design of the electrical power system for a rc-toy car
Transcription
design of the electrical power system for a rc-toy car
Bogdan DOROBANŢU DESIGN OF THE ELECTRICAL POWER SYSTEM FOR A RC-TOY CAR Abstract: This paper presents the process of designing the electrical propulsion system for a radio controlled toy car by analyzing the resistant forces and the necessary power to overcome these forces. Keywords: design, propulsion, car, modeling, electrical motor. 1. INTRODUCTION The systems of a toy car are as complicated as a real electrical car because it has an electric motor, differential and/or gearbor, control unit, batteries, transmitter and receiver for control, power steering unit and suspension. All these systems are interconnected because of the voltage used by the electrical engine, ex: an electrical motor that uses 7,4 V needs a battery to supply the 7,4 V and a control unit to manage the power to the motor. f[-] 2. ELECTRICAL MOTOR To determine what electrical motor we need for the rc car we must calculate the power necessary to overcome the power losses by the forces that act on the car, like: air drag, rolling resistance of the tires, transmission efficiency, sloping rolling resistence (because all roads have a slope, even if it’s very small). Speed [km/h] Fig. 1 Dependence of the rolling resistance factor with the speed 2.2 Determing the maximum cross-sectional area of the vehicle 2.1 Determing the rolling resistance of the tires Rolling resistance depends on many factors like tire design, speed, tire pressure, road or surface, weight. The rolling factor or coefficient is determined by experimental way based on the results obtained from different empirical formulas, the simplest one based on the speed of the car : f= + ∙V + ∙ There are 2 ways to determine the maximum crosssectional area of the vehicle: • Using the formula: A= ∙ ∙ ∙ ∙ [m²] (1) • where: represents the rolling resistance factor at low speed • [h/km] and [h2/km2] influence factors of the speed, picked from standardized tables. For calculating the rolling resistance we need to know the tires of the car which are 26 mm in radius with a very low section height. And so for our kind of tire the rolling resistance factors are stated below: =1.6115∙ 10 =-9.9130∙ 10 [h/km] =2.3214∙ 10 [h2/km2]. The chart (Fig.1) shows that the rolling resistance values increases with the speed and so for high speed the rolling resistance is higher than for low speed. (2) where: =1 is a shape factor, =0,14 m is the width of the vehicle (including mirrors) - =0,07 m is the height, -h =0,015 m is the ground clearence (height from the road to the lowest part of the bumper) , - N =2 is the number of the tires on the back axle, - B! =0,017 m is the tire section width. A=1 ∙ 0,14 ∙ 0,07 0,015 2 ∙ 0,015 ∙ 0,017 ' =0,00821 m² • Using the contour of the front view of the car To calculate the cross-section area you can use AutoCAD with the command “area” and it calculated for our contour of the car an area of A=0,00754 m², value that will be used to determine the wind resistance or wind drag. JOURNAL OF INDUSTRIAL DESIGN AND ENGINEERING GRAPHICS 13 Design of the electrical propulsion system for a RC-toy car Ga weight of the vehicle is expressed in daN; 3 is the slope angle of the moving vehicle. To calculate the power required to overcome rolling resistance is used the relation: 140mm 4-. ' 70mm 5∙67 ∙89: ;< ∙5 = (4) >?@A To calculate slope resistance we used the formula: ,B ' /C ∗ sin 3 [daN] 15mm Fig. 2 Cross section of the car Power required to overcome this resistance is calculated as follows: 2.3 Determing the wind drag factor Given that the shape of the car body is designed to be very close to that of the real model, we can agree that they have a value of air resistance coefficient close to that of the model, and so : C) =0,25. This value was chosen in the range of [0.25, 0.35] taking into account both its value of the similar model, and the value of the cross-section area. 2.4 Determing the transmission efficiency Power developed by the engine is transmitted to the wheels through the transmission to propel the vehicle. This phenomenon always occurs frictional losses in the transmission, losses are characterized by η* - transmission efficiency. For a car with a main cone transmission and fixed ratio transmission is adopted a value of η* =0,97 from the interval (η=0,96 – 0,98). 4 ' VOLUME 8 │ ISSUE 1 │ JUNE 2013 (6) >?@A , ' J∙K∙5L M = (7) >NCA where: -Ra is air resistance, expressed in daN; -k=0,06125·Cx , is the drag coefficient; -A is the cross-sectional area of the vehicle; Vx=V+Vv [km/h] is the vehicle speed relative to the air. where: - V is the vehicle speed, - Vv is the wind speed. In this case it is considered Vv=0 km/h Power required to overcome air resistance can be calculated with the formula: J∙K∙5L M ∙5 O P (8) >?@A In Fig 3 are centralized all powers necessary to overcome the resistance values and their calculated when the vehicle is moving, no wind, on tier. 0,03 Prul P [KW] 0,03 0,02 Pa 0,02 ∑P 0,01 0,01 0,00 0,00 0 50 100 V[km/h] Rolling resistance using the formula: 14 = 4 ' Forward resistance forces are the forces resulting from the interaction of the vehicle with the environment, as opposed to its advancing. There are several types of resistance : rolling resistance, air resistance and slope resistance. Inertial forces appearing in moving vehicles are considered a drag resistance and is called resistance start or resistance acceleration. In the following calculations it does not appear in the balance of power to the wheel as it considers a motion evenly (without acceleration) and acceleration at maximum speed is 0. We will calculate the drag resistance for two situations: - tier movement (αp=0) - slope movement pmax=8% with αp=arctg(0,08)=4,57⁰; To calculate these forces, were used the relantions presented below: where : ,-. is the rolling resistance; f is the rolling resistance coefficient; 67 ∙GHI ;< ∙5 Air resistance is calculated by the following formula: 2.5 Determing the power loss of the vehicle ,-. ' ∙ / ∙ cos 3 [daN] (5) (3) Fig. 3 Resistance powers an tier. In Fig 4 are centralized all powers necessary to overcome the resistance values and their calculated when the vehicle is moving, no wind, on a slope. P [KW] Design of the electrical propulsion system for a RC-toy car 0,05 0,05 0,04 0,04 0,03 0,03 0,02 0,02 0,01 0,01 0,00 Prul Pa Pp ∑P 0 50 V[km/h] 100 Fig. 4 Resistance powers on a slope Using the formulas presented we calculated that the power required to overcome rolling resistance and air resistance for the car is 0,044 KW to achieve 100 km/h. Total power developed by the electric motor must be greater than that calculated to account for power losses in transmission (ηt = 0.97). [1][2] 4IQR ' S ηT ' ,OO ,U ' 0.045?@ pack it can get up to 40mph with just the standard gearing. With up to 8 NiMH cells or a 3S LiPo (11.1v) pack and higher gearing (using a smaller spur gear and larger pinion), it can get up to 60mph, perfect for massive track or insane speed runs. When geared correctly, the Warp 5700 is equivalent to a high quality 9-turn or 10-turn brushed motor using 6 NiMH cells - a very powerful motor. The Warp 5700 features: -powerful, high-speed brushless motor -excellent pairing of huge power and extraordinary efficiency -same size as standard 540-size motor -sleek black-anodized aluminium casing -zero maintenance design -external solder tabs for easy wire replacement -oversized precision ball bearings for long life -high Torque/ High Temperature Neodymium rotor -slotless stator design delivers smooth, linear torque -easy 4-point mounting for convenient installation -longer run times than a comparable brushed motor -easily rebuildable with bearings and rotor being userreplaceable -compatible with any sensorless ESC (9) 2.6 Chosing the electric motor The electric motor needs to have more power than it is needed to propel the car. The most important parameters for these motors are Kvs, volts and rpm. KV as we use it refers to the rpm constant of a motor - it is the number of revolutions per minute that the motor will turn when 1V (one Volt) is applied with no load attached to the motor. In summary, we call it revs per volt - but do not think you will obtain those revs when you attach a gearwheel; obviously the revs will be reduced because of the load. What does the KV tell us? Well it is related to the power out from a motor, or more usefully the torque level of a motor. It is determined by the number of winds on the armature (or turns) and the strength of the magnets. So KV allows us to get a handle on the torque we can expect from a particular motor. In summary, a low KV motor has more winds of thinner wire - it will carry more volts at less amps, produce higher torque and swing a bigger gearwheel. That may sound confusing, but compare it with a high KV motor which has less winds of thicker wire which will carry more amps at less volts and spin a smaller gearwheel at high revs. For example, a motor of Kv, 5,700 RPM/V, supplied with 11.1 V, will run at a nominal 63,270 RPM (5,700 RPM/V × 11.1 V). The Flux Warp 5700Kv Brushless Motor seems to be a good choice for this project. The Warp 5700 is the top choice for nearly all 1/10th scale electric touring car, buggy and trucks. It can go super-fast on the track and get those blazing speed runs with the same motor! With a standard 6-cell NiMH battery pack or 2S LiPo (7.4 volt) Fig. 5 Flux Warp electric motor The Flux Brushless System is HPI's answer to hobbyists and racers who want a powerful, versatile and affordable brushless motor system. The Warp motors are extremely powerful, very durable and highly efficient to get you going on the road to victory. HPI Warp motors are sensorless type motors, so there are fewer wires to worry about, and less hassle for you. Flux Warp motors must be used with a brushless electronic speed control that is suitable for sensorless motors. [3] 3. BATTERIES For this kind of motor it is used the new Plazma battery pack (47,4 Wh): -voltage: 7.4V -capacity: 6500mAh -current rating: 95C -case type: rectangular LiPo case, sealed plastic -dimensions: 138.6 x 45.8 x 25.1mm 25.1mm) -plug:DeansUltraPlug for extreme high-power JOURNAL OF INDUSTRIAL DESIGN AND ENGINEERING GRAPHICS 15 Design of the electrical propulsion system for a RC-toy car PlazmaPro competition range features two high-end packs designed purely for use on the race track! This pack fits within all accepted maximum pack sizes, allowing it to fit in any competition touring car, buggy, short course truck and other types of racing car. The 95C power rating will give plenty of acceleration while the 6500mAh rating will allow to fully utilise the power of the pack throughout a 5-minute race. It also features a real Dean's connector and a universal balancing plug for simple maintenance.[3] Fig. 8 Electronic speed controller 5. CONCLUSION Fig. 6 Battery pack 4. ELECTRONIC SPEED CONTROLLER Engine control system is called ESC (Electronic Speed Controller) and its role is to change the speed of the electric motor, change the direction of rotation or to serve as a dynamic brake by using the electric motor as a generator. Through a process called PWM (Pulse Width Modulation Figure 7), the controller varies the speed by changing the motor voltage very quick simulating a medium voltage. This switching frequency can reach up to 20 kHz. Analyzing structural variations of similar patterns and trends in the field it is found that the rc-car will be designed to run on flat surfaces, having independent suspension with oil shocks and springs. To overcome the encountered resistances like: rolling resistance, air resistance, slope resistance and the power loses from the transmission resulted from calculations that the car needs a electric motor capable to deliver 45W to achieve the speed of 100 km/h. This speed can be delivered by the Flux Warp 5700Kv brushless motor in conjunction with a 3S LiPo (11.1v) battery pack and a higher gearing transmission. But for this project I chosen a smaller battery pack, the PlazmaPro that delivers 6,5 Ah at 7,4 V and 47,4 Wh. To control the engine speed will be used a type ESC Pulse With Modulation. The power will be transmitted from the engine to the wheels through a gear, differential and drive shafts. Fig. 9 Chassis modeling in CATIA V5 Fig. 7 PWM The Flux Blur speedo is the most powerful brushless speed controller we could find. With the ability to handle twin 3S LiPo batteries (that's a total of 6S LiPo power! it can deal with anything powerful brushless motors. The 6mm bullet connectors secure the motor wires for loss-free connection to the 12-gauge wires, and to connect to each battery pack has attached real Dean's connectors for zero power loss and total efficiency. Topping off the versatility of the Flux Blur speedo is an integrated cooling fan, which allows the speedo to operate at its ideal temperature.[3] 16 VOLUME 8 │ ISSUE 1 │ JUNE 2013 REFERENCES [1] C. Andreescu – “Vehicle dinamics” [2] G. Danciu –“Electric and hibrid vehicles” [3] www.hpiracing.com Author: Bogdan DOROBANTU, Master Student, University Politehnica of Bucharest, Department of Engineering Graphics and Industrial Design E-mail: [email protected]