Potential Energy Calculator

Gravitational and elastic potential energy with AI-powered step-by-step solutions
Find the gravitational potential energy gained by a 5.0 kg box raised 3.0 m
A spring with k = 250 N/m is compressed 12 cm. Find the stored elastic energy.
A 0.50 kg ball is dropped from 20 m. Find its speed just before landing.
How high must a 2 kg mass be lifted to store 100 J?

Gravitational Potential Energy

Potential energy is energy stored by an object's position or configuration. Near the Earth's surface, lifting a mass stores

PEg=mghPE_g = mgh

Symbols and SI units:

  • PEgPE_g — gravitational potential energy, joules (J)
  • mm — mass, kilograms (kg)
  • gg — gravitational field strength, 9.819.81 m/s² at the Earth's surface
  • hh — height above the chosen reference level, metres (m)

Only the change in PEPE has physical meaning, so you are free to put h=0h = 0 wherever it is convenient — the floor, the table top, the ground. Different choices shift every value by the same constant and change no answer.

When it applies: mghmgh assumes gg is constant, which holds while hh is small compared with the Earth's radius. For satellite-scale heights use U=GMm/rU = -GMm/r instead.

The assumption people forget: hh is the vertical rise only. Dragging a box 1010 m up a ramp that climbs 22 m stores mg(2 m)mg(2\ \text{m}), not mg(10 m)mg(10\ \text{m}).

Elastic Potential Energy and Conservation

A stretched or compressed spring stores

PEe=12kx2PE_e = \tfrac{1}{2}kx^2

  • kk — spring constant, newtons per metre (N/m)
  • xx — extension or compression from the natural length, metres (m)

Because xx is squared, stretching and compressing by the same amount store the same energy, and doubling the stretch stores four times as much.

Conservation of mechanical energy ties potential energy to motion. With no friction or air resistance,

PEi+KEi=PEf+KEfPE_i + KE_i = PE_f + KE_f

so a mass falling from rest through a height hh arrives at v=2ghv = \sqrt{2gh}, independent of its mass.

When it applies: 12kx2\tfrac{1}{2}kx^2 needs a spring obeying Hooke's law, F=kxF = kx, within its elastic limit. Conservation needs only conservative forces; friction dissipates energy as heat and breaks the balance.

The assumption people forget: xx is measured from the unstretched length, not from the floor or from any other datum.

Common Mistakes to Avoid

  • Using the distance travelled as hh — only the vertical component counts.
  • Forgetting gg — a 55 kg box raised 33 m stores 147147 J, not 1515 J.
  • Using weight in newtons as mm — divide by gg first to get kilograms.
  • Measuring the spring extension from the wrong origin — it must be from the natural length.
  • Halving after squaring in 12kx2\tfrac{1}{2}kx^2, or squaring kk — only xx is squared.
  • Leaving xx in centimetres1212 cm is 0.120.12 m; forgetting this changes the answer by 1000010\,000.
  • Applying energy conservation with friction present — subtract the energy lost to friction, or the final speed comes out too high.
  • Thinking a negative PEPE is an error — below the reference level it simply is negative.

Examples

Step 1: PEg=mghPE_g = mgh
Step 2: PEg=(5.0 kg)(9.81 m/s2)(3.0 m)PE_g = (5.0\ \text{kg})(9.81\ \text{m/s}^2)(3.0\ \text{m})
Step 3: PEg=147.15 kg\cdotpm2/s2PE_g = 147.15\ \text{kg·m}^2/\text{s}^2
Step 4: PEg147 JPE_g \approx 147\ \text{J}
Answer: PEg147PE_g \approx 147 J

Step 1: Convert: x=12 cm=0.12 mx = 12\ \text{cm} = 0.12\ \text{m}
Step 2: PEe=12kx2=12(250 N/m)(0.12 m)2PE_e = \tfrac{1}{2}kx^2 = \tfrac{1}{2}(250\ \text{N/m})(0.12\ \text{m})^2
Step 3: (0.12 m)2=0.0144 m2(0.12\ \text{m})^2 = 0.0144\ \text{m}^2
Step 4: PEe=12(250 N/m)(0.0144 m2)=1.8 N\cdotpm=1.8 JPE_e = \tfrac{1}{2}(250\ \text{N/m})(0.0144\ \text{m}^2) = 1.8\ \text{N·m} = 1.8\ \text{J}
Answer: PEe=1.8PE_e = 1.8 J

Step 1: PEgPE_g at the top =mgh=(0.50 kg)(9.81 m/s2)(20 m)=98.1 J= mgh = (0.50\ \text{kg})(9.81\ \text{m/s}^2)(20\ \text{m}) = 98.1\ \text{J}
Step 2: All of it converts to kinetic energy: 12mv2=98.1 J\tfrac{1}{2}mv^2 = 98.1\ \text{J}
Step 3: v=2gh=2(9.81 m/s2)(20 m)=392.4 m2/s2v = \sqrt{2gh} = \sqrt{2(9.81\ \text{m/s}^2)(20\ \text{m})} = \sqrt{392.4\ \text{m}^2/\text{s}^2}
Step 4: v=19.8 m/sv = 19.8\ \text{m/s} — the mass cancels, so any dropped object reaches the same speed
Answer: v19.8v \approx 19.8 m/s (with PEg=98.1PE_g = 98.1 J released)

Frequently Asked Questions

For gravitational potential energy multiply mass, gravity and height: PE = mgh, with m in kg, g = 9.81 m/s² and h in metres, giving joules. For a spring use PE = ½kx², with k in N/m and x the stretch from the natural length in metres.

PE = mgh near the Earth's surface, where h is the vertical height above whatever reference level you choose. Only changes in PE matter, so the choice of reference level never affects the final answer.

Yes. If an object sits below the reference level you picked, mgh is negative, which simply says energy would be released getting it there. The gravitational form U = −GMm/r used for orbits is negative by convention everywhere.

Set the potential energy lost equal to the kinetic energy gained: mgh = ½mv², so v = √(2gh). The mass cancels, which is why a heavy and a light ball dropped from 20 m both arrive at about 19.8 m/s in the absence of air resistance.

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