ORIGINAL RESEARCH article

Front. Earth Sci., 19 March 2021

Sec. Volcanology

Volume 9 - 2021 | https://doi.org/10.3389/feart.2021.639459

A Multidisciplinary Investigation Into the Eruptive Style, Processes, and Duration of a Cascades Back-Arc Tholeiitic Basalt: A Case Study of the Brushy Butte Flow Field, Northern California, United States

  • 1. U.S. Geological Survey, Hawaiian Volcano Observatory, Hilo, HI, United States

  • 2. U.S. Geological Survey, California Volcano Observatory, Menlo Park, CA, United States

Abstract

The Cascades back-arc in northern California is dominated by monogenetic tholeiitic basalts that erupted throughout the Pleistocene. Elucidating their eruptive history and processes is important for understanding potential future eruptions here. We focus on the well-exposed monogenetic volcano that emplaced the Brushy Butte flow field, which constructed a ∼150 m tall edifice, has flow lobes up to >10 km long, and in total covers ∼150 km2 with an eruptive volume of 3.5 km3. We use a multidisciplinary approach of field mapping, petrography, geochemistry, paleomagnetism, geochronology, and lidar imagery to unravel the eruptive history and processes that emplaced this flow field. Tholeiitic basalts in northern California have diverse surface morphology and vegetation cover but similar petrographic appearances, which makes them hard to distinguish in the field. Geochemistry and paleomagnetism offer an independent means of distinguishing tholeiitic basalts. Brushy Butte flow field lavas are similar in major-oxide and trace-element abundances but differ from adjacent tholeiitic basalts. This is also apparent in remanent magnetic directions. Additionally, paleomagnetism indicates that the flow field was emplaced during a geologically brief time interval (10–20 years), which 36Cl cosmogenic dating puts at 35.7 ± 1.7 ka. Lidar imagery shows that these flows erupted from at least 28 vents encompassing multiple scoria cones, spatter cones, and craters. Flows can be grouped into four pulses using stratigraphic position and volume. Pulse 1 is the most voluminous, comprising eight eruptions and ∼2.3 km3. Each subsequent pulse started rapidly but decayed quickly, and each successive pulse erupted less lava (i.e., 2.3 km3 for pulse 1, 0.6 km3 for pulse 2, 0.3 km3 for pulse 3, and 0.2 km3 for pulse 4). Many of these flows host well-established lava channels and levees (with channel breakouts) that lead to lava fans, with some flows hosting lava ponds. Similar flow features from tholeiitic eruptions elsewhere demonstrate that these morphologies generally occur over weeks, months, or longer (e.g., Puʻu ʻŌʻō eruption at K–llauea, Hawaiʻi). This multidisciplinary study shows the range of eruptive styles and durations of a Cascades back-arc eruption and illustrates how potential future tholeiitic eruptive activity in the western United States might progress.

Introduction

An important objective of investigating active volcanic terrains is to understand hazards posed and how best to mitigate future risks. Geologic aspects necessary to understanding hazards include: 1) nature of vent(s); a single, long-lived vent vs. numerous, diffuse monogenetic vents, 2) eruptive styles that are predominantly effusive, explosive, or both, 3) erupted volumes, 4) geographic distribution of vents and eruptive products, 5) duration of eruptions or eruptive episodes, and 6) recurrence interval between eruptions or eruptive episodes. Satisfactorily investigating these aspects requires a multidisciplinary approach to unravel the geologic framework of a volcano or volcanic field.

The southern part of the Cascades volcanic arc in northern California, United States (Figures 1A,B), is a region with abundant vents that have experienced diverse eruptive processes and styles. This part of the Cascades volcanic arc encompasses Mount Shasta, Medicine Lake Volcano, and the Lassen Volcanic Center (Figure 1B). The high-standing, morphologically rough appearances of these volcanic regions testify to Late Pleistocene and Holocene eruptions that constructed and modified their edifices. Recognition that these volcanically active areas encompass young lava and pyroclastic flows, and thus pose different potential hazards, has been a motivating factor for geologic investigations that include field mapping, volcanic stratigraphy, petrography, paleomagnetism, geochemistry, and geochronology to elucidate the compositions, styles, durations, and timing of eruptions (e.g., ; ; ; , ; ; ; ; ).

FIGURE 1

). Mesozoic sedimentary and igneous rocks of the Klamath terrane are present west of Quaternary volcanic rocks (after ).

In northern California, the topographically subdued region east of the calc-alkaline arc front is the back-arc (Figure 1B), which is dominated by low-K olivine tholeiitic basalt (also commonly referred to as high-Al olivine tholeiitic basalt) throughout the Pleistocene. These tholeiitic basalts fill valleys and surround many of the older calc-alkaline volcanic edifices (; ; ; ; ). Some of these tholeiitic basalts have rough, primary surface morphologies owing to sparse vegetation in the arid environment, which makes them look youthful (Figures 2A,C,D). used the young appearance of flows to propose that more than a dozen eruptions occurred in the back-arc of northern California during the Holocene. Yet, only a few tholeiitic basalt eruptions in northern California have been studied in detail by field mapping, petrography, geochemistry, and geochronology (e.g., Giant Crater flow field by ; , Hat Creek Basalt by ; , and Eagle Lake tholeiitic basalts by ), with recent studies currently unraveling the volcanic stratigraphy, compositions, and timing of other eruptions in this region (; ; ). Despite the relatively infrequent eruption of tholeiitic basalts (>20 tholeiitic basalt eruptions from 1800 to 24 ka: ), the back-arc of northern California encompasses young-appearing eruptions throughout the Late Pleistocene and is considered volcanically active. Here, we investigate young-appearing, back-arc tholeiitic basalts of the Brushy Butte flow field (Figures 1B, 2A,B).

FIGURE 2

The Brushy Butte flow field differs from other typical monogenetic tholeiitic basalts in northern California in that its eruptions constructed a relatively high-standing edifice ∼150 m tall from at least 29 vents and (or) lava flows that we have grouped into four pulses. The distinct edifice and young appearance of the flow field prompted reconnaissance fieldwork to: 1) establish the veracity of the existing mapping (), 2) determine the age of what was considered a ‘very low threat volcano’ by the California Volcano Observatory (; ), and 3) determine the range of geochemical compositions of lavas from the flow field. This resulted in a multidisciplinary approach (see Supplementary Table S1 in the Supplementary Material for a list of samples and associated analyses undertaken) to resolve the eruptive styles, compositions, duration, and timing of emplacement of the Brushy Butte flow field and put this flow field into context with the surrounding volcanic terrain.

Our data and interpretations demonstrate that the edifice of the Brushy Butte flow field was constructed by a vent complex erupting flows during the Late Pleistocene. The tholeiitic basalts erupted have similar outcrop, hand specimen, and petrographic characteristics that are nearly identical to the characteristics of most surrounding tholeiitic basalts, but each of these basalts has a unique geochemical composition. As such, the Brushy Butte lavas are internally similar but geochemically distinct from surrounding, commonly young-appearing tholeiitic basalts (e.g., the Late Pleistocene flow field of Giant Crater).

The Brushy Butte flow field was emplaced over a geologically short time interval (years to decades) based on similarities in mean remanent directions of magnetization, with individual flows that make up the flow field erupting over weeks to months based on the development of volcanic features that form during long-duration extrusive events (e.g., well-established channels, levees, and lava ponds). Our research on the young-appearing eruptions of the Brushy Butte flow field demonstrates how future tholeiitic basalt eruptions in this region might progress.

Geologic Background

The Cascades volcanic arc is the surface manifestation of volcanism on continental crust of the North American plate due to subduction of the Explorer, Juan de Fuca, and Gorda oceanic plates along the Cascadia subduction zone (Figure 1A). Volcanism is most apparent as the remarkable, high-standing edifices of calc-alkaline stratovolcanoes (e.g., Mount Rainier, Mount Hood, Mount Shasta, etc.) that make up much of the surface expression of the Cascades volcanic arc (). In the southern part of the Cascades volcanic arc in northern California, Quaternary volcanism is concentrated at the long-lived volcanic centers of the Mount Shasta stratovolcano and around the volcanic fields of the Lassen Volcanic Center and Medicine Lake Volcano (Figure 1B). Radiocarbon and radiometric dating confirm the presence of Holocene eruptions from Mount Shasta, Medicine Lake Volcano, and the Lassen Volcanic Center (; ; ), but the only eruption documented first-hand was at Lassen Peak in 1914–1917 (; , ; ).

The southernmost locus of arc-related eruptions during the Quaternary is near Lassen Peak (in the Lassen Volcanic Center). The axis of the arc extends between Mount Shasta and Medicine Lake Volcano farther north into Oregon, Washington, and southern Canada (Figure 1A). For ∼50 km north of Lassen Peak, the arc front is expressed as prominent high-standing Middle and Late Pleistocene calc-alkaline (dominantly andesite and dacite) edifices, such as Magee Volcano, Freaner Peak, Burney Mountain, and Brush Mountain (Figure 1B; ; ; ). North of Brush Mountain for ∼70 km, Pleistocene calc-alkaline volcanic edifices are absent along the arc front. Situated east of the calc-alkaline arc front are relatively thin (typically 10–15 m thick, but thicker where they fill valleys), voluminous and laterally extensive, tholeiitic basalt flows that erupted throughout the Pleistocene (; ; ). These tholeiitic basalts are eruptive products of the back-arc and overlie and surround older Quaternary and Neogene calc-alkaline volcanic edifices that are earlier expressions of the eastward-migrating Cascades volcanic arc (; ).

Older tholeiitic basalts in the back-arc (predominantly those of the Early and Middle Pleistocene) tend to be deeply weathered, densely vegetated, commonly expressed as rounded boulders protruding from well-developed soils (sometimes >10 m thick). Late Pleistocene tholeiitic basalts are more conspicuous owing to the arid environment of northeastern California, with sparse vegetation, soil development, and erosion (Figure 2A). As such, most of the surface morphologies of Late Pleistocene basalt flows in the back-arc are well preserved, lending these tholeiitic basalts a young, rough appearance (Figures 2C–E). This appearance resulted in most of them being assigned to the Holocene (cf., ; ; ). However, several of these back-arc tholeiitic basalts now have isotopic ages showing them to be older than Holocene (Giant Crater flow field in , Hat Creek Basalt in , and Eagle Lake tholeiitic basalts in ).

Mapping of the Brushy Butte flow field and surrounding region was first undertaken by as a U.S. Geological Survey Wilderness Study Area, with their mapped units mostly incorporated into later mapping undertaken farther east by . The Brushy Butte flow field was assigned a Holocene age based on the relatively rough, sparsely vegetated flow surfaces present throughout much of its extent (Figures 2C–E; ; ). This Holocene age assignment resulted in designating the Brushy Butte flow field as having the potential to cause future ash and lava hazards equivalent to the largest basaltic flow and airfall tephra hazards (i.e., up to 10 km from vent) in the northern California back-arc. As a result, the Brushy Butte flow field was considered a ‘very low threat volcano’ in need of monitoring (; ); however, it has recently been taken off the threat list as a result of its stratigraphic position negating the Holocene eruption age () and the recognition that northern California back-arc tholeiitic basaltic eruptions are indicative of monogenetic volcanism (e.g., ; ). Despite being removed from the threat list, none of the aforementioned investigations dealt with the eruptive styles, compositions, or ages of the Brushy Butte flow field or surrounding tholeiitic basalts.

Methods and Results

Geologic Mapping

During this study, tholeiitic basalt flows were mapped in the field using petrographic characteristics in an attempt to identify contacts and stratigraphic superposition. However, petrographic similarities and the unreliable nature of using visual observations based on vegetation cover and type indicated that a multidisciplinary approach for discriminating between flows would be required. Geochemical and paleomagnetic data provide two independent means of discriminating between tholeiitic basalts in the back-arc of northern California (e.g., ; ; ).

Our mapping was supported by 1 m-resolution lidar (available from the U.S. Geological Survey 3D Elevation Program: https://www.usgs.gov/core-science-systems/ngp/3dep) to help identify contacts between flow units and locate potential sampling sites. Processing of lidar data strips away vegetation cover to show the underlying terrain, making the surface morphology of flows and other volcanic landforms more prominent. Flows from the Early and Middle Pleistocene show smoother surface morphologies as a result of extensive soil development and erosion. Late Pleistocene flows, while moderately to sparsely vegetated along internal flow contacts, faults, and in more scoria-rich deposits, still have relatively intact primary surface morphologies (Figures 2C,D). In particular, surface features such as well-established channels and levees, channel breakouts, lava ponds, inflated pāhoehoe surfaces, scoria cones, spatter cones, and craters are evident throughout the Brushy Butte flow field (Figure 2B). This vastly aids in understanding the emplacement history of these flows when integrated with other datasets (e.g., geochemistry, paleomagnetism, and geochronology). Additionally, the lidar imagery provides a vital window into parts of the flow field that cannot be directly sampled because they lie within Pit River tribal lands, Ahjumawi Lava Springs State Park, private property, or in terrain that is difficult to access. Using the lidar imagery, we can interpret stratigraphic context, flow morphologies, and make important inferences as to eruptive styles and emplacement processes. The integration of all of these data has resulted in a detailed geologic map of the Brushy Butte flow field and the flows and other geologic units with which it is in contact (Figure 3 and see Supplementary Figure S1 in the Supplementary Material for a high-resolution version of the geologic map).

FIGURE 3

Geochemistry and Petrography

Geochemical data were helpful for distinguishing various flows and identifying the locations of contacts throughout this region. A total of 82 lava samples from the Brushy Butte region were collected for major-oxide and trace-element analyses by wavelength-dispersive X-ray fluorescence (WD-XRF) spectrometry (after ; see the Supplementary Material for a description of the methods). Forty-three samples are from the Brushy Butte flow field, whereas the other 39 analyses are from surrounding flows and help distinguish them from the Brushy Butte lavas (see Supplementary Table S2 in the Supplementary Material for all analyses). Additionally, six samples from various lobes of the Brushy Butte flow field were analyzed by laser ablation-inductively coupled plasma-mass spectrometry (LA-ICP-MS) as a secondary check on internal variations of different eruptive pulses of the flow field (Table 1; see the Supplementary Material for methods).

TABLE 1

Sample numberB17DD077B18DD132B19DD166B19DD173B18DD147B18DD143Standard Deviations
PulsePulse 1Pulse 1Pulse 1Pulse 1Pulse 2Pulse 3
Unitbb3bb3bb3bb3bb14bb18
Latitude41.1214941.2268541.1721841.1208541.1821041.14699
Longitude−121.52218−121.43839−121.36870−121.37871−121.46946−121.51300
Ag0.030.030.040.040.040.030.00
As0.160.110.220.180.140.120.04
Ba65.4872.2774.2168.7876.4768.723.71
Bi0.010.010.000.010.010.000.00
Cd0.060.060.060.060.060.070.00
Cr207.60207.78212.71205.62204.82212.633.11
Cs0.050.030.030.030.040.040.01
Cu103.6997.64103.60130.62101.09111.7810.95
Ga14.9114.9315.0515.3915.4115.150.20
Hf1.141.141.181.261.201.280.06
Mo0.230.290.180.170.200.190.04
Nb0.750.780.860.740.870.770.05
Ni179.26181.34163.91143.86150.75161.0113.67
Pb0.690.640.650.670.630.670.02
Rb1.130.870.780.991.131.000.13
Sb0.020.020.020.030.020.030.00
Sc37.2237.2938.9441.6339.1438.631.47
Sn0.530.480.550.590.490.530.03
Sr226.13222.47224.32219.00223.19220.042.42
Ta0.110.090.110.090.090.090.01
Th0.150.170.180.140.160.160.01
Tl0.010.010.010.020.010.010.00
U0.050.050.050.030.050.040.01
V203.89201.19210.57219.49229.35209.119.57
Y20.9920.8122.1223.6822.1322.390.95
Zn66.1365.4666.2868.2766.3168.851.23
Zr43.1341.8645.8648.8844.0745.802.26
La2.182.282.392.342.282.340.06
Ce6.296.286.436.806.646.650.19
Pr1.091.101.121.181.111.130.03
Nd5.845.906.076.626.146.290.26
Sm2.022.042.072.262.022.160.09
Eu0.890.880.900.950.870.940.03
Gd2.622.632.802.992.702.830.13
Tb0.510.490.520.570.530.550.03
Dy3.343.393.583.823.613.610.16
Ho0.780.750.820.870.800.810.04
Er2.312.272.422.562.442.460.09
Tm0.360.350.370.400.380.380.02
Yb2.342.342.472.622.542.480.10
Lu0.360.350.380.390.380.380.01

Trace-element geochemical analyses of the Brushy Butte flow field.

Trace-element (as ppm) analysis were performed by laser ablation-inductively coupled plasma-mass spectrometry (LA-ICP-MS) at the Hamilton Analytical Lab at Hamilton College, Clinton, NY, United States (methods of ). Latitude and longitude are reported in WGS84. See the Supplementary Material for details on the method.

All but one of the tholeiitic basalt flows displayed on Figure 3 have very similar petrographic characteristics: diktytaxitic groundmass hosting 1–3% olivine phenocrysts of 1–2 mm diameter and rare (<<1%) plagioclase phenocrysts. The exception is the Thousand Springs flow, which has common (1–2%, to 1–2 mm) plagioclase phenocrysts that have resorbed cores with sieve textures and overgrowth rims. This flow also has a distinctive geochemistry, with a large range for many major-oxide and trace-element abundances. For example, the Thousand Springs composition ranges from 48.77 to 52.52 wt% SiO2 and 0.24 to 1.01 wt% K2O compared to 47.41 to 48.04 wt% SiO2 and 0.09 to 0.15 wt% K2O for the Brushy Butte flow field.

Both major oxides and trace elements are useful for distinguishing the other petrographically similar tholeiitic basalts as a result of magma chemistry being controlled by the degree, depth, and mineralogy of the metasomatized mantle lithosphere undergoing partial melting (e.g., ; ; ). Some of the major-oxide and trace-element abundances overlap, but significant differences allow distinct flows to be defined. Figure 4 shows a suite of plots used to distinguish the different tholeiitic basalt flows displayed on Figure 3. The Brushy Butte flow field tends to have relatively low, but slightly overlapping, abundances of TiO2 (0.69–0.89 wt%) with surrounding tholeiitic basalts at their given MgO abundances (Figure 4). As a result, the Brushy Butte geochemical field (gray area in Figure 4) generally plots in a distinct position for TiO2 versus other major-oxide and trace-elements. A distinct field is also noticeable for trace-element plots, particularly those using Zr, to discriminate the Brushy Butte geochemical field from surrounding tholeiitic basalts.

FIGURE 4

The Giant Crater flow field (Group 5 as mapped by ) directly contacts the west side of the Brushy Butte flow field and closely resembles these lavas (Figures 2A,B). Our whole-rock analyses from Giant Crater overlap the limited range of values for Group 5 presented in and . Brushy Butte and Giant Crater major-oxide abundances plot within close proximity and commonly overlap, although there are observable differences in FeO*, MnO, CaO, and K2O. On the other hand, trace-element values of Brushy Butte and Giant Crater rarely overlap, with characteristic differences in Sc, Cr, Ni, Sr, Rb, and in particular Zr (Figure 4; see Supplementary Table S2 in the Supplementary Material).

The high-standing (∼150 m tall) interior of the Brushy Butte flow field consists of many flows and vent systems that we have mapped as units bb1–bb29 and divided into four eruptive pulses (Figure 3). Geochemical analyses from the flow field shows that the mapped eruptive units, and eruptive pulses, are internally consistent geochemically. Brushy Butte early (?) and pulse 4 have only one analysis each, but both analyses fall within the range of Brushy Butte major-oxide and trace-element abundances from the other pulses (Figure 4). Available geochemical evidence is consistent with lavas from the Brushy Butte flow field being distinct from surrounding tholeiitic basalts with which they are in contact.

As a further evaluation of the internal consistency of the Brushy Butte flow field, six samples were analyzed by LA-ICP-MS (Table 1). These samples include four from pulse 1 (unit bb3), one from pulse 2 (unit bb14), and one from pulse 3 (unit bb18). The six samples analyzed by LA-ICP-MS all have small standard deviations and fall within analytical uncertainty of each other by this method (). For example, Zr abundances for these tholeiitic basalts are generally distinct and these values range from 41.86 to 48.88 ppm (standard deviation of 2.26). The combination of the whole-rock WD-XRF and LA-ICP-MS analyses supports the interpretation that lavas from the Brushy Butte flow field are magmatically identical to one another.

Paleomagnetism

Paleomagnetic data provide an additional and independent test for distinguishing visually and petrographically similar flows and locating contacts. This is a result of the brief timeframe during which the Earth’s magnetic field is stationary (4–5° per century of wander; ).

Paleomagnetic samples were collected, processed, and interpreted using the standard protocols outlined in , with a total of 28 sites from five tholeiitic basalt flows. Twenty of these sites were drilled in the Brushy Butte flow field, whereas the remaining eight sites were drilled in surrounding flows to aid in distinguishing them from the Brushy Butte flow field and each other (Table 2; see the Supplementary Material for methods). The Giant Crater flow field was not drilled for paleomagnetism as part of this study, as this flow field has been well characterized with presenting data from 58 drill sites.

TABLE 2

Unit / Sample NumberLatitudeLongitudeN/NoExp.IDα95kRPlatitudePlongitude
Brushy Butte flow field
B17DD08641.120−121.5408/8Li61.7354.71.414737.9952085.7174.3
B17DD09641.107−121.5209/9Li61.20.11.610398.9923088.8242.0
B18DD09941.113−121.5277/8Li61.9358.61.320496.9970787.7211.3
B18DD11041.193−121.4867/8Li60.90.91.99946.9939689.0280.7
B18DD12241.176−121.3697/8Li61.1348.62.18436.9928981.4159.2
B18DD15141.222−121.4578/9Li61.9356.02.16907.9898686.5182.6
B18DD13241.226−121.4378/8Li61.2356.91.029927.9976687.5173.1
B18DD15241.232−121.4398/8Mx59.9357.32.17727.9909087.9137.0
B18DD12441.147−121.5188/8Li60.2357.22.64747.9852387.9148.0
B18DD15041.184−121.4908/8Li63.02.91.611777.9940586.1271.3
B18DD14941.126−121.52512/122059.4355.61.1168210.9934686.5134.6
3B69841.126−121.37811/123059.1355.11.1175810.9943186.1131.7
B18DD12341.226−121.40811/122060.2357.31.0205110.9951288.0146.6
Pulse 1 average41.140121.47013/1360.9357.01.0163212.9926587.6169.3
B18DD14741.184−121.4726/8Li62.00.81.618365.9972887.8253.4
B18DD14841.185−121.4778/8Li59.8357.41.030487.9977087.9133.9
Pulse 2 average41.184121.4742/260.9359.06.017351.9994289.0195.6
B18DD12741.155−121.5158/8Li58.6357.42.17057.9900887.3107.1
B18DD14341.147−121.5128/8Li59.6354.63.32797.9748785.9139.7
B18DD12941.162−121.5117/7Li59.6359.21.517006.9964789.096.9
B18DD10541.155−121.51712/121057.9354.61.497111.9886785.1118.2
B18DD10641.162−121.51711/1210+58.1358.40.7477610.9979187.386.2
Pulse 3 average41.156121.5155/558.8356.81.334914.9988587.1115.3
Brushy Butte average (all analyses)41.140121.49020/2060.4357.10.8157819.9879687.9154.2
Thousand Springs flow
B17DD07941.209−121.5568/8Li44.46.41.98967.9922074.037.2
B17DD08141.129−121.5387/8Mx44.01.23.63246.9815074.654.4
B18DD10141.145−121.5215/9Li42.82.51.720414.9980473.650.6
B18DD10441.148−121.5248/8Li43.12.23.03437.9795873.851.2
Average41.160121.5304/443.63.12.120063.9998574.148.3
Adobe Flat flow
B18DD11841.230−121.4838/8Li54.526.22.26217.9887468.6336.9
B18DD11641.217−121.5006/8Li55.922.13.24385.9885972.2336.7
Average41.220121.4902/255.224.25.917671.9994370.4336.8
Timbered Crater flow
B17DD08041.190−121.4996/8Li71.242.83.93005.9833258.8285.9
Crum Reservoir flow
B18DD14141.087−121.3158/8Mx−37.0211.22.07927.99120−56.6176.9

Paleomagnetic analyses of the Brushy Butte flow field and surrounding tholeiitic basalts.

N/No, number of cores used compared with the number originally collected at the site; Exp., nature of site demagnetization analysis; Li, indicates that a vector component lines analysis was used, and Mx, indicates that a mixture of lines and planes was used to define the mean remanent direction; I, remanent inclination in degrees; D, remanent declination in degrees; α95, radius of the 95% confidence limit about the mean direction; k, estimate of the Fisher precision parameter; R, length of the resultant vector; Platitude and Plongitude–location in degrees north and east of virtual geomagnetic pole (VGP) calculated from the mean direction of the site. See the Supplementary Material for details on the method.

Figure 5A shows the range of mean remanent directions of magnetization for the Brushy Butte flow field and immediately adjacent tholeiitic basalts. Average inclination and declination values for the Brushy Butte flow field are 60.4° and 357.1° (95% confidence level; α95 = 0.8°), respectively. The most visually and morphologically similar basalt in contact with the Brushy Butte flow field is Group 5 of the Giant Crater flow field, for which four drilled sites give average inclination and declination values of 59.1° and 18.6° (α95 = 1.4°), respectively (). The inclinations of these two tholeiitic basalts are within error of each other, but their declinations are distinct. The other surrounding tholeiitic basalts are morphologically more subdued in general and also have inclinations and declinations distinct from those of the Brushy Butte flow field (Table 2 and Figure 5A), with the Thousand Springs flow having mean inclinations and declinations of 43.6° and 3.1° (α95 = 2.1°) and the Adobe Flat flow at 55.2° and 24.2° (α95 = 5.9°), respectively. The Timbered Crater flow records an excursional remanent direction at 71.2° and 42.8° (α95 = 3.9°), whereas the Crum Reservoir flow is reversely magnetized at −37.0° and 211.2° (α95 = 2.0°). Crum Reservoir is not shown on Figure 5A because of its reverse polarity.

FIGURE 5

Geochronology

Previous investigations in this region used soil development and vegetation to assign age constraints for flows (; ). While useful for assigning relative ages in certain parts of the map area on Figure 3, this approach has limited value as much of the area has been deforested and replanted or cleared for ranch land, and differences in internal surface flow morphologies promote vegetation growth at a range of rates and plant types. Isotopic dating is preferred for understanding the time intervals between eruptions in a given region, although this also is challenging, given the difficulty in finding groundmass or organic matter suitable to analyze from young tholeiitic basalts. Tholeiitic basalts have low abundances of K (0.09–0.15 wt% K2O for the Brushy Butte flow field; see Supplementary Table S2 in the Supplementary Material) and therefore low radiogenic 40Ar, so that Late Pleistocene and Holocene tholeiitic basalts are particularly hard to date by the 40Ar/39Ar method. Analyses of young tholeiitic basalts from northern California by the 40Ar/39Ar method have been successful but only on samples with a nearly perfect coarsely crystalline groundmass lacking vesicles and glass (e.g., ). The young ages of these basalts usually means that there is only minor erosion to expose dense, crystalline groundmass for 40Ar/39Ar dating unless they are cut by major, young faults. Additionally, the 14C method is commonly used for volcanic rocks that erupted <50 ka, but the same arid environment that has allowed remarkable preservation of surface morphologies resulted in the base of the flows not being exposed by erosion. This has made finding organic matter for the 14C method difficult, although not impossible, as collected charcoal samples dated at 12.4 ka from the Giant Crater flow field that stratigraphically overlies the Brushy Butte flow field.

A method that has proved useful for providing ages on young flows in arid environments that lack extensive vegetation cover and erosion is the 36Cl cosmogenic surface-exposure dating (e.g., ; ; ; ; ; ). We utilized the 36Cl cosmogenic method (see Supplementary Material for details on sample collection and analysis) for the Brushy Butte flow field to determine its emplacement age, and we couple this with 40Ar/39Ar ages of surrounding older tholeiitic basalts to better understand the eruptive history of volcanism prior to eruption of the Brushy Butte flow field.

A few dense, coarse-grained, crystalline samples were identified within the most basal exposed parts of the Brushy Butte flow field, and 40Ar/39Ar dating was attempted on five of these (Table 3; see the Supplementary Material for methods and Supplementary Table S3 for all tabulated 40Ar/39Ar data). These samples yielded ages with large analytical uncertainties (all reported at 1 σ) of 41 ± 27 ka, 48 ± 52 ka, 51 ± 17 ka, 51 ± 44 ka, and 165 ± 80 ka, which span from the Middle Pleistocene to Holocene at 95% confidence levels. Calculating a weighted mean age yields smaller analytical uncertainties of 48 ± 13 ka (using four of five analyses) and 52 ± 13 ka (using all five analyses); however, at the 95% confidence level these still span >25 kyr. The large analytical uncertainties using 40Ar/39Ar, and a lack of organic matter for 14C dating, prompted the collection of two primary surface rocks (Figure 2C) to date by the 36Cl cosmogenic surface-exposure method (Table 4; see the Supplementary Material for methods and Supplementary Table S4 for input parameters and output data for calculating the ages). Both surface-exposure ages are nearly identical at 35.4 ± 2.4 ka and 36.0 ± 2.4 ka (analytical uncertainties reported at 1 σ), which yields a weighted mean age of 35.7 ± 1.7 ka. This age overlaps with the 40Ar/39Ar ages but yields a significantly smaller analytical uncertainty and clearly places the Brushy Butte flow field within the Late Pleistocene.

TABLE 3

PlateauIsochronTotal gas
LavaFlow/ Sample NumberLatitudeLongitude% 39Ar (steps, °C)Age ± 1σ (ka)MSWD% 39Ar (steps, °C)Age ± 1σ (ka)MSWD40Ar/39Ari ± 2σAge ± 1σ (ka)
Brushy Butte flow field
B17DD07741.12149−121.5221896 (450–1050)−45 ± 560.396 (450–1050)51 ± 440.2296.8 ± 6.43 ± 66
B17DD08641.11923−121.5414092 (550–1050)191 ± 561.0100 (450–1150)51 ± 171.4302.4 ± 4.1332 ± 68
B17DD08741.12209−121.50322100 (450–1150)−4 ± 521.935 (850–1150)41 ± 271.1301.0 ± 43.868 ± 60
B17DD08841.11275−121.48695100 (450–1150)48 ± 521.8100 (450–1150)−123 ± 381.6302.7 ± 6.180 ± 53
B18DD14341.14699−121.5130083 (450–850)165 ± 801.183 (450–850)300 ± 1301.3296.1 ± 16.5411 ± 98
Weighted Mean Age 148 ± 130.03
Weighted Mean Age 252 ± 130.54
Adobe Flat flow
B18DD11441.24398−121.5050864 (750–1150)309 ± 450.564 (750–1150)309 ± 560.7298.5 ± 7.7621 ± 64
Timbered Crater flow
B17DD08041.18938−121.5003498 (550–1150)571 ± 492.098 (550–1150)428 ± 691.0306.4 ± 8.4760 ± 59
Vestal Swamp flow
B18DD14041.19340−121.3741371 (650–1050)1053 ± 520.871 (650–1050)964 ± 790.3305.7 ± 20.11385 ± 61
Crum Reservoir flow
B18DD14141.08481−121.3178174 (650–1150)1340 ± 590.174 (650–1150)1327 ± 810.2299.3 ± 10.31513 ± 60

40Ar/39Ar ages of the Brushy Butte flow field and surrounding tholeiitic basalts.

All samples are groundmass separates. Preferred ages are in bold. Samples were irradiated at the U.S. Geological Survey TRIGA reactor using 9.7946 ± 0.0033 Ma Bodie Hills sanidine as a neutron flux monitor (). Instrumental mass discrimination was calculated by repeated measurement of atmospheric argon and mass discrimination was calculated assuming atmospheric 40Ar/39Ar = 298.56 ± 0.31 (). Ages and errors were calculated using the 40K decay constants of of λEC = 0.581 × 10-10 yr-1, λβ- = 4.962 × 10-10y-1, and λTotal = 5.543 × 10-10y-1. MSWD — mean square of weighted deviates. Latitude and longitude are reported in WGS84. Weighted mean age 1 is calculated using samples (B17DD077, B17DD086, B17DD087, and B17DD088, whereas weighted mean age 2 is calculated using all five Brushy Butte flow field ages. See the Supplementary Material for details on the method and Supplementary Table S3 for the tabulated data and age-spectra from each sample analyzed.

TABLE 4

Sample numberLatitudeLongitudeElevation (mASL)Thickness (cm)Bulk density (g/cm3)SF36Cl/Cl (10-15) ± 1σ36Cl Atoms g-1 (105) ± 1σ36Cl/37Cl ± 1σ36Cl Ages (ka) ± 1σ
B18DD12641.15652−121.5127210445.52.281.0459.6 ± 9.73.71 ± 0.0815.37 ± 0.2736.0 ± 2.4
B18DD14441.14666−121.50854104662.011.0412.1 ± 9.83.86 ± 0.0911.10 ± 0.0335.4 ± 2.4
Sample numberSiO2TiO2Al2O3Fe2O3MnOMgOCaONa2OK2OP2O5LOIClBLiSmGdUTh
B18DD105a47.480.8217.3510.670.189.9310.972.410.100.080.018.663<101.82.68<0.050.1
B18DD143a47.520.8417.3010.640.189.9411.032.400.090.070.0115.554<102.13.060.140.6

36Cl cosmogenic surface-exposure ages from the Brushy Butte flow field.

All 36Cl cosmogenic surface-exposure ages (in bold) were calculated using the CRONUScalc 36Cl Exposure Age Calculator v2.0 () and the Lifton/Sato nuclide-dependent, time-dependent scaling model (). Whole-rock Cl concentrations were measured by isotope dilution at the Purdue Rare Isotope Measurement (PRIME) laboratory at Purdue University. Major-oxides (as wt%) were measured by wavelength-dispersive X-ray fluorescence (WD-XRF) and trace elements (as ppm) were measured by inductively coupled plasma-optical emission spectrometry (ICP-OES) following . SF is the topographic shielding factor. Latitude and longitude are reported in WGS84 and elevations are in meters above sea level (mASL).

a

Due to secondary minerals filling vesicles of surface samples B18DD126 and B18DD144, the ages for these were calculated using the whole-rock compositions of dense, vesicle-free proximal samples B18DD105 and B18DD143, respectively. See the Supplementary Material for details on the method and Supplementary Table S4 for the input parameters used to calculate the ages for sample analyzed.

Four samples from surrounding tholeiitic basalts in contact with the Brushy Butte flow field were analyzed by the 40Ar/39Ar method (Table 3). These flows underlie the Brushy Butte flow field and their 40Ar/39Ar ages are consistent with their stratigraphic position. The Adobe Flat flow erupted at 309 ± 45 ka, the Timbered Crater flow at 571 ± 49 ka, the Vestal Swamp flow at 1053 ± 52 ka, and the Crum Reservoir flow at 1340 ± 59 ka. Dateable material was not identified from the Thousand Springs flow, which is stratigraphically bracketed by the Brushy Butte flow field at 35.7 ± 1.7 ka and Adobe Flat flow at 309 ± 45 ka. The Timbered Crater cone consists of palagonitized ash that formed during a phreatomagmatic eruption. This cone overlies the Timbered Crater flow, but there is no clear evidence of any eruptive relationship between the cone and flow. A single tholeiitic basalt clast analyzed for geochemistry from the cone does not match the geochemistry of the flow, but it cannot be definitively determined whether this, and similar looking, clasts are juvenile or lithic. The Giant Crater flow field has a 14C age of 12.4 ka (), with reporting that the Giant Crater flow field overlies the Brushy Butte flow field. This relative age relation is remarkably difficult to see in the field or even using the 1 m-resolution lidar (Figures 2A,B). Our age for the Brushy Butte flow field confirms that it is older, and hence underlies, the Giant Crater flow field.

Discussion

The combination of geochemistry and paleomagnetism allows us to reliably map the extent of lavas from the Brushy Butte flow field, and geochronology has allowed them to be placed in their proper volcanic context within the back-arc of northern California (Figures 1B, 3). The 1 m-resolution lidar is a critical tool for interpreting the internal volcanic stratigraphy of the flow field, so that eruptive styles and emplacement processes can be interpreted. Using the 1 m-resolution lidar, we define 29 vents and (or) flows associated with eruption of the Brushy Butte flow field, which we label as units bb1–bb29 on Figure 3. This extends considerably the 12 eruptions proposed for the interior of the flow field. The most extensive and voluminous Brushy Butte flow (unit bb3 on Figure 3) was mapped as unrelated to the flow field by , who named it the Little Hot Springs Valley flow of the regional Modoc Basalt (unit mlhs on their map).

The eruptions that constructed the Brushy Butte flow field produced 26 flows and at least 28 vent areas (totalling 29 combined vents and [or] flows), including several scoria cones, spatter cones, and craters (Figure 3 and Table 5). These vents and flows built an edifice ∼150 m tall, and some of the flows reach >10 km from their vents. We infer the underlying topography to have been relatively flat and level (similar to the present-day Fall River Valley farther south), as the early erupted pāhoehoe flows (primarily unit bb3 on Figure 3) are distributed at mostly equal distances in a radial arrangement around the main central vent area. Later formed vents erupted predominantly ʻaʻā flows (Figures 2C,D) in the interior of the flow field; the ʻaʻā did not flow as far and built most of the interior edifice of the flow field (e.g., ). Table 5 summarizes the characteristics of each Brushy Butte eruptive unit, with areal extents, flow lengths, and eruptive volumes reconstructed where possible for the early flows that were subsequently buried.

TABLE 5

Pulse / Unit NameVent TypeLava Flow MorphologyMaximum Flow Length (m)Area (km2)Eruptive Volume (km3)
Early(?)
bb1At least 6 scoria conesNo lava0.00.820.01
bb25 small cratersPāhoehoe and ʻaʻā1.21.870.03
Pulse 1
bb3No ventDominantly pāhoehoe with minor ʻaʻā12.0140.07a2.10
bb4Scoria coneNo lava0.00.040.00
bb5Crater (300 × 200 m)Poorly-developed channel, predominantly pāhoehoe2.11.06a0.02
bb6Scoria coneNo lava0.00.050.00
bb72 spatter conesPoorly-developed channel and levees, predominantly pāhoehoe1.20.360.01
bb8Spatter coneChannel, levees, lava pond, predominantly pāhoehoe3.21.57a0.02
bb9Spatter coneChannels, levees, channel breakouts, pressure ridges, pāhoehoe and ʻaʻā2.21.130.02
bb102 spatter conesChannels, levees, channel breakouts, pressure ridges, pāhoehoe and ʻaʻā4.47.110.11
Pulse 2
bb117 small cratersChannels, levees, channel breakouts, lava pond, pressure ridges, pāhoehoe and ʻaʻā6.624.330.36
bb122 small cratersChannel, levees, pressure ridges, pāhoehoe and ʻaʻā1.60.570.01
bb132 craters (315 × 250 m for the largest)Channel, levees, perched lava pond, pressure ridges, pāhoehoe and ʻaʻā7.67.95a0.12
bb143 craters (110 × 90 m for the largest)Channels, levees, channel breakouts, lava pond, pressure ridges, pāhoehoe and ʻaʻā2.73.210.05
bb15Spatter coneChannel, levees, pressure ridges, pāhoehoe and ʻaʻā3.21.190.02
bb16Spatter conePoorly-developed channel, levees, predominantly ʻaʻā4.732.81a0.04
bb172 craters (50 × 50 m for the largest)Channels, levees, channel breakouts, pāhoehoe and ʻaʻā1.00.640.01
Pulse 3
bb184 spatter conesChannel, levees, channel breakouts, pressure ridges, pāhoehoe and ʻaʻā7.618.27a0.27
bb19Spatter coneChannel, levees, channel breakouts, pressure ridges, pāhoehoe and ʻaʻā2.91.530.02
bb20Spatter coneChannel, levees, channel breakouts, pressure ridges, pāhoehoe and ʻaʻā4.71.23a0.02
bb21Spatter conePoorly-developed channel and levees, pressure ridges, predominantly ʻaʻā1.30.330.00
bb222 spatter conesChannel, levees, channel breakouts, lava pond, pressure ridges, pāhoehoe and ʻaʻā1.20.490.01
Pulse 4
bb23Spatter coneChannels, levees, channel breakouts, pressure ridges, pāhoehoe and ʻaʻā4.510.620.16
bb24Spatter coneChannel, levees, channel breakout, pressure ridges, pāhoehoe and ʻaʻā1.91.260.02
bb25Spatter coneChannel, levees, pressure ridges, predominantly ʻaʻā, minor pāhoehoe4.81.620.02
bb26Spatter coneMultiple channels, levees, pressure ridges, pāhoehoe and ʻaʻā1.40.920.01
bb27Spatter conePredominantly pāhoehoe0.30.050.00
bb283 spatter cones and 1 crater (70 × 45 m)Pressure ridges, predominantly pāhoehoe, minor ʻaʻā0.60.330.01
bb29Spatter conePredominantly pāhoehoe0.30.090.00

Characteristics of the different vents and lava flows associated with eruption of the Brushy Butte flow field.

a

Denotes areas that were reconstructed due to burial by later lava flows from the Brushy Butte flow field. Reconstructed areas represent the most conservative estimates of areas that were buried.

Many vents can be tied to specific flows, with the exception of some of the early erupted units. For example, the vents of units bb4 and bb6 are within the interior of the Brushy Butte flow field and surrounded by later flows. These could be the vents for exposed flows that are not in contact as younger flows result in stranded cones, but this is difficult to determine based on similarities in geochemistry and paleomagnetism throughout the flow field. Two of the vent areas mapped as part of the flow field (units bb1 and bb2 on Figure 3) create topographic high areas along the southern margin of the flow field but both are stratigraphically below all other adjacent flows related to Brushy Butte. A sample from one of these vent areas (unit bb1) plots geochemically within the Brushy Butte flow field for all major-oxide and trace-element abundances. Access to the other vent system (unit bb2) is restricted, but its high-standing appearance and young-looking morphology suggest that it is also part of the flow field. Both units bb1 and bb2 are inferred to be vent systems for the earliest erupted part of the Brushy Butte flow field and any flows from them are suggested to be covered by younger flows.

Table 5 lists the range of geomorphic flow features present throughout the Brushy Butte flow field. These flows consist of both pāhoehoe (sometimes with inflated surfaces) and ʻaʻā with transitional flow types of slabby and rubbly pāhoehoe to platy ʻaʻā (Figures 2C,D,6A–D). A number of the Brushy Butte units host poorly developed to well-established lava channels and levees (Figures 6A–D), some with channel breakouts (Figure 6D), leading to lava fans. Pressure ridges are a common geomorphic feature for some of the longer ʻaʻā flows (Figure 6C). Some units (bb8, bb11, bb13, bb14, and bb22) host lava ponds (Figure 6B).

FIGURE 6

The Brushy Butte flow field is unusual for a northern California tholeiitic basalt in that multiple vents and flows have constructed a high-standing edifice at ∼150 m tall (Figure 2B). Tholeiitic basalts are generally tube fed and flow a long way (≥10 km) from their vent systems (e.g., ; ; ). The only flow in the flow field with a tube is in unit bb13 and this tube is <1 km long and has collapsed creating skylights (Figure 6B). Typically flow distances (≥10 km) for tholeiitic basalts can be far enough that it is often hard to find the low-lying vent systems from which the lavas erupted. However, the Brushy Butte flow field has constructed an unusually tall edifice, and the flows, particularly for early erupted unit bb3, are located no more than ∼10 km from their associated vent area.

We interpret the high-standing nature of the edifice of the interior of the Brushy Butte flow field to reflect the flat ground of the Fall River Valley (Figures 2A,B). Eruption of lavas on flat ground allowed it to spread out in relatively equal proportions across the landscape, as well as hindering the development of tube systems that would result in flows several tens of kilometers long. The newly emplaced flows, while relatively flat themselves, would create their own topographic barriers and result in the roughly radial pattern around the vent systems in the interior of the flow field. As subsequent flows erupted from new vents within the interior, they took advantage of the new topography and flowed into low-lying areas, filling in the new topography and creating additional barriers within the interior of the flow field. As the eruptive period progressed, significantly reduced erupted volumes resulted in shorter flows. As a result, many of the younger flows were almost entirely confined to the interior of the flow field. The continuing emplacement process gradually constructed the high-standing interior edifice of the Brushy Butte flow field.

Eruptive Pulses

We arranged the units that make up the Brushy Butte flow field into stratigraphic order, where possible, using the 1 m-resolution lidar imagery and field studies. Based on this stratigraphic order and erupted volumes, we have defined pulses of eruptive activity from the flow field (Figure 7). Most Brushy Butte units group into four pulses. Pulse 1 consists of eight Brushy Butte units (bb3–bb10) and total 2.27 km3 in eruptive volume, including the most voluminous (2.10 km3) lava flow in unit bb3. The remaining units in pulse 1 are inferred to have erupted after bb3 based on their high-standing positions within the interior of the flow field, and each has a significantly smaller volume totalling only 0.27 km3 for the other seven units of pulse 1 (Table 5). Pulse 2 consists of seven units (bb11–bb17) totalling 0.61 km3 in eruptive volume, with the first unit (bb11) making up 0.36 km3 of that total. Pulse 3 consists of five units (bb18–bb22) totalling 0.33 km3 in eruptive volume, with the first unit (bb18) making up 0.27 km3 of that total. Pulse 4 consists of seven units (bb23–bb29) totalling 0.22 km3 in eruptive volume, with the first unit (bb23) making up 0.16 km3 of that total.

FIGURE 7

The relative ages for pulses 2 and 3 are easy to reconstruct as there are ample places where direct contacts can be used to determine stratigraphic superposition. In pulses 1 and 4, however, flows are rarely in contact with each other. Therefore, the assigned unit number for flows from these pulses is somewhat arbitrary. For pulse 1, unit bb3 is easily inferred to underlie all flows erupted from the interior of the flow field based on its areal extent, despite its stratigraphic bracketing between units bb1 and bb10. This becomes more difficult for the rest of pulse 1, in which most units have no maximum relative age bracket because they are the oldest units exposed locally, with overlying bracketing units ranging anywhere from bb10 to bb23. Additionally, flows of pulse 1 are partly buried by younger flows from the flow field, with two vents (units bb4 and bb6) in the interior remaining uncorrelated with their flows. These vents could be the source(s) for exposed but disconnected flows, but no correlation can be made with the data on hand. As a result, we have mapped them as individual eruptive units attributed to the Brushy Butte flow field. On the other hand, units assigned to pulse 4 have no overlying units to bracket their relative ages, and none of these units are in direct contact. Underlying units can only constrain their relative ages to younger than bb13 (for bb28) or to younger than bb22 (for bb23). It is notable that map units bb25–bb29 in pulse 4 are relatively well aligned along the regional grain of normal faulting.

Brushy Butte units bb1 and bb2 have not been assigned to any pulse (they are labeled Brushy Butte early (?) on Figure 3), as it is unclear how these southern vent systems relate to the units erupted from the interior of the flow field. Only one sample from bb1 was collected for geochemistry, which is situated within the Brushy Butte geochemical field (Figure 4). The other early (?) erupted Brushy Butte map unit bb2 is densely faulted, but these faults only slightly extend into the overlying unit of bb11. This hints at bb2 being older than overlying Brushy Butte lavas, but not much older.

Despite these stratigraphic limitations, we can demonstrate, based on stratigraphic position, that the first eruption in each pulse 1–3 was the most voluminous, and we rely on this evidence to infer that the most voluminous eruption in pulse 4 (unit bb23) was also the first eruption of that pulse. All other flows assigned to pulse 4 were assigned a unit name arbitrarily, since they are not in direct contact. The erupted volumes of the other units in these pulses are too small to noticeably affect the volume distribution in Figure 7.

Just as each pulse shows an internal decay of eruptive volumes, each pulse itself shows a decrease in total eruptive volume from the previous pulse. Pulse 1 totals 2.27 km3, which decreases to 0.61 km3 for pulse 2, 0.33 km3 for pulse 3, and 0.16 km3 for pulse 4 (Table 5). This represents a decrease in eruptive volume of ∼73% from pulse 1 to pulse 2, ∼46% from pulse 2 to pulse 3, and ∼32% from pulse 3 and pulse 4.

Eruption Duration

Despite no Holocene eruptions occurring outside of the major, long-lived volcanic centers of Mount Shasta, Medicine Lake Volcano, and the Lassen Volcanic Center (Figure 1B), volcanic activity between these centers is a distinct possibility. The lack of a witnessed northern California back-arc eruption makes it unclear how long such an eruption might last. Both field and laboratory evidence from the Brushy Butte flow field, when combined with analogue eruption styles, provide insights into the duration of such an eruption.

Some of the most extensively studied, first-hand accounts of tholeiitic basalt volcanism are from the East Rift Zone on the Island of Hawaiʻi, where Puʻu ʻŌʻō erupted continuously from 1983 to 2018. Over 35 years, the Puʻu ʻŌʻō eruption covered an area of ∼144 km2 and erupted a volume of ∼4.4 km3, while developing many geomorphic flow features (e.g., ; ; ; ). Volcanic landforms are constructed over a range of rates, providing clues as to the duration of eruptive activity in older volcanic terrains. For example, inflated pāhoehoe surfaces as high as 4 m have been observed forming in Hawaiʻi over the course of ∼14 days (; ), a thickness similar to the 3–5 m inflated pāhoehoe from Brushy Butte. Unit bb3 has abundant inflated pāhoehoe surfaces, and we therefore propose that it took several weeks for the flow to be emplaced. The geomorphic features within the Brushy Butte flow field also suggest the possible duration of emplacement. These include well-established channel and levee systems with occasional breakouts and lava ponds (Figures 6A–D). Similar flow features in tholeiitic basalts of the Puʻu ʻŌʻō, as well as other K–llauea eruptions, demonstrate that these sorts of features develop and last over the course of weeks, months, or longer (; ).

Paleomagnetic analysis provides further clues into the eruptive duration of the Brushy Butte flow field. In particular, pulses 1 and 3 both have mean remanent directions of magnetization that yield tight precision with small α95’s. Pulse 1 encompasses 13 drill sites that yield a mean inclination of 60.9°, mean declination of 357.0°, and α95 of 1.0°. Pulse 3 yields a mean inclination of 58.8°, mean declination of 356.8°, and α95 of 1.6° from five drill sites (Figure 5B). While these two directions are very similar, an algorithm by indicates that they are distinct from each other at the 98% confidence level. Pulse 2 overlaps pulses 1 and 3 with a large α95 of 6.0° as a result of only two drill sites. This indicates that a very modest amount of time passed during these eruptions. For example, the immediately adjacent Giant Crater flow field is characterized by two distinct mean directions of remanent magnetization that are separated by 1.27° (from 58 drill sites) that has been modeled as an eruption spanning ∼15 years based on rates of geomagnetic polar wander (). Our results give a probable eruptive duration for the Brushy Butte flow field (at least pulses 1–3) of 10–20 years, based on the average 4–5° per century of wander ().

Conclusion

Our investigation of the Brushy Butte flow field illustrates what eruptive styles and durations of tholeiitic basalt volcanism could occur in the Cascades back-arc of the western United States. A multidisciplinary approach to studying back-arc regions within the western United States demonstrate that these monogenetic tholeiitic basalts can erupt over decades from multiple, migrating vent systems. Their extents and large volumes spread out across the landscape, with the potential to impact populations and infrastructure. Investigations of past monogenetic, tholeiitic back-arc eruptions can provide clues into how a future eruption might progress, such as the eruption and emplacement of the Brushy Butte flow field.

The Brushy Butte flow field erupted at 35.7 ± 1.7 ka, constructing an edifice that is ∼150 m tall, the longest flow lobes are >10 km long, and they cover an area of ∼150 km2 with an eruptive volume of at least 3.5 km3. These flows were erupted from at least 28 vent areas consisting of scoria cones, spatter cones, and craters. The flows contain well-established channels and levees, channel breakouts, lava ponds, lava fans with pressure ridges, and inflated pāhoehoe surfaces. The eruptions can be divided into four pulses based on relative flow stratigraphy and volume. Pulse 1 is the most voluminous at 2.27 km3 from eight eruptions; eruptive volumes decrease significantly to 0.61 km3 for pulse 2, 0.33 km3 for pulse 3, and 0.22 km3 for pulse 4. Geochemical similarities between flow units of these pulses suggest that the eruption was continuous with little or no crustal storage time. The volcanic landforms within the Brushy Butte flow field indicate that individual units erupted over a duration of several weeks to months. Differences in mean remanent directions of magnetization (at least from pulses 1–3) show noticeable differences that do not overlap at the 98% confidence level, and are used to propose that the Brushy Butte flow field erupted over 10–20 years. This investigation documents the migrating eruptive vents and lava flows that could arise during a future monogenetic, tholeiitic basalt eruption in the western United States, with activity possibly occurring in pulses over the course of decades.

Statements

Data availability statement

The original contributions presented in the study are included in the article/Supplementary Material, further inquiries can be directed to the corresponding author.

Author contributions

All authors undertook field mapping, stratigraphic studies, and participated in sample collection for analyses. DD and LM compiled the data into a map of the Brushy Butte flow field and surrounding flows. DD undertook sample preparation and analysis for the 40Ar/39Ar and 36Cl dating. DC undertook sample preparation and analysis for paleomagnetism. MC undertook hand sample and thin section petrography to identify minerals from each flow and help distinguish differences between them. All authors contributed to interpretations and had a hand in writing the article.

Funding

This work was supported by the U.S. Geological Survey California Volcano Observatory.

Acknowledgments

Thanks is owed to Peter Stent for access to his land during mapping and sample collecting. James Saburomaru, Dean Miller, Andrew Calvert, and Mark Stelten are thanked for help with the 40Ar/39Ar experiments. We appreciate the thoughtful reviews of Don Swanson, Aaron Pietruszka, Karoly Németh, Daniel Heaton, and the editorial handling of Rosa Anna Corsaro and Valerio Acocella, which greatly improved this paper. Any use of trade, firm, or product names is for descriptive purposes only, and does not imply endorsement by the United States government.

Conflict of interest

The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Supplementary material

The Supplementary Material for this article can be found online at: https://www.frontiersin.org/articles/10.3389/feart.2021.639459/full#supplementary-material.

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Summary

Keywords

Cascades volcanic arc, back-arc, tholeiitic basalt, lava flows, flow field

Citation

Downs DT, Champion DE, Clynne MA and Muffler LJP (2021) A Multidisciplinary Investigation Into the Eruptive Style, Processes, and Duration of a Cascades Back-Arc Tholeiitic Basalt: A Case Study of the Brushy Butte Flow Field, Northern California, United States. Front. Earth Sci. 9:639459. doi: 10.3389/feart.2021.639459

Received

09 December 2020

Accepted

08 February 2021

Published

19 March 2021

Volume

9 - 2021

Edited by

Rosa Anna Corsaro, National Institute of Geophysics and Volcanology, Italy

Reviewed by

Karoly Németh, Massey University, New Zealand

Daniel Heaton, Oregon State University, Corvallis, United States

Updates

Copyright

*Correspondence: Drew T. Downs,

This article was submitted to Volcanology, a section of the journal Frontiers in Earth Science

Disclaimer

All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article or claim that may be made by its manufacturer is not guaranteed or endorsed by the publisher.

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