Mechanical Advantage Calculator – Simple Machines, Effort and Efficiency
Mechanical advantage is the factor by which a machine multiplies the force you put into it. Push a 200 kg crate straight up and you fight its full weight; roll it up a five-metre ramp that rises a metre and a quarter and you only fight a quarter of it. Nothing is created in that bargain. The machine simply trades force for distance under the rule that governs every one of them, F_effort × d_effort = F_load × d_load. This calculator covers all six classical simple machines — lever, pulley system, wheel and axle, inclined plane, wedge and screw — plus compound machines built by chaining them together.
Ideal advantage comes from geometry alone
The ideal mechanical advantage (IMA) is what a frictionless version of the machine would deliver, and it can be read straight off the dimensions. For a lever it is effort arm ÷ load arm; for a pulley system it is the number of rope strands supporting the movable block; for a wheel and axle it is R ÷ r; for a ramp it is L ÷ h, which is the same statement as 1 ÷ sin θ; for a wedge it is L ÷ t; and for a screw it is 2πR ÷ P. A crowbar with a 2.4 m effort arm against a 0.6 m load arm has an IMA of 4, so a 300 N load yields under 75 N of effort — and the torques balance at 180 N·m on both sides.
Actual advantage comes from measured force
The actual mechanical advantage (AMA) is simply F_load ÷ F_effort with real forces on a real machine. It is always smaller than the IMA, because friction takes its cut. The ratio between the two is the efficiency: η = AMA ÷ IMA = W_out ÷ W_in. A block and tackle with four supporting strands has an IMA of 4, but at 85 % efficiency lifting 800 N costs 200 ÷ 0.85 = 235.29 N of pull rather than 200 N, giving an AMA of 3.4. Check it the other way and the numbers close: the load rises 0.5 m for 400 J of output while you haul 2 m of rope for 470.59 J of input, and 400 ÷ 470.59 is 0.85 again.
Advantage below 1 is a feature, not a fault
A Class 3 lever puts the effort between the fulcrum and the load, so the effort arm is the shorter one and the advantage drops below 1. Your forearm is the standard example: the biceps inserts about 0.05 m from the elbow while the hand sits 0.35 m out, giving an MA of 0.1429. Holding 50 N in your palm therefore costs 350 N of muscle tension. What you buy is speed and range — a small, strong contraction near the joint sweeps the hand a long way, quickly. Tweezers, fishing rods and the human jaw all make the same trade.
Friction, ramps and why screws leak energy
When a coefficient of friction is known, efficiency follows from first principles rather than from a guess. On a ramp the useful component of weight is W·sin θ while friction adds μ·W·cos θ, so η = sin θ ÷ (sin θ + μ·cos θ). A 5 m ramp rising 1.25 m sits at 14.4775°, and at μ = 0.20 it runs at only 56.35 % efficiency: a 200 kg crate needs 870.14 N to push rather than the ideal 490.33 N. Screws are worse still. A jackscrew with a 0.40 m handle and a 5 mm lead has an IMA of 502.65, but the effort travels 2.51 m of circumference for every 5 mm of lift, sliding thread on thread the whole way. At 30 % efficiency a 120 N push still delivers 18.1 kN — enormous, yet most of the work became heat.
Compound machines multiply both ways
Chain machines in series and the ideal advantages multiply — but so do the efficiencies. Two stages of IMA 4 give a total IMA of 16, and two stages at 85 % give 0.85 × 0.85 = 0.7225, or 72.25 %. A 50 N effort therefore delivers 578 N rather than the ideal 800 N. Losses compound rather than average, which is why practical hoists and gear trains use the fewest stages that will do the job.
Whichever machine you choose, the calculator reports the IMA, the AMA, the efficiency, the required effort or delivered load, the velocity ratio and the full work ledger, then verifies the answer a second way through torque balance or conservation of work. When both routes agree, the result is sound.