Yamal’s first giant crater: the field measurements and competing gas-release models

The deep crater discovered on Russia’s Yamal Peninsula in 2014 looked like a sudden hole in an otherwise vegetated landscape. Its walls exposed ice-rich ground, while a rim and scattered blocks showed that material had moved outward. Fieldwork and satellite comparisons turned an initially startling feature into a testable geological problem. The broad explanation involves pressure and gas release within permafrost; researchers have developed competing accounts of how the pressure accumulated and what triggered the eruption.

Four-panel scientific schematic of a proposed Yamal crater eruption, showing gas, water and thawed ground beneath an ice cap.
Proposed cryogenic eruption stages: Figure 3 in Buldovicz and colleagues, Scientific Reports 8, 13534 (2018), CC BY 4.0. Panels show pre-explosion, pneumatic, hydraulic and phreatic stages. Unaltered published schematic, extracted from the original PDF and displayed responsively. One proposed model, not an observed sequence or a crater photograph.

The original crater and its changing shape

This case concerns the first widely studied Yamal crater, subsequently labelled C1 or GEC-1. The original 2015 study by Alexander Kizyakov and colleagues combines visits in 2014 with satellite imagery and digital elevation models. It records a mound at the site before crater formation, ice exposed in the walls, a raised rim of ejected ground and fragments scattered beyond it.

The investigators distinguished the relatively narrow cylindrical lower opening from the wider upper funnel and outer rim. Consequently, different quoted diameters need not describe the same boundary. They also recorded rapid alteration: ice thawed, walls retreated and water rose. A dimension measured on a later visit is not automatically the dimension immediately after the eruption. Their reconstruction depended partly on imagery, with acknowledged difficulty recovering the deep shadowed interior.

The same study inferred formation between 9 October and 1 November 2013 from changing satellite appearances. A 2021 regional mapping paper by Scott Zolkos and colleagues lists a broader October 2013–April 2014 interval for GEC-1. Both place formation before the summer 2014 discovery. This article retains the differing resolutions of those reconstructions rather than treating a discovery flight as the eruption date. No exact incident year is assigned in the catalogue.

What mapping establishes

Zolkos and colleagues used satellite reflectance, elevation and water-extent information to investigate landscape change across the Yamal–Gydan region. Their method detected the seven gas-emission craters reported in the literature at that stage and identified additional crater-like features requiring interpretation. It also found that other kinds of permafrost change were more widespread. An automatic detection therefore needs to be checked against landform characteristics and other evidence; it is not a direct count of witnessed explosions.

For this particular case, earlier and later views support the replacement of a mound by a crater. They do not record the full eruption continuously or directly reveal the former underground cavity. That difference explains why a well-mapped surface feature can still support more than one subsurface model. Other craters elsewhere in the region are comparative research, rather than additional episodes silently folded into C1’s history.

Freezing ground and a carbon-dioxide model

In their 2018 Scientific Reports paper, Sergey Buldovicz and colleagues report field observations, sampled ice and ground, chemical analyses and thermal modelling. They propose a shrinking lake with an unfrozen body of ground beneath it, known as a talik. Freezing around that body concentrates water and gas, builds pressure and creates a mound. Their developed explanation gives carbon dioxide a major role in the eventual release.

The authors distinguish the sampled gases from those of the nearby deep Bovanenkovo gas field, arguing against a simple supply from that reservoir. Their illustrated stages show gas release, water movement and the ejection of thawed ground. Those stages are a reconstruction based on their model, not eyewitness observations of the event. The figure reproduced here is labelled accordingly. The exact quantity of gas formerly present in the unfrozen core was not directly measured.

Could methane pressure alone do it?

Lauren Schurmeier, Gwendolyn Brouwer and Sarah Fagents test another approach in a paper first published on 29 November 2023. The public abstract describes a model constrained by the crater’s observed blocks and their scattering distances. It asks whether accumulated methane could fracture the cap and launch the blocks without requiring additional pressure from freezing ice. Different underground cavity shapes and cap thicknesses are considered.

For a subset of the tested configurations, the calculated pressures were compatible with the strength and overlying load estimated for the cap. The authors conclude that gas pressure alone can account for the observed ejection in those models. This is a significant alternative to making pingo-like freezing essential. It does not mean the original underground geometry was recovered directly. The account here is based on the publisher’s public abstract; the subscription full text was not reviewed.

An osmotic trigger proposed in 2024

Ana Morgado and colleagues offer another physical mechanism in their 2024 Geophysical Research Letters paper. Their model considers a buried lens of salty water, or cryopeg. Differences in salt concentration can draw water toward it through suitable ground. The resulting pressure may fracture surrounding material, permitting methane hydrate breakdown and gas release. This addresses how pressure might build, rather than invoking combustion as a necessary first step.

The proposed system is idealised. Its behaviour depends on ground permeability, salt concentration, geometry and the duration of seasonal thaw. The authors discuss the effect of heterogeneous frozen ground on the predicted timescale. Such calculations identify conditions under which a process could work; they are not a direct measurement of the buried system before C1 formed. This account uses the reviewed public explanation and model sections without claiming an independent recalculation of the equations or a new field test.

Assessment: disagreement within a geological explanation

The classification is Disputed, specifically for the substantial competing geological mechanisms. The reviewed observations support a gas-emission crater in ice-rich ground. The published models differ over freezing pressure, gas composition, accumulation and the trigger for rupture. This disagreement does not give an extraterrestrial impact or any paranormal cause equal evidential standing. It identifies the part of the natural explanation that remains under active interpretation.

It is also important to distinguish a model’s ability to reproduce selected measurements from a unique reconstruction of the original event. Several configurations may yield similar surface results. Continued comparison with sampling, historical imagery and the changing landform can narrow the possibilities. This article reports the evidence and qualified proposals reviewed; it does not announce that one paper has finally settled every aspect of the crater.

Location and access

The map uses the site coordinates reported by Buldovicz and colleagues, rounded to 69.9710°N, 68.3696°E, in the Yamalo-Nenets Autonomous Okrug. This is a general reference for C1, not a borehole, an approach route or a permanently safe crater edge. The exact shape and water level have changed since the early surveys. Current official visitor access has not been established, so the location is not listed as a publicly accessible attraction.