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Ecophysiological Impacts of
Climate Change: Performance,
Fitness, and Extinction
Eric Riddell, PhD
Assistant Professor
Ecology, Evolution, and Organismal Biology (EEOB)
Iowa State University
Caroline Williams, PhD
Associate Professor
Integrative Biology
University of California, Berkeley
Experts discuss their research involving
climate change and the ecophysiological
effects of changing global temperatures
on organismal biology and survival.
Ecophysiological Impacts of
Climate Change: Performance,
Fitness, and Extinction
Winter in a Changing World:
The Critical Importance of Snow
Copyright 2021 C. Williams and InsideScientific. All Rights Reserved.
Caroline Williams, PhD
Associate Professor
Integrative Biology
University of California, Berkeley
Winter is warming faster than summer
Winter warming is having widespread
impacts on biodiversity
Osland et al. 2021 Global Change Biology
Winter warming decreases snowpack
Mote et al. 2018. Clim. Atmos. Sci.
Northern hemisphere spring snowpack
anomalies, 1980 - 2020
Marshall et al. 2020 Curr Opin Insect Sci
Red = decreased
snowpack
Spring snowpack changes,
1955-2016
Sierra Nevada
mountain range,
California USA
Snow cover fluctuates in the Sierra Nevada
Joshua Cripps Photography
June 22nd 2006
June 22nd 2007
Nathan Rank
Many ectotherms overwinter beneath snow
AgPest.co.nz
Ferdinand Bada
Andy Murray
Joseph Berger
Tristram Brelstraff
Jon Costanza
Snow determines soil microclimate, and thermal stress
Cold snap
Big snow fall
“Colder soils in a warmer world”
-Groffman, 2001
Sources of mortality in winter
Energy depletion
Cold mortality
Colder soils in a warmer world:
Loss of snow cover will increase cold stress but decrease energy stress
Organismal traits determine response to
microclimate temperatures
Sinclair et al. 2015 J. Therm Biol
Irwin & Lee. 2003 Oikos
Energy use Cold tolerance
Metabolic
rate
Temperature
LT50 (1hr exposure)
Moving up a
mountain…
We do not know
how thermal
stress on
overwintering
ectotherms in the
soil changes
along a snowy
elevational
gradient
Energy
depletion
Cold
mortality
Soil temperature ???
Air temperature
Snow cover
Research question
How does changing snow cover impact cold and
energetic stress, for organisms that overwinter in
the soil in snowy mountains?
Sierra willow leaf beetle,
Chrysomela aeneicollis
Southern range edge of species range
illustrations: Hiroko Udaka
Sierra Nevada
Rich history of study
1980 – 2020
Microclimate
monitoring network
Beetle surveys
Physiology and
genetics
Collaborators Elizabeth Dahlhoff and Nathan Rank, with
PhD candidate Kevin Roberts
Bishop CA
How does snow impact cold stress and energy stress on
overwintering beetles along an elevational gradient?
Environment
Microclimate temperatures
Spatial and temporal variation in
snow cover
Laboratory
Metabolic rate-temperature
curves
Cold tolerance limits (acute and
chronic exposures)
Energy reserve assays
Field
Population surveys (phenology)
Snow manipulation experiments
Ecophysiological Models
Energy and Cold Stress
test
test
Kevin Roberts
Environment: spatial and temporal
variation in snow cover
Roberts et al. in review GCB
Snowy
Dry
28 sites,
1980 – 2020
Hourly soil
temperatures
5 replicate transects
Bishop CA
Spatial variation Interannual variation
climate
change
Snow alters elevational gradients
in cold exposure
Cold exposure peaks at
mid-elevation, and is
higher in dry years
Roberts et al. in review GCB
Ecophysiological energy use model
1) Estimate metabolic rate –
temperature curves using respirometry
2) Input microclimate data to estimate
oxygen consumption throughout winter
3) Select start and end dates and sum to
get oxygen used over winter (repeat
iteratively for range of start and end
dates observed in field)
4) Convert to energy used (2L oxygen =
1g lipid, compare to empirical
measurements
Snow
Present
Snow
Excluded
Field
Experiment
0.589 mg 0.398 mg
Model
Estimate
0.591 mg 0.417 mg
Model
Accuracy
99.7% 95.2%
Validated model is >95%
accurate in predicting energy use
in snowy and dry conditions
Lab validation of energy use models
Roberts et al. in prep
Energy use across elevation
Energy use declines with
increasing elevation, steeper
decline in snowy years due
to very high energy use at
low elevations
Snowy years are longer, and
more energetically demanding
Roberts et al. in review GCB
Climate change will alter cold exposure
and energy use across the mountains
Long Lake, Bishop Creek
Roberts et al. in review GCB
Cold mortality likely occurs due to long freezing
periods
LT50 (1hr exposure)
Lethal time frozen
Cold and energy stress across elevation
• Probability of lethal
cold is highest at
mid-elevations, not
impacted by
interannual variation
in snow cover
Roberts et al. in review GCB
• Probability of lethal
cold is highest at
mid-elevations, not
impacted by
interannual variation
in snow cover
• Probability of lethal
energy depletion is
highest at low
elevations, and in
snowy years
Cold and energy stress across elevation
Roberts et al. in review GCB
Conclusions
• Trade-off between cold mortality and energy depletion is
modulated by interannual variation in snow cover
• Snow alters elevational gradients in cold and energy stress,
potentially altering selective gradients on these traits for
overwintering ectotherms
• Impact of interannual variation in snow cover depends on
elevation – high elevations will be buffered due to persistent
snow cover, and mid elevations will experience increased cold
stress
• Environment (microclimate) and organismal traits together
determine stress exposure
Take-home message:
Climate Change Global Warming
“Colder soils in a warmer world”
– Groffman 2001
Thank you!
Collaborators:
Kevin Roberts
Nathan Rank
Elizabeth Dahlhoff
Jonathon Stillman
Doris Bachtrog
Ryan Bracewell
Andre Szejner Sigal
Lisa Treidel
Christina Lee
Varun Bahl
Rose Kang
Kamalakar Chatla
Colleagues:
Brent Sinclair
Dan Hahn
Ray Huey
John Smiley
Greg Ragland
Michael Kearney
Research Facilitation:
White Mountain Research Station
Denise Waterbury
Williams lab: Ecological and Evolutionary Physiology
https://www.cmwilliamslab.com/
Sable Systems for all the great respirometry equipment!
Using Ecophysiology to
Predict Extinction Risk
From Climate Change
Copyright 2021 E. Riddell and InsideScientific. All Rights Reserved.
Eric Riddell, PhD
Assistant Professor
Ecology, Evolution, and Organismal Biology (EEOB)
Iowa State University
How does physiology determine the niche?
Ecophysiology
Understanding how organisms
function in their environment
Ecophysiology
Understanding how organisms
function in their environment
Organism
Organ
Organism
Tissue
Organ
Organism
Cell
Tissue
Organ
Organism
Genes
Cell
Tissue
Organ
Organism
Temperature
Humidity
Organism Environment
Biophysics links physiology to the local environment
𝜇 = 𝜇0
𝑇0 + 𝐶
𝑇 + 𝐶
×
𝑇
𝑇0
3
2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
𝑟𝑏 =
0.93 × 𝜌 × 𝐶𝑝
ℎ𝑐
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics links physiology to the local environment
𝜇 = 𝜇0
𝑇0 + 𝐶
𝑇 + 𝐶
×
𝑇
𝑇0
3
2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
𝑟𝑏 =
0.93 × 𝜌 × 𝐶𝑝
ℎ𝑐
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Environment
Performance
Biophysics links physiology to the local environment
𝜇 = 𝜇0
𝑇0 + 𝐶
𝑇 + 𝐶
×
𝑇
𝑇0
3
2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
𝑟𝑏 =
0.93 × 𝜌 × 𝐶𝑝
ℎ𝑐
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Organism Environment
Organism
𝜇 = 𝜇0
𝑇0 + 𝐶
𝑇 + 𝐶
×
𝑇
𝑇0
3
2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝑟𝑏 =
0.93 × 𝜌 × 𝐶𝑝
ℎ𝑐
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Environment
𝜇 = 𝜇0
𝑇0 + 𝐶
𝑇 + 𝐶
×
𝑇
𝑇0
3
2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
𝑟𝑏 =
0.93 × 𝜌 × 𝐶𝑝
ℎ𝑐
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics
Southern Grey-cheeked Salamander
Plethodon metcalfi
Southern Grey-cheeked Salamander
Plethodon metcalfi
Natural and life history
Fossorial
Nocturnal
Fully terrestrial
Lungless
High water loss rates restrict salamanders to high elevations
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics
Physiology
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Activity
Biophysics
Physiology
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Foraging
Activity
Biophysics
Physiology
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Foraging
Activity
Biophysics
Physiology
Fitness
Foraging
Activity
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics
Physiology
Fitness
Net energy balance (J)
Activity time (hr)
30-
0 -
-30-
7-
3.5-
0-
Riddell et al. 2017; Ecol. Monogr.
83% of known localities can reproduce
Physiology helps to predict geographic range of salamanders
30-
0 -
-30-
7-
3.5-
0-
Physiology helps to predict geographic range of salamanders
Riddell et al. 2017; Ecol. Monogr.
Net energy balance (J)
Activity time (hr)
83% of known localities can reproduce
Organism
𝜇 = 𝜇0
𝑇0 + 𝐶
𝑇 + 𝐶
×
𝑇
𝑇0
3
2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝑟𝑏 =
0.93 × 𝜌 × 𝐶𝑝
ℎ𝑐
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Environment
𝜇 = 𝜇0
𝑇0 + 𝐶
𝑇 + 𝐶
×
𝑇
𝑇0
3
2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
𝑟𝑏 =
0.93 × 𝜌 × 𝐶𝑝
ℎ𝑐
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics
Organism
𝜇 = 𝜇0
𝑇0 + 𝐶
𝑇 + 𝐶
×
𝑇
𝑇0
3
2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝑟𝑏 =
0.93 × 𝜌 × 𝐶𝑝
ℎ𝑐
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
𝜇 = 𝜇0
𝑇0 + 𝐶
𝑇 + 𝐶
×
𝑇
𝑇0
3
2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
𝑟𝑏 =
0.93 × 𝜌 × 𝐶𝑝
ℎ𝑐
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics
Organism
𝜇 = 𝜇0
𝑇0 + 𝐶
𝑇 + 𝐶
×
𝑇
𝑇0
3
2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝑟𝑏 =
0.93 × 𝜌 × 𝐶𝑝
ℎ𝑐
𝜇 = 𝜇0
𝑇0 + 𝐶
𝑇 + 𝐶
×
𝑇
𝑇0
3
2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
𝑟𝑏 =
0.93 × 𝜌 × 𝐶𝑝
ℎ𝑐
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics
Organism
𝜇 = 𝜇0
𝑇0 + 𝐶
𝑇 + 𝐶
×
𝑇
𝑇0
3
2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝑟𝑏 =
0.93 × 𝜌 × 𝐶𝑝
ℎ𝑐
Climate
Change
𝜇 = 𝜇0
𝑇0 + 𝐶
𝑇 + 𝐶
×
𝑇
𝑇0
3
2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
𝑟𝑏 =
0.93 × 𝜌 × 𝐶𝑝
ℎ𝑐
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics
Will climate change threaten salamanders with extinction?
Phenotypic plasticity
The expression of multiple phenotypes
from a single genotype
Temperature
(°C)
VPD
(kPa)
Riddell et al. 2018, Science Advances
Salamanders experience seasonal changes in the environment
N = 180 N = 180
Resistance
(s/cm)
Oxygen
Consumption
(uL/hr)
Salamanders adjust metabolism and water loss to seasonal changes
Linking plasticity to extinction risk from climate change
Climate
Linking plasticity to extinction risk from climate change
Climate
Microclimate
Linking plasticity to extinction risk from climate change
Climate
Microclimate
Physiology
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Linking plasticity to extinction risk from climate change
Climate
Microclimate
Physiology
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics
Linking plasticity to extinction risk from climate change
Climate
Microclimate
Physiology
Activity
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics
Linking plasticity to extinction risk from climate change
Climate
Microclimate
Physiology
Activity
Foraging
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics
Linking plasticity to extinction risk from climate change
Climate
Microclimate
Physiology
Activity
Foraging
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics
Fitness
Linking plasticity to extinction risk from climate change
Climate
Microclimate
Physiology
Activity
Foraging
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics
Fitness
Linking plasticity to extinction risk from climate change
Climate
Microclimate
Physiology
Activity
Foraging
Extirpation
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics
Fitness
Linking plasticity to extinction risk from climate change
5 -
0 -
-5 -
Current
0 200 km
Net
energy
balance
(kJ)
Energy balance and extinction without plasticity
Riddell et al. 2018, Science Advances
5 -
0 -
-5 -
2100
0 200 km
Net
energy
balance
(kJ)
Energy balance and extinction without plasticity
Riddell et al. 2018, Science Advances
5 -
0 -
-5 -
Current
0 200 km
Net
energy
balance
(kJ)
Energy balance and extinction without plasticity
Riddell et al. 2018, Science Advances
5 -
0 -
-5 -
0 200 km
Net
energy
balance
(kJ)
Current
Energy balance and extinction with plasticity
Riddell et al. 2018, Science Advances
5 -
0 -
-5 -
2100
0 200 km
Net
energy
balance
(kJ)
Riddell et al. 2018, Science Advances
Energy balance and extinction with plasticity
5 -
0 -
-5 -
0 200 km
Net
energy
balance
(kJ)
Current
Identify mechanisms and targets of selection
Riddell et al. 2018, Science Advances
Riddell et al. 2019, Nature Commun.
Lower water loss rates were associated with more skin lipids
Vasoconstriction
Angiogenesis
Lower water loss rates were associated vasoconstriction
Riddell et al. 2019, Nature Commun.
Can physiology predict responses to climate change?
Grinnell Resurvey Project: 100 Years of Ecology
the wind came up again about 9
o’clock and has blown disgustingly
all day.
Grinnell Resurvey Project: 100 Years of Ecology
MVZ, UC Berkeley
Retracing the steps of Grinnell et al.
Birds and mammals sampled at the same sites over the last 100 yrs
Physiological consequences of habitat selection
Riddell et al. 2021, Science
Physiological consequences of habitat selection
Riddell et al. 2021, Science
Organism
𝜇 = 𝜇0
𝑇0 + 𝐶
𝑇 + 𝐶
×
𝑇
𝑇0
3
2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝑟𝑏 =
0.93 × 𝜌 × 𝐶𝑝
ℎ𝑐
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Environment
𝜇 = 𝜇0
𝑇0 + 𝐶
𝑇 + 𝐶
×
𝑇
𝑇0
3
2
𝐹𝑝 =
1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉
2𝑥
2𝑠𝑖𝑛−1 1 − 𝑥2
1 − 𝑥2
𝑟𝑏 =
0.93 × 𝜌 × 𝐶𝑝
ℎ𝑐
ℎ𝑐 =
0.48 × 𝐺𝑟
1
4 + 𝑘
𝐷
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
𝐺𝑟 =
𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3
𝑣2
Biophysics
Collaborators
Steve Beissinger
Mike Sears
Blair Wolf
Barry Sinervo
Cameron Ghalambor
Kelly Zamudio
Christina Wells
Robert Baldwin
Kyle Barrett
Michael Carlo
Ofir Levy
Scott Sillett
Evan Apanovich
Danielle Perryman
Richard Ramirez
Kelly Iknayan
Undergraduates
Carlie Blankenship
Justyn Plaskon
Jared McPhail
Jonathan Odom
Jason Damm
Meredith Rutledge
Megan Matlack
Lunden Simpson
Chris Gerstle
Faye Romero
Megan Banke
Josh Vanee
Walid Naseri
Emma Roback
Jennifer Tutijan
Riggs Mathews
Acknowledgements
Eric Riddell, PhD
Assistant Professor
Ecology, Evolution, and Organismal Biology (EEOB)
Iowa State University
Caroline Williams, PhD
Associate Professor
Integrative Biology
University of California, Berkeley
Thank you for participating!
CLICK HERE to learn more and
watch the webinar

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Ecophysiological Impacts of Climate Change: Performance, Fitness and Extinction

  • 1. Ecophysiological Impacts of Climate Change: Performance, Fitness, and Extinction Eric Riddell, PhD Assistant Professor Ecology, Evolution, and Organismal Biology (EEOB) Iowa State University Caroline Williams, PhD Associate Professor Integrative Biology University of California, Berkeley
  • 2. Experts discuss their research involving climate change and the ecophysiological effects of changing global temperatures on organismal biology and survival. Ecophysiological Impacts of Climate Change: Performance, Fitness, and Extinction
  • 3. Winter in a Changing World: The Critical Importance of Snow Copyright 2021 C. Williams and InsideScientific. All Rights Reserved. Caroline Williams, PhD Associate Professor Integrative Biology University of California, Berkeley
  • 4. Winter is warming faster than summer
  • 5. Winter warming is having widespread impacts on biodiversity Osland et al. 2021 Global Change Biology
  • 6. Winter warming decreases snowpack Mote et al. 2018. Clim. Atmos. Sci. Northern hemisphere spring snowpack anomalies, 1980 - 2020 Marshall et al. 2020 Curr Opin Insect Sci Red = decreased snowpack Spring snowpack changes, 1955-2016 Sierra Nevada mountain range, California USA
  • 7. Snow cover fluctuates in the Sierra Nevada Joshua Cripps Photography June 22nd 2006 June 22nd 2007 Nathan Rank
  • 8. Many ectotherms overwinter beneath snow AgPest.co.nz Ferdinand Bada Andy Murray Joseph Berger Tristram Brelstraff Jon Costanza
  • 9. Snow determines soil microclimate, and thermal stress Cold snap Big snow fall “Colder soils in a warmer world” -Groffman, 2001
  • 10. Sources of mortality in winter Energy depletion Cold mortality Colder soils in a warmer world: Loss of snow cover will increase cold stress but decrease energy stress
  • 11. Organismal traits determine response to microclimate temperatures Sinclair et al. 2015 J. Therm Biol Irwin & Lee. 2003 Oikos Energy use Cold tolerance Metabolic rate Temperature LT50 (1hr exposure)
  • 12. Moving up a mountain… We do not know how thermal stress on overwintering ectotherms in the soil changes along a snowy elevational gradient Energy depletion Cold mortality Soil temperature ??? Air temperature Snow cover
  • 13. Research question How does changing snow cover impact cold and energetic stress, for organisms that overwinter in the soil in snowy mountains?
  • 14. Sierra willow leaf beetle, Chrysomela aeneicollis Southern range edge of species range illustrations: Hiroko Udaka Sierra Nevada
  • 15. Rich history of study 1980 – 2020 Microclimate monitoring network Beetle surveys Physiology and genetics Collaborators Elizabeth Dahlhoff and Nathan Rank, with PhD candidate Kevin Roberts Bishop CA
  • 16. How does snow impact cold stress and energy stress on overwintering beetles along an elevational gradient? Environment Microclimate temperatures Spatial and temporal variation in snow cover Laboratory Metabolic rate-temperature curves Cold tolerance limits (acute and chronic exposures) Energy reserve assays Field Population surveys (phenology) Snow manipulation experiments Ecophysiological Models Energy and Cold Stress test test Kevin Roberts
  • 17. Environment: spatial and temporal variation in snow cover Roberts et al. in review GCB Snowy Dry 28 sites, 1980 – 2020 Hourly soil temperatures 5 replicate transects Bishop CA Spatial variation Interannual variation climate change
  • 18. Snow alters elevational gradients in cold exposure Cold exposure peaks at mid-elevation, and is higher in dry years Roberts et al. in review GCB
  • 19. Ecophysiological energy use model 1) Estimate metabolic rate – temperature curves using respirometry 2) Input microclimate data to estimate oxygen consumption throughout winter 3) Select start and end dates and sum to get oxygen used over winter (repeat iteratively for range of start and end dates observed in field) 4) Convert to energy used (2L oxygen = 1g lipid, compare to empirical measurements Snow Present Snow Excluded Field Experiment 0.589 mg 0.398 mg Model Estimate 0.591 mg 0.417 mg Model Accuracy 99.7% 95.2% Validated model is >95% accurate in predicting energy use in snowy and dry conditions
  • 20. Lab validation of energy use models Roberts et al. in prep
  • 21. Energy use across elevation Energy use declines with increasing elevation, steeper decline in snowy years due to very high energy use at low elevations Snowy years are longer, and more energetically demanding Roberts et al. in review GCB
  • 22. Climate change will alter cold exposure and energy use across the mountains Long Lake, Bishop Creek Roberts et al. in review GCB
  • 23. Cold mortality likely occurs due to long freezing periods LT50 (1hr exposure) Lethal time frozen
  • 24. Cold and energy stress across elevation • Probability of lethal cold is highest at mid-elevations, not impacted by interannual variation in snow cover Roberts et al. in review GCB
  • 25. • Probability of lethal cold is highest at mid-elevations, not impacted by interannual variation in snow cover • Probability of lethal energy depletion is highest at low elevations, and in snowy years Cold and energy stress across elevation Roberts et al. in review GCB
  • 26. Conclusions • Trade-off between cold mortality and energy depletion is modulated by interannual variation in snow cover • Snow alters elevational gradients in cold and energy stress, potentially altering selective gradients on these traits for overwintering ectotherms • Impact of interannual variation in snow cover depends on elevation – high elevations will be buffered due to persistent snow cover, and mid elevations will experience increased cold stress • Environment (microclimate) and organismal traits together determine stress exposure
  • 27. Take-home message: Climate Change Global Warming “Colder soils in a warmer world” – Groffman 2001
  • 28. Thank you! Collaborators: Kevin Roberts Nathan Rank Elizabeth Dahlhoff Jonathon Stillman Doris Bachtrog Ryan Bracewell Andre Szejner Sigal Lisa Treidel Christina Lee Varun Bahl Rose Kang Kamalakar Chatla Colleagues: Brent Sinclair Dan Hahn Ray Huey John Smiley Greg Ragland Michael Kearney Research Facilitation: White Mountain Research Station Denise Waterbury Williams lab: Ecological and Evolutionary Physiology https://www.cmwilliamslab.com/ Sable Systems for all the great respirometry equipment!
  • 29. Using Ecophysiology to Predict Extinction Risk From Climate Change Copyright 2021 E. Riddell and InsideScientific. All Rights Reserved. Eric Riddell, PhD Assistant Professor Ecology, Evolution, and Organismal Biology (EEOB) Iowa State University
  • 30.
  • 31. How does physiology determine the niche?
  • 32.
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  • 34.
  • 37.
  • 43.
  • 44.
  • 47.
  • 48.
  • 49.
  • 50.
  • 51.
  • 53. Biophysics links physiology to the local environment
  • 54. 𝜇 = 𝜇0 𝑇0 + 𝐶 𝑇 + 𝐶 × 𝑇 𝑇0 3 2 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 𝑟𝑏 = 0.93 × 𝜌 × 𝐶𝑝 ℎ𝑐 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics links physiology to the local environment
  • 55. 𝜇 = 𝜇0 𝑇0 + 𝐶 𝑇 + 𝐶 × 𝑇 𝑇0 3 2 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 𝑟𝑏 = 0.93 × 𝜌 × 𝐶𝑝 ℎ𝑐 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Environment Performance Biophysics links physiology to the local environment
  • 56. 𝜇 = 𝜇0 𝑇0 + 𝐶 𝑇 + 𝐶 × 𝑇 𝑇0 3 2 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 𝑟𝑏 = 0.93 × 𝜌 × 𝐶𝑝 ℎ𝑐 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Organism Environment
  • 57. Organism 𝜇 = 𝜇0 𝑇0 + 𝐶 𝑇 + 𝐶 × 𝑇 𝑇0 3 2 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝑟𝑏 = 0.93 × 𝜌 × 𝐶𝑝 ℎ𝑐 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Environment 𝜇 = 𝜇0 𝑇0 + 𝐶 𝑇 + 𝐶 × 𝑇 𝑇0 3 2 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 𝑟𝑏 = 0.93 × 𝜌 × 𝐶𝑝 ℎ𝑐 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics
  • 59. Southern Grey-cheeked Salamander Plethodon metcalfi Natural and life history Fossorial Nocturnal Fully terrestrial Lungless
  • 60. High water loss rates restrict salamanders to high elevations
  • 61.
  • 62. 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2
  • 63. 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics
  • 64. 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics Physiology
  • 65. 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Activity Biophysics Physiology
  • 66. 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Foraging Activity Biophysics Physiology
  • 67. 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Foraging Activity Biophysics Physiology Fitness
  • 68. Foraging Activity 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics Physiology Fitness
  • 69. Net energy balance (J) Activity time (hr) 30- 0 - -30- 7- 3.5- 0- Riddell et al. 2017; Ecol. Monogr. 83% of known localities can reproduce Physiology helps to predict geographic range of salamanders
  • 70. 30- 0 - -30- 7- 3.5- 0- Physiology helps to predict geographic range of salamanders Riddell et al. 2017; Ecol. Monogr. Net energy balance (J) Activity time (hr) 83% of known localities can reproduce
  • 71. Organism 𝜇 = 𝜇0 𝑇0 + 𝐶 𝑇 + 𝐶 × 𝑇 𝑇0 3 2 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝑟𝑏 = 0.93 × 𝜌 × 𝐶𝑝 ℎ𝑐 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Environment 𝜇 = 𝜇0 𝑇0 + 𝐶 𝑇 + 𝐶 × 𝑇 𝑇0 3 2 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 𝑟𝑏 = 0.93 × 𝜌 × 𝐶𝑝 ℎ𝑐 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics
  • 72. Organism 𝜇 = 𝜇0 𝑇0 + 𝐶 𝑇 + 𝐶 × 𝑇 𝑇0 3 2 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝑟𝑏 = 0.93 × 𝜌 × 𝐶𝑝 ℎ𝑐 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 𝜇 = 𝜇0 𝑇0 + 𝐶 𝑇 + 𝐶 × 𝑇 𝑇0 3 2 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 𝑟𝑏 = 0.93 × 𝜌 × 𝐶𝑝 ℎ𝑐 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics
  • 73. Organism 𝜇 = 𝜇0 𝑇0 + 𝐶 𝑇 + 𝐶 × 𝑇 𝑇0 3 2 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝑟𝑏 = 0.93 × 𝜌 × 𝐶𝑝 ℎ𝑐 𝜇 = 𝜇0 𝑇0 + 𝐶 𝑇 + 𝐶 × 𝑇 𝑇0 3 2 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 𝑟𝑏 = 0.93 × 𝜌 × 𝐶𝑝 ℎ𝑐 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics
  • 74. Organism 𝜇 = 𝜇0 𝑇0 + 𝐶 𝑇 + 𝐶 × 𝑇 𝑇0 3 2 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝑟𝑏 = 0.93 × 𝜌 × 𝐶𝑝 ℎ𝑐 Climate Change 𝜇 = 𝜇0 𝑇0 + 𝐶 𝑇 + 𝐶 × 𝑇 𝑇0 3 2 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 𝑟𝑏 = 0.93 × 𝜌 × 𝐶𝑝 ℎ𝑐 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics
  • 75. Will climate change threaten salamanders with extinction?
  • 76. Phenotypic plasticity The expression of multiple phenotypes from a single genotype
  • 77. Temperature (°C) VPD (kPa) Riddell et al. 2018, Science Advances Salamanders experience seasonal changes in the environment
  • 78. N = 180 N = 180 Resistance (s/cm) Oxygen Consumption (uL/hr) Salamanders adjust metabolism and water loss to seasonal changes
  • 79. Linking plasticity to extinction risk from climate change
  • 80. Climate Linking plasticity to extinction risk from climate change
  • 81. Climate Microclimate Linking plasticity to extinction risk from climate change
  • 82. Climate Microclimate Physiology 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Linking plasticity to extinction risk from climate change
  • 83. Climate Microclimate Physiology 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics Linking plasticity to extinction risk from climate change
  • 84. Climate Microclimate Physiology Activity 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics Linking plasticity to extinction risk from climate change
  • 85. Climate Microclimate Physiology Activity Foraging 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics Linking plasticity to extinction risk from climate change
  • 86. Climate Microclimate Physiology Activity Foraging 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics Fitness Linking plasticity to extinction risk from climate change
  • 87. Climate Microclimate Physiology Activity Foraging 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics Fitness Linking plasticity to extinction risk from climate change
  • 88. Climate Microclimate Physiology Activity Foraging Extirpation 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics Fitness Linking plasticity to extinction risk from climate change
  • 89. 5 - 0 - -5 - Current 0 200 km Net energy balance (kJ) Energy balance and extinction without plasticity Riddell et al. 2018, Science Advances
  • 90. 5 - 0 - -5 - 2100 0 200 km Net energy balance (kJ) Energy balance and extinction without plasticity Riddell et al. 2018, Science Advances
  • 91. 5 - 0 - -5 - Current 0 200 km Net energy balance (kJ) Energy balance and extinction without plasticity Riddell et al. 2018, Science Advances
  • 92. 5 - 0 - -5 - 0 200 km Net energy balance (kJ) Current Energy balance and extinction with plasticity Riddell et al. 2018, Science Advances
  • 93. 5 - 0 - -5 - 2100 0 200 km Net energy balance (kJ) Riddell et al. 2018, Science Advances Energy balance and extinction with plasticity
  • 94. 5 - 0 - -5 - 0 200 km Net energy balance (kJ) Current Identify mechanisms and targets of selection Riddell et al. 2018, Science Advances
  • 95. Riddell et al. 2019, Nature Commun. Lower water loss rates were associated with more skin lipids
  • 96. Vasoconstriction Angiogenesis Lower water loss rates were associated vasoconstriction Riddell et al. 2019, Nature Commun.
  • 97.
  • 98. Can physiology predict responses to climate change?
  • 99.
  • 100.
  • 101.
  • 102. Grinnell Resurvey Project: 100 Years of Ecology
  • 103. the wind came up again about 9 o’clock and has blown disgustingly all day. Grinnell Resurvey Project: 100 Years of Ecology
  • 104. MVZ, UC Berkeley Retracing the steps of Grinnell et al.
  • 105. Birds and mammals sampled at the same sites over the last 100 yrs
  • 106.
  • 107. Physiological consequences of habitat selection Riddell et al. 2021, Science
  • 108. Physiological consequences of habitat selection Riddell et al. 2021, Science
  • 109.
  • 110.
  • 111.
  • 112.
  • 113.
  • 114. Organism 𝜇 = 𝜇0 𝑇0 + 𝐶 𝑇 + 𝐶 × 𝑇 𝑇0 3 2 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝑟𝑏 = 0.93 × 𝜌 × 𝐶𝑝 ℎ𝑐 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Environment 𝜇 = 𝜇0 𝑇0 + 𝐶 𝑇 + 𝐶 × 𝑇 𝑇0 3 2 𝐹𝑝 = 1 + (𝑥2 − 1) × 𝑐𝑜𝑠2𝜉 2𝑥 2𝑠𝑖𝑛−1 1 − 𝑥2 1 − 𝑥2 𝑟𝑏 = 0.93 × 𝜌 × 𝐶𝑝 ℎ𝑐 ℎ𝑐 = 0.48 × 𝐺𝑟 1 4 + 𝑘 𝐷 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 𝐺𝑟 = 𝑔 × 𝛽 × 𝛿𝑇 × 𝐷3 𝑣2 Biophysics
  • 115.
  • 116. Collaborators Steve Beissinger Mike Sears Blair Wolf Barry Sinervo Cameron Ghalambor Kelly Zamudio Christina Wells Robert Baldwin Kyle Barrett Michael Carlo Ofir Levy Scott Sillett Evan Apanovich Danielle Perryman Richard Ramirez Kelly Iknayan Undergraduates Carlie Blankenship Justyn Plaskon Jared McPhail Jonathan Odom Jason Damm Meredith Rutledge Megan Matlack Lunden Simpson Chris Gerstle Faye Romero Megan Banke Josh Vanee Walid Naseri Emma Roback Jennifer Tutijan Riggs Mathews Acknowledgements
  • 117. Eric Riddell, PhD Assistant Professor Ecology, Evolution, and Organismal Biology (EEOB) Iowa State University Caroline Williams, PhD Associate Professor Integrative Biology University of California, Berkeley Thank you for participating! CLICK HERE to learn more and watch the webinar