Geology 345 Lake Mead Field Report T. Saylor IV The structural geology class of 2012 took a field trip to Lake Mead, Nevada and studied the geology and historical stress states of the surrounding area. The trip took us to a complex area which has experienced multiple periods of tectonic activity and includes influence from the Sevier orogeny, the Laramide orogeny and currently, the spreading of the Great Basin and Range. In order to better understand how tectonics helped to create this varied topography, the class was introduced to different geological structures at several separate locations. These include the Rogers Spring strike-slip fault, the Pinto Ridge strike-slip fault, a section of the Lovell Wash and the Valley of Fire State Park. Each of these stops had different types of structural features which formed due to different states of stress, different stages of deformation and varying orientations of the major stress fields. To say that this area is geologically complex would be an understatement. The first part of the Lake Mead story begins with the geologic units found in this section of the basin. The oldest unit seen in the field was the Mississippian Monte Cristo, a dark limestone which was deposited in a marine environment. Above it is the Pennsylvanian Bird Spring Formation, another marine limestone. The Pennsylvanian ended with the deposition of the Red Beds / Hermit Shale. Sitting on top of that is the Permian aged Kaibab and Toroweap Limestone. These two layers, which in other areas are uniquely separate, are undifferentiated in the Lake Mead basin. The Triassic has two units to itself; the first being the Moenkopi Formation and then the Chinle formation. Possibly the most noticeable unit in the Lake Mead area is the Aztec sandstone, a counterpart to the famous Navajo sandstone of Colorado and Utah. Above the Aztec lays the Cretaceous Baseline Sandstone. The last unit seen is the Tertiary Horst Spring formation, which is comprised of the Rainbow Gardens, Thumb, Bitter Ridge Limestone and Lovell Wash members. All of these units have been folded and faulted, deformed and thrust all over the place and have created a gorgeous landscape of painted deserts, huge mountains and impressive valleys. The core of structural field work can be broken into three sections: geometry, kinematics, and mechanics. The first thing that needs to be done when interpreting structural features is to describe their form. What type of feature is it? What is its strike and dip? What is the size and magnitude of the feature? Are there any specific characteristics of the feature? Utmost detail needs to be used when describing a specific features geometry. It is important to accurately describe a feature seen in the field because this forms a basis for later interpretation. When those questions have been answered, it is time to look for indications of kinematics, or in other words, how did the feature move? This can be done in several ways: you can look for displacements along its length. When looking at a fault, is there any indication of how much movement occurred? In what direction did it move? Other things a geologist can look at are shears. 1 Shears indicate sense of motion and are broken up into several categories, but the main ones seen in the studied field areas include Riedel, conjugate Riedel and P-shears. These form in an en echelon manner, where a left stepping pattern indicates dextral motion and a right stepping pattern indicates sinistral motion. Folds can also have en echelon geometry but when a right stepping fold system is seen, it indicates right lateral motion, and vice-a-versa for left stepping. Thrust faults and normal faults can also occur in this en echelon pattern. Horsetail cracks represent relative motion as well. A joint with tail cracks oriented clockwise off of it mean that the relative motion the rock experienced was right lateral. Counter-clockwise tail cracks are indicative of left lateral motion. An interesting side note, large strike-slip faults can have subsidiary normal faults form on their flanks which when seen from a regional scale look like large tail cracks. They form due to the surrounding strata relieving pressure which the main fault (or joint) has imposed. A large scale normal fault tail crack system can be seen at the Pinto Ridge field location. Some of the best kinematic indicators are slickenlines. These features form on the plane of a fault as a result of grains crushing against each other during motion. They leave grooves in the surface which show the exact sense of motion which the fault has had. They do not however show how much displacement has occurred. In order to figure that out specific piercing points, such as matching beds or fold axes need to be positively identified. One of the main focuses of the field trip was to locate, describe and interpret faults and fault systems. We looked at a variety of fault styles, including strike-slip, normal and thrust. Each of these formed due to different tectonic activities. The thrust faults we saw were formed due to the Sevier orogeny, which took rocks from the Cambrian age up to the Monte Cristo, Bird Spring and Kaibab / Toroweap formations and thrust them over the Aztec sandstone. This motion occurred during the Cretaceous when the accretion of terranes from the West pushed the land Eastward. This thrust, known as the Muddy Mountain thrust created an impressive mountain chain. Later, during the Miocene, the basin and range system seen today began to form. This created large strike-slip faults and subsidiary normal faults which proceeded to chop up the landscape creating alternating mountain ranges and valleys. Faults form due to applied stresses. New faults may form in response to tectonic activity and utilize a pre-existing fault already located at that site. This means that a strike-slip fault may form where there once was a normal fault. This would occur due to changes in the stress orientations. For a normal fault σ1 would have originally been vertical to the plane and σ3 perpendicular horizontally, but as the stress state changed, σ1 would need to form at an angle of near 30° horizontal to the fault plane with σ3 90° off of that (still horizontally) for it to be 2 reactivated as a strike-slip fault. Fault growth can also be influenced through joint systems which already exist in beds. As a fault grows, it can mechanically feel the gaps made by the joints. Since it is easier for a fault to grow through an opening that is already there rather than break through solid rock, it will utilize these pre-existing features. Faults are great fluid controls. They can either be a super highway or they can impede fluid flow completely. Springs can form on the edges of faults, creating oasis’ in arid areas such as Nevada. The water eventually finds an outlet, and localized areas grow large amounts of vegetation. The first major fault the class conducted research at was the Roberts Spring fault, which created an oasis of its own. Roberts Spring is a massive sinistral oblique slip fault, which is the dominate form of strike-slip motion that faults in the Southern Nevadan basin have experienced. The fault strikes at 090° and has a dip of 66°. Slickenlines were apparent on a section of the exposed fault plane (Figure 1) and had a pitch of 80°east which is indicative of largely dip-slip rather than strike-slip motion. For strike-slip motion to occur along a fault, an optimal stress field with a σ1 oriented 30° to the fault plane would need to be present. This means that σ1 would need to be oriented approximately NE-SW. Later on in our field work, we would find that a stress field with this basic orientation holds true for most of the basins structural features, but not all. The Rogers Spring fault bisected a large section of Mississippian Monte Cristo, but towards the Western edge, a large section of Quaternary Alluvium was situated next to it. When one looked closely at the Alluvium, a deformation band could be seen. If a fault strikes through a bed which is currently in a state of deposition, and has a deformation band oriented similarly to it inside of its lithologic section, then one can assume that the fault has been active since the most recent period of its deposition. In the case of the Roberts Spring fault, this would be during the Quaternary which makes it a currently active fault. The topographic feature known as Pinto Ridge was created due to a large fault striking at 222° with a dip of 90°. This fault, named the Pinto Ridge fault, is made of Permian Kaibab a heavily silicified layer with large chert nodules all along its beds. When the fault was examined closely from a map view, rather than a cross-sectional view, Riedel and P shears could be seen. Their orientations were at roughly 025° and 232°, respectively. With their right stepping sense of geometry, a history of left-lateral motion could be assumed. Pinto Ridge is a large anticlinal fold with the beds folded on each side of the fault. This means that folding occurred first, and was later followed by faulting. With the age of the folded beds, an approximate age on the folding event can be determined. Since the youngest unit seen is the Moenkopi, which is of Jurassic age, then folding must have occurred after its deposition. This means that folding is post-Jurassic and with the 3 knowledge that spreading occurred in the Miocene (Dubendorfer et al, 1994), the fault must be of similar age, but older that the folding. When looked at from a regional scale, numerous other faults can be seen striking in a clockwise manner off of the central Pinto Ridge fault. These are all normal faults which formed in a horsetail manner with the relieving of pressure within the rocks. Our class ventured into one of these normal faults to look closer. It was on the South Eastern side of the Pinto Ridge fault and striked at 175° and had a dip of ~ 50° across its length. With Pinto Ridge striking at 222°and being sinistral in its motion, then an approximate orientation for σ 1 and σ3 can be determined. Since σ1 needs to be at an angle of near 30°to a fault plane in order for it to slip, then the shear system which created Pinto Ridge would lie about NE to SW for σ1 and NW to SE for σ3. A third major fault system which the class studied was the large Las Vegas Valley Shear Zone. To get there, we hiked through a section of the Lovell Wash on a day remembered as el marzo de muerte by some. Before reaching the main section of the shear zone, we mapped out numerous faults all trending in an East to West manner. Most of them turned out to be sinistral strike-slip faults, but a few normal faults with apparent oblique motion were found. Kinematic indicators such as Riedel shears informed us that the most recent period of motion has been leftlateral (Figure 2). However, these shears were crosscut by longer left stepping shears. Using the rules of crosscutting relations, the longer shears had to have occurred first, followed by the shorter shears beginning and ending inside of them. This means that our faults had to have two separate periods of motion, the first being right-lateral, and the second being left-lateral. This story was found all along Lovell Wash in a string of faults. When the class reached the Las Vegas Valley Shear Zone, we studied the outcrop on the Southern side of the fault. Although it was heavily weathered Moenkopi limestone, a shear sense could still be discerned in the outcrop. Again, it was found that long left stepping Riedels cross cut short right-stepping Riedels. If there are two separate motion events, then the stress orientations have changed at least twice. This means that an older paleostress was oriented at NW to SE for σ1 and NE to SW for σ3, which allowed the fault to move dextrally. At a later point in time, σ1 and σ3 swapped and allowed for left lateral motion. This new σ1 orientation at NE to SW is the same as it was for the creation of the Pinto Ridge fault. Pinto Ridge possibly developed around the same time the Las Vegas Valley Shear Zone began moving sinistrally but only after it had finished moving dextrally. While mapping in the Lovell Wash area, several interesting features which were not faults were noticed. The first interesting thing was a section of an old stream bed which had ripples along its length. The ripples were asymmetric and show the direction of flow. By using stereographic 4 projection (attached) where the tilted bed is back rotated to horizontal, the direction of the original stream flow was ascertained. The stream is located in the Thumb member and in that area strikes at 317° with a dip of 79°. The current ripple direction was marked 55° off of West along the bedding plane. When the bed was back rotated to horizontal, a paleo-current direction was found of 012° NE. Along the length of a small thrust fault found higher up in the Wash, a fault propagation fold could be seen on the hanging wall while a fault bend fold had formed on the footwall. The folding could be seen in a dark green shale layer. It is uncommon but not unheard of for these features to form in tandem, but it would be more likely to have occurred in the opposite sense, or on the other wall. At the end of the Lovell Wash, several layers of parasitic folds were found within a larger fold. Another stereographic projection found their original axes orientation before they had been tilted. The final studied area was the Valley of Fire State Park. The entire park is made up of the gorgeous aeolian Aztec sandstone. Due to the nature of its surrounding stress field, the rocks are all massively deformed. Numerous structures can be seen in the park, including plumose and growth lines on exposed joint surfaces (Figure 3). If one looks at specific outcrops, compaction bands can be seen. There is a large amount of these compaction bands, each with their particular wavy geometry. At one outcrop two main sets of nearly parallel bands can be seen. The oldest bands formed at approximately 165° - 170° and crosscut a younger set oriented at 020° - 040°. These two band trends create a conjugate set in map view. A feature not commonly found in rocks, but everywhere in the Aztec of the Valley of Fire is a shear-enhanced compaction band. Different from normal compaction bands, these have a zigzagging pattern which occurs when there is an almost equal component of shear as well as compaction (Eichhubl et al, 2009). Compaction bands also commonly form in the Navajo sandstone, the Aztec’s counterpart in Arizona, Utah and Colorado. Compaction bands are excellent aquatards. Understanding in which orientation these bands form can help us interpret how fluid flow is controlled in the rocks. Since a compaction band is impermeable due to the grain cataclasis which creates it, liquids will flow along their trends (Fossen et al, 2011). At one outcrop in the Valley of Fire, fluid was seen slowly seeping through the rocks on the outer edges of several bands. There are a number of large strike-slip faults within the Valley of Fire. The class spent some time at one fault system and endeavored to interpret its geometry, motion, and past movement history (Figure 4). A large amount of gouge was present in the basin of one of the faults. It was fine and powdery which implies a large amount of motion occurred along its length. This particular fault had Riedel evidence for left lateral motion and trended N-NE. A second fault was connected to the 5 first one and had shear evidence for right-lateral motion. It trended N-NW. The angle between the two faults was approximately 60°and defined a conjugate set for a specific stress state. In this case, σ1 trended at 335° but later rotated about 50°to create subsidiary horsetail cracks which could be seen in the outcrop. Our field interpretation agrees with the research that Flodin and Aydin conducted on the Valley of Fire in 2004. This trend of a North Eastern σ1 follows the same stress state as the Pinto Ridge and Rogers Spring faults and places their age in a similar time frame. In the case of these faults, this puts them sometime after the Sevier orogeny but before the Miocene aged tectonics. Overall, the story told by the faults keeps this stress orientation for the most recent strike-slip motion in the Lake Mead region. The field trip to Lake Mead hammered in the processes of structural field work. Describing geometry, locating kinematic indicators, and interpreting the mechanics of an area lead to a better understanding of what happened in the past. Getting up close and personal with structural features outside is the best way to learn about them. The region of land around Lake Mead has had an incredible tectonic influence. Features of all shapes and sizes abound in the rocks which make it an excellent location to learn the basics of structural geology. Set all of that information in a scenic locale close to sin city and you have a perfect classroom. 6 Figure 1: The exposed fault plane at Rogers Spring fault. Note the slickenlines which show movement direction. Photo by Simon Kattenhorn Figure 2: A fault plane from the Lovell Wash. Students are locating kinematic indicators. Photo by Simon Kattenhorn Figure 4: A large left lateral fault with high amounts of gouge in its center. Photo by Simon Kattenhorn Figure 3: Plumose features and growth lines shown nicely on an exposed joint surface. Photo by Simon Kattenhorn 7 References • Dubendorfer, Ernest M., and David A. Simpson. "Kinematics and Timing of Extension in the Western Lake Mead Region, Nevada." Geological Society of America Bulletin(1994): 1057-073. Print. •Eichhubl, Peter, John N. Hooker, and Stephen E. Laubach. "Pure and Shear-enhanced Compaction Bands in Aztec Sandstone." Journal of Structural Geology 32.12 (2010): 1873886. Print. • Flodin, Eric A., and Atilla Aydin. "Evolution of a Strike-slip Fault Network, Valley of Fire State Park, Southern Nevada." Geological Society of America Bulletin 116 (2004): 42-59. Print. • Fossen, Haakon, Richard A. Schultz, and Anita Torabi. "Conditions and Implications for Compaction Band Formation in the Navajo Sandstone, Utah." Journal of Structural Geology 33.10 (2011): 1477-490. Print. 8