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.
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.
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.
- 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.
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.
| Machine | Peak power | Assumed active mass |
|---|---|---|
| A: Roadster-era induction | 185 kW | 52 kg |
| B: Model S Performance-era copper-rotor induction | 310 kW (416 hp) | 75 kg |
| C: IPM-SynRM | 200 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?
(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·mAnswer: 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?
screenWhat is an IPM-SynRM, and why did Tesla use one for the Model 3's rear motor?
deepWhy does the Model S Plaid's rotor need a carbon-fiber sleeve, and how does that raise power?
deepHow would you sanity-check the second-generation Roadster's announced numbers?
screenWhat is field weakening, and why does it give a motor a constant-power region?
Quiz
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.
- 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.
- 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.
- Reportfree online
Read: How a lab benchmarks a drive unit, the way teardown reports judge Tesla's.
- Book
James Larminie and John Lowry (2012). Electric Vehicle Technology Explained. Wiley, 2nd edition.
Read: The vehicle-level context.