Roads over lava tubes in Cheju Island, South Korea
Transcription
Roads over lava tubes in Cheju Island, South Korea
Engineering Geology 66 (2002) 53 – 64 www.elsevier.com/locate/enggeo Roads over lava tubes in Cheju Island, South Korea A.C. Waltham a,*, H.D. Park b a Civil Engineering Department, Nottingham Trent University, Nottingham NG1 4BU, UK School of Civil, Urban and Geosystem Engineering, Seoul National University, Seoul 151-742, South Korea b Accepted 18 January 2002 Abstract There are 59 known lava tubes in the basalts of Cheju Island, South Korea. They have formed by either crusting or injection, and the structural properties of the rock over them vary with their formative processes. Two tubes are crossed by roads that stand on very thin rock arches. One road has been built on a bridging concrete slab, the other is unprotected, but both appear to be stable. A ratio of 3:1 for tube width to roof thickness appears to ensure integrity under normal engineering loads. D 2002 Elsevier Science B.V. All rights reserved. Keywords: Lava; Cave; Collapse; Ground stability; Highways 1. The shield volcano of Cheju Island 2. Lava tubes in basalt Cheju Do (Cheju Island) lies 80 km south of mainland Korea, almost midway between China and Japan. It is 75 km long and 30 km wide (Fig. 1), and consists entirely of a single shield volcano, which is distinguished by having over 360 parasitic cones on its flanks. The central peak of Hallasan rises to 1950 m. It last erupted in 1007 AD. On the higher slopes, open grassland covers roughly the area formed by the Hallasan volcanics, with woodland forming a zone at lower altitude. Nearly a million people thrive on farming and tourism in a well-developed coastal strip. This is formed of old basaltic lavas, which generally provide stable ground, except over the old lava tubes. Though layers of scoria and aa (blocky) rubble can create zones of loose and weak rock, most basalt solidifies into a very strong rock. Good ground conditions are however compromised where lava tubes have been left to form extensive voids just below the ground surface. A lava tube may be formed where a lava flow develops a cooled and solidified crust, while molten lava continues to flow beneath the surface (Kauahikaua et al., 1998). Alternatively, liquid basalt may be injected beneath a crust of solidified basalt from an earlier stage of the eruption; in this style, lava flows are inflated by new material that arrives through tubes and may solidify before ever reaching the surface (Walker, 1991; Hon et al., 1994). When an eruption ceases suddenly, or when flow is switched to another outlet, the molten lava may drain out, to leave an empty tube down the axis of the lava flow. Most extensive basaltic lava flows are tube-fed. Heat loss to the atmosphere means that lava can rarely * Corresponding author. Tel.: +44-115-848-2133. E-mail addresses: [email protected] (A.C. Waltham), [email protected] (H.D. Park). 0013-7952/02/$ - see front matter D 2002 Elsevier Science B.V. All rights reserved. PII: S 0 0 1 3 - 7 9 5 2 ( 0 2 ) 0 0 0 3 0 - 3 54 A.C. Waltham, H.D. Park / Engineering Geology 66 (2002) 53–64 Fig. 1. Main features of the topography and geology of Cheju Island. flow on the surface for more than a few kilometres, before it cools and solidifies. But a lava stream that has a solidified roof crust suffers negligible heat loss, and can flow underground for many kilometres. The mechanisms of lava tube formation and extension are a complex function of the lava’s rheology, its supply rates and chemistry, and the ground topography beneath the flow. Most active tubes observed on Hawaii are less than a metre in diameter, and these must be regarded as the normal state in shield volcano basalts. However, lava tube caves, which are generally 2– 10 m in diameter, can form as the main feeder within a long and mature flow. These may subsequently drain out to survive as open tubes—that are known to be up to 40 km long. Though tubes are a feature of most basalts, they only drain out to leave open tubes where the lava’s viscosity and gradient permit; others are sealed as the lava solidifies within them or as hot lava deforms and closes in on them. Many basalt flows have no open tubes, and some tubes were filled by lava in later stages of the same eruption. Many tubes at high level within older lavas have been lost by subsequent surface lowering; there are few long tubes recorded in lavas older than about 200,000 years. Tubes formed by injection may lie beneath basalt tens of metres thick. However, tubes formed by roofing of surface flows lie just below the surface, and consequently provide a potential hazard for engineering construction. The crusts of rock over these tubes are normally no more than a few metres thick. Nearly all entrances to lava tubes are through sections of roof collapse. Some of these collapses occurred at an early stage, when lava was still flowing beneath; skylights are commonly seen in active lava flows, where the thin crust has fallen in, so that molten lava can be seen flowing within the tube (Fig. 2). Other collapses occur at later dates. The minor earthquakes that are common on active volcanoes have caused tube roof collapses 5 or 10 years after the eruption ended and the lava cooled, revealing tubes that had not previously been seen or known. And some collapses occur much later in response to weathering and weakening of the thin basalt arches above the tubes. A.C. Waltham, H.D. Park / Engineering Geology 66 (2002) 53–64 55 Fig. 2. A skylight into an active lava tube on Hawaii. The opening is 2 m across and yellow-hot lava can be seen 3 m below, flowing in a tube about 5 m in diameter. 2.1. The lava tubes of Cheju There are 59 known lava tubes on Cheju Island. They have a combined length of over 42 km, and eight tubes have lengths greater than a kilometre. All but 700 m of the known tubes are in the Pyoseonri lavas (Fig. 1). Most of the known tubes lie beneath the developed lands of the coastal strip, and there are undoubtedly more tubes that have no roof collapses, as yet, and therefore remain inaccessible and undocumented. Three of the tubes visited by the authors are worthy of note. 3. Manjang Gul The longest single lava tube on Cheju is Manjang Gul (located on Fig. 1). It has a mapped length of nearly 8 km, though its accessible ends are merely collapse zones, beyond which the open tube continues. A notable feature of Manjang Gul is the large size of its tube (in comparison to most others in the world); much of it is 15 m wide and 10 m high (Fig. 3), and some sections are 20 – 25 m wide. The entrance is through a simple natural collapse, about 12 m across, where the original tube rose slightly and the roof was less than 4 m thick. The cave is now a popular tourist site. Precautionary engineering works are modest, but include a sprayed concrete lining under the entrance arch where it is exposed to weathering above the show- cave path. This entrance is in a high-level loop off the main tube. Just up-flow of the tourist entrance, the two tubes merge at the lower level, beneath solid rock over 10 m thick (Fig. 3). Along the kilometre of tube that contains the tourist trail, the floor is a pahoehoe surface with a uniform gradient of 0.4j. Most of the roof appears to be a broad, stable arch. Sections where the roof is only about 3 m high have profiles that are almost circular arches. Hanging from the smooth arches are small stalactites of glassy basalt. These formed where a glaze dripped from the roof after it was heated to melting point by hot gasses above the molten lava stream within the tube. Their presence indicates that the roof is in its original state, with no subsequent collapse. Some other sections of the roof are much higher, but lack any collapse debris beneath them. The thick cover of basalt over this tube suggests that it was formed by injection, when the lava could flow over loops under its own hydrostatic pressure. The crests of the loops may have been modified by block plucking and roof erosion by the lava when it was under pressure within its tube. Roof blocks that collapsed into the hot lava were swept away downstream; some blocks survive, welded into the lava floor, and with no sign of roof collapse directly above them. The uniform profile of the floor indicates that any original rises were removed by thermal erosion and entrenchment of the lava. Other sections of tube contain high collapse domes above extensive piles of blockfall, with individual 56 A.C. Waltham, H.D. Park / Engineering Geology 66 (2002) 53–64 Fig. 3. The large main tube in Manjang Gul. The roof structure appears to indicate some weathering along fracture lines, but there is no collapse at this point. blocks up to 4 m across. Some of these sites are monitored, but there are no observed cases of new rockfall, and it appears that the roofs have developed into stable voussoir arches within the fractured rock. Some high sections have roof joints, at a spacing of about 1.5 m, along which there are zones of discoloration that widen at the joint intersections. It appears that roof collapse has stopped upwards into basalt of weathering zone II, with the first traces of spheroidal weathering, where the ground surface is about 7 m above the cavern roof. 4. Sung Gul Almost at the western tip of Cheju (Fig. 1), Sung Gul is a lava tube nearly a kilometre long beneath the village of Shinchang; it is sometimes known as Fig. 4. The collapse entrance to Sung Gul, between the houses of Shinchang. A.C. Waltham, H.D. Park / Engineering Geology 66 (2002) 53–64 57 Fig. 5. Outline plan survey of the Sung Gul lava tube where it lies beneath the island’s perimeter road. Shinchang Gul. It also extends beneath the island’s main perimeter road. The entrance to Sung Gul is an ancient collapse hole, formed where the roof was thinnest over a gentle upward loop in the tube profile. It lies between the houses of Shinchang (Fig. 4), and there are steps down to the cave floor, as villagers use it for cool storage of farm produce. Down-flow, the tube is easily followed for 400 m, as it is all 2– 4 m high and 5– 14 m wide (Fig. 5). The floor is a rough and partly broken pahoehoe (smooth or ropy skinned) lava, and the gradient is less than a degree. Most of the roof of the Sung Gul tube is a broad, flat arch, with small glaze structures that indicate it is in its original state. At the upper end of the two oxbow loops, the tube is 14 m wide, with an almost flat roof that shows no sign of collapse (Fig. 6). For much of its length, the tube is lined with at least one shell of lava, 200 –400 mm thick. This was formed after the tube was partly drained, so that its roof cooled slightly. A subsequent pulse of lava re-filled the tube, and the shell was formed where it chilled against the cooler roof. Some small sections of this shell have fallen away (Fig. 7); most of these falls are old, and Fig. 6. An almost flat roof 14 m wide just up from the down-flow ox-bow loop in the Sung Gul lava tube, with no sign of rockfall or collapse. 58 A.C. Waltham, H.D. Park / Engineering Geology 66 (2002) 53–64 Fig. 7. Breakdown of the chilled basalt shell that lines part of the Sung Gul lava tube. there are no signs of collapse of the rock outside the detaching shell. Five short sections of the tube have more extensive roof collapse (Fig. 5). Irregularly shaped blocks up to 2 m across have fallen away to create large piles of breakdown under higher, domed sections of roof. Some of these dome roofs appear to have developed into stable arches within the jointed basalt (Fig. 8), and there are no signs of ongoing collapse on any of them. The collapse section furthest down-flow extends into an area of total roof failure (Fig. 9). This has created a rocky depression at least 15 m long (now partly backfilled) on the surface. Part of the tube Fig. 8. The third collapse zone down-flow from the village entrance in the Sung Gul lava tube. A.C. Waltham, H.D. Park / Engineering Geology 66 (2002) 53–64 59 Fig. 9. Sketch profile along the lower part of Sung Gul. The tube has an unbroken roof where it passes beneath the road, but has extensive breakdown down-flow of the road as far as the zone of total collapse through which lies the access pipe. survives round the north side of the collapsed blocks (Fig. 5), and it appears that the roof failure occurred in a very wide section of the tube. Access through the blockfall is now via a 500-mm-diameter concrete pipe that opens into the side of a concrete culvert built across the collapse depression. 4.1. The road over Sung Gul Cheju Island’s perimeter road crosses over the Sung Gul tube between its two down-flow collapse sections (Fig. 5). The road was a rough track until 1961, when it was paved. This was widened to two lanes in 1974, and to four lanes in 1998. It was not realised that the cave in Shinchang village extended under the road until it was found in 1994 during the site investigation for the last phase of road widening. No diversion of the road was then considered, as the line was already established. Purely by good luck, the line of the road lay over the most stable part of the cave, where a smooth arch barely 6 –10 m wide rises 2 m above a clean floor of ponded lava (Fig. 10). A shell of chilled lava lines part of the walls; it is incomplete, but there are no fallen blocks beneath, and any fallen shell sections may have been carried away when the lava was still flowing. Glaze drips on the roof show that it is in its original state. Assessment of the cave in 1994 found that the roof consisted of 3.5 m of rock and 2 m of soil. The internal report (unpublished) concluded that ‘‘the rock seems to be strong enough, but jointing and fractures could be a potential problem for stability of the road’’. Fig. 10. The stable arch in the Sung Gul lava tube, directly beneath the main road. 60 A.C. Waltham, H.D. Park / Engineering Geology 66 (2002) 53–64 Lack of data on the rock structure precluded any quantitative analysis, but it was deemed necessary to strengthen the ground. The soil was removed, and a flat surface was prepared by placing clean sand at least 100 mm deep over the uneven rockhead. For a 20 m length of the road over the cave, two layers of expanded polystyrene blocks (each 500 mm thick) were placed on the sand for the full 11.2 m width of the road (Fig. 9). Centred on this, a slab of reinforced concrete 400 mm thick and 30 m long, also 11.2 m wide, completely spans the cave (Fig. 5). The road pavement is 50 mm thick over the concrete. The reinforced slab can act as a single-span bridge element (Fig. 11), eliminating any hazard from even a complete failure of the lava tube roof. 4.2. The stability of Sung Gul beneath the road Any analysis of rock stability over an underground void relies on adequate information concerning the density and pattern of the fractures within the rock arch. These data are almost impossible to obtain for a unique site, and can only be an approximation for a site where exposures, comparisons and destructive test data are available. As intact rock, basalt is very strong, with UCS normally over 200 MPa, but it varies enormously in its fracture patterns and consequently in its rock mass strength. The state and strength of the rock forming the roof of a lava tube depends largely on how the lava stream was roofed over, or whether it was formed by injec- tion into an inflating flow. There are various possibilities, especially for the surface channel roofing: 1. accretion onto the banks and levees on both sides, until they coalesce over the flow, leaving vertical fractures in the arch centre; 2. accretion and wedging of floating slabs, leaving an irregular blocky structure; 3. crust formation by toes and small sheets of pahoehoe lava, leaving a pattern of fractures around sub-horizontal lava lenses (as in Fig. 2); 4. tube formation by injection beneath a thin or thick roof of solid lava; 5. addition of shells inside the tube, formed when lava pulses fill the tube and leave chilled linings against the cooler roof and walls; 6. addition of subsequent lava layers to thicken the roof. Where tubes originated as surface channels, process nos. 1 –3 normally form the initial roof. This may be thickened by process nos. 5 –6, or may be thinned by subsequent melting away of part of the roof (thermal erosion). In all cases, the ‘‘fractures’’ within the basalt may be important potential weaknesses, especially where they have opened up during cooling contraction. Alternatively, they may weld while still hot, to represent minimal structural weakness in what appears to be very massive basalt. Fractures may develop subsequently, under changes of tectonic stress (which is common in an active volcano), or in res- Fig. 11. Cross section through the Sung Gul lava tube and the concrete slab that carries the main road above it. A.C. Waltham, H.D. Park / Engineering Geology 66 (2002) 53–64 ponse to weathering disturbance. Injection tubes, formed by process no. 4, normally have more massive rock roofs. Tensile fracturing of their roofs, caused by inflation pressure, is recorded in the form of lava tumuli and breakouts (Walker, 1991), but many of these fractures are subsequently filled and welded by lava inflow. Most of the roof rock that is visible within the Sung Gul tube does appear to be in good condition, with few major structural weaknesses. There are fractures in the basalt, but they are mostly tight and irregular. It therefore appears that the rock mass factor of the basalt is high, and its mass strength under compression is close to its intact strength. The internal shells that are falling away from open fractures are not relevant to stable arches that can form in the overlying rock; multiple shells could exist (and remain invisible until they partially fail), but concentric arched fractures would have little influence on a compression arch formed parallel to them. Fractures within the basalt have little effect on tube roof integrity where they lie within the zone of compression that creates a self-supporting arch over a void. Rock that remains beneath the compression zone is in tension and is subject to deformation under loading. The rock arch over the Sung Gul tube has been examined by Finite Difference Analysis within a FLAC Ubiquitous Joint Model that was originally applied to assessment of cave roofs in sandstone (Waltham and Swift, in prep). A worst-case scenario was created for the road over Sung Gul, with a cave width of 12 m and a thickness of rock roof of 3 m. The basalt UCS was taken as 160 MPa, and a rock mass factor of 0.1 was applied as a reduced strength on the ubiquitous joints. Failure of the tube roof occurs under a vertical loading of 4000 kN applied on a square pad of 0.5 m edge length. This is far in excess of any possible highway loading or design criteria. However, the figure relies on estimates of the fracture weakness within the basalt, and is unrealistic. The FLAC programme that models relatively homogeneous rocks is inappropriate for the investigation of strong, fractured basalt. Further analysis was outside the scope of this short field project. The available data suggest that the concrete slab may not have been entirely necessary to ensure integrity of the road. Volcanologists recognise that it is extremely difficult to interpret how a tube formed, 61 merely by inspecting its cold state; by implication, it is equally difficult to appreciate the fracture state of an in situ rock roof. The cost of the concrete slab was small as a proportion of the project costs, and its inclusion was a reasonable precaution. A layer of heavy geogrid in the road sub-base offers a cheaper precautionary measure against potential ground collapse; but this is inappropriate over such a large rock void at shallow depth where any failure is likely to cause instantaneous total collapse of an area perhaps 8 m in diameter. The alternative options of collapsing the tube and building over the stabilised breakdown, or filling the tube with concrete, both represented higher costs than the simple bridging slab where sound rock was available on each side. The integrity of the smaller rock arch, just 500 mm thick, over the Sung Gul entrance (Fig. 4) also relies on a lack of critical fractures within the basalt. It could not be adequately modelled on the FLAC programme. The rock appears to be intact, and modelling intact rock produces failure at far in excess of any construction loading. The arch thickens as the roof descends immediately inside the cave, where it becomes even stronger. A crack within the wall of the house on top of the cave indicates settlement at one end, but this appears to be related to soil compaction under the very shallow footings. The end wall of the house appears to be completely safe, despite its impressive location. 5. Cheamchon Gul Close to the village of Hyopchae, Cheju’s old perimeter road passes over the short lava tube of Cheamchon Gul. A new section of road, further inland, avoids the cave crossing (Fig. 1). Only about 100 m of this tube is open and accessible. Most of this is 8 m wide, with its roof no more than 3 m below ground level. Just north of where it crosses beneath the road, the tube is completely collapsed over a length of 40 m, and its partially collapsed continuation is flooded. Adjacent to the road crossing, the tube has two collapse windows (Fig. 12). The larger is the entrance with steps down into the cave, where a level floor has been created for occasional use as a village night club. The smaller skylight is in the soft shoulder of the road, 62 A.C. Waltham, H.D. Park / Engineering Geology 66 (2002) 53–64 Fig. 12. Sketch survey of Cheamchon Gul lava tube where it lies beneath the old main road. Fig. 13. The two roof collapses that create the entrance and the skylight in Cheamchon Gul, seen from the tube’s continuation beneath the road. A.C. Waltham, H.D. Park / Engineering Geology 66 (2002) 53–64 63 Fig. 14. Fracture opening recorded in the roof of Cheamchon Gul lava tube when vehicles passed over the road above (by courtesy of KICT). immediately adjacent to the tarmac, from which it is separated by a low steel fence. Parts of the tube roof have an irregular profile left by past block collapse (Fig. 13). The low wide profile of the tube suggests that it may have originated by lava injection, beneath 2 –3 m of older basalt. Among the irregular fractures in the roof rock, there appears to be a crude arched layering that may represent inflated flows of pahoehoe older than the tube. The road stands on rock that is about 3 m thick, except where it tapers to only 2 m thick at the southern edge (Fig. 12). The fractured basalt appears to have stabilised in a low compression arch. This arch thins between the two skylights (Fig. 13), where its more broken structure suggests any future failure is most likely to occur. The rock under the road is in better condition, less fractured, and forming a thicker and wider arch. Exposed fractures in the roof of the cave have been monitored under dynamic loading by traffic on the road directly above. Strain gauges were attached across two roof fractures, one at the tube centre and one near the wall. When light trucks passed over the cave, the fractures opened by about 7 Am (Fig. 14); the effect of cars was not easily recognisable. After unloading, the fractures closed again, as the entire rock mass was behaving as an elastic material. This rock arch over the cave appears to be stable, and does not warrant a reinforcing concrete slab, even though part of the arch is thinner than that over Sung Gul. 6. The lava tube hazard Any construction project on young basalt lavas may encounter a potential hazard from open tubes at shallow depth. The statistical chance of a tube lying beneath a particular engineered structure is extremely small, but it is impossible to predict where they lie beneath a mature landscape. Direct exploration and mapping of tubes from accessible collapse entrances is the cheapest method of establishing their positions, but many tubes exist without known accessible entrances. Borehole exploration is expensive. Geophysical searches can be productive, and various investigators of lava tubes have preferred resistivity (Kwon et al., 1998) or magnetic (Wood, 2001) surveys; these methods may be more economical than the microgravity surveys that are most useful for void detection in rocks less conductive than basalt. Recorded collapses of lava tubes (in Hawaii) have all been in the initial stages of road building, when very large bulldozers provide point loadings far heavier than those of road traffic; their use appears to offer a convenient means of load testing the ground before a road is in use. 64 A.C. Waltham, H.D. Park / Engineering Geology 66 (2002) 53–64 The high strength of basalt means that most lava tubes are stable even where their roofs are disconcertingly thin. A ratio of 3:1 for tube width to roof thickness (in unweathered rock) would appear to be adequate to establish a sound rock arch that will bear all but the heaviest structures. This ratio should provide an appropriate safety factor where the basalt lava has only the low density of fractures that is typically observed in tube roofs. Zones of more fractured lava can account for weaker tube roofs. As a by-product from a geophysical cavity search, a measured field seismic velocity could indicate rock mass quality by correlation with existing empirical data. Highways and light structures can stand in full safety above the great majority of lava tubes, but heavy structural loadings should only be applied to basalt lava after appropriate investigation of the local ground conditions. Acknowledgements The Royal Society generously provided a grant for travel costs in support of the programme of academic exchange between members of the Geohazards Group in Nottingham Trent University and members of the Department of Geological Engineering at Seoul National University. The authors thank colleagues at the Korean Institute of Construction Technology (KICT) for contributing their data on the Cheamchon Gul roof monitoring, Bill Halliday and Chris Wood for helpful comments in discussion, and Jun Yong Lee for assistance in the field. Part of this work was supported by SNU Research Institute of Engineering Science and BK project 21 in 2001. References Hon, K., Kauahikaua, J., Denlinger, R., Mackay, K., 1994. Emplacement and inflation of pahoehoe sheet flows: observations and measurements of active lava flows on Kilauea Volcano, Hawaii. Geological Society of America Bulletin 106, 351 – 370. 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