1. Tides, Sea Level and Water Currents |
1.1 Basic theory
|
|
|
|
|
|
Most introductions, including Our Restless Tides and Professor Tomczak's website, explain tides in terms of a balance between gravitational and centrifugal forces. It is such an explanation that led to the figure above. Alternatively, introducing the concept of the "tidal potential" many of the complexities (such as illustrated in the figure above) of the force balance can be avoided. The Canadian Tidal Manual (Warren, 1983), online (in pdf format), discusses both approaches. This text requires slightly more advanced mathematical knowledge, but only by understanding the tidal potential can one understand the theoretical basis for the harmonic method of tidal analysis. It is more than twenty years old, but the theory has not gone out of date. Finally, Pugh (1987) and Pugh (2004) have chapters on tidal theory written in a modern, textbook style. |
1.2 Tidal terminology |
|
|
|
|
1.3 Analysis and prediction |
|
|
|
|
| Constant | Definition |
|---|---|
|
Major Diurnal Constants |
|
O1 |
|
K1 |
|
|
Major Semi-Diurnal Constants |
|
M2 |
|
S2 |
|
1.3.1 Tidal analysis |
|
|
|
|
1.3.2 Tide prediction packages |
|
|
|
|
1.3.3 Tidal classification |
|
|
"All tides are composed of both semi-diurnal and diurnal components, the latter introducing inequality in successive heights of high or low water and also in the times. When this diurnal inequality reaches a certain limit, it becomes more informative to list the average heights of the higher and lower high and low waters rather than the average spring and neaps values. The division between diurnal and semi-diurnal tides is arbitrary. In these tables the following criterion is used: When (K1 + 01)/(M2 + S2) is less than or equal to 0.5,
the tide is considered to be semi-diurnal. When (K1 + 01)/(M2 + S2) is
greater than 0.5, the tide is considered to be diurnal. In some areas these
formulae are unsatisfactory and a more detailed study of the harmonic
constants is necessary to determine tidal characteristics". |
|
1.3.4 Analysis of tidal currents |
|
|
|
|
1.3.5 Long term sea level variability |
|
|
|
|
1.4 Environmental effects on sea level |
|
|
|
|
1.4.1 Weather-related effects |
|
|
The appendices of the NSW
Coastline Management Manual contains descriptive reviews of coastal processes and
the effects on beaches of storms and other weather-related events. The
climate-related information is primarily focused on NSW, but the majority
of the information is more general. Warren (1983) (Chapter 4) describes wind set-up of sea level
at the coast, wind-driven currents, atmospheric pressure effects, storm
surges, seiches, precipitation, and runoff, written for the purposes of the
tidalist. Pugh (1987) also covers most of those topics. Some nice
illustrations and discussion of coastal processes can be found in Chapter 4 of
Shelf and Coastal Oceanography by Prof. M. Tomczak.
The effect of CTWs on coastal sea level is clearly visible in the
preceding figure. A typical case begins somewhere in the vicinity of
Hillarys, WA on 10 July. Onshore winds with peak gusts of 25 m/s (about 50
knots) drove water forward onto the shelf, sending sea levels at the tide
gauge to about 30 cm above the predicted tidal value and initiating a CTW.
CTWs travel along coastlines over the continental shelf. In the southern
hemisphere the direction of travel is such that the coastline is to the
left of the wave, so the CTW propagated southwards from Hillarys. It was
evidently reinforced over the following days by onshore or north-westerly
winds. The wave rounds the southwest corner of Australia, then turns to the
east, successively raising sea levels by a half-metre or so at Esperance,
Thevenard, Port Stanvac (Adelaide), Portland, and Lorne, finally entering
Bass Strait a day or two after leaving Hillarys. A second CTW appears to be
generated in the Bight itself on the 21st, with large residuals
observed first at Esperance, and then stations to the east. |
|
1.4.2 Shallow water effects |
|
|
"Ports which are situated in shallow water may have distorted tidal profiles, and this distortion may take many forms. In some cases, the distortion takes the form of a short period of rising tide and a long period of ebb, and at some places this can take the extreme form of a bore, particularly at spring tides. At other ports, the shallow water effects may cause double high or low waters, or perhaps a stand of tide lasting several hours; again the effect can vary considerably between spring and neap tides." An
introductory-level discussion is contained in Warren (1983). Many, but not
all, shallow water effects on tides can be accounted for by use of the full
112-constituent analysis. Tsunamis are well-known for their destructive impacts on many coastal areas. These also are essentially shallow-water phenomena since the generating wave is barely discernible in the open ocean. Recordings of tsunami are rare in Australian waters, but not unknown (see the Geoscience Australia factsheet). IOC Vol.1 states: "A
tsunami is a wave generated by seismic activity and as such falls outside
the two categories of forces responsible for normal sea level changes,
tides and the weather. Not all submarine earthquakes produce tsunami. The
important element is a vertical crustal movement which displaces the sea
bed. The tsunami wave characteristics will depend on the amplitude of the
displacement and the dimensions of the sea bed involved. Horizontal
displacements of the seabed will be relatively ineffective. The waves
travel at a speed given by (water depth • gravitational acceleration)½.
Amplitudes in deep water are small, probably not more than 1 metre. The
Pacific Ocean and its coastlines are the most vulnerable to tsunami because
of the seismically active surrounding plate boundaries. As the wave
approaches shallow coastal waters its amplitude increases and there are
multiple reflections and refractions which combine to give very large local
amplitudes. A network of reporting tide gauges in the Pacific enables
warnings of tsunami arrival to be given some hours in advance." |
|
1.5 Tidal datum epoch |
|
|
|
|
1.6 Tidal planes and levels |
|
|
|
|
1.6.1 Harmonics-based definitions |
|
|
The following definitions, based on the tidal harmonics, are taken from the ANTT. The harmonic definitions can be considered convenient simplifications. The Intergovernmental Committee on Surveying and Mapping (ICSM), Tidal Interface Working Group (TIWG), has produced a 103-page compendium of terms related to the legal definition of the land-sea boundary in Australia. It can also be found as a summary . In the following, Z0 represents the mean sea level, and the other symbols are the usual harmonic constants. For semi-diurnal ports: Mean High Water Springs: MHWS = Z0
+ (M2 + S2) Mean High Water Neaps: MHWN = Z0
+ |M2 - S2| . Mean Low Water Springs: MLWS = Z0
- (M2 + S2) Mean Low Water Neaps: MLWN = Z0
- |M2 - S2| For diurnal ports: Mean Higher High Water: MHHW = Z0
+ (M2 + K1 + O1) Mean Lower High Water: MLHW = Z0
+ |M2 - (K1 + O1)| . Mean Higher Low Water: MHLW = Z0
- |M2 - (K1 + O1)| Mean Lower Low Water: MLLW = Z0
- (M2 + K1 + O1) |
|
1.6.2 Observations-based definitions |
|
|
The harmonic-based definitions are not universally accepted, in part
because they assume that M2, S2, O1,
and K1 are the dominant four components, which is not
always the case. For this reason, many authorities (e.g., MSQ and NOAA)
adhere strictly to observation-based definitions of the tidal planes. The
TIWG list of standard terms in the table below gives observation-based
definitions from the Australian
Hydrographic Office tidal glossary. Variations of the definitions may
apply in current legislation.
|
|