Disclaimer: The views expressed within this website do not represent the views of the National Oceanographic Centre of Southampton; University of Southampton; or Falmouth Marine School. We would like to thank Falmouth Marine School for the collaborative efforts involved.


Home Offshore Estuarine Geophysical Pontoon

 Overview


With the use of the King Harry Pontoon halfway down the Fal River, group 5 carried out sampling of the surrounding water. A Secchi disc, current meter, light meter and YSI probe were used to measure the following parameters: temperature, salinity, depth, dissolved oxygen, pH, current speed and direction and light. Measurements were taken every 30 minutes starting at 0845UTC and finishing at 1215UTC. The results from all groups were collated in order to obtain a time series. The pontoon can be found at the points 50° 12.57’ N 005° 01.37’ W.



YSI Probe

Temperature

The temperature of the water column is higher at the surface and decreases with depth as shown by (figure). The increased temperature at the surface is due to solar radiation heating the top layer of the water column. A change of around 1°C is indicated between the surface and the depth. Around 1000UTC the water column is, on a whole, warmer than at 1130UTC, due to warmer water penetrating further down the water column. As the tidal height increased, increasing the sample depth, the temperature of the lower water column decreases.

Salinity

Salinity increases with depth as indicated in (figure). The salinity is lowest at the surface due to the freshwater riverine input, and also high rainfall from the previous day. The freshwater is less dense and therefore sits on top of the more dense salty water. The salinity increases at depth due the intrusion of sea water from the flowing tide.

Density

Density is directly influenced by temperature and salinity. The density profile of the water column (figure) generally increases over the duration of the time series. This is a direct result of the general decrease in temperature and increase in salinity observed. Both of these property changes are due to the influence of colder, more saline water from the flowing tide.

Dissolved Oxygen

Dissolved oxygen  saw a sharp increase from 82% to 92%, peaking at 1015UTC, see (figure). This gradient of increase then flattened out and dissolved oxygen throughout the water column became far more uniform over the 2 hour time period. Dissolved oxygen is affected by the temperature of the water, with the capacity for dissolved oxygen increasing with decreasing temperature; a trend that was present during the observation. Dissolved oxygen is also influenced by levels of primary production in the area, however without any recorded data regarding this parameter, any reference to it would be speculative.

pH

Despite the increase of dissolved oxygen in the water column, which generally results in a more basic pH value, the pH profile of the water column decreases at roughly 0945UTC, see (figure). This decrease in pH is very small at 0.4, but due to the scale of the graph it appears to be more dramatic. This pH change is not very significant and could be due to systematic or human error.



 Reference


Estep, L. 1992, ‘Profile models of the diffuse attenuation coefficient’, Environmental Software, 7, 2, 95-102.

 Current Meter


Current magnitude and direction

The current magnitude and direction are represented by a series of vector plots over the duration of the study (from after low tide to just before high tide). (Figure) shows the tidal current increasing in intensity (up to 0.13 m.s-1) as the tide comes in, as well as the general river flow (average of 0.1 m.s-1) and the increase in tidal height (2.3 m over the 3.5 h). The profile at 1215UTC is closest to HW, and may show turbulence through the water column. However, the instrument might have been biased as certain depths recorded a velocity of 0 m.s-1, which is not consistent with the profiles, therefore the picture depicted from this data is not complete.


 Light Meter


Irradiance

From the (figure), it is clear that the strongest irradiance is at the surface. For the majority of the time series, there was 8/8 oktas cloud cover, meaning that the overall irradiance would be relatively low (i.e below 200 µmol.m-2.s-1), as shown in. Due to local disturbances, there are some fluctuations in irradiance throughout the times series; this may have been due to local variations in cloud thickness or – more importantly – variations in suspended particulate matter. The continuing reoccurrence of local boats and ferries may have contributed to some of this increased suspended material in the water column. The most noticeable area of higher irradiance in occurs after 1145UTC, where values of up to 300 µmol.m-2.s-1 were recorded. This could have been due to small breaks in the cloud cover, as brief pockets of sunshine did appear towards the end of the time series. As 1145UTC is approaching the time of the day where incoming solar radiation is strongest, this could have also contributed to the high irradiance values recorded. The Secchi disk depths correspond well to the levels of recorded irradiance from the light meter e.g. during the times of strongest irradiance, the Secchi disk depth increases, as the light is able to penetrate deeper.

Attenuation coefficient

During the sampling of the shallow waters, at the pontoon on the River Fal, the 1% light depth, as estimated by both the Secchi disk and the light probe and PAR meter, was not reached. This is because the water column was too shallow. Light attenuation coefficients, k values, vary significantly in depths shallower than the 1% light depth and therefore they have not been calculated at the pontoon (Estep, 1992).

Time Series

temp.jpg sal.jpg dens.jpg disoxy.jpg ph.jpg current.jpg irrad.jpg

Temperature

Salinity

Density

Dissolved Oxygen

pH

Current

Irradiance