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Sandbox Physics

FR15-A · Look behind the projection

Free Energy Hides a Dimension

Why does a low potential-energy route sometimes look unlikely in a free-energy profile? Probability depends on how many configurations fit at each position as well as their energies. A narrow low-energy passage can carry less equilibrium weight than a wider valley. A free-energy profile sums over the hidden configurations.

Rotate a coordinate across a two-dimensional landscape. Follow thermal paths, compare free energy with the lowest potential energy, and open a slice to see the motion hidden by the projection.

Interactive modelFree Energy Hides a Dimension
Projection angle0∘0^{\circ}
Central free-energy rise3.843.84
Hidden-coordinate spread0.9430.943
Selected coordinate00

Independent numerical quadrature

One coordinate contains many places

Cyan sums the probability along each slice; dashed gold keeps only its lowest potential energy. Click the upper plot to choose a slice.

Continue the course on free energy and rare events

Physics tutorial

A profile sums over the directions you cannot see

BackgroundA thermal particle explores a two-dimensional landscape. Recording only one coordinate folds many distinct positions onto the same point.

Why it mattersA low point in potential energy says where one configuration is cheap. A free-energy profile asks how much probability all compatible configurations carry together.

Start with the essentials

Focus question
What changes when the same landscape is viewed along another coordinate?
One-sentence intuition
Free energy contains the energy and the number of hidden configurations.

Core mathematical model

Choose the visible and hidden coordinates

s=xcos⁡θ+ysin⁡θ,h=−xsin⁡θ+ycos⁡θs=x\cos\theta+y\sin\theta,\qquad h=-x\sin\theta+y\cos\theta

Both configuration coordinates are dimensionless. This is a rotation, so the area element is unchanged. The reflecting square becomes a rotated square in these coordinates.

Add the Boltzmann weights along a slice

F(s)=−kBTln⁡ ⁣∫Ωse−U(s,h)/(kBT) dh+CF(s)=-k_{\rm B}T\ln\!\int_{\Omega_s}e^{-U(s,h)/(k_{\rm B}T)}\,dh+C

The integral includes every allowed hidden coordinate at the chosen position. The additive constant makes the displayed minimum zero. The gold minimum-energy curve is shifted separately.

Ask where the hidden coordinate lies

p(h∣s)=e−U(s,h)/(kBT)∫Ωse−U(s,h′)/(kBT) dh′p(h\mid s)=\frac{e^{-U(s,h)/(k_{\rm B}T)}}{\int_{\Omega_s}e^{-U(s,h')/(k_{\rm B}T)}\,dh'}

Two peaks at one visible coordinate mean the projection merges two regions. A free-energy profile alone does not tell how quickly the particle moves between them.

Common difficulties

A probability profile is not a speedometer

Typical misconceptionOnce the free-energy barrier is known, the reaction time follows directly.

Better mental modelA rate also needs mobility and a coordinate that resolves slow motion. The kinetics experiment keeps equilibrium fixed and changes friction to show this directly.

Run the experiment

  1. 01

    Look through the middle

    Start with Hidden twin routes. Keep Selected slice at the center and inspect the lower distribution.

    What to observe: The hidden coordinate has two preferred regions. The single central value on the horizontal axis contains both.
  2. 02

    Rotate the projection

    Drag across the terrain or move Projection angle. Compare See along the valley.

    What to observe: The terrain stays fixed but its projection changes. Peaks can merge or separate because different positions are added together.
  3. 03

    Predict the effect of warming

    Compare Warm landscape with the initial preset. Keep the angle fixed when adjusting Thermal energy yourself.

    What to observe: Higher-energy configurations carry more weight as temperature rises. The difference between free energy and the minimum energy can change.

Related experiments and articles

Free energy and rare events · Reading path

From Boltzmann probabilities to reaction paths

Articles on this path that use this experiment, followed by the other experiments they suggest.

  1. ArticleWhy the deepest potential well need not be the most populated
  2. ArticleHow metadynamics gradually fills a visited valley
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