The Spacetime Metric

Historical research guide · 1092 · 2008

Static and dynamic traversable wormholes

Jarosław P. Adamiak

In one minute

A wormhole is a shortcut — a throat joining two distant regions of spacetime so that the trip through is shorter than the trip around. Jarosław Adamiak’s study, written as a master’s dissertation in applied mathematics at the University of South Africa and carried to the Eleventh Marcel Grossmann Meeting in Berlin, is a careful tour of what general relativity actually says about such objects. He begins with the Morris-Thorne framework, the list of properties a wormhole would need before a human being could fly through it, and then spends the heart of the work on the single real obstacle: the energy conditions. Those are not part of relativity itself, Adamiak stresses. They are extra restrictions physicists impose to keep solutions reasonable — and the Casimir effect and a non-zero cosmological constant already break them. He then asks whether letting the wormhole move helps. Evolving wormholes and rotating ones both lower the price, he finds, without abolishing it.

Connection

Chapter 17 is the negative-energy budget, and this is the clearest short statement of why that budget is the whole engineering problem: the geometry is free, general relativity permits it, and everything turns on how much exotic material the throat needs and for how long. Adamiak’s two dynamic answers — that the bill shrinks when the wormhole is allowed to evolve, and that rotation can move the exotic matter out of a traveller’s path — are exactly the levers that chapter follows.

From the source

  1. The energy conditions are not part of general relativity. They are additional limitations imposed on the stress-energy tensor to assure the physical reasonability of solutions to the Einstein field equations — which is why violating them is a licence question rather than a law of physics, and why the whole wormhole problem reduces to how much violation is needed.Chapter 3 Energy Conditions, section 3.1; restated in Chapter 6 Summary, second paragraph

  2. Known physics already violates them. Between two Casimir plates the energy density is negative — minus pi squared times the reduced Planck constant, over seven hundred and twenty times the plate separation to the fourth power — so the weak and dominant conditions fail there, and because energy density plus the pressure along the plate normal is negative the null and strong conditions fail too. Adamiak adds the topological version, in which periodic boundary conditions imposed on the universe itself violate all of them, and a non-zero cosmological constant, whose term is identified with the vacuum energy density and includes the zero-point fluctuations of every field-theory degree of freedom.Section 3.2 Violations, equations 3.28 to 3.33

  3. The nine requirements a traversable wormhole has to meet, as Adamiak lists them after Morris and Thorne: the metric spherically symmetric and static; the solution obeying the Einstein field equations everywhere; a throat connecting two asymptotically flat regions; no horizon, since a horizon would prohibit two-way travel; tidal gravitational forces reasonably small; a crossing time acceptable from the point of view of both the traveller and an outside observer; a physically reasonable stress-energy tensor; stability; and the requirement that it must be possible to assemble the thing.Section 2.1 Desired Properties of Traversable Wormhole, the numbered list of nine

  4. How much exotic matter is measured, not assumed. Adamiak reviews the volume-integral quantifiers of averaged-null-energy-condition-violating material, and the three conditions a proper integration measure must satisfy: it must be natural, so that the resulting total mass is the same in any coordinate system; it must reproduce, at least to first order, the scalar charge of a solution where a scalar field plays the role of exotic matter; and the mass must obey a conservation principle. His verdict is that there is a strong indication the amount of exotic matter needed to support a wormhole may not be as huge as was thought a decade earlier, and that introducing dynamics usually makes that amount smaller still.Section 3.3 Quantification of exotic matter, equations 3.49 and 3.50; Chapter 6 Summary, numbered point 3

  5. The evolving-wormhole result, stated in his own terms: writing the metric with a time-dependent conformal factor and imposing the weak energy condition gives three inequalities, and the flare-out condition at the throat forces the combination of the conformal factor and its first two time derivatives to stay positive. That constraint cannot be satisfied over the whole domain for a conformal factor that is positive and bounded. So although wormholes can be created without exotic matter, their lifetime is limited, because the controlling function sooner or later becomes negative.Section 4.2 Conformal Approach, equations 4.5 to 4.10 with Figure 4.2

  6. The rotating-wormhole result, in two parts. Rotation does not remove the need for exotic matter — an energy-condition violation is always present near the throat. But the exotic matter can be moved around the throat, so that some class of infalling observers would never encounter it. In Teo’s solution the throat radius picks up a term in the angular momentum and the cosine of the polar angle, giving the throat a dumbbell-like shape, and at substantial rotation speed the time-time component of the metric can turn positive outside the throat — an ergoregion.Chapter 5 Rotating Wormholes, the two numbered results after equation 5.13, with the Teo solution at equation 5.14

The way in

https://doi.org/10.1142/9789812834300_0357

How to cite it

Jarosław P. Adamiak (2008) Static and dynamic traversable wormholes doi:10.1142/9789812834300_0357

Where it sits in the curriculum

Provenance: Retrieved 2026-09-09

Summary by: The Spacetime Metric editorial rail (AI draft from the source text, 2026-09-07)

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