F = m · a
Force is proportional to mass and acceleration; friction and opposing forces must be added separately.
Force is proportional to mass and acceleration; friction and opposing forces must be added separately.
Select a target and calculate.
Force is proportional to mass and acceleration; friction and opposing forces must be added separately.
100 kg · 10 m/s² = 1,000 N.
Straight-line translation; weight, friction and drag are excluded.
This calculator finds the missing quantity among force F, mass m and acceleration a from the other two, based on Newton's second law. It explains the difference between mass and weight force and shows why F always refers to the resultant (net) force.
By Newton's second law, the resultant force acting on a body is proportional to its mass and the acceleration it produces: F = m·a. When several forces act at once, F is the vector sum of all individual forces.
An empty and a fully loaded shopping cart push differently: to reach the same acceleration, the heavier, fully loaded cart needs a considerably larger force, because its mass is greater.
F = m · a
F = m · am = F / aa = F / m| Symbol / input | Meaning |
|---|---|
| Resultant force F | The total net force acting along the direction of motion – the sum of all individual forces that actually accelerate the body (opposing forces such as friction are already subtracted). Source: a force measurement (load cell, spring scale), or, when it is the unknown, from m·a. Positive along the positive axis. |
| Mass m | The inertial mass of the body – how much matter must be accelerated, independent of its weight at a given location. Source: weigh it on a scale, or take it from a drawing/parts list; include attachments or payload only if they move along with it. |
| Acceleration a | The rate of change of velocity in the same direction as F. Source: a measurement (accelerometer, or Δv/Δt from two speeds), a design specification, or as the result of F/m. Positive along the direction of motion, negative against it. |
Enter two of the three quantities. Force requires mass and acceleration, mass requires force and acceleration, acceleration requires force and mass. F denotes the resultant force in the direction of motion, not necessarily a single applied force.
Select the target quantity and enter the two known values with units. If several forces act on the body (e.g. drive force and friction), first form their vector sum along the direction of motion before entering the result as F.
Given m = 100 kg and a = 10 m/s², substitution gives F = 100 kg · 10 m/s² = 1,000 N. This is the resultant net force needed to accelerate the 100 kg mass at 10 m/s²; opposing forces such as friction would additionally need to be overcome.
A resultant force of 1,000 N means the 100 kg mass experiences an acceleration of 10 m/s² under this net force. If the actual drive force applied is larger than 1,000 N, the difference is absorbed by opposing forces such as friction or drag.
The SI unit of force is the newton (N = kg·m/s²). Larger forces are given in kN; lbf is common in the US, with 1 lbf equal to about 4.448 N.
F = m·a is used to design drives, brakes, conveyor systems, vehicle acceleration, and to estimate dynamic loads in structural mechanics.
The formula applies to the resultant force on a body of constant mass at non-relativistic speeds. If mass changes during the process (e.g. a rocket losing propellant), the more general momentum form F = dp/dt is required. Rotational motion additionally needs the corresponding torque equation.
Common mistake: Do not confuse mass and weight force: weight force is itself a force (weight force = m·g) and must not be substituted directly as mass in F = m·a. Also, F is the resultant of all individual forces, not automatically a single applied force such as a drive or pull force.
Only if gravity is the sole force acting, with no other forces such as buoyancy or friction present. In general, F is the vector sum of all forces acting.
Then the resultant (net) force must first be found by vector addition of all individual forces, before applying F = m·a.
Near the speed of light, the classical form no longer holds exactly; at the much lower speeds of everyday engineering it remains an excellent approximation.