Hardware Academy
EV Powertrain

Tesla Roadster and motor evolution

From the 2008 Roadster's induction motor to carbon-sleeved rotors and the second-generation Roadster claims.

Day 12 · 55 min

After this lesson

  • You can describe the 2008 Roadster's powertrain with numbers.
  • You can trace Tesla's motor evolution and explain each change.
  • You can discuss the second-generation Roadster claims critically.

Fifteen years of Tesla drive units

Tesla's motors are a compact history of EV engineering: each generation fixed the constraint that limited the one before. The constraints are always the same four: torque per unit of rotor volume, how fast the rotor can spin, how much heat can be removed, and how efficiently the inverter switches.

2008 Roadster: proving the idea

The first Roadster was built on a Lotus Elise-derived chassis with a rear-mounted three-phase AC induction motor of about 185 kW. Its 53 kWh pack held 6,831 18650 cells, the laptop-battery format, which gave 0-60 mph in 3.7-3.9 s and 244 miles of EPA range. A two-speed gearbox was planned and then abandoned for a single fixed reduction: an electric motor makes full torque from standstill and keeps making power over a far wider speed range than a piston engine, so a second gear added mass and failure points for little gain.

Why induction? The rotor is a stack of steel laminations with conducting bars shorted by end rings, and no magnets. The stator's field rotates slightly faster than the rotor (the slip), induces currents in the bars, and those currents make torque. No magnets means no rare-earth supply risk and no demagnetization at high temperature. It also means no field when the inverter is off, so an unpowered induction motor freewheels with almost no drag and cannot generate a dangerous voltage after a fault at high speed.

Model S (2012): induction, scaled up

The Model S kept the recipe and scaled it: a liquid-cooled induction motor with copper rotor bars, which have lower resistance than the usual cast aluminium and so make less rotor heat, fed by an 85 kWh pack of 7,104 18650 cells in 16 modules. Dual-motor versions arrived in 2014 with a second induction motor at the front.

Model 3 and Model Y: magnets arrive

The Model 3 (deliveries from July 2017) introduced a rear IPM-SynRM: permanent magnets buried in V-shaped pockets inside the rotor laminations, plus air-filled flux barriers that make the rotor magnetically uneven. Torque comes from the magnets pulling on the stator field and from reluctance torque, the steel trying to align its easy flux path with that field. At highway cruise the motor runs at light load, where an induction machine spends current magnetizing its rotor and heating its bars; magnets provide that field for free, so range improves. Dual-motor cars kept an induction motor at the front, because a part-time motor that freewheels without drag suits induction. The Model 3 also moved its inverter to silicon carbide MOSFETs, which lose far less than silicon IGBTs, especially at partial load.

Plaid (2021): speed is power

Mechanical power is torque times angular speed, P = T × ω. Torque is set by rotor size and current, so the cheapest way to get more power from the same size is to spin faster. The Model S Plaid uses three motors (one front, two rear) with carbon-fiber-sleeved permanent-magnet rotors that run to about 20,000 rpm, for 1,020 hp. The sleeve matters because hoop stress grows with the square of speed: at 20,000 rpm the surface of a rotor 140 mm across moves at about 147 m/s. Carbon fiber is far stronger for its weight than steel, non-magnetic and much less conductive than a metal sleeve, so it holds the rotor together without adding much eddy-current loss.

Cybertruck (2023): the electrical system moves

The Cybertruck changed the architecture around the motors: an 800 V-class high-voltage system, which halves the current for the same power; a 48 V low-voltage system instead of 12 V, a quarter of the current for the same power and so a lighter harness; and steer-by-wire, with no mechanical link from the steering wheel to the rack.

Cross-sections of an induction rotor and an interior permanent magnet rotor inside their statorsInduction rotorRoadster, Model S, Model 3/Y front motorCopper bars, shorted by end rings, carry induced currentNo magnets: no field and almost no drag when unpoweredInterior permanent magnet rotor (IPM-SynRM)Model 3/Y rear motorBuried V-shaped magnets plus flux barriers (air pockets)Magnets are always on: back-EMF and drag when coastingcoppermagnet, N polemagnet, S polelaminated steelcarbon sleeve
Left: an induction rotor, laminated steel with copper bars shorted by end rings. Right: an interior permanent magnet rotor with V-shaped buried magnets and flux barriers, the Model 3/Y rear-motor type. The dashed ring marks where a carbon-fiber sleeve sits on a high-speed PM rotor such as the Plaid's.

The second-generation Roadster: claims, not specifications

Tesla unveiled a second-generation Roadster in November 2017 and announced these figures: 0-60 mph in 1.9 s, a 200 kWh battery, 620 miles of range, a top speed above 250 mph and three motors, later joined by a “SpaceX package” of cold-gas thrusters. Every one of them is an announced claim, not a shipped specification. The car was promised for 2020 and has been delayed repeatedly, so check Tesla's site for its current status before quoting any of these numbers. The claims are still worth testing with physics. Reaching 60 mph in 1.9 s averages about 1.44 g, at or beyond the grip limit of road tires, and the thrusters were pitched as a way past that limit. At 160-200 Wh/kg for a whole pack, 200 kWh would weigh roughly 1,000-1,250 kg, heavy for a roadster.

Beyond Tesla: where motors are going

  • Hairpin windings: rectangular copper bars bent like hairpins, pushed into the slots and welded, fill around 70 % of the slot versus roughly 40-50 % for round wire, cutting copper loss and conducting heat out better.
  • Oil cooling: oil sprayed on the end windings and pumped through the rotor shaft removes heat where it is made, which raises continuous power.
  • Axial-flux motors: disc-shaped rotors and stators, short and torque-dense; YASA, bought by Mercedes-Benz in 2021, is the best-known maker.
  • Rare-earth-free magnets: Tesla said at its 2023 Investor Day that its next permanent-magnet motor would use no rare-earth elements, while BMW's fifth-generation eDrive uses an electrically excited rotor instead of magnets. Treat unshipped designs as claims.
  • Integrated drive units: motor, inverter and reducer in one housing sharing one coolant loop.
  • 800 V with SiC: Hyundai's E-GMP cars (Ioniq 5, 2021) use it to charge faster through thinner cables.

Interactive: the motor timeline and the torque-speed envelope

Step through the timeline from the 2008 Roadster to today. The second-generation Roadster sits above the line as a dashed diamond because it is a set of announced claims, not a shipped car.

Tesla motor timeline, 2008 to today

Pick a point on the timeline. Green markers are shipped cars; the amber diamond is the second-generation Roadster, which exists only as announced claims.

Timeline from 2008 to today; selected: Roadster (2008)2008201020122014201620182020202220242026RoadsterModel SModel 3Roadster 2: claims announced Nov 2017PlaidCybertruckToday
Jump to

Roadster (2008)

Shipped
Chassis
Lotus Elise-derived
Motor
Three-phase AC induction, about 185 kW
Battery
53 kWh from 6,831 × 18650 cells
0-60 mph
3.7-3.9 s
Range
244 mi (EPA)
Gearbox
Single speed; the planned two-speed was abandoned

Proved that thousands of small laptop-class cells, monitored and cooled as one pack, could power a fast car. The induction motor needed no magnets, and its wide speed range made a second gear unnecessary.

Then compare machine types. Hold the speed at 15,000 rpm and switch motors: the induction curve has already lost power, while the carbon-sleeved PM is still at its peak.

Torque-speed envelope

Below base speed the inverter's current limit caps torque. Above it the back-EMF reaches the battery voltage, so the controller weakens the field and power stays roughly flat (P = T × ω) until that runs out.

Torque and power against speed for the IPM-SynRM motor, operating point at 9000 rpmconstant torqueconstant powerfalling power0100200300400500010020030005k10k15k20kmotor speed, rpmtorque, N·mpower, kWpeak 211 kWConstant power (field weakening)
Motor speed
9,000 rpm
Road speed*
82 mph
Torque
224 N·m
Power
211 kW
Peak power
211 kW
Max speed
17,000 rpm

IPM-SynRM: Buried magnets supply the field and flux barriers add reluctance torque, so a negative d-axis current can weaken the field over a wide speed range. Partial-load efficiency is high because no current is spent magnetizing the rotor.

Motor
Illustrative envelopes with round numbers: the shapes follow each machine type, but none is measured data for a production motor. *Road speed assumes a 9:1 single-speed reduction and a 0.35 m tire radius.

In practice

Practice

Specific power across motor generations

A drive-unit team compares four machines. Power figures A, B and D come from the cars; C's power and all four masses are round assumptions for practice (active stator and rotor only), not published Tesla data.

MachinePeak powerAssumed active mass
A: Roadster-era induction185 kW52 kg
B: Model S Performance-era copper-rotor induction310 kW (416 hp)75 kg
C: IPM-SynRM200 kW (assumed)40 kg
D: carbon-sleeved PM, one motor's average share of the Plaid's 1,020 hp?35 kg

(1) Convert 1,020 hp to kW and find D's average share. (2) Compute each machine's specific power in kW/kg. (3) By what factor did specific power grow from A to D? (4) If D makes its peak power from 6,000 rpm upward, what torque does that imply?

text
(1) 1,020 hp × 0.7457 kW/hp      = 760.6 kW total; ÷ 3 motors = 253.5 kW
(2) A: 185 ÷ 52                  = 3.6 kW/kg
    B: 310 ÷ 75                  = 4.1 kW/kg
    C: 200 ÷ 40                  = 5.0 kW/kg
    D: 253.5 ÷ 35                = 7.2 kW/kg
(3) 7.2 ÷ 3.6                    ≈ 2.0×
(4) ω = 6,000 × 2π ÷ 60          = 628.3 rad/s
    T = P ÷ ω = 253,500 ÷ 628.3  ≈ 403 N·m

Answer: D averages about 253.5 kW per motor; specific power rises from about 3.6 to 7.2 kW/kg, roughly double, with about 403 N·m at a 6,000 rpm base speed. The gain comes from speed, because the sleeve lets the same torque spin faster and P = T × ω; from magnets that need no magnetizing current; and from better cooling and copper fill that let the same copper carry more current. The SiC inverter does not make the motor lighter, but it cuts the losses the pack must cover.

Real-world scenario

Real-world scenario

Design review: the front motor that cost 4 % of highway range

An EV startup is reviewing its dual-motor crossover before design freeze. To share parts, the team fitted the same 150 kW interior permanent magnet motor to both axles. The rear motor drives the car while cruising; the front motor is commanded to zero torque and only joins in for hard acceleration, low grip or towing. Prototype range at a steady 70 mph comes in 4 % below target, and the drive-unit team has to explain why.

Symptoms

  • Coast-down tests show about 600 W more drag at 70 mph than the rear-drive prototype, and the gap grows faster than linearly with speed.
  • The front inverter draws current at high speed even when the front torque command is zero.
  • The front stator warms up on long highway runs although the motor produces no torque.
  • City-speed range is within 1 % of target; almost all of the shortfall is at highway speed.

Interview questions

screenWhy did the 2008 Roadster and the first Model S use induction motors?
An induction motor has no magnets: the rotor is laminated steel with conducting bars shorted by end rings, and the stator field induces the rotor current through slip. That avoided rare-earth cost and supply risk and any demagnetization limit, and the rotor is very robust at high speed. With the inverter off there is no rotor field, so a fault at speed cannot generate uncontrolled voltage and the motor freewheels with little drag. Tesla made it efficient enough with copper rotor bars, liquid cooling and careful inverter control.
screenWhat is an IPM-SynRM, and why did Tesla use one for the Model 3's rear motor?
It is an interior permanent magnet motor whose rotor also has flux barriers, so it makes magnet torque plus reluctance torque from the steel trying to align with the stator field. The magnets supply the rotor field without any magnetizing current, so efficiency is high at light load, which is where a car spends most of its highway driving. The reluctance contribution lets designers use less magnet and gives a wide field-weakening range for power at high speed. The costs are magnet supply risk, a demagnetization limit at high temperature, and drag from the magnets when the motor spins unpowered.
deepWhy does the Model S Plaid's rotor need a carbon-fiber sleeve, and how does that raise power?
Power is torque times speed, and torque is set by rotor size and current, so spinning faster is the cheapest way to get more power from the same size of machine. Centrifugal hoop stress grows with the square of speed; at about 20,000 rpm the surface of a rotor 140 mm across moves at roughly 147 m/s, enough to tear magnets and thin steel bridges loose. A carbon-fiber sleeve wound under tension pre-loads the rotor so it stays together, and because it is non-magnetic and far less conductive than metal it adds little eddy-current loss. The trade-offs are heat, since the sleeve insulates the rotor while the magnets must stay below their demagnetization temperature, and a slightly larger magnetic gap.
deepHow would you sanity-check the second-generation Roadster's announced numbers?
First label them correctly: they are claims from the November 2017 announcement, the car was promised for 2020 and has been delayed repeatedly, so I would check Tesla's site for its current status before quoting them. Then test them with physics. 0-60 mph in 1.9 s means reaching 26.8 m/s in 1.9 s, an average of about 14 m/s² or 1.44 g, at or beyond the grip limit of road tires. A 200 kWh pack at 160-200 Wh/kg would weigh 1,000-1,250 kg, and 620 miles from 200 kWh implies about 320 Wh per mile, plausible for a fast, heavy car. So the range claim is physically consistent, while the acceleration claim depends on tires, the launch surface and the proposed thrusters.
screenWhat is field weakening, and why does it give a motor a constant-power region?
A motor's back-EMF rises with speed, and once it reaches what the inverter can produce from the DC bus, no more current can be pushed in to make torque. The controller then drives current that opposes the rotor field: negative d-axis current in a permanent-magnet machine, or less magnetizing current in an induction machine, which keeps the back-EMF within the bus voltage. Torque then falls roughly as 1/speed, so power stays roughly constant until losses, current limits or breakdown torque take over. That wide constant-power band is why a single fixed gear can cover a car's whole speed range.

Quiz

1. What kind of motor drove the 2008 Tesla Roadster?
2. The 2008 Roadster's 53 kWh pack was built from
3. Why are the Model S Plaid's permanent-magnet rotors wrapped in a carbon-fiber sleeve?
4. Which statement about the second-generation Roadster's 0-60 mph time of 1.9 s is accurate?
5. Why is an induction motor a good choice for a part-time front motor?
6. What does a hairpin stator winding improve?
7. The Model 3's traction inverter switches with

References and further reading

Where the ideas in this lesson come from, and what to read next. Books are the standard texts; papers are the original sources; standards are what employers work to.

  1. Book

    Austin Hughes and Bill Drury (2019). Electric Motors and Drives: Fundamentals, Types and Applications. Newnes, 5th edition.

    Read: Induction versus PM machines, to judge Tesla's choices.

  2. Book

    J. R. Hendershot and T. J. E. Miller (2010). Design of Brushless Permanent-Magnet Machines. Motor Design Books.

    Read: Rotor construction and magnet retention.

  3. Reportfree online

    Tim A. Burress et al., Oak Ridge National Laboratory (2011). Evaluation of the 2010 Toyota Prius Hybrid Synergy Drive System. ORNL/TM-2010/253.

    Read: How a lab benchmarks a drive unit, the way teardown reports judge Tesla's.

  4. Book

    James Larminie and John Lowry (2012). Electric Vehicle Technology Explained. Wiley, 2nd edition.

    Read: The vehicle-level context.