JPWO2019035159A1 - Moving body - Google Patents

Abstract

The automobile 1 includes a fluid discharge device that discharges a fluid having a lower air density than the outside air toward the outside of the automobile 1 from a fluid discharge position 3 defined on the surface of the automobile 1 ahead in the traveling direction.

Description

The present invention relates to a moving body including means for discharging a fluid to the outside.

Conventionally, cooling devices such as a vehicle engine and an engine that cools the inside of an engine rule with air when necessary have been known (Patent Document 1). When the temperature inside the engine rule exceeds a certain level, air from the engine compartment flows out of the vehicle through a gap above the end of the engine on the passenger compartment side.

JP-A-57-48123

On the other hand, the inventors of the present invention reduce the air density in the region (mainstream) outside the region (boundary layer) where the flow velocity of air in the vicinity of the moving body is slow in order to reduce the air resistance of the moving body. Was found to be effective.

However, in Patent Document 1, since the air in the engine compartment is discharged from the gap above the end on the vehicle interior side of the engine, the air density of the mainstream in a limited narrow range among the mainstreams around the moving body is lowered. I can only do that.

The present invention has been made in view of such conventional problems, and an object of the present invention is to reduce the air density of the mainstream around the moving body to reduce the air resistance of the moving body.

The moving body according to one aspect of the present invention discharges a fluid having a lower air density than the outside air toward the outside of the moving body from a fluid discharge position defined on the surface of the moving body in front of the moving body in the traveling direction.

According to one aspect of the present invention, it is possible to reduce the air density of the mainstream around the moving body to reduce the air resistance of the moving body.

FIG. 1 is a schematic diagram showing the flow of air along the surface of the automobile 1 generated around the traveling automobile 1 and a graph showing the pressure coefficient Cp of the fluid. FIG. 2 is a cross-sectional view showing a bumper fascia of the front bumper 4 of the automobile 1. FIG. 3 is a perspective view showing a duct 5 formed on the bumper fascia of the front bumper 4. FIG. 4 is a schematic view showing an embodiment in which the exhaust gas of the engine 8 is discharged from the duct 5. FIG. 5 is an enlarged cross-sectional view showing the area Xe of FIG. 1 in an enlarged manner. FIG. 6A is a graph showing the relationship between air temperature and air density. FIG. 6B is a graph showing the relationship between the molecular weight of air and the density of air. FIG. 6C is a graph showing the relationship between the partial pressure of water vapor in the air and the density of the air. FIG. 7 is a schematic diagram showing an example of an apparatus that generates a fluid having a temperature higher than that of the outside air. FIG. 8 is a schematic diagram showing an example of an apparatus for generating a fluid having a higher partial pressure of water vapor than the outside air. FIG. 9 is a schematic view showing a flow rate control valve 66 that changes the discharge flow rate of the exhaust gas from the engine 8. FIG. 10A is a graph showing three control patterns 52a, 52b, and 52c that control the air discharge amount of the blower 32 based on the moving speed. FIG. 10B is a graph showing three control patterns 53a, 53b, and 53c that control the amount of air discharged from the blower 32 based on the temperature of the fluid. FIG. 10C is a block diagram showing an example of a control system that controls the amount of air discharged from the blower 32 based on the temperature of the fluid or the moving speed of the automobile 1. FIG. 11A is a block diagram showing an example of a control system that controls the open / closed state of the radiator shutter 36 according to the discharge flow rate of the fluid. FIG. 11B is a schematic view showing a state in which the radiator shutter 36 is closed. FIG. 11C is a flowchart showing an example of a control procedure in the control system of FIG. 11A. FIG. 11D is a graph showing control patterns 54a, 54b, 54c that control the opening degree of the radiator shutter 36 based on the flow rate of the fluid.

An embodiment of the present invention will be described with reference to the drawings. In the description of the drawings, the same parts are designated by the same reference numerals and the description thereof will be omitted. In the following, a case where the moving body is an automobile will be described.

<Air flow around the moving car 1>
As shown in FIG. 1, when viewed in a stationary system of the automobile 1, an air flow along the surface of the automobile 1 is generated around the traveling automobile 1. FIG. 5 enlarges and displays the area Xe of FIG. In the vicinity of the surface 20F of the automobile 1, the flow of air is slowed by the viscous friction generated between the air and the surface 20F of the vehicle body 20, and the boundary layer 41 is formed. In the boundary layer 41, the speed of air increases as the distance from the surface 20F of the vehicle body 20 increases, and the speed of air approaches the relative speed of the automobile 1 with respect to air.

In the outer region 43, away from the surface 20F of the vehicle body 20 and outside the boundary 42, the effect of viscous friction between the air and the surface 20F of the vehicle body 20 is no longer present, and the velocity of the air is the velocity of the vehicle relative to the air. It is almost equal to the relative velocity. The air flow in the outer region 43 is called the mainstream 2.

Returning to FIG. 1, the automobile 1 is a fluid discharge device that discharges a fluid having a lower air density than the outside air toward the outside of the automobile 1 from a fluid discharge position defined on the surface of the automobile 1 in front of the automobile 1 in the traveling direction. To be equipped with. As shown in the upper sectional view of FIG. 1, the fluid discharge position is, for example, the stagnation point 3 in front of the automobile 1 in the traveling direction. As shown in the graph at the bottom of FIG. 1, the stagnation point 3 is the point where the pressure of the fluid becomes maximum, so that the fluid discharged from the stagnation point 3 flows as the mainstream 2 to the entire surface of the automobile 1. Therefore, the air density of the mainstream 2 in a wide range can be reduced. Further, the spring from the stagnation point 3 does not easily disturb the streamline of the uniform flow and has the least influence. Therefore, since the fluid flows over the entire surface of the automobile 1, the air resistance of the automobile 1 can be reduced. The horizontal axis of the graph at the bottom of FIG. 1 indicates the position of the automobile 1 in the traveling direction, and the vertical axis indicates the pressure coefficient Cp.

In the embodiment, the fluid discharge position is not limited to the stagnation point 3. In addition to this, for example, as shown in FIG. 2, the fluid discharge position can be determined on the bumper fascia of the front bumper 4 of the automobile 1. That is, the fluid discharge device may discharge a fluid having a lower air density than the outside air toward the outside of the vehicle 1 from a fluid discharge position defined on the bumper fascia of the front bumper 4 of the vehicle 1. Specifically, the fluid discharge position can be arbitrarily determined between the upper end 4a and the lower end 4b of the front bumper 4.

Regardless of whether or not the stagnation point 3 in FIG. 1 is located on the bumper fascia of the front bumper 4, the fluid discharge position can be determined on the bumper fascia of the front bumper 4. The fluid discharged from the bumper fascia of the front bumper 4 flows to a wide range on the surface of the automobile 1 as the mainstream 2. Therefore, the air density of the mainstream 2 in a wide range can be reduced.

<Specific configuration example of the fluid discharge device>
Next, a specific configuration example of the fluid discharge device will be described. The fluid discharge device includes a fluid discharge hole formed at the fluid discharge position. The fluid discharge device includes a duct 5 formed on the bumper fascia of the front bumper 4 as a fluid discharge hole, as shown in FIG. The fluid discharge device discharges a fluid having a lower air density than the outside air from the duct 5. The fluid discharge device includes a pipe 7 having one end connected to a duct 5. The other end of the pipe 7 is connected to, for example, the exhaust port of the engine 8 which is an example of the drive source of the automobile 1 as shown in FIG. The exhaust gas discharged from the engine 8 passes through the pipe 7 and is discharged from the duct 5 to the outside of the automobile 1. That is, the fluid discharge device discharges the exhaust gas discharged from the engine 8 as an example of a fluid having a lower air density than the outside air.

The exhaust gas discharged from the engine 8 contains more water vapor than the atmosphere and is hotter than the atmosphere. Therefore, the molecular weight of the air in the mainstream 2 decreases, and the temperature of the mainstream 2 rises. Therefore, since the air density of the mainstream 2 is lowered, the air resistance of the automobile 1 can be reduced.

The drive source of the automobile 1 includes not only the engine 8 but also a fuel cell and a motor. That is, the automobile 1 includes a fuel cell vehicle (FCV), an electric vehicle (EV), and a hybrid vehicle (HV, PHV) having two or more of these drive sources. The fuel cell includes at least a solid oxide fuel cell (SOFC) and a polymer electrolyte fuel cell (PEFC). Further, the engine 8, the fuel cell and the motor are also heat generating parts, and the air around them is hotter than the atmosphere. In addition, the gas discharged from the fuel cell contains a large amount of water vapor. Therefore, the air density of the mainstream 2 is reduced by recovering the high-temperature gas around the drive source or the gas discharged from the drive source and discharging it from the duct 5.

<Mechanism for reducing air resistance>
Next, a mechanism for reducing the air resistance of the automobile 1 by reducing the air density of the mainstream 2 will be described.

Generally, the force received from the air by the traveling automobile 1 is represented by the force in each of the front-rear, left-right, and up-down axial directions of the automobile 1 and the moment around each axis, and is collectively called an aerodynamic six-component force. Normally, the force received from the air by the moving automobile 1 is expressed dimensionlessly, and in particular, the air resistance F, which is a force in the front-rear direction, is expressed by the air resistance coefficient Cd expressed by the following equation (1). .. Here, ρ is the density of air in the outer region 43, A is the front projected area with respect to the traveling direction of the automobile 1, and V is the relative velocity of the automobile 1 with respect to the mainstream.

Drag coefficient Cd is the product of the air dynamic pressure "pV ^2/2" and front projection area A, a value obtained by dividing the air resistance F. The air resistance coefficient Cd is an amount determined depending on the shape of the automobile 1, and affects fuel efficiency, maximum speed, acceleration performance, and the like during traveling. The air resistance F of an object such as the automobile 1 is dominated by the pressure resistance when viewed as a whole of the automobile 1, and the frictional resistance which becomes a problem in the aircraft is small in the automobile 1. Therefore, in order to reduce the air resistance F in the automobile 1, it is effective to pay attention to reducing the pressure resistance.

Reviewing the mathematical formula (1) based on the above attention, in the design of a normal automobile, the front projected area A is regarded as a parameter that can be dealt with in the design of the vehicle in order to reduce the pressure resistance. On the other hand, the mainstream air density ρ and the speed V are not regarded as parameters that can be dealt with in the design of the vehicle because they can fluctuate according to the driving environment of the automobile.

However, without being bound by the above-mentioned existing concept, the inventor of the present invention considered that the mainstream air density ρ can be a parameter that can be dealt with in vehicle design in order to reduce the pressure resistance. Focusing on the fact that the pressure resistance that occupies most of the air resistance F is proportional to the mainstream air density ρ, it is possible to reduce the air resistance F by lowering the air density ρ of the mainstream 2. I got the knowledge.

As shown in FIG. 5, since the air in the mainstream 2 is located away from the surface 20F of the vehicle body 20, it cannot be directly heated. However, the fluid discharge device discharges a fluid having a lower air density than the outside air toward the outside of the vehicle 1 from a fluid discharge position defined on the surface of the vehicle 1 in front of the vehicle 1 in the traveling direction. The discharged fluid forms a mainstream 2 located behind the fluid discharge position in the traveling direction. As a result, the air density ρ of the mainstream 2 can be lowered, so that the air resistance F of the automobile 1 can be reduced.

<Relationship between each physical property value of fluid and fluid density>
Next, the relationship between each physical property value of the fluid (air) discharged from the fluid discharge position and the air density will be described. FIG. 6A is a graph showing the relationship between air temperature and air density. The higher the temperature of the air, the lower the density of the air. Therefore, by discharging the fluid having a temperature higher than that of the outside air, the temperature of the main stream 2 becomes higher, and the air density of the main stream 2 can be lowered.

The fluid having a temperature higher than that of the outside air includes the exhaust gas of the engine 8 shown in FIG. In addition to this, for example, as shown in FIG. 7, the blower 32 (including the compressor) sends air to the heat generating component 31 mounted on the automobile 1, and the high temperature air heated by the heat generating component 31 is sent. It may be collected and sent to the duct 5 via the pipe 7. The heat generating component 31 mounted on the automobile 1 includes an engine 8, a fuel cell, a radiator, a brake, a shock absorber, and a high electric component (including a drive battery, a drive motor, and an inverter for driving the motor).

FIG. 6B is a graph showing the relationship between the molecular weight of air and the density of air. The smaller the molecular weight of air, the lower the density of air. Therefore, by releasing a fluid having a molecular weight smaller than that of the outside air, the molecular weight of the mainstream 2 becomes smaller, so that the air density of the mainstream 2 can be lowered.

For example, the molecular weight of water (18.01528 g / mol) is smaller than the average molecular weight of air (28.966 g / mol). FIG. 6C is a graph showing the relationship between the partial pressure of water vapor in the air and the density of the air. The higher the partial pressure of water vapor in the air, the lower the density of the air. Therefore, by releasing a fluid having a higher partial pressure of water vapor than the outside air, the molecular weight of the main stream 2 becomes smaller, so that the air density of the main stream 2 can be lowered.

The fluid having a higher partial pressure of water vapor than the outside air may be generated by using the device shown in FIG. 8 in addition to the exhaust gas discharged from the engine 8 or the fuel cell. That is, the water discharged from the air conditioner 35 included in the automobile 1 is collected in the container 33, a fine mist is generated by using the ultrasonic vibrator 34 arranged at the bottom of the container 33, and the mist is generated by using the blower 32. Is sent from the pipe 7 to the duct 5.

<Control of fluid discharge flow rate>
The fluid discharge device can control the discharge flow rate of the fluid. For example, as the moving speed of the automobile 1 increases, the speed of the mainstream 2 also increases, and the flow rate of the mainstream 2 also increases. Therefore, the fluid discharge device changes the fluid discharge flow rate according to the moving speed of the automobile 1. Specifically, the fluid discharge device increases the fluid discharge flow rate as the moving speed of the automobile 1 increases.

For example, the fluid discharge device includes a controller 61, as shown in FIG. 10C. The controller 61 controls the amount of air discharged from the blower 32 based on the moving speed detected by the vehicle speed sensor 63. As the control pattern, any one of the three control patterns 52a, 52b, and 52c shown in the graph of FIG. 10A can be used.

Further, as the temperature of the fluid discharged by the fluid discharge device is higher, the temperature of the mainstream 2 can be raised by a smaller discharge flow rate. Therefore, the fluid discharge device changes the discharge flow rate of the fluid according to the temperature of the discharged fluid. Specifically, the fluid discharge device reduces the discharge flow rate of the fluid as the temperature of the discharged fluid increases.

For example, as shown in FIG. 10C, the controller 61 controls the amount of air discharged from the blower 32 based on the temperature of the fluid detected by the temperature sensor 62. Specifically, the controller 61 reduces the amount of air released as the temperature of the fluid increases. As the control pattern, any one of the three control patterns 53a, 53b, and 53c shown in the graph of FIG. 10B can be used.

As shown in FIG. 9, when the fluid discharged by the fluid discharge device is the exhaust gas from the engine 8, the controller 61 controls the opening degree of the flow rate control valve 66. The flow rate control valve 66 adjusts the ratio of the flow rate discharged from the duct 5 to the flow rate sent to the exhaust manifold 65 in the total flow rate of the exhaust gas discharged from the engine 8. Increasing the opening degree of the flow rate control valve 66 increases the proportion of the flow rate discharged from the duct 5, and decreasing the opening degree of the flow rate control valve 66 decreases the proportion of the flow rate discharged from the duct 5.

<Both cooling of engine 8 and reduction of air resistance>
A radiator that dissipates heat from the engine 8 to the outside air may be arranged near the stagnation point 3 or the front bumper 4 in front of the automobile 1 in the traveling direction. However, if a fluid having a temperature higher than the outside air temperature is discharged from the fluid discharge position, the fluid having a temperature higher than the outside air temperature flows into the radiator, which may deteriorate the cooling performance of the radiator.

Therefore, the fluid discharge device changes the opening degree of the radiator shutter that controls the flow rate of the air flowing into the radiator according to the discharge flow rate of the fluid discharged by the fluid discharge device. As a result, the air resistance of the automobile 1 can be reduced without deteriorating the engine cooling performance of the radiator. Specifically, the larger the discharge flow rate of the fluid discharged by the fluid discharge device, the smaller the opening degree of the radiator shutter. If the discharge flow rate of the fluid is small, it is difficult for the fluid having a temperature higher than the outside air temperature to flow into the radiator, so even if the opening degree of the radiator shutter is large, the influence on the cooling performance of the radiator is small. If the discharge flow rate of the fluid is large, the opening degree of the radiator shutter is reduced so that the fluid having a temperature higher than the outside air temperature does not flow into the radiator. As a result, it is possible to achieve both cooling of the engine 8 and reduction of the air resistance of the automobile 1.

For example, as shown in FIGS. 11A and 11B, each of the radiator shutters 36 is rotatably supported by a fixed shaft 37, and one end of each radiator shutter 36 is connected to a movable link 38. The movable link 38 is driven in the vertical direction by the motor 60 and the gear 39. As a result, the opening degree of the radiator shutter 36 changes between the state in which the radiator shutter 36 shown in FIG. 11A is open and the state in which the radiator shutter 36 shown in FIG. 11B is closed. The controller 61 controls the opening degree of the radiator shutter 36 by controlling the motor 60 based on the discharge flow rate of the fluid discharged by the fluid discharge device detected by the flow rate sensor 64.

For example, the controller 61 controls the opening degree of the radiator shutter 36 based on the flow rate of the fluid detected by the flow rate sensor 64 by using any of the control patterns 54a, 54b, and 54c shown in FIG. 11D.

The control patterns 54a, 54b, 54c of FIG. 11D continuously change the opening degree of the radiator shutter 36. The controller 61 may change the opening degree of the radiator shutter 36 discontinuously. For example, as shown in FIG. 11C, the flow rate sensor 64 detects the flow rate of the fluid (S01) and determines whether or not the detected flow rate is equal to or higher than a predetermined threshold value (predetermined value) (S03). When it is equal to or higher than the threshold value (YES in S03), the controller 61 controls the opening degree of the radiator shutter 36 to the closed state shown in FIG. 11B (S05). When it is less than the threshold value (NO in S03), the controller 61 controls the opening degree of the radiator shutter 36 to the open state shown in FIG. 11A (S07).

As described above, according to the embodiment, the following effects can be obtained.

The automobile 1 includes a fluid discharge device that discharges a fluid having a lower air density than the outside air toward the outside of the automobile 1 from a fluid discharge position defined on the surface of the automobile 1 in front of the automobile 1 in the traveling direction. As a result, the air density of the mainstream 2 in a wide range among the mainstreams 2 around the automobile 1 is lowered, so that the air resistance of the automobile 1 can be reduced.

The fluid discharge position is the stagnation point 3 in front of the traveling direction. Since the stagnation point 3 is the point where the pressure of the fluid is maximized, the fluid discharged from the stagnation point 3 flows over the entire surface of the automobile 1. Therefore, the air density of the mainstream 2 in a wide range can be reduced. The spring from the stagnation point 3 is less likely to disturb the streamline of the uniform flow and has the least effect. Therefore, the fluid discharged from the stagnation point 3 flows over the entire surface of the automobile 1, and the air resistance of the automobile 1 can be reduced.

The fluid discharge position may be set in the bumper fascia of the front bumper 4 of the automobile 1. The fluid discharged from the fluid discharge position on the bumper fascia flows over the entire surface of the automobile 1. Therefore, the air density of the mainstream 2 in a wide range can be reduced.

The fluid discharged from the fluid discharge position is a fluid whose temperature is higher than the outside air temperature. If the fluid is hotter than the outside air temperature, the temperature of the mainstream 2 can be raised. As the temperature of the mainstream 2 rises, the air density of the mainstream 2 decreases, so that the air resistance of the automobile 1 can be reduced.

The fluid discharged from the fluid discharge position is a fluid having a molecular weight smaller than that of the outside air. Since the molecular weight of the fluid is smaller than that of the outside air, the molecular weight of the air in the mainstream 2 is lowered. Therefore, since the air density of the mainstream 2 is lowered, the air resistance of the automobile 1 can be reduced.

The fluid discharged from the fluid discharge position is a fluid having a higher partial pressure of water vapor than the outside air. Since the molecular weight of water is smaller than that of air, if the partial pressure of water vapor is made higher than that of the outside air, the air density of the mainstream 2 decreases. Therefore, the air resistance of the automobile 1 can be reduced.

The fluid discharged from the fluid discharge position is the exhaust gas discharged from the engine 8 included in the automobile 1. The exhaust gas discharged from the engine 8 contains more water vapor than the atmosphere and has a high temperature. Therefore, the molecular weight of the air in the mainstream 2 decreases, and the temperature of the mainstream 2 rises. Therefore, since the air density of the mainstream 2 is lowered, the air resistance of the automobile 1 can be reduced.

The fluid discharge device changes the discharge flow rate of the fluid according to the moving speed of the automobile 1. It is possible to discharge a fluid having a discharge flow rate required to reduce the air resistance of the automobile 1.

The fluid discharge device changes the discharge flow rate of the fluid according to the temperature of the fluid. A fluid with a discharge flow rate required to raise the temperature of the mainstream 2 can be discharged.

The fluid discharge device changes the opening degree of the radiator shutter 36 included in the automobile 1 according to the discharge flow rate of the fluid. The air resistance of the automobile 1 can be reduced without deteriorating the engine cooling performance of the radiator. That is, it is possible to achieve both engine cooling and reduction of air resistance.

Although the contents of the present invention have been described above with reference to the embodiments, it is obvious to those skilled in the art that the present invention is not limited to these descriptions and various modifications and improvements can be made.

In the above-described embodiment, the case where the moving body is an automobile has been described, but the present invention is applicable to a moving body moving in the air other than the automobile. Examples of moving objects include motorcycles, railroads, aircraft, rockets, etc., in addition to automobiles.

In the above-described embodiment, the case where the fluid discharged from the fluid discharge position satisfies any of the conditions of higher temperature, lower molecular weight, and higher partial pressure of water vapor as compared with the outside air has been described. Is not limited to this. The fluid may simultaneously satisfy two or more conditions arbitrarily selected from the above.

Further, the fluid discharge device may control the discharge flow rate of the fluid based on the combination of the moving speed of the automobile 1 and the temperature of the fluid.

1 Moving body 20F Surface 3 Stagnation point (fluid discharge position)
4 Bumper Fascia 8 Engine 36 Radiator Shutter

Conventionally, a cooling device such as an engine to be cooled by air are known at the time of need within the engine and engine Lou beam of a vehicle (Patent Document 1). When the engine Lou beam becomes equal to or higher than a predetermined temperature, the air from the engine room, and flows out from the cabin side end portion above the gap of the engine to the outside of the vehicle.

For example, the molecular weight of water (18.01528 g / mol) is smaller than the average molecular weight of air (28.966 g / mol). FIG. 6C is a graph showing the relationship between the partial pressure of water vapor in the air and the density of the air. The higher the partial pressure of water vapor in the air, the lower the density of the air. Thus, by releasing the fluid high partial pressure of water vapor than the outside air, since the molecular weight of the main 2 is reduced, it is possible to lower the air density mainstream 2.

Therefore, the fluid discharge device changes the opening degree of the radiator shutter that controls the flow rate of the air flowing into the radiator according to the discharge flow rate of the fluid discharged by the fluid discharge device. As a result, the air resistance of the automobile 1 can be reduced without deteriorating the engine cooling performance of the radiator. Specifically, the larger the discharge flow rate of the fluid discharged by the fluid discharge device, the smaller the opening degree of the radiator shutter. The less release the fluid flow rate, since the high temperature fluid than the outside air temperature is less likely to flow into the radiator, the influence of the cooling performance of the radiator even by increasing the degree of opening of the radiator shutters is small. If the discharge flow rate of the fluid is large, the opening degree of the radiator shutter is reduced so that the fluid having a temperature higher than the outside air temperature does not flow into the radiator. As a result, it is possible to achieve both cooling of the engine 8 and reduction of the air resistance of the automobile 1.

Claims (10)

A moving body including a fluid discharging device that discharges a fluid having a lower air density than the outside air toward the outside of the moving body from a fluid discharging position defined on the surface of the moving body in front of the moving body in the traveling direction. The moving body according to claim 1, wherein the fluid discharge position is a stagnation point in front of the traveling direction. The moving body according to claim 1 or 2, wherein the fluid discharge position is defined in the bumper fascia of the moving body. The moving body according to any one of claims 1 to 3, wherein the fluid is a fluid having a temperature higher than the outside air temperature. The moving body according to any one of claims 1 to 4, wherein the fluid is a fluid having a molecular weight smaller than that of the outside air. The moving body according to any one of claims 1 to 5, wherein the fluid is a fluid having a higher partial pressure of water vapor than the outside air. The moving body according to any one of claims 1 to 6, wherein the fluid is an exhaust gas discharged from an engine included in the moving body. The moving body according to any one of claims 1 to 7, wherein the fluid discharging device changes the discharge flow rate of the fluid according to the moving speed of the moving body. The moving body according to any one of claims 1 to 8, wherein the fluid discharge device changes the discharge flow rate of the fluid according to the temperature of the fluid. The moving body according to any one of claims 1 to 9, wherein the fluid discharging device changes the opening degree of the radiator shutter included in the moving body according to the discharge flow rate of the fluid.

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