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FR06 · Longitudinal expansion

Bjorken Expansion

Why does a plasma cool differently when it can push along its expansion? Longitudinal pressure does work as the matter expands, so its energy density falls faster. Collisions replenish that pressure; freely streaming particles instead lose longitudinal momentum and exert progressively less pressure along the expansion.

Compare an initially isotropic free-streaming gas, an ideal fluid and a relaxing shear stress at equal initial energy. Follow their cooling and their unequal longitudinal and transverse pressures.

Interactive modelBjorken Expansion
Proper time2.46 τ02.46\,\tau_0
Energy density0.335 e00.335\,e_0
Longitudinal / transverse pressure0.3430.343
Energy-matched temperature0.761 T00.761\,T_0

Pressure changes how the energy falls

Cyan: MIS relaxation. Amber: ideal fluid. Violet: initially isotropic free streaming. All begin at the same energy density; the initial shear control changes only MIS.

Energy density during expansion e/e0e/e_0
Longitudinal pressure relative to transverse pressure PL/PTP_L/P_T
Interpretation and units

Time is in units of the initial proper time; energy density is in units of its initial value. Natural units are used. The pressure shape above encodes normalized tensor components and carries no physical length scale.

Physics tutorial

The work done by expanding matter

BackgroundAfter a heavy-ion collision, neighbouring slices of matter rush apart along the beam. In a boost-invariant description each slice has the same history when followed with its own clock.

Why it mattersDilution removes energy from a unit volume. Longitudinal pressure also does work, so the cooling rate tells us about the stress along the beam.

Start with the essentials

Focus question
Why does a plasma cool differently when it can push along its expansion?
One-sentence intuition
Larger longitudinal pressure makes the energy density fall faster at the same instantaneous energy.

Core mathematical model

Energy conservation in a comoving slice

dedτ=−e+PLτ,PL=e3−ϕ,PT=e3+ϕ2\frac{de}{d\tau}=-\frac{e+P_L}{\tau},\qquad P_L=\frac e3-\phi,\quad P_T=\frac e3+\frac\phi2

Proper time is the time measured along a comoving trajectory. Positive longitudinal pressure adds pressure work to dilution. The shear convention lowers longitudinal pressure when the shear variable is positive.

A shear stress with a finite response time

τπdϕdτ=4η3τ−ϕ−4τπϕ3τ,τπ=CτπT,η=Cηseq\tau_\pi\frac{d\phi}{d\tau}=\frac{4\eta}{3\tau}-\phi-\frac{4\tau_\pi\phi}{3\tau},\quad\tau_\pi=\frac{C_{\tau\pi}}T,\quad\eta=C_\eta s_{\mathrm{eq}}

The expansion drives shear stress and a finite relaxation time delays its response. The last term follows the conformal MIS closure. The quadratic BRSSS term is set to zero.

The ideal conformal limit

e(τ)=e0(τ0τ)4/3,T(τ)=T0(τ0τ)1/3e(\tau)=e_0\left(\frac{\tau_0}{\tau}\right)^{4/3},\qquad T(\tau)=T_0\left(\frac{\tau_0}{\tau}\right)^{1/3}

Set shear stress to zero and integrate energy conservation. The ideal branch has equal pressures at every time. The temperature is defined by energy matching in every branch.

Common difficulties

Flow and equilibrium

Typical misconceptionA hydrodynamic description requires equal pressures at every instant.

Better mental modelViscous hydrodynamics predicts unequal pressures. The residual measures agreement with a chosen constitutive approximation; the pressure ratio measures isotropy.

Run the experiment

  1. 01

    Match the starting energy

    Choose Three cooling histories and leave the initial MIS shear at zero.

    What to observe: All three start isotropic. Their subsequent longitudinal pressures differ, so their cooling histories separate.
  2. 02

    Change the response time

    Compare Quickly relaxing shear and Long-lived anisotropy.

    What to observe: Relaxation and expansion compete. A slow stress response preserves anisotropy for longer.
  3. 03

    Inspect one time

    Pause and drag the glowing time handle. Read the energy and pressure plots at the moving marker.

    What to observe: The ideal branch follows the analytic power law. Free streaming starts with finite longitudinal pressure and approaches a slower late-time dilution law.

Related experiments and articles

Heavy-ion matter and hydrodynamics · Reading path

From directional pressure to transport inference

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

  1. ArticleFind the rest frame of expanding matter
  2. ArticleFollow the clock carried by the expanding matter
  3. ArticleCompare ideal flow with particles that never collide
  4. ArticleLet shear stress relax over a finite time
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