Net Force Calculator
Calculate net force using F = ma or vector sum of up to 3 force vectors. Includes direction, equilibrium check, free body diagram, and force vector chart.
Net Force
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N
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Direction (°)
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Net Fx (N)
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Net Fy (N)
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Balanced?
Force Vector Diagram
Free Body Diagram
Calculation Steps
Enter values and press Calculate to see steps.
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How to use this calculator
F = ma tab: Enter mass and acceleration to find net force directly from Newton’s second law. Negative acceleration means the net force opposes motion.
Vector Sum tab: Enter up to three forces with their magnitudes (N) and directions (degrees from positive x-axis, counterclockwise). The calculator adds the vector components and finds the resultant net force magnitude and direction.
Example: two forces at right angles
Force 1: 30 N at 0° (east). Force 2: 40 N at 90° (north). Net Fₓ = 30, Net Fᵧ = 40. |F_net| = √(30² + 40²) = 50 N at arctan(40/30) = 53.1° (northeast).
What is net force?
Net force is the vector sum of all forces acting on an object. When multiple forces act simultaneously, they do not cancel each other out unless they are equal and opposite. The net force determines the object’s acceleration through Newton’s second law.
If F_net = 0, the object is in equilibrium: it either remains at rest or moves at constant velocity (Newton’s first law). This is called a balanced force situation.
If F_net ≠ 0, the object accelerates in the direction of the net force. This is an unbalanced force situation.
Free body diagrams
A free body diagram (FBD) is a visual tool for identifying all forces on an object and determining the net force. Rules for drawing an FBD:
- Represent the object as a simple shape (usually a box or dot)
- Draw arrows for each force, with arrow length proportional to force magnitude
- Label each arrow with the force name and magnitude
- Choose a coordinate system and resolve diagonal forces into components
- Sum components in each direction to find net force components
Common forces in FBDs:
- Weight (W = mg): Always points straight down
- Normal force (N): Perpendicular to the contact surface
- Tension (T): Along a rope or string, away from the object
- Friction (f): Along the surface, opposing motion
- Applied force (F_a): In the direction applied
Adding force vectors: components method
When forces are not along the same line, add them using components:
- Resolve each force into x and y components: Fₓ = F cos θ, Fᵧ = F sin θ
- Sum all x-components: ΣFₓ = F₁cos θ₁ + F₂cos θ₂ + …
- Sum all y-components: ΣFᵧ = F₁sin θ₁ + F₂sin θ₂ + …
- Find magnitude: |F_net| = √(ΣFₓ² + ΣFᵧ²)
- Find direction: θ = arctan(ΣFᵧ / ΣFₓ)
Three forces on an object:
F₁ = 50 N at 0°: Fₓ = 50, Fᵧ = 0 F₂ = 30 N at 120°: Fₓ = 30cos120° = -15, Fᵧ = 30sin120° = 25.98 F₃ = 20 N at 240°: Fₓ = 20cos240° = -10, Fᵧ = 20sin240° = -17.32
ΣFₓ = 50 - 15 - 10 = 25 N ΣFᵧ = 0 + 25.98 - 17.32 = 8.66 N |F_net| = √(25² + 8.66²) = 26.46 N at arctan(8.66/25) = 19.1°
Equilibrium and net force = 0
When the net force on an object is zero, it is in static or dynamic equilibrium. Newton’s first law states that an object remains at rest or in uniform motion unless acted upon by a net force.
Static equilibrium: Object is at rest, net force = 0 and net torque = 0. Example: a book resting on a table, a bridge under load.
Dynamic equilibrium: Object moves at constant velocity, net force = 0. Example: a car driving at constant speed on a level road (thrust = drag + friction), a skydiver at terminal velocity.
For an object on an inclined plane in equilibrium: the component of gravity along the plane must equal the friction force. If the plane is too steep, gravity along the plane exceeds maximum static friction and the object slides.
Net force in circular motion
An object moving in a circle at constant speed has a changing velocity (direction changes), so it has acceleration. This centripetal acceleration requires a net force directed toward the center:
This centripetal net force is not a new type of force: it is always provided by an existing force. For a satellite, gravity provides the centripetal force. For a car on a curved road, friction provides it. For a ball on a string, tension provides it.
If the centripetal force is removed (the string breaks), the object moves in a straight line tangent to the circle, not outward as the “centrifugal force” intuition suggests.
Net force in structural engineering
Structural engineers ensure that buildings, bridges, and machines are in equilibrium under all expected loads. The sum of all forces and torques must equal zero for a static structure.
Load combinations: A bridge must support its own weight (dead load), traffic (live load), and environmental forces (wind, seismic, temperature expansion). Engineers calculate the net force on each structural member and size it to handle those forces with appropriate safety factors.
Safety factors: Structures are not designed to just barely achieve equilibrium. Safety factors of 1.5 to 3 (sometimes higher for critical applications) multiply the expected forces to account for material variations, unexpected loads, and degradation over time.
Redundancy: Modern structural design incorporates multiple load paths so that if one member fails, forces redistribute rather than causing progressive collapse.
Net force and Newton’s laws summary
Newton’s First Law (Inertia): An object remains at rest or in uniform motion unless F_net ≠ 0. Net force is the condition that changes motion.
Newton’s Second Law: F_net = ma. The net force determines the acceleration. This is the quantitative link between net force and motion change.
Newton’s Third Law: For every action (force), there is an equal and opposite reaction. Net force on a system includes only external forces; internal action-reaction pairs cancel.
These three laws, plus the ability to add force vectors to find net force, form the foundation of classical mechanics. Every problem in Newtonian dynamics reduces to: identify all forces, find the net force vector, and apply F_net = ma.
Frequently Asked Questions
What is net force?
Net force is the vector sum of all forces acting on an object. When multiple forces act simultaneously, you add their components: sum all x-components for the total horizontal force and all y-components for the total vertical force, then use the Pythagorean theorem to find the resultant magnitude. If net force equals zero, the object is in equilibrium.
What is the difference between balanced and unbalanced forces?
Balanced forces have a net force of zero. The object remains at rest or continues moving at constant velocity (Newton's First Law). Unbalanced forces produce a non-zero net force, which causes acceleration in the direction of the net force. For example, a book on a table has balanced forces: gravity pulls it down and the normal force pushes it up equally.
How does net force relate to acceleration?
Newton's Second Law states F_net = m × a. A larger net force on the same mass produces greater acceleration. Doubling the net force doubles the acceleration. The direction of acceleration always matches the direction of net force. If net force is zero, acceleration is zero and velocity stays constant.
How do you add force vectors?
To add force vectors, resolve each force into x and y components using trigonometry: Fx = F × cos(θ), Fy = F × sin(θ), where θ is the angle from the positive x-axis. Sum all x-components to get the total Fx, and all y-components for total Fy. The resultant magnitude is √(Fx² + Fy²) and the angle is atan2(Fy, Fx).
What is net force in equilibrium?
In static equilibrium, the net force and net torque are both zero. All forces balance: ΣFx = 0 and ΣFy = 0. This means the object does not accelerate linearly. A suspension bridge cable, a hanging sign, or a book on a shelf are all in static equilibrium because each force is balanced by equal and opposite forces.
What does Newton's First Law say about net force?
Newton's First Law states that an object at rest stays at rest, and an object in motion stays in motion at constant velocity, unless acted upon by a net external force. This is the law of inertia. Zero net force means no change in motion state. Any change in speed or direction requires a non-zero net force.
What are everyday examples of net force?
A car accelerating: the engine thrust minus road friction is the net force. A skydiver reaching terminal velocity: gravity and air drag balance, net force = 0. Pushing a box that does not move: your push and static friction cancel. A soccer ball being kicked: the foot applies force, net force accelerates the ball. A satellite in orbit: gravity provides the net centripetal force.
How do you draw a free body diagram?
Represent the object as a simple shape (dot or box). Draw each force as an arrow pointing in its direction, originating from the object. Label each arrow with the force name and magnitude. Common forces include weight (down), normal force (perpendicular to surface), friction (opposing motion), tension (along rope), and applied force. The net force is the vector sum of all arrows.
What is net force in circular motion?
In circular motion, there is always a net centripetal force directed toward the center of the circle. This net force causes the direction of velocity to change continuously even if speed is constant. The magnitude is F_c = m × v² / r = m × ω² × r. For a car turning, friction provides this centripetal net force. For a satellite, gravity provides it.
How does net force change on an inclined plane?
On an inclined plane at angle θ, weight W = mg acts downward. The component along the slope is W sin(θ), and the component perpendicular to the slope is W cos(θ). The normal force N = W cos(θ). If friction force f = μN, the net force along the slope is W sin(θ) - μ × W cos(θ) = mg(sin θ - μ cos θ). A steeper angle increases the driving force and reduces the normal force.
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