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Talk	for	ICLR,	22	March	2019
Julian	Brimelow
Meteorological	Service	of	Canada
Hail:	Challenges,	Solutions	and	Future	Prospects
Fir0002/Flagstaffotos
Page 2 – March 22, 2019
http://orf.media/
Observing and forecasting hail
is as difficult, if not more
difficult, than is forecasting
tornadoes
Orf.media
http://ccc2.atmos.colostate.edu
Page 3 – March 22, 2019
How	Big	Can	Hail	Get?
Page 4 – March 22, 2019
Background
• Hail	science	is	difficult	and	challenges	abound
Kumjian et	al.	
(2015,	MWR)
• Final	size	of	hail	on	the	ground	determined							
by	myriad	of	processes	occurring	across	wide	
range	of	spatiotemporal	scales
• Imperfect	understanding	of:
i. Microphysics	
ii. Storm-scale	processes
iii. Connections	between	storm	environ-
ment and	storm	processes
• Hail	size	not	unique	to	a	given	environment
• Reliable	observations	sorely	lacking
• Lack	of	coordination	and	collaboration	(most	research	done	in	parallel)
Page 5 – March 22, 2019
The	Elusive	Hail	Climatology
Allen	and	Lepore (in	review)Mroz et	al.	(2017)
Prein &	Holland																	
(2018)
Page 6 – March 22, 2019
But	it	is	not	all	bad
• How	do	we	best	leverage	these	developments?
Cray
• Incredible	advances	in	computing	
power	and	availability	of	remote	
sensing	data
• Can	run	CAMs	and	3D	models	using	
multi-moment	microphysics	schemes
Dennis and Kumjian (2017, JAS)
• Dual-polarization	radar	more	common;												data	
processing	techniques	improving
Ryzhkov et	al.	(2017,	JAMC)
• Emergence	of	laser	scanners	and	3D	
printers;	miniaturization	of	sensors	
UC	Irvine
IBHS
IBHS
• Social	media	is	now	an	important	data	source
Page 7 – March 22, 2019
Forecasts
Nowcasts
Alerts
Risk	mitigation	&	
Assessment
Observations
Size,amount&
weight
Microphysics
Modelling (NWP
& CAM)
Identification
&discrimination
Remote sensing
Experiments
& in-situdata
Wind tunnel
Aircraft
DATA	AND	
KNOWLEDGE	
GAPS
Coordination
&
Collaboration
Page 8 – March 22, 2019
Hail	datasets	have	significant	limitations,	in	part	
because	of	high	spatiotemporal	variability													
of	hail	swaths.	Other	issues:
• Sparse	observation	networks
• Population	and	measurement	biases	
• Timing	and	location	errors
• Confusion	in	reporting	methods	
• Focus	on	reporting	only	large	hail	sizes
• Do	reports	reflect	true	storm	severity?
• Lack	of	long-term	datasets	for	climate	studies
Gap	1:	Observations
Page 9 – March 22, 2019
Diverse,	yet	complementary,	tools	available:
• Social	media	and	reporting	apps
• Public	education	and	outreach
• Weigh	hailstones	instead	of	focussing	on	size
• More	intensive	field	studies	to	collect	hail
HailSTONE,	SHAVE,	IBHS,	CHAT,	CoCoRaHS
• Maintain	and	expand	hailpad networks
• Install	networks	of	impact	disdrometers
• Use	remote	sensing	data	to	identify	hailswaths
and	estimate	maximum	hail	size
Gap	1:	Possible	Solutions	
Social
media
𝑫 =	 $
𝟔𝑴
𝝅𝝆𝒊
𝟑
	
IBHS
HailSens
Page 10 – March 22, 2019
Leveraging	Social	Media
• Could	images	of	hail	posted	on	social	media	provide	a	source	of	objective	
and	accurate	hail	size	measurements?	
• Scanned	Twitter	feeds	for	#abstorm,	#skstorm and	#mbstorm for	
summers	of	2014	through	2016	for	Tweets	including	images	of	hail	
and/or	references	to	hail.	Sorted	hail	images	into	four	categories	
Damage Scene No	Scale Scalable
Page 11 – March 22, 2019
Estimating	the	Size	of	Hail
• Calculated	equivalent	spherical	diameter	(De)	of	largest	stones
• Diameter	important	because	kinetic	energy	scales	with	D4
• Use	scaling	&	assuming	stones	are	spheroids	(typically	tri-axial	ellipsoids)
Page 12 – March 22, 2019
Report	Statistics	for	2016
• Very	few	images	of	hail	Tweeted	by	chasers
• Over	70%	of	images	Tweeted	from	home
• Almost	80%	of	images	of	little	or	no	use	for	our	purposes
Page 13 – March 22, 2019
So Many Problems…
1) No	location	provided	or	vague	reference	to	location.
2) Tweet	posted	tens	of	minutes	to	hours	after	storm.
3) Uncertainty	in	event	time	(disagreement	between	time	stamp	on	Tweet											
and	time	provided	in	Tweet).
4) Using	objects	that	don’t	have	a	fixed	size	or	have	an	indeterminable	size.
5) Photos	of	hail	being	held	in	hand	is	a	huge	issue.
6) Photos	taken	after	hail	experienced	significant	melting.
7) Photos	taken	at	oblique	angles.
8) Showing	“wrong”	side	of	coin	(i.e.,	heads).
9) Photos	of	scalable	object	and	hailstones	in	different	planes.
10) Combinations	of	the	above.
Page 14 – March 22, 2019
• Measuring	hail	is	fiddly	and	difficult:
• Most	reports	made	from	home	where																																																			
people	have	access	to	a	kitchen	scale
• Can	also	take	along	when	chasing	
• Quick	&	easy	to	weigh	stones	(M)									accurately calc.	D
An Alternative Approach
𝑫 =	 $
𝟔𝑴
𝝅𝝆𝒊
𝟑
Page 15 – March 22, 2019
Incomplete	knowledge	of	key	microphysical	processes																																					
and	outdated	parameterization	schemes
• Fall	mode	and	terminal	velocity	of	hailstones
• Partitioning	of	cloud	condensate	in	updrafts	
• Collection	efficiency	of	ice	during	dry	growth
• Role	of	updraft	volume	in	size	and	amount	of																																																																			
hail;	environmental	factors	controlling	volume	
• Residence	time	in	the	hail-growth	zone
• Trajectories	of	hailstones	in	storms
Gap	2:	Microphysics	and	Modelling	
List	(2014,	JAMC)NWSChalon	et	al.	(1976,	MWR)
Page 16 – March 22, 2019
Leverage	advances	in	computing,	models,	sensor	
miniaturization	and	computation	fluid	dynamics
•Collection	of	cloud	base	to	top	microphysics	data
• Vertical	wind	tunnel	with	mixed-phase	particles
• Carefully	designed	numerical	experiments	using							
CM-1	and	other	3D	cloud	models	
• Impact	of	environment	&	storm-relative	flow	on	
updraft	properties	and	residence	time	in	HGZ
• Improve	access	to	computational	fluid	dynamics	
• Machine	learning	to	improve	microphysics	schemes
• High-speed	photography	(>	1000	fps)	to	analyze	
motion	of	3D	printed	hailstones
Gap	2:	Possible	Solutions	
www.dlr.de/IPA
University	of	Mainz
Dennis	and	Kumjian (2017,	JAS)Dennis and Kumjian (2017, JAS)
Cheng	et	al.	(2014,	JAS)
Page 17 – March 22, 2019
Identifying	hail	and	hail	size	with	or	without	radar
•Current	operational	techniques	limited	to	areas						
with	radar	coverage
• Limited	ability	to	discriminate	between	hail	size
•Few	validated	operational	tools	to	quantify															
mass	of	hail	on	ground	(kinetic	energy)
•Satellite	techniques	can	only	identify	hail	aloft	
•Maximum	Expected	Hail	Size	(MESH)— needs			
refining,	could	incorporate	dual-pol	radar	data?
Gap	3:	Identification	of	Hail	
Ortega et al. (2016, JAMC)
Witt et al. (1998, WAF)
Page 18 – March 22, 2019
• Cube	sats can	identify	hail	swaths	in	near-
real	time	(e.g.,	Planet	Labs)
• GPM	data	(dual-wavelength	space	radar)
• New	generation	geostationary	satellites	
(e.g.,	GOES-16,	Himawari-9,	METEOSAT)	
• Identify	overshooting	tops,	indicator	of	
updraft	width?
• Lightning	data	(lightning	mapping	arrays)
• Combine	above	with	concomitant	storm	
environment	data	from	global	NWP	models
• Ongoing	development	of	conventional	radar																																																											
and	DP	radar	metrics
Gap	3:	Possible	Solutions	
Mroz et	al.	(2017,	JAMC)
Bedka	et	al.	(2010,	JAMC)
Emersic et	al.	
(2011,	MWR)Bedka	et	al.	(2018,	JAMC)
Page 19 – March 22, 2019
MESH	Introduction
Fortunately,	the	answer	is	a	cautious	“YES”:
Maximum	Expected	Size	of	Hail	(a.k.a.	MESH)
• MESH	is	a	radar-derived	hail	size	product	based	on	a	combination	of	
theory	and	empirical	analysis	that	is	used	for	nowcasting of	hail	
• IF found	to	be	reliable,	MESH	could	be	used	as	a	proxy	for	hail	reports
• Allow	high	spatiotemporal	resolution	and	accurate	information	on	
location	and	size	of	hail	in	near-real	time
• Are	there	alternative	data	sources	that	can	help	us	solve	the	myriad	of	
issues	facing	traditional	severe	storm	reports?
Page 20 – March 22, 2019
#1 #2 #3 #4
Dmax 4.8 4.4 4.2 4.1
Dmin 4.2 3.9 3.8 3.7
α 0.88 0.90 0.91 0.89
De 4.6 4.2 4.1 4.0
MESH = 3.5
20-160 km
MESH = 3.8
MESH = 3.0
#2
#3
#4
#1
MESH	Verification
This MESH value
(maximum within
10 km radius) used
for verification
Page 21 – March 22, 2019
Results	2014-2016
1:1
r = 0.70; p << 0.01
Page 22 – March 22, 2019
MESH	Data	vs.	Reports
Unfiltered	cell	counts	2014-2016
Filtered	cell	counts	2014-2016
Severe	Hail	Reports	2014-2016
MESH	≥	3	cm	2014-2016
Page 23 – March 22, 2019
Stagnation	of	lab	experiments	and	in-situ	cloud	data
• Incredibly	innovative	and	ingenious	icing	wind	
tunnel	experiments	in	50s	through	80s
• Very	little	ice	tunnel	research	for	hail	obtained	
since	the	early	1990s
• Most	ice	tunnel	experiments	conducted	using	static	
hail	growth	and	supercooled water	only
Gap	4:	Experiments
Lesins and List
(1986, JAS)
Page 24 – March 22, 2019
• Replacement	for	T-28	(Thunderbolt?)
• Study	hail	growth	in	vertical icing	
tunnel	with	mixture	of	supercooled
droplets	and	ice	crystals	
• Embrace	unconventional	thinking
• Alternatives	to	icing	tunnels	exist	
• Fall	behaviour	of	natural	and	
instrumented	3D	printed	stones
• Develop	instrumented,	artificial	
hailstones	(“smartdust”)
• Release	HailPods into	storms
Gap	4:	Possible	Solutions	
T-28Thunderbolt	II
Iflyworld.com
Xu and Li (2015, Sensors)
Orf.media
Page 25 – March 22, 2019
Dual-Polarization	Radar	Network
Radisson, SK
• Less	attenuation	
• Superior	for	observing	large	hydrometeors
• Allows	for	precipitation	classification
• Network	uniformity	hardware	&	software
• 6-min	scans	(10-min	previously),	better	coverage
Page 26 – March 22, 2019
Rollout
Doppler Overlap
Completed
Location to be Confirmed
• 13	weeks	to	install
• 5	installed	to	date
• 20	(33)	new	radars
• 7	installs	per	year
• Radar	relocations
• Completion		~2022
• 2019	installs:
Exeter; Bethune
Marion	Bridge
Chipman;	Mtl River	Hbr
Landrienne
Strathmore
Page 27 – March 22, 2019
Specifications
Provider:	Leonardo/Selex	
Germany
Power:	1MW
Source:	Klystron
Beam	Width:	0.88º
Sensitivity:	-115	dBm
Dish:	9.1	m
Doppler	Range:	250	km
Page 28 – March 22, 2019
Summary
• Hail	presents	a	significant	and	costly	threat	to	society
• All	aspects	of	hail	science,	monitoring	and	prediction	are	difficult
• Hail	is	a	complex	and	multi-faceted	natural	hazard
BUT
• We	have	entered	a	new	era	of	hail	research
• New	technologies,	opportunities	and	instrumentation	are	available	
• Our	scientific	understanding	has	advanced
NEXT
• Need	an	infusion	of	long-tem	funding
• Need	collaboration,	including	a	multi-season	field	program
• Still	much	science	to	be	done!
Page 29 – March 22, 2019
Thank	You	– Merci Beaucoup
The changing hail threat over
North America in response to
anthropogenic climate change
Julian Brimelow, William Burrows &
John Hanesiak
Meteorological Service Canada
Hail: A costly and vexing problem
• Anthropogenic climate change (ACC) predicted to
increase the number of severe storm environments
• Low confidence and uncertainty surrounding how
future hailstorms will respond to ACC
• Uncertainty stems from the limited number of
studies, empirical nature and conflicting results
• How hail frequency and size might respond to ACC
is important, need to address limitations
31
Previous Work
32
• Research on the response of severe storms to ACC has focussed on
CAPE-BWD6 phase space
• Greater the CAPE and BWD6 => greater potential for severe storms
• Empirical relationships derived for the current climate between
atmospheric parameters and damaging hail days => applied to future
Diffenbaugh et al. (2013, PNAS)
33
• Explicitly model response of hail to ACC using
HAILCAST and three AOGCM-RCM pairings
HadCM3-MM5; HadCM3-HRM3 & CCSM3-MM5
• 1971-2000 and 2041-2070
• ~50 km grid; ~5000 points (~ 1 billion profiles)
• 1 March to 30 September
• Identified largest hailstone for each day from HAILCAST
• Aggregated exceedances (e.g., D > 2 cm) by month,
season and year for each of 15 ecoregions
“Current” Hail Climate
34
MAM
Days D ≥ 2 cm
MAM
AKE(J) Days with HALO
MAMJJAJJAJJAM-S M-SM-S
Accumulated Kinetic energy (AKE)
Function of #hail days and D on hail days
Key drivers and processes
35
Instability
Moisture
Suff. CAPE
Suff. BWD
Low CIN
Trigger
HAIL
• Factors do not operate independently
• Complex interplay of drivers and processes
• Instability and moisture expected to increase
• Increases CAPE, but can increase CIN
• HigherT also increases melting potential
• Changes in BWD unclear
• Changes in triggers difficult to simulate
• Use CAM or look at synoptic & meso forcing
Suff. Updraft
LWC
Embryos
Growth time
Vol. updraft
SRW
HAIL
Meso and
Synoptic Scale
Macro and
Microscale
36
Future Changes
Days D ≥ 1 cm Days D ≥ 2 cm Ds (cm) AKE (J)
Summary
37
• First study to explicitly model response of hail to warming
• Complex interplay of drivers and processes
• Response of hail to ACC over N. America varies by region and by season
• Fewer hail days expected over most areas in the future
• Marked decrease in hail damage potential over east and southeast
• BUT, increase in hail diameter on days with hail
• Result is greater hail damage potential over most areas in MAM;
higher latitudes and mountains in JJA
• More work to be done (e.g., CORDEX data), expand globally
• Use CAMs and WRF-HAILCAST

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ICLR Friday Forum: Hail: Challenges Solutions and Future Prospects (March 22, 2019)

  • 2. Page 2 – March 22, 2019 http://orf.media/ Observing and forecasting hail is as difficult, if not more difficult, than is forecasting tornadoes Orf.media http://ccc2.atmos.colostate.edu
  • 3. Page 3 – March 22, 2019 How Big Can Hail Get?
  • 4. Page 4 – March 22, 2019 Background • Hail science is difficult and challenges abound Kumjian et al. (2015, MWR) • Final size of hail on the ground determined by myriad of processes occurring across wide range of spatiotemporal scales • Imperfect understanding of: i. Microphysics ii. Storm-scale processes iii. Connections between storm environ- ment and storm processes • Hail size not unique to a given environment • Reliable observations sorely lacking • Lack of coordination and collaboration (most research done in parallel)
  • 5. Page 5 – March 22, 2019 The Elusive Hail Climatology Allen and Lepore (in review)Mroz et al. (2017) Prein & Holland (2018)
  • 6. Page 6 – March 22, 2019 But it is not all bad • How do we best leverage these developments? Cray • Incredible advances in computing power and availability of remote sensing data • Can run CAMs and 3D models using multi-moment microphysics schemes Dennis and Kumjian (2017, JAS) • Dual-polarization radar more common; data processing techniques improving Ryzhkov et al. (2017, JAMC) • Emergence of laser scanners and 3D printers; miniaturization of sensors UC Irvine IBHS IBHS • Social media is now an important data source
  • 7. Page 7 – March 22, 2019 Forecasts Nowcasts Alerts Risk mitigation & Assessment Observations Size,amount& weight Microphysics Modelling (NWP & CAM) Identification &discrimination Remote sensing Experiments & in-situdata Wind tunnel Aircraft DATA AND KNOWLEDGE GAPS Coordination & Collaboration
  • 8. Page 8 – March 22, 2019 Hail datasets have significant limitations, in part because of high spatiotemporal variability of hail swaths. Other issues: • Sparse observation networks • Population and measurement biases • Timing and location errors • Confusion in reporting methods • Focus on reporting only large hail sizes • Do reports reflect true storm severity? • Lack of long-term datasets for climate studies Gap 1: Observations
  • 9. Page 9 – March 22, 2019 Diverse, yet complementary, tools available: • Social media and reporting apps • Public education and outreach • Weigh hailstones instead of focussing on size • More intensive field studies to collect hail HailSTONE, SHAVE, IBHS, CHAT, CoCoRaHS • Maintain and expand hailpad networks • Install networks of impact disdrometers • Use remote sensing data to identify hailswaths and estimate maximum hail size Gap 1: Possible Solutions Social media 𝑫 = $ 𝟔𝑴 𝝅𝝆𝒊 𝟑 IBHS HailSens
  • 10. Page 10 – March 22, 2019 Leveraging Social Media • Could images of hail posted on social media provide a source of objective and accurate hail size measurements? • Scanned Twitter feeds for #abstorm, #skstorm and #mbstorm for summers of 2014 through 2016 for Tweets including images of hail and/or references to hail. Sorted hail images into four categories Damage Scene No Scale Scalable
  • 11. Page 11 – March 22, 2019 Estimating the Size of Hail • Calculated equivalent spherical diameter (De) of largest stones • Diameter important because kinetic energy scales with D4 • Use scaling & assuming stones are spheroids (typically tri-axial ellipsoids)
  • 12. Page 12 – March 22, 2019 Report Statistics for 2016 • Very few images of hail Tweeted by chasers • Over 70% of images Tweeted from home • Almost 80% of images of little or no use for our purposes
  • 13. Page 13 – March 22, 2019 So Many Problems… 1) No location provided or vague reference to location. 2) Tweet posted tens of minutes to hours after storm. 3) Uncertainty in event time (disagreement between time stamp on Tweet and time provided in Tweet). 4) Using objects that don’t have a fixed size or have an indeterminable size. 5) Photos of hail being held in hand is a huge issue. 6) Photos taken after hail experienced significant melting. 7) Photos taken at oblique angles. 8) Showing “wrong” side of coin (i.e., heads). 9) Photos of scalable object and hailstones in different planes. 10) Combinations of the above.
  • 14. Page 14 – March 22, 2019 • Measuring hail is fiddly and difficult: • Most reports made from home where people have access to a kitchen scale • Can also take along when chasing • Quick & easy to weigh stones (M) accurately calc. D An Alternative Approach 𝑫 = $ 𝟔𝑴 𝝅𝝆𝒊 𝟑
  • 15. Page 15 – March 22, 2019 Incomplete knowledge of key microphysical processes and outdated parameterization schemes • Fall mode and terminal velocity of hailstones • Partitioning of cloud condensate in updrafts • Collection efficiency of ice during dry growth • Role of updraft volume in size and amount of hail; environmental factors controlling volume • Residence time in the hail-growth zone • Trajectories of hailstones in storms Gap 2: Microphysics and Modelling List (2014, JAMC)NWSChalon et al. (1976, MWR)
  • 16. Page 16 – March 22, 2019 Leverage advances in computing, models, sensor miniaturization and computation fluid dynamics •Collection of cloud base to top microphysics data • Vertical wind tunnel with mixed-phase particles • Carefully designed numerical experiments using CM-1 and other 3D cloud models • Impact of environment & storm-relative flow on updraft properties and residence time in HGZ • Improve access to computational fluid dynamics • Machine learning to improve microphysics schemes • High-speed photography (> 1000 fps) to analyze motion of 3D printed hailstones Gap 2: Possible Solutions www.dlr.de/IPA University of Mainz Dennis and Kumjian (2017, JAS)Dennis and Kumjian (2017, JAS) Cheng et al. (2014, JAS)
  • 17. Page 17 – March 22, 2019 Identifying hail and hail size with or without radar •Current operational techniques limited to areas with radar coverage • Limited ability to discriminate between hail size •Few validated operational tools to quantify mass of hail on ground (kinetic energy) •Satellite techniques can only identify hail aloft •Maximum Expected Hail Size (MESH)— needs refining, could incorporate dual-pol radar data? Gap 3: Identification of Hail Ortega et al. (2016, JAMC) Witt et al. (1998, WAF)
  • 18. Page 18 – March 22, 2019 • Cube sats can identify hail swaths in near- real time (e.g., Planet Labs) • GPM data (dual-wavelength space radar) • New generation geostationary satellites (e.g., GOES-16, Himawari-9, METEOSAT) • Identify overshooting tops, indicator of updraft width? • Lightning data (lightning mapping arrays) • Combine above with concomitant storm environment data from global NWP models • Ongoing development of conventional radar and DP radar metrics Gap 3: Possible Solutions Mroz et al. (2017, JAMC) Bedka et al. (2010, JAMC) Emersic et al. (2011, MWR)Bedka et al. (2018, JAMC)
  • 19. Page 19 – March 22, 2019 MESH Introduction Fortunately, the answer is a cautious “YES”: Maximum Expected Size of Hail (a.k.a. MESH) • MESH is a radar-derived hail size product based on a combination of theory and empirical analysis that is used for nowcasting of hail • IF found to be reliable, MESH could be used as a proxy for hail reports • Allow high spatiotemporal resolution and accurate information on location and size of hail in near-real time • Are there alternative data sources that can help us solve the myriad of issues facing traditional severe storm reports?
  • 20. Page 20 – March 22, 2019 #1 #2 #3 #4 Dmax 4.8 4.4 4.2 4.1 Dmin 4.2 3.9 3.8 3.7 α 0.88 0.90 0.91 0.89 De 4.6 4.2 4.1 4.0 MESH = 3.5 20-160 km MESH = 3.8 MESH = 3.0 #2 #3 #4 #1 MESH Verification This MESH value (maximum within 10 km radius) used for verification
  • 21. Page 21 – March 22, 2019 Results 2014-2016 1:1 r = 0.70; p << 0.01
  • 22. Page 22 – March 22, 2019 MESH Data vs. Reports Unfiltered cell counts 2014-2016 Filtered cell counts 2014-2016 Severe Hail Reports 2014-2016 MESH ≥ 3 cm 2014-2016
  • 23. Page 23 – March 22, 2019 Stagnation of lab experiments and in-situ cloud data • Incredibly innovative and ingenious icing wind tunnel experiments in 50s through 80s • Very little ice tunnel research for hail obtained since the early 1990s • Most ice tunnel experiments conducted using static hail growth and supercooled water only Gap 4: Experiments Lesins and List (1986, JAS)
  • 24. Page 24 – March 22, 2019 • Replacement for T-28 (Thunderbolt?) • Study hail growth in vertical icing tunnel with mixture of supercooled droplets and ice crystals • Embrace unconventional thinking • Alternatives to icing tunnels exist • Fall behaviour of natural and instrumented 3D printed stones • Develop instrumented, artificial hailstones (“smartdust”) • Release HailPods into storms Gap 4: Possible Solutions T-28Thunderbolt II Iflyworld.com Xu and Li (2015, Sensors) Orf.media
  • 25. Page 25 – March 22, 2019 Dual-Polarization Radar Network Radisson, SK • Less attenuation • Superior for observing large hydrometeors • Allows for precipitation classification • Network uniformity hardware & software • 6-min scans (10-min previously), better coverage
  • 26. Page 26 – March 22, 2019 Rollout Doppler Overlap Completed Location to be Confirmed • 13 weeks to install • 5 installed to date • 20 (33) new radars • 7 installs per year • Radar relocations • Completion ~2022 • 2019 installs: Exeter; Bethune Marion Bridge Chipman; Mtl River Hbr Landrienne Strathmore
  • 27. Page 27 – March 22, 2019 Specifications Provider: Leonardo/Selex Germany Power: 1MW Source: Klystron Beam Width: 0.88º Sensitivity: -115 dBm Dish: 9.1 m Doppler Range: 250 km
  • 28. Page 28 – March 22, 2019 Summary • Hail presents a significant and costly threat to society • All aspects of hail science, monitoring and prediction are difficult • Hail is a complex and multi-faceted natural hazard BUT • We have entered a new era of hail research • New technologies, opportunities and instrumentation are available • Our scientific understanding has advanced NEXT • Need an infusion of long-tem funding • Need collaboration, including a multi-season field program • Still much science to be done!
  • 29. Page 29 – March 22, 2019 Thank You – Merci Beaucoup
  • 30. The changing hail threat over North America in response to anthropogenic climate change Julian Brimelow, William Burrows & John Hanesiak Meteorological Service Canada
  • 31. Hail: A costly and vexing problem • Anthropogenic climate change (ACC) predicted to increase the number of severe storm environments • Low confidence and uncertainty surrounding how future hailstorms will respond to ACC • Uncertainty stems from the limited number of studies, empirical nature and conflicting results • How hail frequency and size might respond to ACC is important, need to address limitations 31
  • 32. Previous Work 32 • Research on the response of severe storms to ACC has focussed on CAPE-BWD6 phase space • Greater the CAPE and BWD6 => greater potential for severe storms • Empirical relationships derived for the current climate between atmospheric parameters and damaging hail days => applied to future Diffenbaugh et al. (2013, PNAS)
  • 33. 33 • Explicitly model response of hail to ACC using HAILCAST and three AOGCM-RCM pairings HadCM3-MM5; HadCM3-HRM3 & CCSM3-MM5 • 1971-2000 and 2041-2070 • ~50 km grid; ~5000 points (~ 1 billion profiles) • 1 March to 30 September • Identified largest hailstone for each day from HAILCAST • Aggregated exceedances (e.g., D > 2 cm) by month, season and year for each of 15 ecoregions
  • 34. “Current” Hail Climate 34 MAM Days D ≥ 2 cm MAM AKE(J) Days with HALO MAMJJAJJAJJAM-S M-SM-S Accumulated Kinetic energy (AKE) Function of #hail days and D on hail days
  • 35. Key drivers and processes 35 Instability Moisture Suff. CAPE Suff. BWD Low CIN Trigger HAIL • Factors do not operate independently • Complex interplay of drivers and processes • Instability and moisture expected to increase • Increases CAPE, but can increase CIN • HigherT also increases melting potential • Changes in BWD unclear • Changes in triggers difficult to simulate • Use CAM or look at synoptic & meso forcing Suff. Updraft LWC Embryos Growth time Vol. updraft SRW HAIL Meso and Synoptic Scale Macro and Microscale
  • 36. 36 Future Changes Days D ≥ 1 cm Days D ≥ 2 cm Ds (cm) AKE (J)
  • 37. Summary 37 • First study to explicitly model response of hail to warming • Complex interplay of drivers and processes • Response of hail to ACC over N. America varies by region and by season • Fewer hail days expected over most areas in the future • Marked decrease in hail damage potential over east and southeast • BUT, increase in hail diameter on days with hail • Result is greater hail damage potential over most areas in MAM; higher latitudes and mountains in JJA • More work to be done (e.g., CORDEX data), expand globally • Use CAMs and WRF-HAILCAST