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I ceI ceU d t di f t th i i itor .. Understanding frost weathering in-situ
Samuel Weber1, Lucas Girard2, Stephan Gruber2, Jan Beutel11ETHZ TIK 2UZH Geography 3G1ETHZ, TIK -- 2UZH, Geography, 3G
Lab experiment Reality
2006
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What stresses near-surface bedrock ?What stresses near-surface bedrock ?What stresses near surface bedrock ?What stresses near surface bedrock ?
A. Hasler
What stresses near-surface bedrock ?What stresses near-surface bedrock ?What stresses near surface bedrock ?What stresses near surface bedrock ?
Constant mechanical loads:Constant mechanical loads:• Gravity• (Overburden pressure)
A. Hasler
What stresses near-surface bedrock ?What stresses near-surface bedrock ?What stresses near surface bedrock ?What stresses near surface bedrock ?
Constant mechanical loads:Constant mechanical loads:• Gravity• (Overburden pressure)
Fluctuating loads:Fluctuating loads:• Water pressure, Ice formation in pores/cracks• Thermo-mechanical forcing
E h kEarthquakes
A. Hasler
What stresses near-surface bedrock ?What stresses near-surface bedrock ?What stresses near surface bedrock ?What stresses near surface bedrock ?
Constant mechanical loads:Constant mechanical loads:• Gravity• (Overburden pressure)
Fluctuating loads:Fluctuating loads:• Water pressure, Ice formation in pores/cracks• Thermo-mechanical forcing
E h kEarthquakes
A. Hasler
State of the artState of the artState of the artState of the art
Theoretical & lab. insights:Theoretical & lab. insights:
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State of the artState of the artState of the artState of the art
Theoretical & lab. insights: Transfer to field conditions, where rock Theoretical & lab. insights:already contains flaws/cracks ?
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State of the artState of the artState of the artState of the art
Theoretical & lab. insights: Transfer to field conditions, where rock Theoretical & lab. insights:already contains flaws/cracks ?
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) Range of temperature ? Sensitivity to liquid water content ?
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Sensitivity to liquid water content ? Nucleation of new cracks or
ti f i ti ?
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propagation of existing ones ?
(Mur
Measurement strategyMeasurement strategyMeasurement strategyMeasurement strategy
Acoustic emission (AE) monitoring:Acoustic emission (AE) monitoring:detect small “damage increments”
F 20 100 kHFrequency range: 20-100 kHz• Chose for expected source size Detection range:p• Length scale 1-10cm• Displacement scale 0 1-1μm
g• controlled by freq. range• expect most signals from <0 5 to 1mDisplacement scale 0.1 1μm
• Eq. magnitude -6 to -5expect most signals from <0.5 to 1m
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AE monitoring system: instrumentation and field set-upAE monitoring system: instrumentation and field set-upAE monitoring system: instrumentation and field set upAE monitoring system: instrumentation and field set up
12 V
AE node
AE Sensors(at 10 & 50 cm depth)(at 10 & 50 cm depth)
Temperature probe
Capacitance probe
10
Capacitance probe
WSN d 10cmWSN nodes
50cm
100cm
Depth
The measurement positionsMeasurement site at Jungfraujoch: 2 complete installationsMeasurement site at Jungfraujoch: 2 complete installationsMeasurement site at Jungfraujoch: 2 complete installationsMeasurement site at Jungfraujoch: 2 complete installations
September MarchM1September MarchM1M1M1Spur
M2
M2Densely fractured crystaline rock: GullyDensely fractured crystaline rock:• 5 - 20 clefts / meter• Crack opening .1-1mm
AE signal characteristicsAE signal characteristicsAE signal characteristicsAE signal characteristics
Signal waveform Spectrogram
(kH
z)
100
(dB
)
65
70
75
0
1
2
(V)Hammer
Freq
. (
0
50 Am
p.
55
60
2
−1
0A
mp.test
Time (msec)0 0.5 1 1.5 2
00 0.5 1 1.5 2
−2
Time (msec)
AE signal characteristicsAE signal characteristicsAE signal characteristicsAE signal characteristics
Signal waveform Spectrogram
(kH
z)
100
(dB
)
65
70
75
0
1
2
(V)Hammer
Freq
. (
0
50 Am
p.
55
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−1
0A
mp.test
Time (msec)0 0.5 1 1.5 2
00 0.5 1 1.5 2
−2
Time (msec)
kHz)
100
dB)58
60
0.5
(V)
Freq
. (k
50 Am
p. (d
52
54
560
Am
p.
Acoustici i
Time (msec)
0 0.2 0.4 0.6 0.8 1 1.2 1.4
00 0.2 0.4 0.6 0.8 1 1.2 1.4
−0.5
Time (msec)
2
emissions(real ones!)
. (kH
z) 100
p. (d
B)
65
70
75
1
2
p. (V
)
( )
Freq
0 0 5 1 1 5 2
0
50 Am
55
60
0 0 5 1 1 5 2−1
0Am
Time (msec)0 0.5 1 1.5 20 0.5 1 1.5 2
Time (msec)
AE signal characteristicsAE signal characteristicsAE signal characteristicsAE signal characteristics
Signal waveform Spectrogram
(kH
z)
100
(dB
)
65
70
75
0
1
2
(V)Hammer
Freq
. (
0
50 Am
p.
55
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−1
0A
mp.test
Time (msec)0 0.5 1 1.5 2
00 0.5 1 1.5 2
−2
Time (msec)
kHz)
100
dB)58
60
0.5
(V)
Freq
. (k
50 Am
p. (d
52
54
560
Am
p.
Acoustici i
Time (msec)
0 0.2 0.4 0.6 0.8 1 1.2 1.4
00 0.2 0.4 0.6 0.8 1 1.2 1.4
−0.5
Time (msec)
2
emissions(real ones!)
. (kH
z) 100
p. (d
B)
65
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p. (V
)
( )
Freq
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50 Am
55
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0 0 5 1 1 5 2−1
0Am
Time (msec)0 0.5 1 1.5 20 0.5 1 1.5 2
Time (msec)
0.2
0.4
V)
Hz)
100 B)60
62
N i−0.2
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Am
p. (V
Freq
. (kH
50
100
Am
p. (d
B
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58Noise(rubbish)
0 0.5 1 1.5 2−0.4
Time (msec) Time (msec)
0 0.5 1 1.5 2
0( )
1year timeseries: rock temperature AE activity1year timeseries: rock temperature AE activity1year timeseries: rock temperature, AE activity1year timeseries: rock temperature, AE activity
Rock temperaturep
10cm5 cm
50cm
Temp. gradientTemp. gradient
10-20 cm5-10 cm
10 20 cm20-50 cm
Spur site (M1)10cm
Spur site (M1)
50cm
Gully site (M2)Gully site (M2)
1year timeseries: rock temperature AE activity1year timeseries: rock temperature AE activity1year timeseries: rock temperature, AE activity1year timeseries: rock temperature, AE activity
Simple facts:p
1year timeseries: rock temperature AE activity1year timeseries: rock temperature AE activity1year timeseries: rock temperature, AE activity1year timeseries: rock temperature, AE activity
Simple facts:p
Energy rates under frozen conditions are roughly 100 times larger than g y gunder thawed conditions
d f hSustained freezing vs. Freeze-Thaw:• February= sustained freezing +1 cycle• March = 17 cycles• E(February) > 15*E(March)( y) ( )
1year timeseries: rock temperature AE activity1year timeseries: rock temperature AE activity1year timeseries: rock temperature, AE activity1year timeseries: rock temperature, AE activity
Simple facts:p
Energy rates under frozen conditions are roughly 100 times larger than g y gunder thawed conditions
d f hSustained freezing vs. Freeze-Thaw:• February= sustained freezing +1 cycle• March = 17 cycles• E(February) > 15*E(March)( y) ( )
Energy rates in the gully (M2) are 10 times larger than on the spur (M1) under frozen conditionsu de o e co d t o s
Rock freezing characteristic curveRock freezing characteristic curveRock freezing characteristic curveRock freezing characteristic curve
Decrease in liquid water content during freezingDecrease in liquid water content during freezing
Gully siteGully site(M2)
S itSpur site(M1)( )
Measurements from capacitive probes (Envirosmart)Data: Oct 2011 Oct 2012Data: Oct 2011 – Oct 2012
Influence of freezing on AE activityInfluence of freezing on AE activityInfluence of freezing on AE activityInfluence of freezing on AE activity
Only events at 50cm considered here
Spur site (M1)5050cm
Gully site (M2)50cm50cm
Are AE scaling properties affected by the loading mode ?Are AE scaling properties affected by the loading mode ?Are AE scaling properties affected by the loading mode ?Are AE scaling properties affected by the loading mode ?
Frozen = T<0 in the whole rock column (5cm – 100cm)Thawed = T>0 at 5- 100cmThawed = T>0 at 5- 100cm
3 03.0
i i i iMicro-seismic events in large rock slide: 2.6Earthquakes: 2.0(Helmstetter & Garambois 2010,
)Kagan 1999)
Energy, duration, waiting times also power-law distributed
ConclusionsConclusionsConclusionsConclusions
At our site, frost cracking is the largest damage driver N f t ki i d No frost cracking window Strong control of water availability on frost cracking Strong control of water availability on frost cracking
Factor ~10 here
Rock damage dynamics appear independent of the loadingRock damage dynamics appear independent of the loading mode (i.e. freezing vs. thermo-mechanical forcing)o ( g g) Similar flaws activated by both loading modes D i d d b ti f i ti fl / k Damage induced by propagation of existing flaws/cracks Suggests the importance “Macro-gelivation” Suggests the importance Macro gelivation
Frost heave in soils: growth of ice lenses through cryo-suctionFrost heave in soils: growth of ice lenses through cryo-suctionFrost heave in soils: growth of ice lenses through cryo suction Frost heave in soils: growth of ice lenses through cryo suction
IceUnfrozen water
ColderColder
OverburdenOverburdenpressure
IceDepression= Ice
Liq water
Depression=Suction of liq. water
Liq. water
Disjoining
GrainSoil particle
Disjoiningforces
Warmer
(Taber 1930, Rempel 2007, …)
Frost heave in soils: growth of ice lenses through cryo-suctionFrost heave in soils: growth of ice lenses through cryo-suctionFrost heave in soils: growth of ice lenses through cryo suction Frost heave in soils: growth of ice lenses through cryo suction
IceUnfrozen water heave
ColderColder
Rupture Ice lens
Grain
Warmer
(Taber 1930, Rempel 2007, …)
How can freezing deform materials?How can freezing deform materials?How can freezing deform materials?How can freezing deform materials?
When freezing, Under sustained freezing:When freezing,water expands by 9%
Under sustained freezing:growth of ‘segregated ice’
- expulsion of liquid water towards unfrozen zones
- fueled by suction of water towards already frozen zonesunfrozen zones
- in rapid freezing conditions: already frozen zones
- can fracture rock and heave soilsp gincrease of pore pressure damage ? damage ?
(Murton et al. 2006)
let rock crack, let cracks rock 25
AE monitoring systemAE monitoring systemAE monitoring systemAE monitoring system
AE sensorAE sensor– Piezoelectric sensor R6α-sensor:
35-100 kHz, resonant at 55 kHzAE rodAE-rod
– Houses the piezoelctric sensorHouses the piezoelctric sensor– Rock-sensor acoustic coupling
with ~2 dB lossAdjustable sensor depth– Adjustable sensor depth
– Other rod materials reflect & attenuate acoustic wavesOther rod materials reflect & attenuate acoustic wavesAE-node
– acquisition, processing andt i i f AE d ttransmission of AE data
– 2 channels 500 kHz sampling rate2 channels, 500 kHz sampling rate– Wireless data transmission– Threshold remotely adjustable
Estimating rock liquid water contentEstimating rock liquid water contentEstimating rock liquid water contentEstimating rock liquid water content
Sentek Envirosmart:Sentek Envirosmart:Material dielectric constant as a proxy for liquid water content
Generate electrical field in radio‐freq range measure resonant frequency (and material capacitance)obtain material dielectric constant εmatεmat strongly depends on liquid water content
Freq. range 100‐300 MHzDielectric constants involved:•εrock=2‐5•εair=1•εice=3•εwater=80‐100
Fabbrriet al. 2006
AE signals: how to select the right ones ?AE signals: how to select the right ones ?AE signals: how to select the right ones ?AE signals: how to select the right ones ?> 650 000 events detected> 650 000 events detected
Analogy to lab. rock fracturing experiments:D= k1 * A + k2
fracturing experiments:1 2
(Cox & Meredith 1993)
AE signals: how to select the right ones ?AE signals: how to select the right ones ?AE signals: how to select the right ones ?AE signals: how to select the right ones ?> 650 000 events detected> 650 000 events detected
Analogy to lab. rock fracturing experiments:fracturing experiments:D= k1 * A + k2
(Cox & Meredith 1993)1 2
Event generated by an artificial rock fall
+an artificial rock fall(~50 liters)
We cannot strictly exclude the effects of rock falls,l h f d t t!or snow avalanches from our dataset!
Results: AE signalsResults: AE signals103
Results: AE signalsResults: AE signals
102
10Class 1Class 2Class 3Cl 4
+ Class 1Cl 2
101Class 4Class 2
Class 3
10−1
100
PD
F
Class 4
10−2
P
−4
10−3
−1 010−5
10−4
10 1 100
Amplitude (V)
100
2
Class 1Class 2Class 3Class 4
10−2 Class 4
10−4
PD
F
10−6
P
10−8
101 102 103 104 105
10 10 10 10 10Duration (s)
Are AE scaling properties affected by the loading mode ?Are AE scaling properties affected by the loading mode ?Are AE scaling properties affected by the loading mode ?Are AE scaling properties affected by the loading mode ?1 96 2 30 1 99Frozen = T<0 in the whole rock column (5cm – 100cm)
102expo:3.07, expo:3.72, expo:3.35,
frozen
102expo:1.96, expo:2.30, expo:1.99,
frozenth d
( )Thawed = T>0 at 5‐ 100cm
101
frozenthawedall 100
thawedall
100
3.0 10−2
2.010−1
3.0
10−4
PDF 2.0
10−2
10−6
10
10−3
10 6
10−1 10010−4 10−2 100 10210−8
Energy (V2)
expo:3 20 expo:3 28 expo:3 2310 10Amplitude (V)
Energy (V )100
expo:3.20, expo:3.28, expo:3.23,
frozenthawedMicro‐seismic events in rock slide: 2.6
10−2
thawedallEarthquakes: 2.0
(Helmstetter & Garambois 2010,
F 3 2
Kagan 1999)
10−4
PD
F 3.2
10−6
8
102 10310−8
Duration (s)
Freezing vs thermo-mechanical forcingFreezing vs thermo-mechanical forcingFreezing vs. thermo mechanical forcingFreezing vs. thermo mechanical forcing