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Cyclone and Storm Surge - Iczmpwb.org

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4.24<br />

Δ p<br />

p(r) = p( ∞)<br />

−<br />

[1+ (r/R )<br />

2 1 / 2<br />

]<br />

(Isozaki, 1970) (28)<br />

Δ p<br />

p(r) =1010 −<br />

2<br />

[1+ (r/R ) ]<br />

(Das et al., 1974) (29)<br />

p(r) = p( ∞)<br />

−Δ p exp ( −r/R)<br />

(John <strong>and</strong> Ali, 1980) (30)<br />

where, p (r) <strong>and</strong> p (∞) represent sea level pressure at r <strong>and</strong> at the cyclone periphery, R is the radius of<br />

maximum winds <strong>and</strong> Δp is the pressure drop.<br />

The wind distribution in the cyclone is then calculated from the cyclostrophic wind or gradient wind<br />

formula. The cyclostrophic wind corresponding to the pressure field given by (29) is:<br />

V<br />

2<br />

= 4V<br />

2<br />

m<br />

2<br />

2 2<br />

[ μ ÷ (1+ μ ) ]<br />

where, μ = r/R <strong>and</strong> Vm is the maximum wind at R. The maximum wind (in knots) <strong>and</strong> the pressure drop<br />

(mb) may be related by:<br />

1<br />

V 2<br />

m = C ( Δ p)<br />

(32)<br />

where, “C” is a numerical constant.<br />

Johns <strong>and</strong> Ali (1980) use the following gradient wind formula for computing the wind distribution<br />

corresponding to the pressure field (30):<br />

(31)<br />

V = −<br />

fr<br />

2<br />

⎡f<br />

r<br />

+ ⎢<br />

⎣ 4<br />

1<br />

2 2<br />

2<br />

r ∂ p⎤<br />

+ ⎥<br />

ρ<br />

a<br />

∂ r ⎦<br />

where, ρa is the density of the air, taken as 1.293 kg m-3.<br />

(33)<br />

A number of other cyclone models compute the wind field by one of the following expressions:<br />

V = V<br />

m<br />

⎛<br />

⎜<br />

⎝<br />

r<br />

R<br />

3<br />

2<br />

⎞<br />

⎟<br />

⎠<br />

, 0<br />

≤ r ≤ R<br />

, (Jelseninanski, 1965) (34)<br />

V = V<br />

m<br />

⎛ R ⎞<br />

⎜ ⎟<br />

⎝ r ⎠<br />

1<br />

2<br />

,<br />

r > R<br />

, (35)

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