The twice-per-day tides bringing in warm, saline wa-
Table 5. Ice design criteria for Cook Inlet pe-
ter from the Gulf of Alaska,
troleum industry platforms. (After Visser
The tides moving ice from freshwater areas where it
1992, p. 148.)
grows more rapidly to more saline water where it
tends to melt, and
Design Criteria
North- and northeast-trending winds during the win-
ter, which move ice down-Inlet to areas of melting.
Original
API (1988)
Design parameter
design
Recommended
Less-predictable negative factors include the incidence
and amounts of solar radiation and snow cover on the
Ice thickness, level ice (m)
1.1
0.60.9
ice. Also, southern air masses with above-freezing air
Ice thickness, rafted ice (m)
NA
1.21.5
temperatures can sometimes blanket the region for
Compressive strength,
3.8
3.44.1
unconfined (MPa)
days at a time, causing rapid decay of a well-
Compressive strength,
300
275330
established ice cover. Occasionally volcanic eruption
confined (MPa)
has been known to melt the ice cover. This was in-
40 106
42 106
Maximum load (MN)
deed the case in January 1976, when an eruption of
Mount St. Augustine during a 5-day period raised the
water temperature at the Dolly Varden platform
(approximately 24 km NNE of West Foreland) from
2.2 to +1.0C. At the same time the ice concentration
in the Inlet reportedly went from 95% to less than 50%
(Schulz 1978).
3.3 Theoretical ice growth and melt
Sea ice growth and decay is a highly complex sub-
Compared to other arctic regions where multi-year
ject that relates to a wide array of environmental fac-
ice and icebergs occur, Cook Inlet ice conditions might
tors, such as air temperature, solar input, salinity of
be considered mild. However, they are significant be-
the water and the ice, and exposure to wind, waves,
cause the first offshore developments in ice-infested
and tides. In Cook Inlet it is especially difficult to pre-
waters for the petroleum industry were built in Cook
dict ice conditions because of the extreme magnitudes
Inlet. Four oil fields and one natural gas field were
and constant fluctuation of the variables discussed in
developed in the early 1960s in Upper Cook Inlet. The
Section 3.2. However, since Poole and Hufford (1982)
first fourteen offshore drilling and production plat-
determined a reasonable correlation between accumu-
forms were built during 19641968 (Visser 1992), and
lated FDDs and Upper Inlet freeze-up, temperature
environmental data necessary for their design were
appears to be the best single indicator of the severity
largely nonexistent. Some of the earliest ice environ-
of the ice season. In this section we calculate theoreti-
ment studies in Cook Inlet were financed by the pe-
cal ice sheet thickness values for Cook Inlet using
troleum industry to ensure that the structures were con-
simple models based on the average air temperatures
structed to withstand the forces imposed by the moving
in Anchorage. The models assume that when the mean
ice pack. The fact that there are now hundreds of plat-
daily air temperature is less than a specified value, ice
form-years of performance experience without a ma-
will form, and when the temperature is higher than a
jor failure testifies to the competence of the structural
specified value, the ice will melt.
designs. Several published sources describe the data,
LaBelle et al. (1983) stated that Brewster's calcu-
procedures, and assumptions that engineers used to
lations of ice growth in Cook Inlet were made using a
design the offshore and along-shore structures in Cook
reformulation of Zubov's (1945) model:
Inlet (e.g., Blenkarn 1970, Sanderson 1988, Visser
1992, Utt and Turner 1992, Bhat and Cox 1995). Visser
I 2 + 50 I = 8R
(1)
(1992) listed parameters that governed design of the
original platforms and compared them with recom-
where I is the ice thickness (cm) and R is the number
mended guidelines that were later adopted by the
of freezing degree-days that had accumulated in An-
American Petroleum Institute (API 1988). These are
chorage, assuming a base temperature of 0C. Solv-
shown in Table 5. The original design assumed a level,
ing the quadratic equation in the manner of Bowditch
undeformed ice thickness of 1.1 m, which the API later
(1979) yields a form of the equation from which the
amended to 0.60.9 m in its guidelines. The API also
ice growth, Ig, can more easily be determined as a func-
recommends a design thickness of 1.21.5 m for rafted
tion of the sum of FDDs. That is,
ice.
17