Energy Is Conserved as It Changes Form
Atlas stands at the top of a roller coaster hill, holding a clipboard and pointing downward at a cart poised at the peak, with a twisting track stretching below through loops and valleys, illustrating the moment before a dramatic energy transformation.
- Explain what it means for a system to be isolated and why total energy is constant within one.
- Identify how energy converts between kinetic, potential, and thermal forms during motion.
- Calculate kinetic and gravitational potential energy using KE = ½mv² and PE = mgh.
- Predict how the speed of an object changes as it moves between different heights in an isolated system.
- Compare ideal (frictionless) and real systems in terms of energy conservation and thermal losses.
Key terms
- Isolated system
- A system that exchanges neither matter nor energy with its surroundings, so its total energy is constant.
- Mechanical energy
- The sum of an object's kinetic and gravitational potential energy at a given moment.
- Conservative force
- A force such as gravity whose work depends only on start and end positions, allowing potential energy to be defined.
- Thermal energy
- The internal random kinetic energy of molecules, which friction generates from organized mechanical energy.
- Energy transformation
- The conversion of energy from one form to another without any change in the total amount.
The Work-Energy Foundation
Conservation of mechanical energy follows from the work-energy theorem, which states that the net work done on an object equals its change in kinetic energy. When the only force doing work is gravity, that work can be rewritten as a loss of gravitational potential energy. Setting the kinetic-energy gain equal to the potential-energy loss yields KE₁ + PE₁ = KE₂ + PE₂. This bookkeeping holds at every point along the path and is independent of the shape of the track, which is what makes energy methods so much faster than force analysis.
Frictionless Versus Real Systems
In an idealized frictionless model, mechanical energy is conserved and the cart's speed at any height is fully determined by v = √(2g·Δh). In real systems, kinetic friction and air drag are nonconservative forces that convert organized mechanical energy into disordered thermal energy and sound. Total energy is still conserved — the missing mechanical energy reappears as heat in the rails, wheels, and air — but the recoverable mechanical portion steadily decreases, so a real cart always arrives slower than the ideal prediction.
Worked examples
A 2.0 kg cart is released from rest at a height of 10 m on a frictionless track. Find its speed at the bottom.
- Apply conservation of mechanical energy: PE at top equals KE at bottom, so mgh = ½mv².
- Cancel the mass m from both sides, leaving gh = ½v².
- Solve for v: v = √(2gh) = √(2 × 9.8 × 10) = √196.
- Take the square root to get v = 14 m/s.
Answer: 14 m/s (mass cancels and is not needed).
On a real track, the same 2.0 kg cart from 10 m arrives at the bottom at only 12 m/s. How much energy was lost to friction?
- Compute initial PE: mgh = (2.0)(9.8)(10) = 196 J.
- Compute final KE: ½mv² = ½(2.0)(12)² = ½(2.0)(144) = 144 J.
- Energy lost to friction = initial PE − final KE = 196 − 144.
- This 52 J became thermal energy and sound.
Answer: 52 J of mechanical energy was converted to heat and sound.
Activity
Drag each energy label to the correct position on the roller coaster track diagram to show how energy transforms from start to finish.
Practice
A pendulum bob swings down from a height of 0.45 m; find its speed at the lowest point assuming no friction.
Explain why the mass of a frictionless roller-coaster cart does not affect the speed it reaches at the bottom of a hill.
Common mistakes to avoid
- A real cart reaches the same bottom speed as a frictionless cart because energy is conserved.Total energy is conserved, but friction diverts some mechanical energy into thermal energy, so less kinetic energy remains and the real cart moves slower.
- Heavier carts always reach the bottom faster than lighter ones.On a frictionless track the mass cancels out of mgh = ½mv², so all masses reach the same speed for the same drop in height.
Check your understanding
A 500 kg roller coaster cart starts from rest at a height of 20 m. Assuming no friction, what is the cart's speed at ground level? (g = 9.8 m/s²)
A student claims that a real roller coaster cart reaches the same maximum speed at the bottom of a hill as a perfectly frictionless cart would, because 'energy is conserved.' What is wrong with this reasoning?
At which point on a frictionless roller coaster track does the cart have the greatest gravitational potential energy?
Recap
Energy is never created or destroyed; in an isolated frictionless system mechanical energy KE + PE stays constant, so falling height converts cleanly into speed. Real systems lose mechanical energy to friction as thermal energy, but total energy is always conserved.
Reflect
When was a time you noticed energy changing form in everyday life?