P. Flanagan et R. Eccles, SPONTANEOUS CHANGES OF UNILATERAL NASAL AIR-FLOW IN MAN - A REEXAMINATION OF THE NASAL CYCLE, Acta oto-laryngologica, 117(4), 1997, pp. 590-595
It is now over 100 years since Kayser (Arckiv fur Laryngol Rhinol 1895
; 3: 101-120) first reported in the scientific literature that the hum
an nasal passages exhibit spontaneous changes in unilateral nasal airw
ay resistance, yet our understanding of this unusual phenomenon is sti
ll very confused. Spontaneous. reciprocal changes in unilateral nasal
resistance are often referred to as a ''nasal cycle'' and although thi
s term is now commonly used to describe spontaneous changes in nasal r
esistance in man and animals, there is little evidence for any true pe
riodicity. A major problem in increasing our knowledge and understandi
ng of the so-called ''nasal cycle'' is that most studies have relied o
n simple descriptions of the changes in nasal resistance and have not
developed any numerical parameters to quantify the changes in resistan
ce over time. This lack of definition of what actually constitutes a n
asal cycle has meant that the literature of the present day generally
accepts the views put forward by Heetderks (Am J Med Sci 1927: 174: 23
1-244) and Stoksted (Acta Otolaryngol (Stockh) 1953; Suppl 109:159-175
) that around 80% of the healthy population exhibit a regular cycle. I
n order to define the characteristics of the spontaneous changes in na
sal airway resistance we have used numerical measures of reciprocity a
nd also developed a measurement of the division of airflow between the
nasal passages over time. With these two parameters it is possible to
describe the nature of the spontaneous changes in airflow in numerica
l terms and to define what exactly constitutes a nasal cycle. Fifty-tw
o volunteers underwent hourly measurement of unilateral nasal airflow
for 8 h. For each volunteer, two values were derived from the graph of
unilateral nasal airflows against time: the correlation coefficient b
etween unilateral airflows (r) and the airflow distribution ratio betw
een the two nasal airways (ADR). The spread of different types of airf
low pattern (nasal cycle) throughout the population was illustrated by
plotting r against ADR for each subject. A nasal cycle was defined as
having an I value between -0.6 and -1.0, and an ADR value between 0.7
and 1.0. Only 21% (11 of the 52 volunteers) exhibited airflow pattern
s that could be defined as a nasal cycle in these terms. This finding
contradicts the generally accepted, but undefined, view that around 80
% of the population exhibit a regular nasal cycle. The numerical defin
ition of a nasal cycle in terms of both reciprocity and airflow distri
bution. as described in this payer may help to clarify our understandi
ng of this interesting phenomenon and allow rhinologists to describe t
he spontaneous changes in nasal airflow in more exact terms than have
been used previously in the literature.