Four fundamental physical quantities describe the behaviour of mechanical systems: force, torque, speed, and power. Mastery of their definitions, units, interrelationships, and calculations is essential for analysing and designing mechanical systems in VCE Systems Engineering.
KEY TAKEAWAY: Force is the push/pull on an object; torque is the rotational equivalent of force; speed describes how fast motion occurs; power is the rate at which work (energy) is transferred.
Force (\(F\)) is a push or pull that causes, or tends to cause, a change in motion.
| Symbol | Quantity | SI Unit |
|---|---|---|
| \(F\) | Force | Newton (N) |
| \(m\) | Mass | kilogram (kg) |
| \(a\) | Acceleration | m/s² |
In static mechanical systems (no acceleration), the forces are in equilibrium:
\$\(\sum F = 0\)\$
Worked example:
A 20 kg object rests on a surface. What force must a lever exert to lift it?
\$\(F_{load} = mg = 20 \times 9.8 = 196 \text{ N}\)\$
EXAM TIP: Always use \(g = 9.8\) m/s² (or 10 m/s² if the question specifies) when converting mass to weight force.
Torque (\(\tau\)) is the rotational equivalent of force — it is the turning effect of a force about a pivot point.
where:
- \(\tau\) = torque (N·m)
- \(F\) = force applied (N)
- \(d\) = perpendicular distance from the pivot to the line of action of the force (m)
Principle of moments (equilibrium):
\$\(\tau_{clockwise} = \tau_{anticlockwise}\)\$
Worked example:
A spanner applies 25 N at 0.3 m from the bolt centre.
\$\(\tau = 25 \times 0.3 = 7.5 \text{ N·m}\)\$
If a second force of 15 N acts on the other side at distance \(d\):
\(\$15 \times d = 7.5 \quad \Rightarrow \quad d = 0.5 \text{ m}\)\$
VCAA FOCUS: Torque in gear systems: when a gear reduces speed, it multiplies torque proportionally (and vice versa). This is directly related to the gear ratio.
Torque in gear trains:
If gear ratio \(GR = T_{driven}/T_{driver}\):
\$\(\tau_{driven} = \tau_{driver} \times GR \quad (\text{ignoring losses})\)\$
A 3:1 reduction gear triples the output torque.
In mechanical systems, two types of speed are used:
Linear speed (\(v\)): Distance per unit time
\$\(v = \frac{d}{t} \quad \text{(m/s or m/min)}\)\$
Rotational speed (\(N\)): Revolutions per minute (rpm) or radians per second
Relationship between linear and rotational speed:
\$\(v = \omega r = \frac{2\pi N r}{60}\)\$
where \(r\) = radius (m), \(N\) = speed in rpm, \(\omega\) = angular velocity (rad/s).
Worked example:
A pulley of diameter 0.2 m rotates at 300 rpm. Find the belt speed.
\$\(r = 0.1 \text{ m}, \quad v = \frac{2\pi \times 300 \times 0.1}{60} = \frac{60\pi}{60} = \pi \approx 3.14 \text{ m/s}\)\$
Speed in gear trains:
\$\(\frac{N_{driver}}{N_{driven}} = \frac{T_{driven}}{T_{driver}}\)\$
A step-up gear train increases output speed; a step-down increases output torque.
REMEMBER: Speed and torque trade off against each other in a gear train. The product (power) is approximately constant (minus losses).
Power (\(P\)) is the rate at which work is done or energy is transferred:
For rotational systems:
\$\(P = \tau \times \omega = \frac{2\pi N \tau}{60}\)\$
| Symbol | Quantity | SI Unit |
|---|---|---|
| \(P\) | Power | Watt (W) |
| \(W\) | Work | Joule (J) |
| \(t\) | Time | second (s) |
| \(\tau\) | Torque | N·m |
| \(\omega\) | Angular velocity | rad/s |
Worked example:
A motor produces 8 N·m of torque at 1500 rpm. Find the power output.
\$\(\omega = \frac{2\pi \times 1500}{60} = 50\pi \approx 157 \text{ rad/s}\)\$
\$\(P = 8 \times 157 = 1257 \text{ W} \approx 1.26 \text{ kW}\)\$
COMMON MISTAKE: Forgetting to convert rpm to rad/s before using \(P = \tau\omega\). Always convert: \(\omega = 2\pi N/60\).
These relationships mean that when a gear train reduces speed (smaller \(\omega\)), torque (\(\tau\)) increases proportionally to maintain constant power (minus losses).
A machine requires 50 N·m torque at 200 rpm. The motor provides 10 N·m at 1000 rpm.
Required gear ratio:
\$\(GR = \frac{1000}{200} = 5:1 \text{ reduction}\)\$
Torque check (ideal):
\$\(\tau_{out} = 10 \times 5 = 50 \text{ N·m} \checkmark\)\$
Power check:
\$\(P_{motor} = \frac{2\pi \times 1000 \times 10}{60} = 1047 \text{ W}\)\$
\$\(P_{output} = \frac{2\pi \times 200 \times 50}{60} = 1047 \text{ W} \checkmark \text{ (ideal)}\)\$
APPLICATION: When selecting a motor for a system, calculate the required torque and speed at the output, then work backwards through the drive train using gear ratios to determine what the motor must provide.
| Quantity | Unit | Conversion |
|---|---|---|
| Force | N | 1 kgf ≈ 9.8 N |
| Torque | N·m | — |
| Linear speed | m/s | 1 km/h = 1/3.6 m/s |
| Rotational speed | rpm or rad/s | \(\omega = 2\pi N/60\) |
| Power | W (Watt) | 1 kW = 1000 W |