I have been
playing with the idea of removing every gear in the drive system in a car by
installing directly the motor on the axle of the wheel.
As an
example in my calculation, I’ve decided to take my Toyota Yaris. Here the data:
Wheel size
(diameter D): 355.6mm (14 inch)
Tire size (diameter
D): 610mm (24 inch)
At 100km/h.
the RPM of the motor is around 2650 RPM (44 rev/s).
We know
that we have gear ratios but let’s put this aside for a minute. We can calculate
the speed of a car just by knowing the RPM of the motor and the wheel
circumference. In my case, the wheel circumference Cr = πD, 1916.5mm (75.45
inch). The speed v = rev/s • Cr = 84 320 mm/s and yields to 84.32 m/s.
Converting this into km/h yields to 303.5 km/h (188.6 MPH)! Ok, this excludes
the final gear ratio. The thing is; do I need a high speed motor such as
5000/6000RPM? The answer is no but what is the minimum acceptable?
Let’s start
by targeting the maximum speed that I would like to achieve; 160 km/h (100mph).
We need to convert all this to m/s and yields to 44.4 m/s. We need to transform
the speed equation v = rev/s • Cr into rev/s = v/Cr : 44.4 / 1.916 = 23.2 rev/s
= 1390 RPM!
It would
explain why most of all the car EV conversion, there’s always a gear ration
somewhere in amateur likes the big companies. In the big companies, they have
left out the transmission. What I have seen and red in the amateur EV world,
often, the transmission and the transaxle are kept. I assume that it’s a way to
reduce the cost of the conversion because adding two motors, two inverters,
will almost double the conversion. In the big companies like the Mitsubishi
Miev, the Nissan Leaf, or the Ford eFocus (and others), all have a transaxle reducing
gear. I’m no mechanical engineer but I would assume that having a transaxle
ratio of 1:1 would be very large!
Let's reduce the current to save energy
My objective
in this enterprise is to get rid of all unnecessary mechanical parts.
Motor in wheel
are a good choice but I am a bit skeptical about their durability in the long term.
I opted to connect two motors to each axle that drives the front or the rear
wheels. This is direct drive.
All calculations
and simulations made on the Quadrupole motor/generator are based on a 100A and 5 turns. This
gives a magnetomotive force (MMF) of 500 At (amp turn). Because it’s a double stator design, three torque
constants 3 are available: 0.375, 0.205 and 0.145 Nm/A. Since we could, at 144 Vdc
bus, achieve almost 3500 RPM at 0.372 Nm/A and with the calculation above for direct drive, we
can reduce the maximum RPM to 1390 RPM. Taking in mind that we need to achieve
the maximum RPM with the maximum torque constant. This will reduce even more the
current without any compromises.
Let’s start
by reformulating everything, first the BEMF constant Ke. The BEFM is
the maximum EMF or the generated voltage divided by the maximum angular speed.
So for a 144Vdc bus and because of voltage losses, let's arbitrarily assume
that a BEMF of 125V peak with a 144Vdc bus.
So;
Ke
= 125Vdc / (1390 rpm / 9.55) = 125Vdc / 13 275 rad • s-1 = 0.859
V/ rad • s-1
Since the
BEMF constant is equal to the torque constant, we can rewrite Te = Tk =
0.859 Nm / A
The torque
constant Kt muliplyed by the currant give the torque as shown in the equation below:
T = Kt
• I
Since Kt
as change, the value of the current must change. So the
currant will be:
I = T / Kt
The maximum
continuous torque of the Quadrupole motor is 41 Nm (41 Nm is the last available
numbers of the Quadrupole motor/generator).
I = 41 Nm /
0.859 Nm/A = 47.7 A
We need to calculate
the number of turn required to maintain the MMF at 500 At as to maintain 41 Nm/A.
The torque constant equation is below:
Kt
= N • Bp • L • D • p
Where:
- N is number of turns and it is unitless,
- Bp is the average flux in the air-gaps in Tesla (T) and equal 0.9718 T
- L is the depth of the saliency of the each stator pole in metre (m) and is equal to 0.0381 m,
- D is the diameter of the air gaps in metre (m).
- p is number of pole pairs ( numbers of pole /2) and it is unitless
We have to separately
calculate the Tk of the inner and the outer stator and add them
together to get the sum of Tk. Since we have two stators, Kt(inner)
and Kt(outer) they will very since the D and Bp are not
the equal in both stators. The maximum constant torque Kt = Kt(inner)
+ Kt(outer). However, the number of turns remains the same in both stators.
So, a MMF of 500 At and feeding hit at 100 A of current, this means that I have 5 turns.
Insolating N from the MMF will be N = MMF / I.
Let's recap. 47.4 A is required for the new toque constant and that MMF = 500 At. Using the above equation, 500 At / 47.7 A = 10.5 turns. We will round it down to 10 since we have taken
into account the voltage drop at the motor wires.
Lower amps per torque
So 50 Amps
only at 144Vdc for 1390 rpm and 41 Nm, this is very good since the heat loss
will be lower and will have less impact for on the magnet. However, since there is more turns, and to accommodate this, we
need to reduce the wire size. By adding more turns and reducing the wire size, iIt will increase the resistance of the winding
and also decrease the efficiency of the motor.
Yes, only
50 A per motor (2 required for each axle) to achieve an incredible torque at
very low power. On less that I'm wrong, it’s not the power that will make the car go forward
but the torque.
I will be
running further simulation for a 50A but even at a lower current intensity. The
cons is that I will need to increase the voltage.
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