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Newark Bay Study - Passaic River Public Digital Library

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1-14<br />

Bottom sediments were also characterized in detail as part of this early sampling program<br />

(~100 surface sediment samples). The results indicated that the surface sediments of the northern<br />

region of <strong>Newark</strong> <strong>Bay</strong> are primarily composed of particulate material having a grain size that is<br />

representative of silt. The lower Hackensack <strong>River</strong> sediments have a somewhat coarser texture than<br />

the lower <strong>Passaic</strong> <strong>River</strong> and northern <strong>Newark</strong> <strong>Bay</strong> sediments. The sediment composition becomes<br />

coarser in texture in the direction of South <strong>Newark</strong> <strong>Bay</strong>, a trend that likely reflects the more intense<br />

long-term dredging activity and relatively high current speeds in that area, particularly in the Kill van<br />

Kull. Surficial bottom sediment concentrations were also measured, with a focus on levels of total<br />

organic carbon (TOC) and 8 metals: Hg, Cd, Pb, As, Cu, Zn, Cr and Ni. The concentrations of<br />

these constituents will be discussed in a later section of this report.<br />

Suszkowski used the 1976 monthly monitoring data, supplemented by additional sources of<br />

information on velocity profiles at the 4 <strong>Newark</strong> <strong>Bay</strong> boundaries, to develop a detailed inorganic<br />

solids balance for the system. The approach was to evaluate the surface and bottom layer flows at<br />

each of the four points of entry to the <strong>Bay</strong> (discussed above), and to then assign the observed<br />

average TSS concentration to each of these. (It is of interest to note that the boundary at the <strong>Passaic</strong><br />

<strong>River</strong> had a distinctly different TSS profile than the other locations, with the surface layer TSS being<br />

consistently higher than the bottom layer TSS concentration.) The product of the flow and TSS<br />

concentration in the surface and bottom layers yields an estimate of the mass flux rate, and the<br />

difference between the surface and bottom layer fluxes represents an estimate of the net flux across<br />

each <strong>Newark</strong> <strong>Bay</strong> boundary. Additional internal sources of solids, including TSS inputs from<br />

wastewater treatment plants, urban runoff and phytoplankton production were also quantified.<br />

Finally, a net solids balance for the entire <strong>Bay</strong> was obtained by evaluating the sum of all of these<br />

inputs.<br />

The results of Suszkowski’s solids balance analysis are summarized on Figure 1-3. It is<br />

evident from these results that the <strong>Passaic</strong> <strong>River</strong>, Kill van Kull and Arthur Kill were all net sources<br />

of TSS to <strong>Newark</strong> <strong>Bay</strong>, while the Hackensack <strong>River</strong> was a net sink of solids at the time of this<br />

investigation. This latter finding was recently confirmed by simulations performed with the <strong>Newark</strong><br />

<strong>Bay</strong> model by Pence (2004). The simulations involved the initialization of a particle concentration<br />

of 1 mg/L in the <strong>Passaic</strong> <strong>River</strong>, on a monthly basis, and then tracking the movement over these<br />

particles over the course of an annual cycle. The particles tended to move from the <strong>Passaic</strong> <strong>River</strong>,<br />

into <strong>Newark</strong> <strong>Bay</strong>, and then left <strong>Newark</strong> <strong>Bay</strong> by transport into the Hackensack <strong>River</strong>, or by transport<br />

out of the system in the surface layers of the Arthur Kill and Kill van Kull. The difference in<br />

transport regimes for the Hackensack and <strong>Passaic</strong> <strong>River</strong>s is partly explained by the relatively low<br />

freshwater flow in the Hackensack <strong>River</strong>, as this facilitates the upstream transport of solids from the<br />

<strong>Bay</strong>. Additionally, during high flow events there is relatively little upstream storage in the <strong>Passaic</strong><br />

<strong>River</strong>, so peak flow rates propagate through the system with relatively little attenuation. This differs<br />

from the situation in the Hackensack <strong>River</strong>, where upstream reservoir storage will absorb many of

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