dissipation capability of the first coil holding member 4A was approximately <NUM>% higher than that of the coil holding member <NUM> according to the comparative example. In addition, the heat dissipation capability of the second coil holding member 4B was approximately <NUM>% higher than that of the coil holding member <NUM> according to the comparative example. The reasons for this can be considered as follows.

First, a temperature rise ΔT of the coil <NUM> is expressed by the following (formula <NUM>) using a thermal resistance R and a heating value W.

In other words, when the heating value W is constant, the temperature rise ΔT is determined by thermal resistance R. This thermal resistance R is then expressed by the following (formula <NUM>) using a heat transfer coefficient h and a heat dissipation area A.

In other words, the larger the heat dissipation area A and the higher the heat transfer coefficient h, the smaller thermal resistance R and the smaller the temperature rise ΔT. That is, the heat dissipation capability is enhanced.

Here, the coil holding members 4A and 4B provided with the notched section <NUM> have a larger heat dissipation area than that of the coil holding members <NUM> not provided with the notched section <NUM>. The reasons for this are as follows.

That is, in the coil holding members 4A and 4B provided with the notched section <NUM>, the contact area between the coil conductor <NUM> and the spacer section <NUM> is locally small in the portion where the notched section <NUM> is provided (<FIG>). For example, when comparing the first coil holding member 4A and the coil holding member <NUM> according to the comparative example in which the widthwise dimensions L0 of the spacer section <NUM> are equal to each other, the coil holding member 4A provided with the notched section <NUM> has a smaller contact area between the coil conductor <NUM> and the spacer section <NUM> by the total area of the region cut out by the notched section <NUM> than the coil holding member <NUM> not provided with the notched section <NUM>. Put another way, by the provision of the notched section <NUM>, the gap G (4A), which is a flow channel through which the cooling medium is distributed, is expanded by the total area of the notched region. Therefore, the contact area (that is, the heat dissipation area) between the cooling medium and the coil conductor <NUM> is secured to be wide by this total area. Thus, by providing the notched section <NUM>, the heat dissipation area is increased by the total area of the notched region. As described above, the heat dissipation capability is improved in proportion to the increase in the heat dissipation area.

As illustrated in <FIG>, in the present simulation, the improvement in the heat dissipation capability derived from the increase in the heat dissipation area was approximately <NUM>% to <NUM>% for the first coil holding member 4A and approximately <NUM>% for the second coil holding member 4B, and the improvement in the heat dissipation capability derived from the increase in the heat dissipation area was larger for the second coil holding member 4B than for the first coil holding member 4A. This is considered to be because the second coil holding member 4B has a smaller widthwise dimension L0 of the spacer section <NUM> than that of the first coil holding member 4A, and thus the contact area between the spacer section <NUM> and the coil conductor <NUM> is smaller (i.e., the heat dissipation area is larger).

Needless to say, in order to increase the heat dissipation area, the contact area between the spacer section <NUM> and the coil conductor <NUM> may be reduced, and it is desirable to adjust the dimension L0 of the spacer section <NUM>, the number, disposition, shape, dimensions L1 and L2, and the like of the notched section <NUM>, so as to hold the coil conductor <NUM> with the minimum necessary contact area. However, as will be discussed below, each of these values also affects the heat transfer coefficient and pressure loss. Therefore, while taking these influences into consideration, it is preferable to adjust each value in such a manner that the increase in the heat dissipation area is as large as possible.

In addition, the coil holding members 4A and 4B provided with the notched section <NUM> have a higher heat transfer coefficient than that of the coil holding members <NUM> not provided with the notched section <NUM>. The reasons for this are as follows.

That is, while the heat transfer coefficient is higher when the temperature difference (in this case, the temperature difference between the surface of the coil conductor <NUM> and the cooling medium in the vicinity thereof) is larger, this temperature difference becomes smaller and the heat transfer coefficient becomes lower as the flow distance of the cooling medium becomes longer. Then, when the flow distance of the cooling medium exceeds a predetermined distance called an approach section, the heat transfer coefficient converges to a constant value.

Here, the gap G(<NUM>) formed by the coil holding member <NUM> not provided with the notched section <NUM> has a straight shape with a constant width (<FIG>). In contrast, in the gaps G(4A) and G(4B) formed by the coil holding members 4A and 4B provided with the notched section <NUM>, a wide portion Gw that is relatively wide appears in the middle of the extension thereof. In other words, the gaps G(4A) and G(4B) have a non-straight shape in which the wide portion Gw that is relatively wide and a narrow portion Gn that is relatively narrow appear alternately, that is, an uneven shape in plan view (<FIG>).

When the cooling medium is distributed in the non-straight shaped gaps G(4A) and G(4B), turbulence is generated in the flow of the cooling medium and the cooling medium is stirred. Then, the positional exchange between the relatively high temperature portion and the relatively low temperature portion in the cooling medium is promoted, and the temperature of the cooling medium in the vicinity of the surface of the coil conductor <NUM> becomes lower. This increases the region before the flow distance passes through the approach section, that is, the region with relatively high heat transfer coefficient, and the heat transfer coefficient is improved. As mentioned above, the heat dissipation capability is improved as the heat transfer coefficient is improved.

As illustrated in <FIG>, in the present simulation, the improvement in the heat dissipation capability derived from the improvement in the heat transfer coefficient was approximately <NUM>% for the first coil holding member 4A and approximately <NUM>% for the second coil holding member 4B, and the improvement in the heat dissipation capability derived from the improvement in the heat transfer coefficient was larger for the second coil holding member 4B than for the first coil holding member 4A. It is considered that this is because the second coil holding member 4B has a larger number of notched sections <NUM> than that of the first coil holding member 4A, and thus has a larger number of wide portions Gw appearing in the gap G(4B) and a higher stirring effect of the cooling medium.

In the present simulation, the range of improvement in the heat transfer coefficient was larger when the number of notched sections <NUM> is increased without changing the ratio of the lengthwise dimension L1 of the notched section <NUM> to the lengthwise dimension of the unnotched section. However, if the number of notched sections <NUM> is increased without changing the ratio of the lengthwise dimension L1 of the notched section <NUM> to the lengthwise dimension of the unnotched section, it is considered that when the number of notched sections <NUM> exceeds a certain upper limit, the range of improvement in the heat transfer coefficient becomes smaller as the number of notched sections <NUM> increases (virtual line in <FIG>). This is because as the number of notched sections <NUM> increases, the lengthwise dimension of the unnotched section becomes shorter, and the cooling medium tends to stagnate in the wide portion Gw.

Thus, when the number of notched sections <NUM> is increased without changing the ratio of the lengthwise dimension L1 of the notched section <NUM> to the lengthwise dimension of the unnotched section, the range of improvement in the heat transfer coefficient is considered to follow the transition of initially increasing and then decreasing in the middle. Therefore, under given conditions, there exists a range of the number of notched sections <NUM> such that the heat transfer coefficient can be made higher than a predetermined value. Accordingly, it is also desirable to specify the number of the notched sections <NUM> within such a range. Specifically, for example, it is also preferable to specify by experiment or simulation a range of the number of notched sections <NUM> such that the heat transfer coefficient can be made higher than an arbitrarily selected predetermined value, and to set the number of notched sections <NUM> to a value selected from the specified range.

By the way, the pressure required to distribute the cooling medium in the gap G is defined by the pressure loss when the cooling medium is distributed in the gap G. In order to reduce the burden on the pump <NUM> and to achieve its downsizing, or the like, it is preferable that this pressure loss be small. Here, as described above, the gaps G(4A) and G(4B) formed by the coil holding members 4A and 4B provided with the notched section <NUM> have non-straight shapes in which the wide portion Gw and a narrow portion Gn appear alternately. As mentioned above, gaps G(4A) and G(4B) of this shape provide the advantages of increased heat dissipation area and improved heat transfer coefficient, but on the other hand, they appear to have the disadvantage of higher pressure loss compared to the straight shaped gap G(<NUM>). In reality, however, this is not always the case.

<FIG> illustrates the results of a simulation calculation of the pressure loss when a cooling medium is distributed in the gaps G(4A) and G(4B) formed by the respective coil holding members 4A and 4B. However, here again, the pressure loss when the cooling medium is distributed in each of the gaps G(4A) and G(4B) is indicated in the ratio when the pressure loss when the cooling medium is distributed in the gap G(<NUM>) formed by the coil holding member <NUM> according to the comparative example is set to "<NUM>".

In the present simulation, the cooling medium is assumed to be oil (cooling oil), and its density is "<NUM>/m<NUM>". The flow velocity of the cooling medium delivered to the gaps G(<NUM>), G(4A), and G(4B) is set to "<NUM>/s". Under these conditions, the pressure loss in the gaps G(4A) and G(4B) formed by the respective coil holding members 4A and 4B was approximately <NUM>% lower than the pressure loss in the gap G(<NUM>) formed by the coil holding member <NUM> according to the comparative example. The reasons for this can be considered as follows.

First, when the cooling medium is distributed in the gaps G(<NUM>), G(4A), and G(4B), a pressure loss derived from friction (hereinafter referred to as "friction pressure loss") ΔP1 occurs. Further, when the cooling medium is distributed in the non-straight shaped gaps G(4A) and G(4B) formed by the coil holding members 4A and 4B provided with the notched section <NUM>, a further pressure loss ΔP2 occurs when the cooling medium passes through the boundary between the narrow portion Gn and the wide portion Gw. In other words, in the non-straight shaped gaps G(4A) and G(4B), a pressure loss derived from the fact that the shape is non-straight (hereinafter referred to as "shape pressure loss") ΔP2 occurs in addition to friction pressure loss ΔP1. Needless to say, in the straight-shaped gap G(<NUM>) formed by the coil holding member <NUM> not provided with the notched section <NUM>, the shape pressure loss ΔP2 is zero.

The friction pressure loss ΔP1 is given by (formula <NUM>) below with the use of a friction coefficient λ, a length L of the flow channel formed by the gap G, a representative length (average flow channel width) d, a density ρ of the cooling medium being distributed, and a flow velocity U of the cooling medium.

However, the friction coefficient λ includes the reciprocal of the flow velocity (<NUM>/U), and ΔP1 is proportional to the flow velocity U.

On the other hand, the shape pressure loss ΔP2 derived from one notched section <NUM> (i.e., the shape pressure loss generated when passing through one wide portion Gw) is given by (formula <NUM>) below with the use of a loss factor ζ, the density ρ of the cooling medium being distributed, and the flow velocity U of the cooling medium.

However, the loss factor ζ is at most "approximately <NUM>".

Under the present conditions, the shape pressure loss ΔP2 calculated from the above (formula <NUM>) was approximately <NUM> kPa, while the calculated friction pressure loss ΔP1 calculated from the above (formula <NUM>) was more than <NUM> times larger than this shape pressure loss ΔP2. In other words, under the condition of relatively slow flow velocity of the cooling medium and relatively high viscosity of the cooling medium, as in the present condition, the friction pressure loss ΔP1 becomes dominant and the shape pressure loss ΔP2 is sufficiently small to be negligible with respect to the friction pressure loss ΔP1.

In addition, this friction pressure loss ΔP1 is proportional to the flow velocity U by the above (formula <NUM>). Here, the gaps G(4A) and G(4B) formed by the coil holding members 4A and 4B provided with the notched section <NUM> have the wide portion Gw in the middle thereof. Here, the cross-sectional area (i.e., the cross-sectional area of the flow channel of the cooling medium) of the gaps G(4A) and G(4B) is locally widened. Therefore, the flow velocity of the cooling medium decreases when passing through the wide portion Gw. As a result, the friction pressure loss ΔP1, which is proportional to the flow velocity, becomes small.

Thus, at least under the conditions where the flow velocity of the cooling medium is relatively slow and the cooling medium is oil (or a substance having the same level of density and viscosity as oil), the shape pressure loss ΔP2 derived from the notched section <NUM> becomes sufficiently small with respect to the friction pressure loss ΔP1, and the reduction effect of the friction pressure loss ΔP1 by the formation of the wide portion Gw appears large. Therefore, it is considered that the pressure loss in the gaps G(4A) and G(4B) formed by the respective coil holding members 4A and 4B is lower than the pressure loss in the gap G(<NUM>) formed by the coil holding member <NUM> according to the comparative example. As a matter of fact, if the conditions such as the flow velocity and type of the cooling medium are different, the relation between the friction pressure loss ΔP1 and the shape pressure loss ΔP2 and each value also change, and thus the pressure loss is not always low when the notched section <NUM> is provided. However, at least under conditions similar to those described above, it can be said that the disadvantage of increased pressure loss due to the provision of the notched section <NUM> is unlikely to occur.

As illustrated in <FIG>, in the present simulation, the gap G(B) formed by the second coil holding member 4B had a larger reduction in pressure loss than the gap G(A) formed by the first coil holding member 4A. It is considered that this is because the second coil holding member 4B has a larger number of notched sections <NUM> than that of the first coil holding member 4A, and has a smaller widthwise dimension L0 (4B) of the spacer section <NUM>, and the reduction in the flow velocity of the cooling medium is large.

In the present simulation, the pressure loss decreased when the lengthwise dimension L1 of the notched section <NUM> is shortened without changing the ratio of the lengthwise dimension L1 of the notched section <NUM> to the lengthwise dimension of the unnotched section. However, if the lengthwise dimension L1 of the notched section <NUM> is further shortened without changing the ratio of the lengthwise dimension L1 of the notched section <NUM> to the lengthwise dimension of the unnotched section, when the dimension L1 falls below a certain lower limit, the effect of the shape pressure loss ΔP2 becomes non-negligible, and thus the pressure loss is considered to turn to increase (virtual line in <FIG>).

Thus, when the lengthwise dimension L1 of the notched section <NUM> is reduced without changing the ratio of the lengthwise dimension L1 of the notched section <NUM> to the lengthwise dimension of the unnotched section, the pressure loss is considered to follow the transition of initially decreasing and then increasing in the middle. Therefore, under given conditions, there exists a range of the lengthwise dimension L1 such that the pressure loss can be equal to or less than a predetermined value. Accordingly, it is also desirable to specify the lengthwise dimension L1 of the notched section <NUM> within such a range. Specifically, for example, it is also preferable to specify a maximum value of the allowable pressure loss on the basis of the capacity of the pump <NUM> or the like, and further specify a range of the dimension L1 such that the pressure loss can be reduced to this maximum value or less by experiment or simulation, and set the lengthwise dimension L1 of the notched section <NUM> to a value selected from the specified range.

The rotating electric machine <NUM> according to the above embodiment has the rotor <NUM>, the stator <NUM>, and the coil <NUM> including the coil conductor <NUM> wound around teeth 21b provided on at least one of the rotor <NUM> and the stator <NUM>, and includes the spacer section <NUM> configured to extend along the slot S formed between the teeth 21b and to be inserted between turns of the coil conductor <NUM> to define the gap G between the turns, and the cooling medium supply section <NUM> configured to distribute a cooling medium in the gap G. In addition, the notched section <NUM> cut out in such a manner that a widthwise dimension of the spacer section <NUM> is relatively short is provided in a middle of an extension of the spacer section <NUM>.

According to this configuration, the gap G is formed between the turns of the coil conductor <NUM>, and the cooling medium is distributed therein, and thus the contact area between the coil conductor <NUM> and the cooling medium is sufficiently secured, and the coil <NUM> is effectively cooled. In addition, the notched section <NUM> is provided in the middle of the extension of the spacer section <NUM> to form a locally wide region Gw in the middle portion of the gap G that is a flow channel of the cooling medium. The turbulence in the flow of the cooling medium and the stirring of the cooling medium as it passes through the non-straight shaped flow channel improves the heat transfer coefficient. In addition, the notched section <NUM> provided in the spacer section <NUM> reduces the contact area between the coil conductor <NUM> and the spacer section <NUM>, which increases the contact area (that is, the heat dissipation area) between the coil conductor <NUM> and the cooling medium. The improvement in the heat transfer coefficient and the increase in the heat dissipation area both lead to the improvement in the heat dissipation capability, thus achieving high cooling performance.

In addition, in the rotating electric machine <NUM> according to the above embodiment, a plurality of the notched sections <NUM> are provided in the middle of the extension of the spacer section <NUM>.

According to this configuration, a plurality of locally wide regions Gw are formed in the middle portion of the gap G that is a flow channel of the cooling medium. Therefore, the stirring action of the cooling medium is enhanced, and the heat transfer coefficient (and thus the heat dissipation capability) is greatly improved. This allows for particularly high cooling performance.

In addition, in the rotating electric machine <NUM> according to the above embodiment, the plurality of notched sections <NUM> are disposed at a fixed pitch.

According to this configuration, the heat dissipation capability is less likely to be biased depending on the location, and the coil <NUM> is uniformly cooled.

In addition, in the rotating electric machine <NUM> according to the above embodiment, it is preferable that the lengthwise dimension L1 of the notched section <NUM> is specified within a range such that a pressure loss when a cooling medium is distributed in the gap G is equal to or less than a predetermined value.

According to this configuration, since the pressure loss when distributing the cooling medium in the gap G is equal to or less than a predetermined value, the load on the mechanism (e.g., the pump <NUM>) for distributing the cooling medium can be reduced.

The shape of the notched section <NUM> provided in the spacer section <NUM> is not limited to the one illustrated in the above embodiment. That is, in the above embodiment, the notched section <NUM> is rectangular in plan view with the corner portions being right-angled, but the shape of the notched section <NUM> is not limited thereto.

For example, each corner portion 1211u and 1211d may have a round shape, such as the notched section <NUM> illustrated in <FIG>. In addition, for example, each corner portion 1211u and 1211d may have a taper shape (C-chamfered), such as the notched section <NUM> illustrated in <FIG>. In addition, for example, as illustrated in the notched section <NUM> in <FIG>, the corner portion (upstream side corner portion) 1211u on the upstream side with respect to the flow of the cooling medium may be made into a round shape, and the corner portion (downstream side corner portion) 1211d on the downstream side with respect to the flow of the cooling medium may be made into a taper shape. Moreover, for example, the upstream side corner portion 1211u may be made into a round shape and the downstream side corner portion 1211d may be made into a right angle shape, as in the notched section <NUM> illustrated in <FIG>. Furthermore, for example, the upstream side corner portion 1211u may be made into a taper shape and the downstream side corner portion 1211d may be made into a right angle shape, as in the notched section <NUM> illustrated in <FIG>.

The shape of the corner portions 1211u and 1211d of the notched section <NUM> affects the ease of occurrence of stagnation Q. That is, when the corner portions 1211u and 1211d of the notched section <NUM> have, for example, a right angle shape (<FIG>), the flow channel width changes abruptly at the boundary between the wide portion Gw and the narrow portion Gn. Then, depending on the conditions, at the point where the cooling medium flows from the narrow portion Gn into the wide portion Gw, the flow of the cooling medium may be separated into one that goes straight and the other that stays in the wide portion Gw. Similarly, at the point where the cooling medium flows from the wide portion Gw to the narrow portion Gn, the flow of the cooling medium may be separated into one that stays in the wide portion Gw and one that goes straight. When these flow separations occur, the stagnation Q of the cooling medium is generated in the vicinity of the corner portions 1211u and 1211d. Since the flow channel of the cooling medium is close to zero in such stagnation Q, the heat transfer coefficient is reduced and the effective heat dissipation area is also reduced. Therefore, the heat dissipation capability may be reduced.

In this regard, when at least one of the corner portions 1211u and 1211d is made into a round shape or a taper shape, as the notched section <NUM> illustrated in <FIG>, the change in the width of the flow channel is gradual. Thus, the flow separation is less likely to occur at the corner portions 1211u and 1211d, and the occurrence of stagnation Q of the cooling medium is less likely to be generated in the vicinity of the corner portions 1211u and 1211d. Therefore, the reduction in heat dissipation capability derived from the occurrence of stagnation Q is suppressed.

The effect of suppressing the occurrence of stagnation Q is highest when the corner portions 1211u and 1211d are made into a round shape, then in a taper shape, and lowest in a right angle shape. Therefore, from the viewpoint of suppressing the occurrence of the stagnation Q, a round shape is most preferable as the shape of the corner portions 1211u and 1211d, followed by a taper shape, and followed by a right angle shape.

The flow separation is more likely to occur at the upstream side corner portion 1211u than at the downstream side corner portion 1211d, and the stagnation Q is particularly likely to occur in the vicinity of the upstream side corner portion 1211u. Therefore, it is also preferable that at least the upstream side corner portion 1211u be made into a round shape or a taper shape.

In addition, the shape of the corner portions 1211u and 1211d also affects the ability to stir the cooling medium. That is, the cooling medium flowing through the gap G is stirred by greatly disturbing the flow when passing through the corner portions 1211u and 1211d of the notched section <NUM>. The action of stirring the cooling medium is highest in a right angle shape, then in a taper shape, and lowest in the round shape. As mentioned above, the greater the stirring of the cooling medium, the higher the heat transfer coefficient and the better the heat dissipation capability. Therefore, from the viewpoint of stirring the cooling medium, a right angle shape is most preferable as the shape of the corner portions 1211u and 1211d, followed by a taper shape, and followed by a round shape.

In particular, the shape of the corner portions 1211u and 1211d is made into a taper shape to suppress the occurrence of stagnation Q of the cooling medium in the vicinity of the corner portions, while also ensuring the stirring effect of the cooling medium at the corner portions 1211u and 1211d. Therefore, it is possible to improve the heat transfer coefficient by stirring the cooling medium while suppressing the decrease in the heat transfer coefficient derived from the stagnation Q, and the heat dissipation capability can be increased in a balanced manner.

The cooling medium is particularly prone to stirring as it passes through the downstream side corner portion 1211d. Therefore, in order to effectively stir the cooling medium, it is preferable that at least the downstream side corner portion 1211d be made into a right angle shape or a taper shape.

Further, the shape of the corner portions 1211u and 1211d also affects the ease of bubble occurrence, pressure loss, and the like. For example, the tapered and rounded corner portions 1211d and 1211d are less prone to bubble occurrence and have lower pressure loss than the right-angled corner portions 1211u and 1211d. Therefore, in order to suppress the occurrence of bubbles or to reduce the pressure loss, it is preferable that the corner portions 1211u and 1211d be made into a round shape or a taper shape.

Needless to say, the shape of the corner portions 1211u and 1211d may be other than a right angle shape, a round shape, and a taper shape. In addition, the shape of the upstream side corner portion 1211u and the downstream side corner portion 1211d may be different, and the combination of the shapes is also free.

In the above embodiment, the spacer section <NUM> is provided in the base section <NUM>, and the coil holding member <NUM> includes each of these sections <NUM> and <NUM>, but the manner of providing the spacer section <NUM> is not limited thereto. For example, as illustrated in <FIG>, a partition wall <NUM> may be provided with a spacer section <NUM>. The configuration of the spacer section <NUM> in this case can be the same as that of the spacer section <NUM> provided in the base section <NUM>.

When the spacer section <NUM> is provided in the partition wall <NUM>, the coil holding member <NUM> may be omitted. However, as illustrated in <FIG>, if the coil holding member <NUM> is provided with the spacer section <NUM> and the partition wall <NUM> is provided with the spacer section <NUM>, the coil conductor <NUM> is held by the spacer sections <NUM> and <NUM> at both ends in the width direction, and thus the posture of the coil conductor <NUM> is maintained flat compared with the case where the coil conductor <NUM> is held only at one end in the width direction. As a result, the heat dissipation performance is stably maintained and the pressure loss in the flow channel formed by the gap G is hardly increased.

In addition, by providing the spacer section <NUM> in the coil holding member <NUM> and the spacer section <NUM> in the partition wall <NUM>, the shape of the flow channel formed by the gap G can be adapted in various ways. For example, by making the disposition of the notched section provided in each of the spacer sections <NUM> and <NUM> in the same phase (i.e., by providing the notched section in facing positions), the difference between the wide portion Gw and the narrow portion Gn in the flow channel formed by the gap G can be increased. In addition, by shifting the disposition of the notched section in each of the spacer sections <NUM> and <NUM> by a half phase, the flow channel formed by the gap G can be made to be a meandering shape.

The number, disposition, shape, dimensions L1 and L2, and the like of the notched section <NUM> provided in the spacer section <NUM> are not limited to those illustrated in the above embodiment.

For example, the number of the notched section <NUM> provided in the middle of the extension of the spacer section <NUM> may be one. When one notched section <NUM> is provided, it is also preferable to provide the notched section <NUM> near the center of the spacer section <NUM> in the extending direction. In addition, the notched section may be provided not only in the middle of the extension of the spacer section <NUM>, but also at the end of the extending direction of the spacer section <NUM>.

For example, the notched section <NUM> needs not necessarily be disposed at a fixed pitch, and for example, the pitch may become narrower toward the center of the spacer section <NUM> in the extending direction.

In addition, for example, the widthwise dimension L2 of the notched section <NUM> may be smaller than the widthwise dimension of the spacer section <NUM>.

The number, disposition, shape, lengthwise dimension, widthwise dimension L0, and the like of the spacer section <NUM> provided in the base section <NUM> are not limited to those illustrated in the above embodiment.

For example, in the above embodiment, each long portion 41a is provided with a number of spacer sections <NUM> equal to the number of turns of the coil conductor <NUM> plus one, and the spacer sections <NUM> are disposed on both sides of all turns of the coil conductor <NUM>, but the number of spacer sections <NUM> may be equal to or less than the number of turns. For example, the number of the spacer sections <NUM> may be made smaller than the number of turns, and the spacer section <NUM> may be inserted between the turn bundles composed of a plurality of turns, and a gap G may be defined between the turn bundles.

In addition, for example, in the above embodiment, the plurality of spacer sections <NUM> provided in each long portion 41a are disposed at a fixed pitch, but the pitch between the spacer sections <NUM> need not be fixed.

Moreover, for example, in the above embodiment, the longitudinal dimension of the spacer section <NUM> is approximately the same as the dimension of the long portion 41a, but the longitudinal dimension of the spacer section <NUM> may be shorter than the dimension of the long portion 41a. That is, the spacer section <NUM> does not necessarily have to extend from one end of the long portion 41a to the other end.

In addition, the spacer section <NUM> may be formed from a single integrally formed part, or may be formed by assembling a plurality of divided parts. In the latter case, the plurality of parts may be disposed separately to form the spacer section <NUM>, or the plurality of parts may be connected to form the spacer section <NUM>.

Moreover, the thickness of the spacer section <NUM> can also be specified as appropriate. However, the smaller the thickness of the spacer section <NUM> (i.e., the thinner it is), the smaller the thickness of the gap G (i.e., the thickness of the flow channel of the cooling medium) defined between the turns of the coil conductor <NUM>. As the thickness of the flow channel decreases, the temperature boundary layer of the cooling medium flowing through the flow channel becomes thinner, and the thickness of the relatively cold layer portion of the cooling medium flowing through the flow channel becomes thinner. In addition, the thinner the temperature boundary layer, the larger the temperature difference between the surface of the coil conductor <NUM> and the cooling medium in the vicinity thereof, and the better the heat transfer coefficient. In other words, the smaller the thickness of the spacer section <NUM>, the better the heat transfer coefficient. Therefore, it is preferable that the thickness of the spacer section <NUM> be as small as possible as long as the function of the spacer section <NUM> (i.e., the function of holding the coil conductor <NUM> between the spacer sections <NUM> of adjacent stages and the function of defining the gap G between turns) is not impaired. As an example, the thickness of the spacer section <NUM> can be, for example, approximately <NUM>/<NUM> to <NUM>/<NUM> of the thickness of the coil conductor <NUM>.

In each of the above embodiments, the configurations of the rotor <NUM>, the stator <NUM>, and the coil <NUM>, and the like are not limited to those illustrated above. For example, the rotor <NUM>, or (and) the stator <NUM> may have a structure in which a plurality of electromagnetic steel plates are stacked in the axial direction. In addition, for example, the rotor may be configured as an outer rotor type in which the rotor is arranged outside the stator. Moreover, for example, the teeth may be formed on the side of the rotor.

In each of the above embodiments, a case has been illustrated in which the present invention is applied to a rotating electric machine (rotary electric machine) <NUM> used as a fan motor for propulsion of an aircraft, but it goes without saying that the present invention can be applied to various other rotating electric machines.

Claim 1:
A rotating electric machine (<NUM>) having a rotor (<NUM>), a stator (<NUM>), and a coil (<NUM>) including a coil conductor (<NUM>) wound around teeth (21b) provided on at least one of the rotor (<NUM>) and the stator (<NUM>), the rotating electric machine (<NUM>) comprising:
a coil holding member (<NUM>) that is attached to the teeth (21b) and holds the coil (<NUM>); and
a cooling medium supply section (<NUM>) configured to supply a cooling medium to a coil housing space (<NUM>) formed in each of slots (S) formed between the teeth (21b),
characterized in that
the coil holding member (<NUM>) includes a base section (<NUM>) around which the coil conductor (<NUM>) is wound, and a spacer section (<NUM>) that is protruded on an outer surface of the base section (<NUM>) in such a posture that the long direction is along an extending direction of the base section (<NUM>) and the width direction is along a normal direction of the outer surface of the base section (<NUM>),
the spacer section (<NUM>) extends along one of the slots (S) formed between the teeth (21b), is inserted between turns of the coil conductor (<NUM>), and is arranged alternately with the turns to separate the turns,
a notched section (<NUM>) is provided in a middle of an extension of the spacer section (<NUM>), the notched section (<NUM>) being cut out of the spacer section (<NUM>) in such a manner that a widthwise dimension (L2) of the spacer section (<NUM>) along the width direction of the spacer section (<NUM>) is shorter where the notched section (<NUM>) is formed than where the notched section (<NUM>) is not formed,
the spacer section (<NUM>) defines a gap (G) between the turns, the gap including a wide portion (Gw) expanded by a total area of the notched section (<NUM>) cut out of the spacer section (<NUM>), and
when the cooling medium supply section (<NUM>) supplies the cooling medium to the coil housing space (<NUM>), the coil conductor (<NUM>) disposed in the coil housing space (<NUM>) is directly cooled by the cooling medium and a portion of the cooling medium flows into the gap (G) and is distributed in the gap (G), so that the contact area between the coil conductor (<NUM>) and the cooling medium is sufficiently secured and the coil (<NUM>) is effectively cooled.