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Title	:		RESPIRATORY	VIRUS		PATTERN	OF	DIFFUSION	:	SIZE
INFLUENCE
	
Authors:
1)	Luisetto	m	IMA	ACADEMY	Marijnskaja	NATURAL	SCIENCE
BRANCH	itlay	29121
2)	Naseer	Almukthar,	Professor,	Department	of	Physiology	/College	
of	Medicine,		University	of	Babylon,				Iraq
3)	Prof.	Giulio	Tarro	Primario	emerito	dell’	Azienda	Ospedaliera	“D.
Cotugno”,Napoli
Chairman	della	Commissione	sulle	Biotecnologie	della	Virosfera,
WABT	-
UNESCO,	Parigi,	Rector	of	the	University	Thomas	More	U.P.T.M.,
Rome
Presidente	della	Fondazione	de	Beaumont	Bonelli	per	le	ricerche
sul	cancro	-ONLUS,	Napoli
4)Behzad	Nili	Ahmadabadi,	Innovative	Pharmaceutical	product
development	specialist,	USA
	
5)Ahmed	Yesvi	Rafa	,	Founder	and	President,	Yugen	Research
Organization;	Undergraduate	Student,	Western	Michigan	University,
MI,	USA	49008
6)Ghulam	Rasool	Mashori	Department	of	Medical	&	Health	Sciences
for	Woman,	Peoples	University	of	Medical	and	Health	Sciences	for
Women,Pakistan
	
7)Tuweh	Prince	GADAMA	the	great,	Professor,Cypress	University
Malawi
8)Oleg	Yurievich	Latyshev	IMA	academy	president
Corresponding	author:	luisetto	m	maurolu65@gmail.com	italy	29121	zip
code
	
	
	
	
	
	
	Chapther		1	Abstract
	
Aim	of	this	work	is	to	verify	difference	in	spread	attitudes	of	covid-19	and
other	coronavirus	versus	Smalpox	and	try	to	seek	rational	explain	of	the
specific	pattern	of	diffusion.
	
The	rapid	increase	of	covid-		19	cases	in	FRANCE	in	second	wave	in	fisrt	
day	of	october	2020	seem	to	follow	not	only	a	diffusion	related	direct	
contact	and	by	droplet	but	also	by	airborne	trasmission.
	
A		real	fact	is	the	diffenece	in	size	of	virus	smalpox	vs	coronaviruses.
	
Virus	size	is	an	relevant	factor	involved	in	kind	of	spread.
	
Keywords	:	COVID-19	,	CORONAVIRUS	,	SMALPOX	,	RESPIRATORY
VIRUS,	SPREAD,	DIFFUSION	,	AIRBORNE	,WIND	EFFECT,	TIME	OF
SPREAD,	VENTILATION	EFFECT
	
	
	
	
Chapther	2	Introduction
Related	covid-19	pandemia	it	is	interesticg	to	notice	that	many	document	
related	past	SPANISH	FLU	was	extremely	similar		to	nawadays	allert	
produced	by	public	intrnational	health	organization	to	prevent	spread	of
this	dangerosu	disease	(	see	fig.	1)
	
	
	
Fig.n	1	Chicago	theaters	displayed	posters	like	this	one	to	slow	the
spread	of	the	Spanish	flu	during	the	1918	pandemic.
	
	
At	the	same	time	it	is	interesting	to	observe	the	difference	in	size	of
some	respiratory	virus	:	from	the	more	great	size	of	smallpox	to	the
small	SARS	virus.
	
This	variability	in	size	can	be	responsible	of	the	different	kind	of	diffusion
of	this	virus?
	
Smallpox	more	diffused	by	direct	contact	and	by	droplets	then	other
coronavirus	and	this	instead	seem	involved	also	in	airborne
transmission.
The	kinetics	of	the	diffusion	of	this	virus	seem	to	tell	us	that	in	the	cases	
of	covid.19	second	wave	in	France		where	numerous	cases	increased	
but	in	very	rapid	ay	(	weeks)	in	October	2020	is	a	patter	different	to	the	
spread	of	smallpox		diffusion	in	north	America	in		1781	in	HUSTON	BAY	
.
	
	
FIG.	N.	2	virus	size	and	dimension	(	variola	–	smallpox)
	
	
Chapther	3	Material	and	methods
	
Whit		an	observational	methods	some	relavant	maps	and	images		related	
some	respiratory	virus	diffusion	in	the	world	are	analysed	.
Also	some	literature	involved	and	useful	to	this	topic	is	presented	in	order
to	produce	a	global	conclusion
Fact-related.
All	literature	comes	from	Pub	med	or	other	open	science	journal	.
	
It	is	used	in	this	work	a	VISUAL	method	to	find	the	final	conclusion	and
some	relevant	figure	are	reported.
Various	respiratory	virus	are	analyzed	and	also	covering		since	smallpox		
epidemy	in	north	america	after	columbus	travel.
	
	
	
Chapther	4	Results
	
In	this	section	are	reported		relevant	figure	involved	in		respiratory	virus	
diffusion:
	
Related	kind	of	spread,	timing,	velocity	of	the	process.
	
we	do	know	that	the	airborne	-transmission	has	been	shown	to	be	a	predominant	route-	way	of
transmission	for	a	number	of	communicable	kind	of	diseases,	including	the	rhinovirus	and
influenza.
Fig.	n	3
Fig.	n.	4						10	march	2020	The	locations	of	people	who	have	tested	positive
covid-19	in	the	U.S.
Source	The	new	York	times
Fig.	n	5	USA	population	2016
Fig.n	6	covid	cases	September	2020	from	jama	network
Fig.	n	7	form	Business	insider
	
	
Fig	n	8	H1N1	Swine	Flu	Spread	June	2014		form	
Rachael	Rettner,	LiveScience
FIG.	n	9
	
	
Amos	Ssematimba	et	al:
	
“We	calculate	the	distance-dependent	probability	of	infection	for	farms	down-
wind	of	an	infected	farm	by	combining	our	model	predictions	of	the	hourly
depositions	with	the	virus	amount	and	infection	probability	models,	the
inhalation-model	and	the	within-flock	epidemic	model	as	described	in
the	Materials	and	Methods	section.	We	use	the	Dutch	2003	epidemic	data	to	test
whether	wind-borne	HPAI	spread	was	possible	and	if	so,	determine	its	possible
contribution	during	the	epidemic	by	comparing	our	model	-predictions	with	the
observed	pattern	in	the	epidemic.	As	can	be	seen	from	equations	reported	,	for
small	infection-	probability	per	inhalation	the	model-predicted	probabilities	are
to	a	very	good	approximation	proportional	to	the	deposition	pattern	.	As	a	result,
in	the	parameter	range	of	interest	here,	the	distance-dependence	of	the	model-
predicted	probabilities	is	practically	indistinguishable	from	that	of	the
deposition-	pattern.
The	comparison	in	figure	reported		more	importantly	shows	a	qualitative
difference	in	the	tail.	Compared	to	the	observed	pattern,	there	is	a	faster	drop	in
the	predicted	infection	probability	beyond	0.45	km.	At	all	distances	from	the
source,	the	predicted	probabilities	are	smaller	than	the	observed-	risk.	Also,
beyond	1	km	distance	the	predicted	risk	of	solo	wind-borne	infection	is	decaying
significantly-	faster	with	distance	than	the	observed	-risk.	The	observed	rapid
decrease	of	the	predicted	-risk	with	distance	is	only	very	weakly	sensitive	to	the
precise	value	of	pathogen	-decay	rate,	settling	velocity	and	the	within-flock	basic
reproduction	ratio	as	shown	in	figure	reported.	Based	on	these	results,	we
conclude	that	the	wind-borne	route	alone	could	not	explain	the	pattern	of	the
2003	-epidemic.”
	
	
	
Fig.	n	10	Spanish	flu	1918	spread	and	death
Fig.	n	11	SPANISH	FLU	1918	SPREAD
	
	
	
Fig.	n	12	HONG	KONG	flu		1968	diffusion
Fig.	n	13	smalpox	spread	USA	case	of	smallpox	during	the	1775-82
epidemic.
	
The	strange	truth	about	smallpox	and	Native	Americans
Posted	on	June	15,	2019	Memories	of	the	people
	
	
“Did	Europeans	deliberately	give	smallpox-infected	blankets	to	Native-
Americans?	Absolutely.	There	is	1	proven	case	and	many	other	suspicious	ones.
But	the	largest	smallpox	outbreak,	the	one	that	killed	possibly	hundreds	of
thousands	of	Natives,	started	during	the	Revolutionary	-War.	While	the	war
naturally	brought	people	–	and	the	virus	–	together	and	then	re-distributed	them,
the	virus	was	also	spread	when	the	British-	army,	most	of	whom	had	already
been	exposed	to	the	disease,	deliberately	tried	to	infect	American-	colonists	with
smallpox.”
Figure	n	14			smallpox	1837	
	
	
https://alchetron.com/1837-Great-Plains-smallpox-epidemic:
	
“The	1837	Great	Plains	smallpox-	epidemic	spanned	from	1836
through	1840,	but	reached	its	height	after	the	spring	of	1837	when	an
American	Fur-	Company	steamboat,	the	S.S.	St.	Peter,	carried	infected
people	and	supplies	into	the	Missouri-	Valley	area	.	More	than	15,000
Native	-Americans	died	along	the	Missouri	River	alone,	with	some	tribes
becoming	nearly	extinct.	Having	witnessed	the	effects	of	the	epidemic	on
the	Mandan	-tribe,	fur	trader	F.	Chardon	wrote,	"the	small-pox	had	never
been	known	in	the	civilized-	world,	as	it	had	been	among	the	poor
Mandans	and	other	Indians	tribu’.	Only	twenty-seven	Mandans	were	left
to	tell	the	tale.
Smallpox	has	afflicted	the	Native-	Americans	since	it	was	carried	to	the
western-	hemisphere	by	the	Spanish	conquerors,	with	credible	accounts
of	epidemics	dating	back	to	at	least	1515.	The	Mandan	-tribe,	also
named	the	People	of	the	Pheasants,	had	previously	experienced	a	major
smallpox	-epidemic	in	1780-81	which	severely	reduced	their	numbers
down	to	less	than	a	few-	thousand.	Many	other	tribes	along	the	Missouri	-
river	suffered	smallpox-	epidemics	during	1801-02	and	1831”
From	CDC	resource	:
Origin	of	Smallpox
“The	origin	of	smallpox	is	unknown.	Smallpox	is	thought	to	date	back	to
the	Egyptian	-Empire	around	the	3rd	century	Before	Common-	Era	,
based	on	a	smallpox-like	rash	found	on	three	mummies.	The	earliest
written-	description	of	a	disease	that	clearly	resembles	smallpox
appeared	in	China	in	the	4th	century	Common-	Era.	Early	written
descriptions	also	appeared	in	India	in	the	7th	-century	and	in	Asia	Minor
in	the	10th-	century
17th	-Century	–	European	colonization	imports	smallpox	into
North	of	America.
	Old	World,	the	most	common	form	of	smallpox	killed	perhaps	30	%
of	its	victims	while	blinding	and	disfiguring	many	others.	But	the
effects	were	even	worse	in	the	Americas,	which	had	no	exposure	to
the	virus	prior	to	the	arrival	of	the	Spanish	and	Portuguese-
conquistadors.	Tearing	through	the	Incas	before	F.	Pizarro	even	got
there,	it	made	the	empire	unstable	and	ripe	for	conquest.	It	also
devastated	the	Aztecs	populations	,	killing,	among	others,	the
second-to-last	of	their	rulers.	In	fact,	historians	believe	that
smallpox	and	other	European	diseases	reduced	the	indigenous
population	of	North	and	South	-America	by	up	to	90	%,	a	blow	far
greater	than	any	defeat	in	battle.	“
	
“	the	Smallpox	-patients	became	contagious	once	the	first
sores	appeared	in	their	mouth	and	throat	(early	rash-
stage).	They	spread	the	virus	when	they	coughed	or	sneezed
and	droplets	from	their	nose	or	mouth-	spread	to	other	people.
They	remained	contagious	until	their	last	smallpox-	scab	fell	off.
These	scabs	and	the	fluid	found	in	the	patient’s	-sores	also
contained	the	variola	-virus.	The	virus	can	spread	through
these	materials	or	through	the	objects	contaminated	by	them,
such	as	bedding	or	clothing.	People	who	cared	for	smallpox	-
patients	and	washed	their	bedding	or	clothing	had	to	wear
gloves	and	take	care	to	not	get	infected.
Rarely,	smallpox	has	spread	through	the	air	in	enclosed	–	kinds
of	settings,	such	as	a	building	(airborne-	route).
Smallpox	can	be	spread	by	humans	only.	Scientists	have	no
evidence	that	smallpox	can	be	spread	by	the	insects	or
animals.”
Smallpox:	Emergence,	Global	Spread,	and	Eradication
Frank	Fenner	1993
Ann	M.Carlos	et	al	:
“The	route	of	infection	is	the	respiratory	tract
This	requires	direct	-contact	with	an	infected	person,	and	transmission,	with	rare
exceptions,	through	inhaled	liquid	-droplets.	Unlike	measles,	patients	with
smallpox	do	not	generally	have	respiratory	symptoms	such	as	coughing	or
sneezing	which	generate	large	clouds	of	infection	in	the	air.	As	a	result,	“direct
and	fairly	prolonged	face-to-face	contact	is	required	to	spread	the	disease	from
one	person	to	another,”	usually	contact	within	about	6	to	seven	7	for	a	period	of
a	few	hours	(CDC,	2010,	“Smallpox	Disease	Overview”).	Although	droplets	or
scabs	that	fall	on	bedding	or	clothing	remain	infectious	in	principle,	laboratory	-
tests	using	vaccinia	virus	indicate	that	infection	is	unlikely	because	of	how	the
material	is	handled	by	the	respiratory-	tract.	Also,	in	experiments	on	the
persistence	of	infectivity,	it	has	been	found	that	the	virus	is	rapidly	inactivated,
even	on	heavily	contaminated	objects.	There	are	instances	of	laundry-	workers
contracting	smallpox,	but	the	documented	cases	of	smallpox	transmission	via
fomites	are	very	rare	.”
Fign	15
	
	
	
Fig.	n16	dengue	pattern	of	spread	form	The	new	York	times	June	2019
Fig.	n	17	from	AWEA
	
In	this	figure	it	is	interesting	to	observe	the	distribution	of	wind
manufacturing	facilities	in	USA
(	an	indirect	indicator	of	wind		status)
	
Zhili	Zuo	et	al	:		
	
	“Normalized	infectious	virus	-size	distribution,	total	virus	-size
distribution,	SMPS	particle	number	distribution,	and	SMPS	particle
volume	distribution	for	airborne	MS2.	Values	are	means	±	one	standard
n	=	3).	Similar	plots	for	TGEV,	SIV,	and	AIV	are	available	online	.	To
better	understand	virus-	transmission	by	aerosols,	it	is	important	to
determine	the	relationship	between	airborne	virus	infectivity/survivability
and	particle	size	.	Only	a	few	studies	are	available	on	this	issue	in	the
scientific-	literature.	To	determine	the	distribution	of	infectious	virus
among	poly-disperse	-particles,	an	Andersen	cascade	impactor	was	used
to	sample	aerosols	of	coxsackie	virus	A-21		and	simian	-rotavirus	.	The
concentration	of	infectious	virus	appeared	to	be	related	to	particle	volume
-distribution	for	particle	size	>0.5	μm.	Using	the	same	instrument,	Appert
et	al.	(2012)	confirmed	the	above	findings	for	MS-2	bacteriophage,	but
not	for	adenovirus.	Tyrrell	(1967)	found	that	rhinovirus	survived	better	in
coarse	-particles	(>4	μm)	than	in	smaller	particles	(0–4	μm),	while
adenovirus	infectivity	was	best	preserved	in	the	size	range	of	0.56–1.9
μm	compared	with	1.9–10	μm	indicating	that	particle	-size	may	also
affect	virus	survivability.	Although	the	use	of	size-segregated	samplers,
such	as	impactors,	provides	size	fractionation	for	virus	infectivity,	not
much	is	known	about	virus	aerosol	particles	of	human	and	animal-
viruses	remains	an	issue	.	The	objective	of	this	study	was	to	examine
infectivity	and	survivability	of	three	airborne	animal	viruses	as	a	function
of	their	carrier	particle	size	in	the	submicron	size-	range	using	a	newly
developed	sampling	method.	In	addition,	the	behavior	of	widely	used
MS2	bacteriophage	was	studied	for	comparative	purposes	.Propagation
and	Titration	of	MS2	Bacteriophage	MS2	bacteriophage	(ATCC	15597-
B1)	is	a	small	(27–34	nm),	icosahedral,	non-enveloped,	single	stranded,
positive	sense	RNA	-virus,	infecting	only	the	male	Escherichia	coli	(those
bearing	an	F	pilus)	.	For	the	purposes	of	this	study,	we	considered	MS2
as	a	model	virus	because	it	has	been	widely	used	in	many	virus	aerosol
studies	.	The	virus	was	propagated	in	E.	coli	famp	(ATCC	700891),	as
described	elsewhere	.	Briefly,	0.1	mL	of	MS2	and	1	mL	of	a	log	phase
culture	of	E.	coli	were	added	to	top	agar	tubes	held	at	48◦C.	After	mixing,
the	contents	of	the	tubes	were	poured	on	trypticase	soy	agar	(TSA)
plates.	The	top	agar	was	allowed	to	solidify	followed	by	inversion	and
incubation	of	plates	at	37◦C	for	24	h.	After	plaques	were	confluent	(within
24	h	of	incubation),	5	mL	of	tryptic	soy	broth	(TSB)	was	added	to	each
plate.	After	2	h	at	room	-temperature,	the	solution	was	aspirated,
centrifuged	at	2500	×	g	for	15	min,	and	sterile-filtered.	The	resulting
bacteriophage	stock	was	aliquoted	into	50	mL	tubes,	followed	by	storage
at	−80◦C	until	use.	The	amount	of	MS2	-bacteriophage	in	virus	stock	and
various	other	samples	was	determined	by	using	a	double	agar-	layer
procedure	as	described	elsewhere	.	The	amount	of	virus	was	expressed
as	plaque	-forming	units	per	unit	volume	of	the	sample	(PFU/mL)”.
	
Fig.	n	18	Schematic	diagram	of	the	experimental	setup	for	the
characterization	of	virus	aerosols.
Fig.	n	19
	
“Four	viruses	MS2	-bacteriophage,	transmissible	gastroenteritis	virus,
swine-	influenza	virus,	and	avian	-influenza	virus)	were	aerosolized,	size
classified	(100–450	nm)	using	a	differential	mobility-	analyzer	(DMA),	and
collected	onto	gelatin	filters.	Uranine	dye	was	also	nebulized	with	the
virus,	serving	as	a	particle	tracer.	Virus	-infectivity	assay	and	quantitative
reverse	transcription-polymerase	chain	reaction	were	then	used	to
quantify	the	amount	of	infectious	virus	and	total	virus	present	in	the
samples,	respectively.	The	virus	-distribution	was	found	to	be	better
represented	by	the	particle	-volume	distribution	rather	than	the	particle
number	distribution.	The	capacity	for	a	particle	to	carry	virus	increased
with	the	particle-	size	and	the	relationship	could	be	described	by	a	power
law.	Virus	survivability	was	dependent	on	virus	type	and	particle-	size”
Nanomedicine	Volume	I:	Basic	Capabilities	Robert	A.	Freitas	Jr.
“Large	Molecule	-Binding,	Sorting	and	Transport	Is	there	any	size	limit	for
target	molecules	to	be	transported?
	
Natural-	receptors	have	already	been	found	for	large	molecules	including
low-density	lipoproteins	(LDLs)	>	1,000,000	daltons426	and	high-density
lipoproteins	(HDLs).The	methods	described	in	earlier	Sections	can	be
adapted	for	binding	large-	molecules	(>1000	atoms;	Fig.	3.15),	including
molecules	far	wider	than	the	binding	device	itself	(	~200-nm	diameter
virus	particles	and	larger).	Making	a	binding	site	for	a	large	molecule
should	be	physically	easier	(albeit	computationally	more	challenging)
than	making	a	binding	-site	for	a	small	molecule	because	of	the	greatly
increased	area	of	interaction.
In	example,	a	binding	energy	of	400	zJ	may	be	realized	by	creating	a
dispersion-force	binding	-area	covering	only	~25%	of	the	surface	of	a	
10,000-atom	target	molecule		or	a	mere	~0.02%	of	a	200-nm	virus-
particle.
Assuming	a	roughly	spherical	large	molecule	and	laminar	fluid	-flow	at	1
atm	forcing	pressure	(Section	9.2.7),	a	10-nm	diameter	molecule	moves
through	a	20-nm	long	pump	(~10-20	kg,	~106	atoms)	in	~10(-6	)sec	at
~0.02	m/sec,	consuming	~0.02	pW	during	transfer.
A	200-nm	virus-size	target	molecule	moves	through	a	400-nm	long	pump
(~10-17	kg,	~109	atoms)	in	~10	(-2)	sec	at	~60	microns/sec,	consuming
~10-16	watts	during	transfer;	at	~0.0002	atm,	release-	time	is	diffusion
limited.
The	transfer	force	exerted	on	a	10-nm	molecule	is	~1	pN,	~600	pN	on	a
200-nm	virion;	a	binding	energy	of	400	zJ	at	a	0.2-nm	contact	distance
gives	a	binding-	force	of	~2300	pN,	sufficient	to	hold	a	particle	of	either
size	firmly	during	transport	and	release”	(4)
	
“As	demonstrated	previously,	the	particle	size	can	significantly	affect
survival	of	airborne	viruses	“	(3)
Zhili	Zuo	et	al	:
“Although	laboratory	generated	virus-	aerosols	have	been	widely	studied	in	terms	of	infectivity	and
survivability,	how	they	are	related	to	particle-	size,	especially	in	the	submicron-	size	range,	is	little
understood.	Survivability	of	the	three	animal	viruses	at	large	particle	-size	(300–450	nm)	was
significantly	higher	than	at	particle	size	close	to	the	size	of	the	virion	(100–200	nm),	which	could
be	due	to	the	shielding	-effect.	The	data	suggest	that	particle	size	plays	an	important	role	in
infectivity	and	survivability	of	airborne	viruses	and	may,	therefore,	have	an	impact	on	the	airborne
transmission	of	viral	illness	and	disease.	The	data	in	this	study	do	not	support	the	use	of	MS2	-
bacteriophage	as	a	general	surrogate	for	animal	and	human	-viruses.	(3)
	
	
	
	
	
	
	
	
	
	
	
	
	
	
	
	
	
Infectious/Total	Virus	Size	Distribution
Figure	reported	represent	the	infectious	virus	and	total	virus	-size	distribution	from	100	nm	to
450	nm	normalized	by	the	maximum-	values.	In	general,	both	the	infectious	and	total	virus-
concentrations	increased	with	particle	size	and	the	maximum	-values	at	400–450	nm	were	around
5000	PFU/cm3
,	35	TCID50/cm3
,	180	TCID50/cm3
,	and	60	TCID50/	cm3
	for	MS2,	TGEV,	SIV,	and
AIV,	respectively,	which	were	several	orders	of	magnitude	lower	than	the	particle	number
concentration	at	the	same	particle	-size.	The	virus	-size	distributions	were	normalized	to	compare
them	more	easily	with	particle	size-	distributions.	As	seen	in	Figures		reported	,	the	infectious	and
total	virus	distributions	had	a	similar	trend,	both	appearing	to	follow	particle	volume	distribution
rather	than	particle	number	distribution.	Infectious	and	total	virus-	concentrations	collected	by	the
gelatin-	filters	are	available	on-line	.
	
		Survivability	of	Airborne	Virus
“Similar	to	RRIV	,	survivability	of	TGEV	and	AIV	was	much	lower	at
200	nm	than	at	larger	-size	.	One	could	argue	that	the	discretization
phenomenon	is	responsible	for	this	finding,	as	the	carrier	particle-	size
gets	smaller	and	approaches	the	size	of	virion,	it	becomes	more	difficult
for	the	particle	to	carry	virus.	the	particle-	size-independent	RRTV	shown
in		figure	reported		suggests	the	presence	of	virus	in	particles	even	at
100	nm.	Therefore,	the	discretization	phenomenon	was	probably	not	the
reason.	The	main	reason	for	the	particle	-size	associated	survivability
could	be	the	shielding-	effect.	More	specifically,	compared	with	virus
existing	as	a	singlet	or	in	association	with	fewer-	organics	(solutes	in	the
nebulizer	-suspension),	the	virus	at	larger	particles	may	be	surrounded
by	more	organic-	material,	which	may	form	a	shield.	Shielding	-effect	has
been	demonstrated	to	better	protect	virus	from	environmental-	stress
such	as	ultraviolet	irradiation	.	It	may	also	reduce	sampling	stress	such
as	desiccation	and	sampler	dependent-mechanical	forces,	thus	better
maintaining	the	infectivity	of	airborne	-virus.	as	particle	-size	increased	to
300	nm	and	above,	virus	survivability	seemed	to	reach	a	plateau,
suggesting	the	shielding-	effect	was	maintained	once	a	specific	particle	-
size	was	reached.	The	same	explanation	applies	to	MS2.	Because	all
collected	particle	-sizes	were	more	than	four	times	the	virion	size	(27–
34	nm),	the	survivability	reached	the	plateau	-regime	and	therefore	was
no	longer	depended	on	particle-	size	.	This	is	supported	by	Lee	(2009),
who	showed	that	survivability	of	MS2	at	120–200	nm	was	higher	than	at
30	nm,	despite	the	large	experimental	variation.”	(3)
	
	
Fig.	n.	20	Schematic	representation	of	the	shielding	effect	of	the
hydration	layer	due	to	the	presence	of	zwitterionic	moieties.	(	from
references)
	
	
	
	
	
	
	
	
	
	
Mahesh	Jayaweera	et	al	:
Behavior	of	droplets	and	aerosols	against	environmental	factors
“The	most	important	environmental-	factors	that	could	impact	on	the	viability	of	airborne	-microorganisms
are	temperature,	humidity,	radiation	(sunlight),	and	open-air	(ventilation)	.	Most	viruses,	including	SARS-
CoV-2,	are	less	than	100	nm	in	size	.	Viruses	in	aerosols	lose	or	gain	the	viability	and	infectivity	because	of
environmental	-stresses	caused	by	temperature,	relative	humidity,	and	sunlight	before	they	reach	a
susceptible	host.	Environmental	-tolerance	of	the	virus-laden	aerosols	depends	on	the	specific-	phenotype
available,	the	composition	of	the	bioaerosols	containing	virus	and	their	payload,	and	physical	-
characteristics	in	the	surrounding	environment	.	As	the	environmental-	factors	play	a	major	role	in
transmitting	payloads	of	SARS-CoV-2	virus	in	different	geographical	-locations	of	outdoor	and	indoor	-
environments,	it	is	worthy	of	exploring	the	effects	of	environmental	factors	on	the	transmission	of	SARS-
CoV-2	virus.	there	have	been	associations	between	air	-pollution	represented	by	air	pollutants	such	as
PM2.5,	PM10,	NO2,	and	O3	and	COVID-19	infection	”	(6)
	
Wan	Yang	et	al	:
	
“The	concentrations	and	size	-distributions	of	airborne	influenza	-viruses	were	measured	in	a
health	centre,	a	day-care	facility	and	aeroplanes	by	qRT–PCR.	During	the	2009–2010	flu	season,
50	per	cent	of	the	samples	collected	(8/16)	contained	IAVs	with	concentrations	ranging	from	5800
to	37	000	genome	-copies	m−3.	On	average,	64	per	cent	of	virus-laden	particles	were	found	to	be
associated	with	particles	smaller	than	2.5	µm,	which	can	remain	airborne	for	hours.	Modelling	of
virus	concentrations	-indoors	suggests	a	source	strength	of	1.6	±	1.2	×	105	genome	copies	m3	h
−1	and	a	deposition	flux	onto	surfaces	of	13	±	7	genome	copies	m−2	h−1.	Doses	of	30	±	18,	236
±	140	and	708	±	419	TCID50	were	estimated	for	1,	8	and	24	h	exposures,	respectively.	As	a
whole,	these	results	provide	quantitative	support	for	the	possibility	of	airborne	-transmission	of
influenza	“(7)
	
	
	
	
Luis	A.	Anchordoqui	et	al	:
“	MODELING	THE	EFFECT	OF	CONVECTION	-CURRENTS	IN	THE	TRANSMISSION	OF
SARS-COV-2	In	the	presence	of	air	resistance,	compact	heavy	objects	fall	to	the	ground	quickly,
while	light	objects	exhibit	Brownian	-motion	and	follow	the	pattern	of	turbulent-	convection	of	the
air.	For	aerosol	-particles	containing	the	virus,	the	boundary	between	these	two	behaviors
depends	on	the	size	of	the	particle.	We	begin	with	a	simple	question:	how	long	does	a	virus	float
in	the	air	under	the	influence	of	gravity?	To	answer	this	query	we	model	the	virus	as	a	sphere	of
radius	r	∼	90	nm	and	mass	m	∼	2.5×10−19	kg,	and	we	assume	that	this	spherical-	particle	is
suspended	in	a	viscous	fluid	(the	air)	feeling	the	Earth’s	gravitational	field.	Herein,	gravity	tends	to
make	the	particles	settle,	while	diffusion	and	convection	act	to	homogenize	them,	driving	them
into	regions	of	smaller	concentration.	On	the	one	hand,	the	convection	mechanism	provides
particle	macro-mixing	within	the	fluid	through	the	tendency	of	hotter	and	consequently	less	dense
material	to	rise,	and	colder,	denser	material	to	sink	under	the	influence	of	gravity.	On	the	other
hand,	the	diffusion	-mechanism	acts	on	the	scale	of	an	individual	particle	(micro-mixing)	slowly
and	randomly-	moving	through	the	media.	Under	the	action	of	gravity,	the	virus	acquires	a
downward	terminal	speed	that	follows	from	Stokes	law.
is	the	virus	-mobility	in	the	fluid,	and	where	η	=	1.8	×	10−5	kg/(ms)	is	the	dynamic	viscosity	of	air	.
Substituting	(2)	into	(1)	we	find	that	the	downward	terminal	speed	of	the	virus	in	dry	air	is	indeed
negligible,	vdown	∼	8	×	10−8	m/s.	It	is	therefore	clear	that	gravity	plays	no	role	in	the	motion	of	an
isolated	-virus	through	the	air.	Rather	it	follows	a	convection	pattern	in	a	manner	similar	to	how
smelly-	substances	move	through	the	air.	The	survival	probability	of	the	virus	in	the	dry-	air	is	then
given	by	the	likelihood	of	survival	outside	its	natural	-environment.	The	half-life	of	SARS-CoV-2	in
aerosols	has	been	found	to	be	about	1.1	hours	.	For	large	droplets	whose	diameters	&	1000	µm,
the	effect	of	air	-resistance	is	negligible	and	so	the	falling	time	can	be	directly	estimated	using
Newton’s	equations	for	gravitational	settling.	For	smaller	droplets	whose	diameters	<	100	µm,	the
falling	times	must	instead	be	determined	using	the	downward	terminal-	speed	given	in	(1)	to
account	for	the	air	resistance	upon	the	falling	droplets.	It	is	now	an	instructive	and	straightforward
exercise	to	show	that	the	time	for	falling	2	m	in	saturated	air	is	0.6	s	for	droplets	with	r	>	500	µm,
6.0	s	for	those	of	r	∼	50	µm,	600	s	(about	10	minutes)	for	those	of	r	∼	5	µm,	and	60,000	s	(about
16.6	hours)	for	those	of	r	∼	0.5	µm.	The	droplet	evaporation	-time	scale,	as	computed	by	Wells
using	droplet	“(8)
	
	
	
Rajiv	Dhand	et	al	:
“In	respiratory-	exhalation	flows,	the	large	droplets	between	60	and	100	mm	in	size	are	expected
to	completely	evaporate	before	traveling	2	m	(30).	These	large	droplets	are	carried	farther	away
when	they	are	expelled	at	high	-velocity,	such	as	with	coughs	and	sneezes.	The	time	it	takes
particles	to	fall	to	the	floor	depends	on	their	size;	particles	100	mm	in	diameter	take	about	10
seconds,	whereas	10-mm–diameter	particles	are	estimated	to	take	17	minutes	to	fall	to	the	floor,
and	1-	to	3-mm–diameter	particles	could	remain	suspended	almost	indefinitely	especially	if	they
are	periodically	elevated	by	air	-current			(VERNON	KNIGHT	1980	“)	.
	
	
Aerosols,	Droplets,	and	Airborne	Spread:	Everything	you	could	possibly	want	to	know
Justin	Morgenstern:
As	is	discussed	below,	this	form	of	aerosolization	is	thought	to	have	spread
SARS	in	the	Amoy	-Garden	apartment	complex	in	Hong	Kong.	(Morawska
2006)
However,	whether	these	aerosols	are	capable	of	transmitting	disease	still
depends	heavily	on	the	number	produced,	the	concentration	of	the	infectious	-
agent,	the	virulence	of	the	microbe,	environmental	-factors	(the	virus	needs	to	be
able	to	survive,	whether	in	the	air	or	on	a	surface,	until	it	enters	a	host),	and	the
health	and	immunity	of	the	host.	(Morawska	2006)	As	I	said,	exact	size	-cutoffs
are	controversial,	but	Chen	(2010)	suggests	that	the	distribution	of	all	droplets
between	0.1	and	200	µm	will	primarily	be	influenced	by	ventilation-	patterns
and	the	initial	velocity	of	the	droplet,	rather	than	gravity.	In	other	words,	these
droplets	do	not	just	drop	to	the	ground	within	1-2	meters	of	the	patient,	as	many
infection	control	practices	assume.,	the	distribution	of	droplets	is	also	influenced
by	a	very	large	number	of	factors,	including	relative	humidity,	temperature,
ventilation	pattern	and	rate,	initial-	velocity,	shape	of	the	human	body,	and
droplet	nuclei	-size	and	composition.	(Xie	2007;	Chen2010)	Most	of	these
factors	are	dynamic	(droplet-	size	changes	as	it	evaporates	and	temperature
changes	as	you	move	away	from	a	febrile-	patient),	making	simplified
calculations	difficult.	At	smaller	-sizes,	Brownian	motion,	electrical	forces,
thermal	gradients,	and	turbulent	diffusion	have	much	bigger	impacts.	(Morawska
2006)	Overall,	it	is	complicated,	there	are	lots	of	formulas,	and	reading	these
papers	generally	left	me	with	a	headache.Any	infection	that	behaves	like
influenza	could	easily	be	spread	through-	aerosols.
Aerosols	are	tiny	and	their	concentration	-drops	off	exponentially	as	you	get
farther	from	the	source	(especially	with	good-	ventilation).	Of	course	we	don’t
frequently	see	transmission	over	large-	distances	or	large	-scale	outbreaks.	The
chances	of	encountering	viable	virus	across	the	room	are	just	too	lw.
that	line	of	reasoning	completely	discounts	close	range	aerosol-	spread.	Aerosols
will	be	most	concentrated	within	a	few	meters	of	the	patient.	At	that	distance,
aerosol	spread	is	almost	indistinguishable	from	droplet	-spread.	In	fact,	it	is
generally	completely	ignored,	because	many	people	just	assume	that	short	range
spread	is	due	to	droplets.	short	range	-aerosol	spread	would	have	significant
implications	for	our	PPE	-choice
Fig.	n	:		21	from	Characteristic	size	ranges	of	atmospheric	particles	and
bioaerosols	(A)	protein	(B)	virus,	(C)	bacteria,	(D)	fungal	spore	and	(E)	pollen
grain	(Fröhlich-Nowoisky	et	al.	2016)
Fig.	n.	22	size	some	virus	and	PM
Fig.	n.	23
Transmission	and	control	of	viruses	via	infectious	droplets	and	aerosols	in	indoor	environments
	
Theodore	A.	Myatt	et	al	:
	
	
“We	detected	airborne	-picornavirus	in	32%	of	air	sampling	-filters	in	office	buildings	using
molecular	methods.	We	show	a	significant	positive	relationship	between	the	frequency	of	virus
detection	in	air-	filters	and	degree	of	building	ventilation	with	outdoor-	air	as	measured	by	average
CO2	concentrations	greater	than	100	ppm	above	the	background.	Thus,	these	data	suggest	that
lower	ventilation	-rates	and	resulting	increased	CO2	concentrations	are	associated	with
increased-	risk	of	exposure	to	potentially	infectious	droplet-	nuclei.	(10)”
	
Martin	Meyer	Weiss	et	al	:
	
“If	one	assumes	that	influenza	is	transmitted	by	respiratory-	droplets	(>	10	μm	in	size,	which
immediately	fall	to	the	ground)	rather	than	by	aerosols	(<	10	μm	in	size,	which	remain	suspended
in	air	for	long	-periods	of	time)”	(11)
	
Larisa	Anghel	et	al	:
“Pulmonary-	activities	such	as	coughing	,	breathing	,	sneezing		or	talking,	are	sources	of	bio-
aerosols	that	can	have	respiratory	tract	infections	pathogens	.	Large	droplets	(>10	microns),
formed	especially	from	coughing	and	sneezing,	fall	on	surfaces	and	objects	not	further	than	1–2
m	from	the	infected	-patient.	People	can	catch	the	infection	directly	by	standing	within	1–2	meters
of	an	infected	person	and	breathing	in	these	droplets.	When	people	are	standing	within	1–2
meters	of	an	infected	-patient	or	when	they	touch	their	mouth,	nose	or	eyes	after	they	touched	the
contaminated	-surfaces	or	objects,	they	can	catch	the	infection	.	Droplets	that	evaporate	(10
microns	droplets	evaporate	in	0.2	s)	and	desiccate,	form	small	particles	(droplet	nuclei	or
residue).	Aerosols	are	small-particles	(<	5	microns	)
with	a	slow	velocity	and	may	remain	suspended	in	the	air	for	hours	and	can	be	transported	long
distances”	(12)
	
Natalie	Pica	et	al	:
	
	
“Viral-	infections	of	the	respiratory	tract	are	common	acute	illnesses	among	humans,	and	virus-
transmission,	by	either	direct	or	indirect	routes,	occurs	in	disparate	regions	around	the	globe.	A
more	detailed	understanding	of	how	these	viruses	transmit	can	have	broad	public	health
implications.	Indeed,	a	variety	of	meteorological	factors	have	at	times	been	associated	with	rates
of	virus	infection	as	well	as	transmission	among-	individuals.	As	presented	in	this	review,
precipitation,	humidity,	temperature,	and	airflow	can	be	determinants	of	virus	infection	and
transmission;	despite	robust	investigation	of	the	effects	of	these	environmenta-l	factors,
inconsistencies	and	uncertainties	in	the	data	remain.	It	is	possible	that	meteorological	-
determinants	play	greater	roles	in	some	geographic-	regions	than	others,	or	simply	that
differences	in	experimental	design	affect	outcomes	and	data	interpretation.	Non-environmental
effects,	including	but	not	limited	to	seasonal-	changes	in	behavior,	family	and	social	structures,
and	pre-existing	immunity,	could	also	be	playing	a	role	in	respiratory	virus	t-ransmissibility	and
rates	of	infection.	Discrepancies	in	collected	data	suggest	that	more	vigilant	surveillance	over
large	geographic	regions	and	further	controlled	experiments	in	animal	-models	and	perhaps	in
humans	will	probably	be	necessary	to	determine	with	increased	certainty	the	role	that
environmental	factors	play	on	the	transmission	of	viral	-pathogens.”	(13)
	
Aaron	Fernstrom	et	al	:
	
	“airborne-	transmission	is	defined	as	the	transmission	of	infection	by	expelled	particles	that	are
comparatively	smaller	in	size	and	thus	can	remain	suspended	in	air	for	long-	periods	of	time.
Airborne-	particles	are	particularly	worrisome	simply	because	they	can	remain	suspended	in	the
air	for	extended	periods	of	time.	Seminal	studies	from	the	1930s	and	1940s	demonstrated	that
airborne	particles	can	remain	airborne	for	as	long	as	one	week	after	initial-	aerosolization,	and
suggested	further	that	these	particles	likely	remained	airborne	for	much	longer.	They	thus
potentially	expose	a	much	higher	number	of	susceptible-	individuals	at	a	much	greater	distance
from	the	source	of	infection	.	Depending	on	environmental-	factors	(	meteorological	conditions
outdoors	and	fluid	dynamic	effects	and	pressure	differentials	indoors),	airborne-	particles	are
easily	measured	20 m	from	their	source	.	These	factors	would	be	of	no	concern	but	for	the	fact
that	airborne	bacterial,	viral,	and	fungal	particles	are	often	infectious	.	Exposure	to	airborne
pathogens	is	a	common	denominator	of	all	human	life	.	With	the	improvement	of	research-
methods	for	studying	airborne	pathogens	has	come	evidence	indicating	that	microorganisms
(e.g.,	viruses,	bacteria,	and	fungal	spores)	from	an	infectious-	source	may	disperse	over	very
great	distances	by	air	currents	and	ultimately	be	inhaled,	ingested,	or	come	into	contact	with
individuals	who	have	had	no	contact	with	the	infectious	-source	.	Airborne	pathogens	present	a
unique	challenge	in	infectious	-disease	and	infection	-control,	for	a	small	percentage	of	infectious
individuals	appear	to	be	responsible	for	disseminating	the	majority	of	infectious-	particles	.	(14)
Chapther	5	Discussion
	
Is	possible	to	verify	the	difference	in	spread	of	virus	smallpox	–	variola	(
high	dimension)	versus	other	small	virus	in	USA	maps	.
Observing	pattern	of	diffusion	in	1870	in	BAY	of	HUSTON	is	possible	to
verify	the	time	(	month)	necessary	to	spread	and	this	reflect	correctly	a
diffusion	by	direct	contact	or	droplets.
	
Instead	COVID-19	diffusion	especially	in	second	wave	in	France	in
October	2020	seem	to	follow	other	model	:	a	logarithmic	explosion	of
cases	in	a	few	week:only	direct	contact	od	droplets	or	other	factors	acts	(
airborne	diffusion	?)
	
Observing	the	spread	of	covid-19	,	SARS,	seasonal	flu	and	suine	flu	it	is
clear	that	there	is	a	not	omogenea
Pattern	of	diffusion	in	all	USA	STATES	whit	a	GRADIENT	(	more	involved
east	region	then	centre		of	USA)	
	
The	spread	of	smallpox	in		North	America	followed	a	gradient	also	from
east	to	west	but	in	more	slowly	way.
	
Even	if	nowadays	modern	travel	system	(	airplane	,	train,	cars	and	other	)
the	spread	of	coronavisus	covid-19	in	march	2020	in	NORTH	America
followed	a	determinate	gradient	versus	.
	
“Virus	survivability	was	dependent	on	virus	type	and	particle	size”
	
According	WHO	:		Airborne	transmission	is	defined	as	the	spread	of	an	infectious	agent
caused	by	the	dissemination	of	droplet-	nuclei	(aerosols)	that	remain	infectious	when	suspended
in	air	over	long-	distances	and	time.
Particulate	matter	(PM)	in	the	air,	whether	in	solid	or	liquid	-
form,	can	affect	our	health.	Particularly	those	particles	of	below
2.5	micrometers	(microns;	μm)	represent	a	hazard,	as	they	are
able	to	enter	our	blood-stream.	Nano-particles	can	be	as	small
as	0.1	right	down	to	0.001	μm.
Sizes	of	Influenza	A	virus:	about	0.08	-	0.12	μm
The	coronavirus	species	COVID-2019,	MERS-CoV	and	SARS-
CoV	range	in	size	from	about	0.06	to	0.2	μm
	
Some	effect	influence	particles	suspended	in	the	air	like	Brownian	–moto.
This	Brownian	motion	(	A.	EINSTEIN	1905)		is	a	random	motion	of	particles	suspended	in	a
medium	(a	liquid	or		gas).
A	random	-fluctuations	in	a	particle's	position	inside	a	fluid	sub-domain,	followed	by	a	relocation	to
another	sub-domain.	Each	re-location	is	followed	by	more-	fluctuations	within	the	new	closed	-
volume.	
Molecules	of	a	fluid	,	under	termic-	shaking	,	produce	casual	moto	of	a	particle	inside	this.
This	fluctuation	influence	the	particle	in	higher	-way	when	this	is	of	lower	-size		the	higher
ones.
	
	
In	example	For	larger-	particles,	the	HEPA	-filter	acts	like	a	net
as	we	would	expect.	Particles	greater	than	about	0.3	μm	in	size
simply	cannot	get	through:	either	they	do	not	fit	through	the
holes	or	they	hit	the	filter-	fibers	due	to	inertia.	For	the	smaller-
particles,	it	would	seem	logical	that	they	can	simply	go	through
the	holes.	(	this	is	not	the	case)	.	The	tiny-	mass	of	particles
less	than	about	0.3	μm	means	they	do	not	fly	straight;	instead,
they	are	bounced	off	other	molecules	as	they	collide	with	them
and	thus	move	in	completely	random	-patterns.	As	a	result,
they	hit	the	filter	-fibers	and	then	remain	stuck	in	them.	This	is
the	principle	of	the	Brownian-	movement	phenomena.
Chapther	6	Conclusion
	
Related	the	figure	and	reference	reported	in	this	work	it	is	possible	to
conclude	that	is	seem	that	related	also	to	the	size	of	respiratory		virus	the	
pattern	of	diffusion	(	time	and	versus	)	is	different.
	
According	literature	AIRBORNE	virus	spread	and	transmission	is	function
of	various	factors	:	carrier	size	,	virus	size	,	distance	,	time	,	subject
characteristic,	phisiopathologic	patient	condition	,	air	pollution	level,
temperature,	humidity	,air	flux	,	Brownian	moto,	air	current	and	other	.
	
Spreading	and	diffusing	of	the	virus	are	definitely	associated	or
correspond	with	virus	size	and	airborne	mechanism.
	
	
Of	this	observation	public	authorities	must	take	in	consideration.
	
	
Source	of	founding	:	self
	
Conflict	of	interests:	none
	
Ethical	consideration:	this	work	is	produced	under	all	ethical	rules	for	this
kind	of	research
	
	
Clarifications:	this	work	is	produced	with	put	any	diagnostic	or
therapeutic	intent	,	only	to	submit	to	the	researcher	a	new	theory
References
1)Luisetto	M,	Almukthar	N,	Rafa	AY,	Jangdey	MS,	Fiazza	C,	et	al.	(2020)	On	Distance	Respiratory
Virus	Transmission:	Sate	of	Evidence.	J	Infect	Dis	Epidemiol	6:150.	doi.org/10.23937/2474-
3658/1510150
	
2)	Amos	Ssematimba,	1	,	2	,	*	Thomas	J.	Hagenaars,	1	and	Mart	C.	M.	de	Jong	2
2012;	Modelling	the	Wind-Borne	Spread	of	Highly	Pathogenic	Avian	Influenza	Virus	between
Farms7(2)	PLoS	One.	doi:	10.1371/journal.pone.0031114
	
	
3)	Zhili	Zuo,Thomas	H.	Kuehn,Harsha	Verma,Sunil	Kumar,Sagar	M.	Goyal,Jessica	Appert,		2012	
Association	of	Airborne	Virus	Infectivity	and	Survivability	with	its	Carrier	Particle	Size	
JournalAerosol	Science	and	Technology	Volume	47,	2013	-	Issue	4Pages	373-382	|
https://doi.org/10.1080/02786826.2012.754841
	
4)	Robert	A.	Freitas	jr.Nanomedicine	Volume	I:	Basic	Capabilities	1999	Landes	Bioscience
5)	Ann	M.CarlosaFrank	D.Lewisb	2012	
Smallpox	and	Native	American	mortality:	The	1780s	epidemic	in	the	Hudson	Bay	region
Explorations	in	Economic	History	Volume	49,	Issue	3,	
	
	
6)	Mahesh	Jayaweera,a,∗	Hasini	Perera,b	Buddhika	Gunawardana,a	and	Jagath	Manatungea			
Transmission	of	COVID-19	virus	by	droplets	and	aerosols:	A	critical	review	on	the	unresolved
dichotomy
2020	Environ	Res.	2020	Sep;	188:	109819.
2020	Jun	13.	doi:	10.1016/j.envres.2020.109819
	
	
7)	Wan	Yang,1	Subbiah	Elankumaran,2	and	Linsey	C.	Marr1,						2011	Concentrations	and	size	
distributions	of	airborne	influenza	A	viruses	measured	indoors	at	a	health	centre,	a	day-care
centre	and	on	aeroplanes	J	R	Soc	Interface.		8(61):	1176–1184.
Published	online	2011	Feb	7.	doi:	10.1098/rsif.2010.0686
8)	Luis	A.	Anchordoqui	and	Eugene	M.	Chudnovsky	2020		A	physicist	view	of	COVID-19	airborne
infection	through	convective	airflow	in	indoor	spaces
Scimedicine	journal	
DOI:	10.28991/SciMedJ-2020-02-SI-5
	
	
9)	Rajiv	Dhand1	and	Jie	Li2	1	Coughs	and	Sneezes:	Their	Role	in	Transmission	of	Respiratory
Viral	Infections,	Including	SARS-CoV-2	2020	American	journal	of	respiratory	and	critical	care	
medicine		vol	2020,	issue	5	
	
	
10)	Theodore	A.	Myatt	,	Sebastian	L.	Johnston	,	Zhengfa	Zuo	,	Matthew	Wand	,	Tatiana
Kebadze	,	Stephen	Rudnick	,	and	Donald	K.	Milton	2004
Detection	of	Airborne	Rhinovirus	and	Its	Relation	to	Outdoor	Air	Supply	in	Office
Environments	American	journal	of	respiratory	ans	criticalcare	medicine
https://doi.org/10.1164/rccm.200306-760OC							PubMed:	14754759
	
	
11)	Martin	Meyer	Weiss,	MD,	Peter	D.	Weiss,	MD,	Danielle	E.	Weiss,	MD,	and	Joseph	B.	Weiss,
MD	2007
Disrupting	the	Transmission	of	Influenza	A:	Face	Masks	and	Ultraviolet	Light	as	Control	Measures
Am	J	Public	Health.	2007	April;	97(Suppl	1):	S32–S37.
doi:	10.2105/AJPH.2006.096214
	
	
	
	
	
12)	Larisa	Anghel	1,2,	Cătălin-George	Popovici	3	,	Cristian	Stătescu	1,2,*	,	Radu	Sascău	1,2,*,
Marina	Verdes,	3	,	Vasilică	Ciocan	3	,	Ionela-Lăcrămioara	S,	erban	4	,	Minela	Aida	Mărănducă	4	,
Sebastian-Valeriu	Hudis,teanu	3	and	Florin-Emilian	T,	urcanu
2020
Impact	of	HVAC-Systems	on	the	Dispersion	of	Infectious	Aerosols	in	a	Cardiac	Intensive	Care
Unit	International	Journal	of	Environmental	Research	and	Public	Health	—	Open	Access	Journal
doi:	10.3390/ijerph17186582
13)	Natalie	Pica1
	and	Nicole	M	Bouvier1,2
Curr	Opin	Virol.	2012	Feb;	2(1):	90–95.	Environmental	factors	affecting	the	transmission	of
respiratory	viruses.	doi:	10.1016/j.coviro.2011.12.003
	
	
14)	Aaron	Fernstrom	1	,*	and	Michael	Goldblatt	2	Aerobiology	and	Its	Role	in	the	Transmission	of
Infectious	Diseases.	2013;
doi:	10.1155/2013/493960		j.	of	pathology

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