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Work, Energy & Power

Work\u2013Energy Theorem Calculator

Apply the work\u2013energy theorem to find net work from speed change, final speed from work input, braking distance from friction, or average force over a distance. Includes step-by-step solutions and unit conversions.

Interactive calculator

Work\u2013Energy Theorem Calculator

Apply the work\u2013energy theorem: W = \u0394KE. Find net work from speed change, final speed from work input, braking distance from friction, or average force over a distance.

Try an example

Mass of the object

Speed at start

Speed at end

Your result will appear here.

Choose a calculation mode, fill in the known values, and click Calculate.

Quick Guide

  • Choose a mode: find net work, final speed, work needed, braking distance, or average force.
  • Enter known values with units.
  • Click Calculate for step-by-step result.

Key Takeaways

  • The work–energy theorem states: net work done on an object equals its change in kinetic energy.
  • Wₙₑₜ = ½m(v₂² − v₁²) connects force, displacement, and speed change.
  • Positive work increases speed; negative work decreases speed.
  • Braking distance d = v²/(2μg) — mass cancels out, and doubling speed quadruples distance.
  • The theorem applies even when multiple forces act simultaneously.
  • It provides a shortcut to kinematics problems without needing acceleration explicitly.
  • Average force can be found from F = W/d when work and distance are known.

What Is the Work–Energy Theorem?

The work–energy theorem is one of the most powerful principles in classical mechanics. It states that the net work done on an object by all forces equals the change in its kinetic energy. This bypasses the need to calculate acceleration, making it ideal for problems where you know forces, distances, and speeds but not time or acceleration.

It is derived directly from Newton’s second law (F = ma) combined with the definition of work (W = Fd). The result connects the world of forces to the world of energy.

Net Work Equals Change in KE

Wnet=KE2KE1=12m(v22v12)W_{net} = KE_2 - KE_1 = \tfrac{1}{2}m(v_2^2 - v_1^2)

Where m is the mass of the object, v1 is the initial speed, and v2 is the final speed. When Wnet > 0, the object accelerates. When Wnet < 0, the object decelerates.

Work–Energy Theorem: W = ΔKE

mv₁KE₁ = ½mv₁²Fₙₑₜdmv₂KE₂ = ½mv₂²W = KE₂ − KE₁

Finding Final Speed from Work

v2=v12+2Wmv_2 = \sqrt{v_1^2 + \frac{2W}{m}}

Rearranging the theorem to solve for the final speed. The quantity under the square root must be non-negative — if the work removed exceeds the initial kinetic energy, the object stops before that work is fully done.

Braking Distance from Friction

d=v22μgd = \frac{v^2}{2\mu g}

When friction (μmg) is the only horizontal force, the work–energy theorem gives this compact braking formula. Notice that mass cancels — stopping distance depends only on initial speed, the friction coefficient, and gravity. Doubling speed quadruples the stopping distance.

Average Force from Work and Distance

Favg=WnetdF_{avg} = \frac{W_{net}}{d}

When you know the net work (from the speed change) and the distance, you can find the average net force that acted on the object. This is essential in crash analysis, ballistics, and impact engineering.

How to Use the Calculator

  1. Select a mode: find net work, final speed, work needed, braking distance, or average force.
  2. Enter known values with appropriate units.
  3. Click Calculate.
  4. Review the result, step-by-step solution, and interpretation.

Example Calculations

Car: 1500 kg, 0 to 60 km/h

W = ½ × 1500 × (16.67² − 0²) ≈ 208,400 J ≈ 208.4 kJ

Braking: 100 km/h, μ = 0.7

d = (27.78)² / (2 × 0.7 × 9.807) ≈ 56.3 m

Runner: 70 kg, 0 to 8 m/s

W = ½ × 70 × 64 = 2,240 J

Crash: 1200 kg, 50 km/h to 0 in 0.8 m

F = [½ × 1200 × 13.89²] / 0.8 ≈ 144,700 N ≈ 145 kN

Common Mistakes

  • Using total force instead of net force. Only the net force determines the change in KE.
  • Forgetting that KE uses speed (magnitude), not velocity. KE is always ≥ 0.
  • Assuming braking distance scales linearly with speed — it scales with speed squared.
  • Ignoring unit conversions (km/h to m/s) when substituting into formulas.
  • Applying the theorem to systems with internal energy changes (deformation, heat) without accounting for them.

Accuracy and Limitations

The work–energy theorem assumes point-particle or rigid-body dynamics. For deformable objects (crashes, collisions), internal energy dissipation must be considered separately. Braking distance assumes a flat surface with constant friction coefficient; real-world conditions (tyre temperature, road camber, ABS pulsing) alter the result. This tool is educational and should not replace professional engineering analysis.

FAQ

What is the work–energy theorem?

It states that the net work done on an object equals the change in its kinetic energy: W_net = KE_final − KE_initial = ½m(v₂² − v₁²).

How is the work–energy theorem different from W = Fd?

W = Fd calculates work from a single force. The work–energy theorem uses the net work from all forces and directly relates it to the change in kinetic energy.

Can the work–energy theorem give negative work?

Yes. When the object slows down, its final KE is less than its initial KE, so net work is negative. This typically happens when friction or braking forces oppose motion.

Why does mass cancel in the braking distance formula?

Both kinetic energy (½mv²) and friction force (μmg) are proportional to mass, so mass cancels when you solve d = v²/(2μg).

Does the work–energy theorem work for curved paths?

Yes. The theorem relates total work to kinetic energy change regardless of the path shape. The net work is the integral of the net force dot displacement along the path.

What units does the theorem use?

In SI: work in joules (J), mass in kilograms (kg), and velocity in metres per second (m/s). The calculator handles unit conversions automatically.

How is braking distance related to speed?

Braking distance is proportional to the square of speed: d = v²/(2μg). Doubling your speed quadruples the stopping distance.

Can I use this for rotational motion?

The translational form W = ΔKE applies to linear motion. For rotation, the analogous theorem is W = ΔKE_rot = ½I(ω₂² − ω₁²), which requires a rotational calculator.

Sources

Manish Kumar

Author & technical reviewer

Manish Kumar

PhysicsCalcs tools are reviewed with an educational focus: clear formulas, transparent assumptions, and practical context for students and science learners.

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