impacts on marine spill
DESCRIPTION
The potential impacts a marine oil spill would have in Shxw’ōwhámel territory.TRANSCRIPT
EmergWest Consulting Trans Mountain Expansion Project
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Summary
This report was undertaken, at the request of the Shxw'owhámel First Nation and Peters Band,
to consider the possible impacts of a crude oil spill from the proposed Trans Mountain Expansion
Project (TMEP) pipeline expansion project. Specifically, this report was to include a review of the
materials provided by TMEP in their application, with a specific view of the fate (how oil will age
and spread when spilled) and the oil spill prevention and response measures proposed by
TMEP.
The report is divided as follows:
1. Human/Health Affects
2. Evacuation of Residents
3. Affects to Groundwater
4. Incident Command System (ICS) Training for First Nations Personnel
5. Oil Spill Response Equipment
6. Spilled Oil Fates
7. Spilled Oil Trajectories
8. Submerged/Sinking Oil
9. References
Because of the significance of the potential for spilled crude to submerge or sink, a considerable
part of the report is dedicated to understanding how and why some oils sink, and the current
state of countermeasures if they do, including a case study of the Enbridge Line 6b incident in
Marshall, MI, USA.
Generally, the TMEP submission, while extensive, lacks key details in terms of many of the
various model inputs (and outputs), and relies on the Gainford Study, which, because it does
not consider fresh or sediment‐laden water spills, is largely irrelevant for predicting spilled oil
fates in the areas important to the Shxw'owhámel First Nation and Peters Band.
While this report focuses on the potential direct affects to the two First Nations (FN), additional
input is provided on the various submissions that, while not directly applying to the FN areas,
have broad response implications in all spill conditions and locations.
While generally spills from pipelines are infrequent, there remains a chance of a spill that could
affect the immediate health and safety of the Shxw'owhámel First Nation and Peters Band, as
well as long‐term affects to both their traditional territories and Reserves.
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1 Human/HealthImpacts
CrudeOilVapourExposuretoResidents
Due to the proximity of the pipeline, and the projected paths (see Section 7) of any spilled
crude oil, it is possible that flammable and/or toxic vapour concentrations could form in air,
thus directly affecting the Peters or Shxw'owhámel First Nations (in the event of a nearby
release), or limiting their ability to safely leave the affected area.
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1.1 PotentiallyFlammable/ExplosiveVapours
Crude oils emit vapours that, if they reach a sufficient concentration in air, can ignite, and if
those expanding vapours meet resistance, can explode. Pure chemicals have very well‐
understood ranges in which these vapours can form flammable mixtures in air. The minimum
amount of fuel in air that can form a flammable mixture is called the Lower Explosive Limit
(LEL). The upper limit, which if exceeded would be too rich, is called the Upper Explosive Limit
(UEL). The range of vapour mixtures (from LEL to UEL) that can ignite is called the flammable
range.
The lower explosive limit of most crude oils is around 1.5% in air. As an example, Cold Lake
Blend (CLB), based on the crudemonitor.com web site, includes numerous constituents (see
Figure 1.1) which include Benzene (LEL of 1.35%), Pentane (LEL of 1.4), Hexane (LEL of 1.1), and
Heptane (LEL of 1.0).
Figure 1.1
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If a CLB spill were to occur, then the Lower Explosive Limit would be approximately 1.5% (fuel in
air). It should be noted that oil spill responders (when responding to crude oil spills) normally
calibrate their vapour monitors using pentane (LEL of 1.4) in order to mimic the anticipated
vapours, thus providing additional support to the following calculations:
The LEL of CLB (1.5 % fuel in air) expressed as a decimal = 0.015
The LEL expressed in parts per million (ppm) = 15,000 ppm
10% of the LEL = 1,500 ppm
A number of models were developed by the author (see Section 1.3.4) to try determine the
potential extent of a vapour plume from a crude oil spill. The model outputs depict the possible
vapour plumes (total hydrocarbons) one hour after a CLB crude oil release near each of the
Shxw'owhámel and Peters Reserves. The blue plume (see Figures 1.7 and 1.8), stretching
approximately 800 m, depicts a range of total hydrocarbons of from 10,000 – 100,000 ppm
(with the high end of the range occurring closer to the source). While these highly‐volatile
vapours are typically transient (they will deplete relatively quickly, usually within a few hours),
there is still potential for potentially‐flammable vapours to form in air, and for those vapours to
drift across HWY 1, the railroad tracks, and to disallow the safe egress out of the affected
Reserves (and the safe ingress for responders).
Further, emergency responders, equipped with vapour monitors are trained to leave the area
immediately if they encounter readings exceeding 10% of the Lower Explosive Limit (for
precautionary safety reasons).
The dark green plume (which stretches approximately 2.5 km) includes a concentration equal to
10% of the LEL, and would not only cross the highway and the rail tracks, but would extend well
beyond the only egress routes (of either affected First Nation), and would reach the homes of
the band members. Again, the potential vapour clouds could, at least for a time, prevent band
members from escaping the area, and could also prevent emergency responders from entering
the area to provide assistance to band members.
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1.2 PotentiallyToxicVapours
Crude oils, due to their complex makeup, can emit a wide range of potentially poisonous (toxic)
vapours. These can include Hydrogen Sulphide (H2S), a vapour which is heavier that air, and is
known to, at higher concentrations, pose potentially‐serious (and life‐threatening) hazards.
Other vapours typically emitted from evaporating crude oils include Benzene, Toluene, Ethyl
Benzene, and Xylene (commonly called BTEXs). Of these, Benzene is considered the most
dangerous, as it is a known carcinogen (the others are suspected carcinogens).
While there are no set limits for exposure to benzene, the US Environmental Protection Agency
states:
Neurological symptoms of inhalation exposure to benzene include drowsiness, dizziness,
headaches, and unconsciousness in humans. Ingestion of large amounts of benzene may
result in vomiting, dizziness, and convulsions in humans. (1)
Exposure to liquid and vapor may irritate the skin, eyes, and upper respiratory tract in
humans. Redness and blisters may result from dermal exposure to benzene. (1,2)
Animal studies show neurologic, immunologic, and hematologic effects from inhalation
and oral exposure to benzene. (1)
Tests involving acute exposure of rats, mice, rabbits, and guinea pigs have demonstrated
benzene to have low acute toxicity from inhalation, moderate acute toxicity from
ingestion, and low or moderate acute toxicity from dermal exposure. (3)
The reference concentration for benzene is 0.03 mg/m3 based on hematological effects
in humans. The RfC is an estimate (with uncertainty spanning perhaps an order of
magnitude) of a continuous inhalation exposure to the human population (including
sensitive groups) that is likely to be without appreciable risk deleterious non‐cancer
effects over a lifetime. (4)
The modelling conducted by TMEP shows potentially‐dangerous vapour plumes drifting as far
as 1‐2 km from the spilled crude (see below, from Volume 7 Part 12 – Oil Spill Study).
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Figure 1.2
The contour shown in Figure 1.2 depicts a benzene concentration in air of up to 1,000 µg/m3
(approximately 0.3 ppm) reaching almost 1 km. Unfortunately, the model output above does
not include any details of:
The crude oil modelled
The volume of oil
The pooled oil thickness or area
The wind speed
Although these is no limit for exposure for benzene, the Time‐Weighted Average (TWA)
threshold for workers (the level at which responders would don respiratory protection) is 0.5
ppm.
Since the TMEP model did not include any details on the parameters that resulted in the output
in Figure 1.2, a number of models were run by the author using various Alberta‐sourced diluted
bitumen crudes (dilbits) and synthetic bitumen crudes (synbits), under a number of conditions
in order to try to characterize the range of potential impacts from evaporating vapours from a
potential crude oil spill in proximity to either the Shxw'owhámel First Nation or Peters Band.
These are included in Section 1.3.
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1.3 AirMapVapourModelling
The vapour plume modelling conducted as part of this study used AirMap, and was developed
by RPS ASA (which has provided oil spill and related modelling and software since 1979, and is
widely‐recognized as an industry leader) AirMap is an atmospheric dispersion model designed
to predict the trajectory and fate of a wide variety of chemical substances and biological agents
in the atmosphere. The model uses physical and chemical properties, such as vapor pressure
and environmental degradation rates, to predict the fate of substances that have been released
into the atmosphere.
The mass is dispersed horizontally by turbulence, either using a user‐input constant rate
(horizontal dispersion coefficient) or following the algorithm from Gifford (1961), as described
in Csanady (1973). The model‐calculated horizontal dispersion coefficient is a function of wind
speed and air stability. Stability is defined as:
Moderately stable
Slightly stable
Neutral
Slightly unstable
Moderately unstable
The US EPA and NOAA (2002) offers the following guidance (based on Turner, 1970) in the
Aloha model regarding atmospheric stability:
“The atmosphere may be more or less turbulent at any given time, depending on the
amount of incoming solar radiation as well as other factors. Meteorologists have defined six
atmospheric stability classes, each representing a different degree of turbulence in the
atmosphere. When moderate to strong incoming solar radiation heats air near the ground,
causing it to rise and generating large eddies, the atmosphere is considered ‘unstable’, or
relatively turbulent. Unstable conditions are associated with atmospheric stability classes A
and B. When solar radiation is relatively weak, air near the surface has less of a tendency to
rise and less turbulence develops. In this case, the atmosphere is considered ‘stable’, or less
turbulent, the wind is weak, and the stability class would be E or F. Stability classes D and C
represent conditions of more neutral stability, or moderate turbulence. Neutral conditions
are associated with relatively strong wind speeds and moderate solar radiation.”
Stability class has a big effect on the modeled dispersion of a gas. Under unstable conditions,
for example, a dispersing gas will mix rapidly with the air around it and the pollutant will be
diluted more quickly below levels of concern then it would for more stable conditions.
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1.4 AirMapModelInputs
The key model inputs used in the AirMap model were the simulation length, crude oil, volume
and spill duration, wind speed and direction, and the various model‐specific criteria.
1.4.1 ModelLocationandSimulationLength
Models were run based using a relatively short duration (2 hours), due to the proximity of the
pipeline to the two Reserves.
Figure 1.3
1.4.2 ModelOil,VolumeandSpillDuration
The crude oil simulated in the models was Cold Lake Blend, at a relatively conservative estimate
of 200 m3. The models were run for 2 hours (the output shown is after 1 hour).
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Figure 1.4
1.4.3 ModelWinds
The winds chosen for the models represents a worst‐case scenario, i.e., light winds (4 knots)
from the SE. The light winds would cause the vapours to drift towards the Reserves, with little
dispersion (reduction in concentration).
Figure 1.5
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1.4.4 AirMapModelParameters
The model parameters chosen were the defaults provided with the model. The shortest
possible time step (1 minute) was used, and the 3D dispersion was calculated by the model. An
open country ground roughness was chosen to best‐represent the area.
Figure 1.6
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1.4.5 AirMapModelOutputs
The model outputs below depict the possible vapour plumes (total hydrocarbons) one hour
after a CLB crude oil release near the Shxw'owhámel and Peters Reserves.
Figure 1.7
Figure 1.8
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1.4.6 PotentialImpactsfromVapours
Based on the example vapour plumes shown in 1.7 and 1.8, the potential down‐wind distance
that could be affected could extend to the First Nations’ egress routes, and in some cases, to
their homes.
If benzene represents as little as 0.1% of the total crude oil (this is typical of many Canadian
Synthetic crudes), then the blue plume contour (from Figures 1.7 and 1.8) represents a range of
10 to 100 ppm of benzene.
Further, if spilled crude oil spreads down‐current, as is predicted by the TMEP models (see
Section 7), there is a real likelihood that residents of either of the affected First Nations would
be well within the corridor of potentially‐toxic or flammable concentrations (or at least
concentrations which could limit the ability of responders to provide support to affected band
members).
Even in a best‐case scenario, it is highly‐unlikely that responders could stop, either the spread
of crude oil, or its evaporating vapours, before it would affect the Reserves. As such, it is
critically important to know what measures TMEP will take to ensure the safety of the Peters
and Shxw'owhámel First Nations in the event of a spill in the area.
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2 Evacuation
There is only one road into/out of the Shxw'owhámel Reserve. Similarly, there is one primary
road, which splits into two exits (one for each direction of the highway), into and out of the
Peters Reserve. Depending on the wind direction, it is possible that the only egress route for
evacuating residents would be blocked by potentially dangerous vapour concentrations.
Based on the overland models (Section 7) and the vapour plume models (Section 1.3), it is
critically important that TMEP provide details of the Plan to provide evacuation options to the
members of the two Reserves, especially given the potential that responders may not be able
to enter the affected area. The Plan should answer the questions:
How will band members know if the egress routes are safe?
How will band members be notified (and by whom)
What vapour monitoring equipment and training will band members have?
Who will make the decision to shelter‐in‐place versus evacuation?
What about band members with disabilities, existing health problems?
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3 GroundwaterImpacts
Residents of both First Nations rely on the groundwater for drinking water, irrigation, and the
cattle farming (Peters).
The proximity of the proposed pipeline makes it next‐to‐impossible for a response to stop
spreading crude oil before it reaches either the Shxw'owhámel or Peters Reserves, (based on
the overland model and the TMEP’s proposed response times). As a result, ground water
contamination is highly likely.
Although benzene is naturally occurring at low concentrations, its presence in the environment
is mostly related to human activities. Gasoline contains low concentrations of benzene (below
1%), and emissions from vehicles are the main source of benzene in the environment. Benzene
can be introduced into water by industrial effluents and atmospheric pollution.
Health Canada has reviewed and assessed all identified health risks associated with benzene in
drinking water, incorporating multiple routes of exposure to benzene from drinking water,
including ingestion and both inhalation and skin absorption from showering and bathing. Health
Canada, in assessing newly available studies and approaches, taking into consideration the
availability of appropriate treatment technology, has established a guideline for benzene in
drinking water at a maximum acceptable concentration (MAC) of 0.005 mg/L (5 μg/L).
The guideline for benzene is established based on cancer end‐points and is considered
protective for all health effects. Benzene is classified as a human carcinogen. Both animal and
human studies report similar toxic effects from exposure to benzene. The most sensitive effects
are found in the blood‐forming organs, including the bone marrow.
The MAC for benzene in drinking water is established based on the incidence of bone marrow
effects and malignant lymphoma in mice, through the calculation of a lifetime unit risk.
For most Canadians, the major source of exposure to benzene is air; this accounts for an
estimated 98–99% of total benzene intake for Canadian non‐smokers. Like food, drinking water
is considered to be only a minor source of exposure to benzene. Benzene can be found in both
surface water and groundwater sources, but it is not generally a concern in surface water,
because benzene tends to evaporate into the atmosphere.
In the event that a crude oil spill affects the groundwater of either First Nation, it is critically
important to know what steps TMEP will take to ensure the mitigation of ground water
impacts, the temporary replacement of safe, reliable water, and the restoration of affected
groundwater.
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4 ICSTrainingforFirstNationsPersonnel
TMEP, in its submission, indicates that, in the event of an incident, TMEP would enter into a
Unified Command which would include affected First Nations.
Volume 7 Part 12 – Oil Spill Study ‐ TMEP was an early adopter of the ICS to manage
emergency response, with introduction of the system in the early 1990s. The ICS
structure outlines clear roles and responsibilities with respect to emergency response
and includes a unified command structure for co‐ordination with the multiple levels of
government; federal, provincial, municipal, and Aboriginal communities, along the
pipeline.
Currently neither the Shxw'owhámel or Peters First Nations personnel have any ICS training
and, as a result, would find it difficult to engage in a Unified Command under ICS. If TMEP
intends to engage First Nations representatives in a Unified Command, it is important to know
if TMEP plans to provide any ICS training to First Nations representatives, and if they will be
asked to attend, and become involved in exercises.
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5 OilSpillResponseEquipment
5.1 LimitationsofOilSpillResponseEquipment
The oil spill response equipment described in the TMEP documents is well‐suited to a relatively
narrow range of real‐life conditions. The oil containment booms described by TMEP (either in
their own Oil Spill Containment and Recovery (OSCAR) trailers, or owned by Western Canada
Marine Response Corp (WCMRC)) work well when containing floating oil in relatively slow (less
than 1 knot) currents, and their ability to deflect floating oil away from sensitive areas
deteriorates quickly in currents exceeding 3 knots. The portable oil skimmers (those that would
be used on spills in rivers) described by TMEP (either in their own OSCAR trailers, or owned by
WCMRC) are designed to work in relatively calm conditions (not in short‐period waves or
turbulence) or in winds exceeding 20 knots. Also, these portable oil skimmers are specifically
designed to recover floating oil, or oil in the top 10‐20 cm of the water column.
During the Deepwater Horizon spill response, the United States Coast Guard (USCG) reports
(see Figure 5.1) that of the approximately 5,000,000 barrels released from the MC 252 well,
around 800,000 barrels (16%) were collected from the devices fitted over the well. If that oil is
taken out of consideration (it is unavailable for recovery), then recovery of oil in open water
using skimmers accounted for around 3% of the oil.
Figure 5.1 – MC252 Oil Deposition (USCG)
The containment and recovery of oil in rivers is often made even more complicated by currents,
limited access, debris, ice, snags safety concerns, and various other issues. Conditions in the
Fraser River would render the use of conventional oil response techniques essentially
impossible during much of the year.
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5.2 Detection,ContainmentandRecoveryofSubmergingandSinkingofOil
Neither TMEP nor WCMRC currently have any spill response equipment suitable for locating,
containing and recovering oil that has submerged or has sunk in moving waters.
Review of Trans Mountain Expansion Project Future Oil Spill Response Approach Plan
Recommendations on Bases and Equipment November 2013 – Page 40 ‐ Oil recovery
devices (commonly referred to as skimmers) remove oil from the surface of the water
using different principles. Skimmers can be either part of a self‐propelled vessel or be a
portable unit assigned to a vessel of opportunity. The proposed skimmer equipment
packages will include a mix of units capable of performing across different operating
environments and in varying weathered oil conditions.
Additionally, neither TMEP nor WCMRC have personnel with experience in the recovery of
submerged/sunken oil in river environments. It is noted that WCMRC personnel were involved
in the Wabamun Lake Bunker C spill, however there are numerous important differences
between the Wabamun Lake spill and a potential spill into the Fraser River, i.e., the oil
properties, the mechanism on sinking/submergence, the currents in the Fraser, and the
techniques available to recover the oil.
The combination of high currents and limited visibility due to suspended sediments would make
the detection and tracking of submerged oil essentially impossible in the Fraser River.
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5.2.1 DetectionofSubmerged/SunkenOil
In order to attempt to contain and ultimately recover submerged/sunken oil, it must first be
located. When spilled oil sinks, or becomes submerged in the water column, it can often be
very difficult to detect. Many different detection techniques have been used and tested over
the years with varying degrees of success.
For spills on the water surface, visual observation is the most common technique used, and
observations can be recorded using photography or video. These visual techniques can
sometimes be used in shallow waters for submerged oils as well, although seaweed and kelp
(and other naturally‐occurring situations) can be easily mistaken for oil. Expert analysis is
essential for this technique (Rymell, 2009).
5.2.1.1Diver‐OperatedRemoteandDetectionSystems
In instances where the visibility on the bottom is a half meter or more, and conditions, i.e.,
currents allow, underwater video detection systems have proved very useful. They provide
documentation of the oil distribution within its limited field of view. However, like most spill
responders, WCMRC and TMEP have no experience with this technology. In these conditions,
helmet‐mounted cameras on divers would likely be required (Rymell, 2009). During the DBL‐
152 spill, a remotely‐operated underwater video recorder was used to successfully provide
quantitative estimates of size and frequency of oil accumulations. Frequent “down” days were
reported because of visibility, and the method could not always determine the exact position of
the spill oil (Counterspil, 2011).
5.2.1.2SorbentDrops
Sorbent drops are generally an ad hoc system consisting of a simple weight and sorbent
material (usually a form of plastic material to which oil will adhere, either through absorption or
adsorption). These are then bounced or dragged along the bottom for short distances, and
then visually inspected for oiling, in an attempt to map oil distribution. These systems are low‐
tech but consist of materials readily‐available on the spill site (Rymell, 2009).
More recently, sorbent cages (see Figure 5.2) have been used in lines to identify oil migration,
as well as being used to try and contain oil from sensitive areas (Rymell, 2009).
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Figure 5.2 – (Photo credit: MPC)
During the response to the M/T Athos 1 incident (a heavy crude oil spill in the Delaware River in
2004), snare samplers consisting of an anchor and sorbent snares connected to a rope with a
float, were deployed downstream of the spill site. Approximately 100 samplers were deployed
in depressions and low‐flow areas where oil was thought to have accumulated. They were then
colour‐coded to indicate the degree of oiling. (Counterspil, 2011) Snare sampling proved to be
ineffective at detecting mobile oil and seemed to push oil away with its wake (Michel, 2008).
Figure 5.3 – Snare Samplers
5.2.1.3ChainDragsandV‐SORS
These systems were designed to be dragged through contaminated water to detect the
presence of submerged oils. Units can vary in size from a single chain with a few snares
attached, to the large Vessel‐Submerged Oil Recovery System (V‐SORS), comprising an 8‐foot
pipe with 28 chains with many snares. It is dragged along or near the bottom through the
water column (Rymell, 2009).
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Figure 5.4 ‐ (Photo credit: US Coastguard and Coastal Response Research Center)
These systems have the advantage of detecting both pooled oil and mobile oil, as well as being
relatively efficient at surveying large areas. They can also be used in vessel traffic lanes (Michel,
2008).
It is difficult to determine the actual value of these systems however, as any oil detected has
been disturbed, and therefore it does not provide data on where oil is, but where it was before
it was disturbed (Rymell, 2009).
There are several limitations to the use of chain‐drags and V‐SORS. The operator cannot
determine the particle size, number of particles, or percent oil cover on the seafloor based on
the visual observations of oil on these systems. As well, the operator cannot determine if the
snares encountered one large patch along the distance of the drag or multiple small patches.
Information is also needed on the efficiency of oil pickup by the snares, as well as the rate of oil
wash‐off from the snares. These systems are also time‐ and labour‐intensive for deployment,
inspection and replacement. Other limitations include strong currents, rough water, vandalism,
and snagging underwater objects (Counterspil, 2011).
During the DBL‐152 spill, both light and heavy V‐SORS systems were used. A large vessel with a
crane was needed for the heavier systems while smaller boats could manually deploy the light
models. Both systems had difficulties in precisely locating the submerged oil (Counterspil,
2011).
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5.2.2 ContainmentofSubmerged/SunkenOil
The Usher (2006) report for the Fresh Water Spills Symposium states “effective containment of
submerged oil is usually next to impossible when currents are present.” (Usher, 2006)
Over the years, many different booms, surface nets, and trawl systems have been used and
tested to contain submerged oil. Results have varied, but have proved useful in some
circumstances. When oil is submerged by thin over‐wash due to weathering, booms can assist
in resurfacing the oil, provided its depth of submergence does not exceed the boom curtain
(Rymell, 2009).
Silt curtains, pneumatic (bubble) barriers have also been suggested. Silt curtains require
contractors who have experience with their deployment and maintenance. In May, 2009, a silt
curtain boom was successfully deployed by Kinder‐Morgan Canada responders during a crude
spill into a retention pond, which stopped the spread of oil entrained in the water column due
to the use of submerged pumps. It must be noted however that the pond had essentially no
currents, unlike the streams and rivers in the Peters and Shxw'owhámel areas of interest.
Nets were ineffective at the Bouchard 155 incident (a bunker fuel spill in Tampa Bay in 1993),
but were effective in the response to the Erika Spill (a bunker spill off the coast of France in
1999), likely due to difference in oil characteristics. Trawl nets have been specially designed for
spill recovery in response to the increased carriage and risks of high viscosity oils (Rymell,
2009). There are commercially‐available net booms, although they only have a depth of 1 to 2
meters, and are restricted to locations with currents below 0.75 knots.₍₂₎ Fishing nets have not
been successful at the recovery of semi‐solid tar balls, and would be even less effective on
more‐liquid oil (Rymell, 2009).
Western Canada Spill Services held trials to evaluate the concepts of sunken oil containment.
They tested fine‐mesh nets as well as sub‐surface containment nets. They concluded in
general that they were not confident the nets were effective at containment or recovery
(Rymell, 2009).
The only documented times sunken oil has been contained, happened naturally when oil
accumulated in low‐flow zones, and existing depressions on the bottom. Trenches and berms
had been considered during the DBL‐152 spill, although it was agreed it would not provide
containment as oil would probably pass over the structure (Rymell, 2009).
Bottom booms, filter fences and trenches must be quickly deployed and their success is highly‐
dependent on bottom current conditions and type of oil (Counterspil, 2011). This would prove
to be next to impossible in the currents found in many parts of the Fraser River.
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5.2.2 RecoveryofSubmerged/SunkenOil
Most non‐floating oil recovery operations have been conducted without the use of
containment. In most cases, the oil has remained in‐situ or has been tracked as it moves.
Despite this, little information is available to verify the effectiveness of not using containment
(Rymell, 2009).
For neutrally‐buoyant oils which remain suspended in the water column, little can be done to
collect it (Michel, 2008).
Experience gained in the Marshall (see Section 8.5) spill is probably the most valuable in terms
of relevance to potential spills from the TMEP expansion project. Once it was determined that
some percentage of the spilled crude oil had made its way to the bottom, a number of
techniques were employed to recover the oil. Sediment poling, a relatively simple technique in
which a pole is pushed into the river sediments to disturb any submerged oil, was found to be
an effective way in locating submerged oil (see Figure 5.5). Work focused on areas of natural
deposition (areas where submerged oil deposits would naturally occur). Once poling identified
submerged oil, sediment coring was conducted to determine the extent of oiling and
penetration into the river bottom (ECRC, 2013).
Figure 5.5 – Sediment Poling (photo credit Enbridge)
Poling was conducted by crews in small boats (see Figure 5.6). This effort was very labour‐
intensive and time consuming, but was effective in refloating oil which collected in low‐current
areas (ECRC, 2013). While it is possible that this technique might be effective in some areas of
the Fraser River such as side channels, water depths and currents would likely reduce their
effectiveness.
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Figure 5.6 – Sediment Poling (photo credit Enbridge)
Numerous platforms were used to agitate sediments including “Flush Boats” (see Figure 5.7)
and Marsh Buggies (ECRC, 2013).
Figure 5.7 – Flush Boat Agitation (photo credit Enbridge)
Another technique used was aeration which was used to agitate sediments, separating the oil
from the sediments and allowing it to refloat (see Figure 5.8), where it would be contained in
conventional booms and recovered with sorbents and skimmers (ECRC, 2013). However, it
should be noted that this technique would only work in low‐current (less than 1 knot) regimes,
which are rare in the Fraser River.
EmergWest Consulting Trans Mountain Expansion Project
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Figure 5.8 – Aeration (photo credit Enbridge)
A number of other technologies exist for recovery of heavy, sunken oil which has accumulated
on the bottom. Two companies have been developing specialized, sunken‐oil recovery
equipment, one expanding upon its knowledge in spill response, the other expanding upon its
dredging operations (Rymell, 2009).
The most common methods for recovering sunken oil include:
Diver‐Directed Pumping
ROV and Mini Submarine Pump Systems
Dredges
Recovery of sunken oil requires multiple systems for recovery, separation of oil/ water/
sediment, and treatment of these waste streams (Michel, 2008).
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5.2.2.1DiversandDiver‐DirectedEquipment
Divers have been used at a number of incidents, both directly for solid oils and in conjunction
with pumps or dredges as they have a number of advantages over other systems in terms of
detecting and recovering oil. With divers, sediment and water collected with the oil is lower,
reducing post‐recovery treatment. They are also able to detect small scattered pieces of oil,
and place them directly into storage containers. Water depth and dive duration limit these
operations as well as the need to regularly decontaminate divers and their equipment (Rymell,
2009).
In a number of incidents including the Bouchard 155, Volgoneft 248, Morris J Berman, Erika and
the spill during the Lebanon war of 2006, divers were employed to use manual recovery
techniques (Rymell, 2009).
Divers are more commonly used to direct vacuum, air lift or negative pressure equipment
(Rymell, 2009). Divers weigh themselves down and crawl along the bottom to vacuum up the
oil. Since size and length of hose can becoming a limiting factor, systems that would allow a
diver to direct larger systems underwater such as power sleds, would greatly increase recovery
rates. Pump and vacuum systems have historically been a successful strategy for sunken oil.
Divers are often used to direct a modified suction head, with which they can manually open and
close the valve (Rymell, 2009).
An important part of this recovery process is the storage and decanting of the oil/water mixture
being recovered. During the DBL‐152 spill, a system including storage tanks, absorbent‐based
recovery components and a filtrations package was mounted on a recovery barge. It is noted
that the water decantation proved difficult due to wave action keeping the oil in a state of
agitation, slowing separation (Usher, 2006).
Divers can also direct equipment used for refloating sunken oil. Some sunken oils may refloat if
it can be separated from the sediment and given impetus to move. Airlifting uses a pipe to
release a steam of air close to the seabed. This air rises and moves towards the surface,
creating a suction pressure that acts as a vacuum to lift sediment and oil. Refloated oil is then
contained and recovered using conventional means. However, there may be limited time to
recover re‐floated oil as incorporated air may be a factor in its renewed buoyancy (Rymell,
2009).
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5.2.2.2ROVandMiniSubmarinePumpingsystems
With the dangers of diver‐operated devices, especially at greater depths, the use of remotely
operated vehicles (ROV’s) has been expanded for many different applications (Counterspil,
2011). These systems allow for sustained operations and operate for periods much longer then
a diver. Remotely‐operated lightering systems are an existing, proven technology for
recovering liquid products from sunken vessel tanks, and shows promise to be built upon
(Rymell, 2009).
Sea Horse (Seagoing Adaptable Heavy Oil Recovery System) is a conceptual design using ROV’s
currently being tested and developed by Alion (Hansen, 2012). The recovery system includes a
ROV power sled, a pump, the nozzle, and the hoses. Initial testing has shown the system to be
slightly underpowered and could only handle currents less than 1.5 knots (Hansen, 2012).
.
Figure 5.9 ‐ Alion Sea Horse (photo credit Hansen et al 2012)
Marine Pollution Control Inc. (MPC) has experience with sunken oil using both divers and diver‐
directed devices. They believe that mounting recovery equipment on a mini submarine would
be effective, and have designed and developed a program to test this concept (Rymell, 2009).
Initially this system only had visual detection capabilities but has since been equipped with an
oil‐discriminating sonar and fluorescence polarization (FP) sensor (Hansen, 2012).
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Figure 5.10 ‐ MPC and SEAmagine Hydrospace Corporation sub sea oil recovery system. Photo
from, RP595 Sunken and Submerged Oils, 2009.
MPC reports that their submersible recovery unit is able to locate, track and recover submerged
oil at depths up to 1600 feet. The 2‐person submarine is equipped with a suction nozzle that is
connected to a hydraulic submersible pump. While this might be useful in quiet areas where oil
has pooled, it is unlikely that this type of device would be practical in the currents of the Fraser
River.
5.2.2.3Dredging
With dredging operations being an established business among coastlines and port harbors,
they have been proposed for a number of incidents involving sunken oil (Rymell, 2009).
When oil is solidified, environmental clamshell dredgers have been used successfully (Rymell,
2009).
Modifications to a large duckbill dredge head have been made to try and reduce the amount of
waste water and sediment recovered (Rymell, 2009).
Dredgers were used during the Marshall spill (see Figure 5.11) in areas of highest oil
concentration, i.e., Ceresco Dam, Mill Ponds and Morrow Lake. Dredging was found to require
extensive treatment infrastructure and had the greatest impact on sediments (ECRC, 2013).
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Figure 5.11 ‐ Amphibex Dredging (photo credit Enbridge)
Dredgers are generally designed to remove large quantities of material rapidly, and they do not
have to be as accurate or careful of disturbance as other techniques. If not carefully controlled,
large amounts of sediment could be removed, resulting in the need for storage and treatment,
as it would be contaminated by the sunken oil. It is also difficult to remove less than 20‐25 cm
of seabed without newer or modified equipment (Rymell, 2009).
Most dredging systems are typically limited to a maximum water depth of 50 meters, although
some specialist systems exist for excavations at greater depths. The offshore oil industry has
also developed systems for excavating pipeline routes, as well as remove drill cuttings (Rymell,
2009).
Figure 5.12 – (photo credit HELCOM/ Hand et al 1978)
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Not all dredges are surface‐based. The Tornado Motion Technologies LLC (TMT) submerged oil
recovery system which is based off of the already‐existing, tracked dredge system. This consists
of a tracked unit on the seabed, with a mounted eddy pump and a moveable controllable
suction head. It is controlled from the surface via remote control, and guided by mounted
cameras on the tracked unit. The seabed unit is also equipped with a GPS tracker. It is
reported to create less turbulence then conventional systems and has a maximum working
depth in excess of 60 meters (Rymell, 2009).
Figure 5.13 – TMT Dredger (photo credit TMT)
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5.3 UnrealisticWindowofOn‐WaterRecovery
The TMEP submission includes numerous references to a 10‐day requirement to complete on‐
water recovery.
WCMRC (Review of Trans Mountain Expansion Project Future Oil Spill Response
Approach Plan Recommendations on Bases and Equipment November 2013) – Page 10 ‐
The results of these tests support the federal standard of continued use of a ten day
period for on water recovery operations. On‐water recovery operations for oil spills in
sheltered waters and unsheltered waters are to be completed within 10 operational days
after the day on which the equipment is first deployed in the affected operating
environments.
The Response Organization (RO) standards are planning standards, not performance standards.
By comparison, the Oil Handling Facilities (OHF) Standards are performance standards.
The RO Standards require the RO (in this case, WCMRC) to plan to deliver an equipment
capability (equipment standards) to recover a predetermined amount of oil based on a number
of tiers (150T, 1000T, 2500T, 10,000T) in a given geographic area in a set period of time (time
standards). In the case of oil on water, the RO must plan to recover free oil on water in 10 days.
The 10 days start once the RO has deployed the required equipment on scene.
The RO standards apply to the RO when responding on request from a ship or OHF (when a ship
is alongside and transferring) members. The RO Standards do not legally apply to spills from
any other member of the RO (such as TMEP). Specifically then, the 10‐day standard does not
apply to potential spills originating from the TMEP, unless those spills occur at the dock in
Burnaby, or from a visiting/transiting oil tanker.
The following is the final paragraph from the introduction to the RO Standards, a paragraph
that is often forgotten and/or misrepresented.
“The standards are intended to be used in the planning process in preparation for a
response to an oil spill incident. Each response plan will be unique, taking into account
the geographic features specific to that region. Since the response to an incident will be
influenced by environmental and other factors, the standards should not be used as a
yardstick against which to measure the appropriateness of the response. Rather, they
seek to ensure that a suitable response infrastructure is in place and ready to be
deployed in the event of any spill, regardless of size and conditions.”
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Although it is not explicitly stated, it is possible that this was the method chosen at which to
conclude the Gainford Study (see Section 8.5).
Unfortunately, when a spill occurs, especially in difficult response conditions, i.e., bad weather,
fast currents, open water, or in areas where a quick response is limited for any reason, the
spilled oil does not adhere to this 10‐day rule. Instead, history has shown that oil, when spilled
on water will quickly spread to a very thin layer, covering a very large area. As a result, the oil
typically can remain on the water for extended periods, or at least strand on a shoreline,
covering many hundreds of kms of shoreline, where it has a potential to remobilize on a rising
tide and refloat, or possibly submerge due to interaction with shoreline sediments.
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5.4 24‐HourOn‐WaterRecoveryOperations
The submission appears to rely on the recovery of oil on water on a 24‐hour basis.
WCMRC (Review of Trans Mountain Expansion Project Future Oil Spill Response
Approach Plan Recommendations on Bases and Equipment November 2013) – Page 23 ‐
The on‐water recovery plan is based on a 24‐hour per day operational period.
Responders will be trained and equipped to operate safely in night time conditions.
While it is possible that some, near‐shore recovery (of already‐contained oil) activities might be
possible, it is highly‐unlikely that any significant amount of free‐floating oil would be recovered.
In WCMRC’s extensive history, no significant recovery of free‐floating oil at night has ever been
realized.
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5.5 DifficultiesRespondinginBadWeather
The submission does recognize the limitations of spill response in bad weather conditions.
WCMRC (Review of Trans Mountain Expansion Project Future Oil Spill Response
Approach Plan Recommendations on Bases and Equipment November 2013) – Page 29 ‐
Although WCMRC equipment is capable of operating in sea states greater than 2, the
effectiveness of those countermeasures is reduced. For example, at Sea State 3 (Beaufort
Scale 4) wave heights exceed 1 m and the wind velocities range from 11 to 16 knots. At
this magnitude, containment booming and skimming is difficult to execute and become
less effective. Additionally, wave agitation may emulsify water and oil into a thick
mousse making oil recovery from the water surface more difficult. Emulsification may
also increase the volume of the spill since hydrocarbon‐water emulsions can incorporate
between 60% and 80% water by volume within two to three hours. It should be noted
that regulations only require response organizations and oil handling facilities to plan
response operations up to and including Beaufort Scale 4.
As noted, there exists (under the existing RO regime) a requirement for Response Organizations
to work in wind speeds of 16 knots or less. However, while the WCMRC report appears to
recognize this fact, the calculations throughout the remainder of the document, as well as the
various models tend to paint a much more‐positive outlook on a potential spill response.
Instead, the WCMRC submission suggests that its on‐water recovery strategy will be dictated by
increased equipment bases and purpose‐designed barges.
WCMRC (Review of Trans Mountain Expansion Project Future Oil Spill Response
Approach Plan Recommendations on Bases and Equipment November 2013) – Page 36 ‐
Two critical components will be: 1) base locations that improve response times; and 2)
purpose‐designed barges that enable efficient use of personnel and materials in support
of on‐water recovery.
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6 SpilledOilFates
The EBA Engineering Consultants Ltd. Study (Modelling the Fate and Behaviour of Marine Oil
Spills for the TMEP Summary Report) is limited in that a number of assumptions are made that
greatly reduce the impacts of potential spills and increases the expectations on on‐water
containment and recovery. Also, wind speeds were used that limited the likelihood that oil
would naturally disperse, thus potentially leading to sinking.
Figure 6.1 (Figure 6.17 of the EBA Study) (shown below) only depicts the spread of a slick after
48 hours (no slick spreading is shown after 48 hours).
Figure 6.1
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However, Figure 6.19 (of the EBA Study) indicates that oil would remain on the surface after 14
days.
Figure 6.2
In the WCMRC (Review of Trans Mountain Expansion Project Future Oil Spill Response
Approach Plan Recommendations on Bases and Equipment November 2013), the review
recognizes that there is a potential for some component of spilled dilbit to sink when spilled
into water:
Page 10 ‐ While the petroleum transported on the Trans Mountain pipeline is limited by
tariff to a maximum specific gravity of 0.94 and viscosity of 350 cSt7 and will float if
released into water, a portion of spilled petroleum could submerge or sink if left to
weather for an extended period.
Unfortunately, the Gainford Study (co‐undertaken by WCMRC) did not determine under which
conditions the sinking of oil was possible/likely.
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It is also noted that a study undertaken in 2012 by SL Ross (Meso‐scale Weathering of Cold Lake
Bitumen/Condensate Blend) is referenced by both the EBA Engineering “Methods for
Estimating Shoreline Oil Retention” prepared by Harper, and the EBA Study “Modelling The Fate
And Behaviour Of Marine Oil Spills For The Trans Mountain Expansion Project Summary
Report”, both contained in TMEP submission, “Vol 8C Part 12 ‐ Oil Spill Study”. In that study,
even though very low wind speeds (less than 5 knots) were used, a small part of the oil slick
(<1% to <5% by observation) was seen to submerge (see Figure 6.3) and hang in the water
column as either neutrally buoyant droplets or blobs while the water circulated in the flume (SL
Ross, 2012).
Figure 6.3 ‐ Droplets of Oil Observed Floating in the Water Column during Tests
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6.1 AdiosIIFatesModels
Since limited work was submitted by TMEP to try to predict the fate (and the potential for
submergence/sinking) of spilled crude oil, a series of fates models were produced and included
in this report. Specifically, hundreds of models were run in order to determine the key
combinations of factors which are discussed in Section 7.1.
The model chosen was the industry‐standard Adios II model developed by NOAA. The crude oils
modelled were:
Alberta Mixed Sweet
Cold Lake Blend
Transmountain Blend
Bow River Blend
For the most part, the key factors that will dictate the tendency of the modelled crude oils to
disperse and/or reach a density close to that of water were wind speed, sedimentation and
water temperature (densities increase as the water temperature decreases).
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6.1.1 ColdLakeBlend
Adios predicts that the key parameters for Alberta Mixed Sweet Crude are wind speeds of 20 mph and a
water temperature of 15°C. Under these conditions, it is predicted that within 36 hours, the oil would
reach a density (0.99) close to that of fresh water, and around 8% of the oil would disperse, and
potentially adhere to river sediments (and sink).
Figure 6.4 – Alberta Mixed Sweet Crude Model Inputs
Figure 6.5 ‐ Alberta Mixed Sweet ‐ Density
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Figure 6.6 ‐ Alberta Mixed Sweet Crude – Percent Oil Dispersed
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6.1.2 ColdLakeBlend
Adios predicts that the water temperature has little effect on the tendency of Cold Lake Blend to
disperse. Also, CLB showed almost no dispersion, even at wind speeds of 40 mph. However, under
these conditions, it is predicted that within 2 days, the oil would reach a density (0.99) close to that of
fresh water, thus making it a candidate for submergence.
Figure 6.7 – Cold Lake Blend Model Inputs
Figure 6.8 – Cold Lake Blend ‐ Density
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Figure 6.9 – Cold Lake Blend ‐ Percent Oil Dispersed
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6.1.3 TransmountainBlend
Adios predicts that the key parameters for Transmountain Blend are wind speeds of 18 mph and a water
temperature of 10°C. Under these conditions, it is predicted that within 2.5 days, the oil would reach a
density (0.99) close to that of fresh water, and around 9% of the oil would disperse, and potentially
adhere to river sediments (and sink).
Figure 6.10 – Transmountain Blend Model Inputs
Figure 6.11 ‐ Transmountain Blend ‐ Density
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Figure 6.12 ‐ Transmountain Blend – Percent Oil Dispersed
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6.1.4 BowRiverBlend
Adios predicts that the key parameters for Bow River Blend are wind speeds of 20 mph and a water
temperature of 10°C. Under these conditions, it is predicted that within 2 days, the oil would reach a
density (0.994) very close to that of fresh water, and around 9% of the oil would disperse, and
potentially adhere to river sediments (and sink).
Figure 6.13 – Bow River Blend Model Inputs
Figure 6.14 – Bow River Blend ‐ Density
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Figure 6.15 – Bow River Blend – Percent Oil Dispersed
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7 SpilledOilTrajectories
The overland and river spill trajectory models developed by RPS‐ASA using OilMap Land, and
included in “Simulations of Hypothetical Oil Spills from the Trans Mountain Expansion Project
Pipeline – P1 V6 Route” (see Figure 7.1) provide little detail of:
The time required for the spilled oil to reach populated areas or the Fraser River
The Slick thicknesses in key areas (necessary to accurately predict vapour
concentrations)
The spread of the spilled oil when it reaches open water (the Fraser River)
Instead, the purple polyline appears to paint a general path of center of the oil slick, which,
once it reaches the Fraser River, stays nicely in the centre of the channel, avoiding the
shorelines. Of course in reality, this would not represent the actual spread of the oil, its
potential areal coverage, and the likely shoreline impacts.
Figure 7.1 ‐ Example Output from OilMap Land
Since it would be useful to have some idea as to the length of time required for spilled oil to
reach key sensitivities in the two First Nations IRs, a series of overland models were developed
by the author to provide some insight into these questions (see Section 7.1).
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7.1 OverlandSpillTrajectoryModels
A series of overland trajectory models were developed by the author, as part of this report in
order to determine how long it might take for spilled crude oil to reach key receptors/locations
in the two Reserves.
7.2 ModelUsed
The model used to determine the projected paths (and timings) of spills was the US EPA’s
Planning Distance model from (40 CFR Ch. I, Pt. 112, App. C). The model is described below:
d = v × t × c
where
d: the distance downstream from a facility within which fish and wildlife and sensitive
environments could be injured or a public drinking water intake would be shut down in
the event of an oil discharge (in miles)
v: the velocity of the river/navigable water of concern (in ft/sec) as determined by Chezy‐
Manning’s equation (see below and Tables 1 and 2)
t: the time interval specified in Table 3 based upon the type of water body and location
(in hours)
c: constant conversion factor 0.68 sec mile/ hr ft (3600 sec/hr ÷ 5280 ft/mile)
Chezy‐Manning’s equation is used to determine velocity: v=1.5/n×r2⁄3×s1⁄2; where v =
the velocity of the river of concern (in ft/sec); n = Manning’s Roughness Coefficient from
Table 1 (see below)
r = the hydraulic radius; the hydraulic radius can be approximated for parabolic channels
by multiplying the average mid‐channel depth of the river (in feet) by 0.667
s = the average slope of the river (unit‐less)
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Stream Description Roughness Coefficient (n)
Minor Streams (Top Width <100 ft.)
Clean
Straight 0.03
Winding 0.04
Sluggish (Weedy, deep pools)
No Trees or Brush 0.06
Trees and/or Brush 0.10
Major Streams (Top Width >100 ft.)
Regular section: (No boulders/brush) 0.035
Irregular section: (Brush) 0.05
Table 7.1 ‐ Manning’s Roughness Coefficient for Natural Streams (Note: Coefficients are
presented for high flow rates at or near flood stage.)
7.2.1 ModelInputs
Model inputs included:
Spill volume (1,000 gallons)
Start elevations*
End elevations*
Segment lengths*
Stream type (from Table 1)
Water depth*
* Input data came from actual GPS readings, measured water depths, and Topo maps (for
verification).
Also, it should be noted there are numerous differences between the spill trajectories depicted
in the RPS‐ASA models and those presented in Section 7.3. The models that follow are based
on observed/actual drainage paths (at the time of the field visits conducted in February and
March, 2015).
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7.3.1 ModelResults–PetersReserve–ScenarioP‐1
The following model output depicts the times required for spilled crude oil to reach key
receptors and/or locations from a spill originating at location 1 (near east‐most creek east of
pond).
Figure 7.2 – Scenario P‐1 Results
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Figure 7.3 ‐ Time to Reach the Pond
Figure 7.4 – Time to Exit Pond
Planning Distance Calculation Worksheet
Segment # 3
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 99 ft 0 m Stream desctiption n
Elevation (end) 67 ft 0 m Minor Streams (top width <100 ft)
Segment Distance 692 ft 0.131061 miles Clean Straight 0.03
Slope (s ) 0.046243 ft/ft Winding 0.04
Stream Type (n) 0.1 Sluggish No trees or brush 0.06
Water depth (if open channel) 0.5 ft Trees and/or brush 0.1
Wetted radius (r ) 0.3335 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 1.540328 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) hours stance (d) 0.131061 miles
d= 0 miles t= 0.125127 hours
Planning Distance Calculation Worksheet
Segment # 4
Segment type Still Water
Volume (V) 1,000.00 gallons
A=105*V
3/4*C= 2,921,713.07 ft
2
C=0.1643
A=(pi)*r2
r=(A/3.14)1/2= 964.61 ft
0.18 miles
Wind speed (v) 5.00 mph
Hours (t) 0.40 hours
Distance= D=r+(v*0.03*t)= 0.24 miles
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Figure 7.5 – Time from the Pond to the Fraser River
Figure 7.6 – Time to Reach Mission Bridge
Planning Distance Calculation Worksheet
Segment # 3
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 67 ft 0 m Stream desctiption n
Elevation (end) 66 ft 0 m Minor Streams (top width <100 ft)
Segment Distance 2428.8 ft 0.46 miles Clean Straight 0.03
Slope (s ) 0.000412 ft/ft Winding 0.04
Stream Type (n) 0.1 Sluggish No trees or brush 0.06
Water depth (if open channel) 0.5 ft Trees and/or brush 0.1
Wetted radius (r ) 0.3335 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 0.145343 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) hours Distance (d) 0.46 miles
d= 0 miles t= 4.6542918 hours
Planning Distance Calculation Worksheet
Segment # 2
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 66 ft m Stream desctiption n
Elevation (end) 33 ft m Minor Streams (top width <100 ft)
Segment Distance 82021 ft 15.53428 miles Clean Straight 0.03
Slope (s ) 0.000402 ft/ft Winding 0.04
Stream Type (n) 0.035 Sluggish No trees or brush 0.06
Water depth (if open channel) 14.7 ft Trees and/or brush 0.1
Wetted radius (r ) 9.8049 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 3.914761 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) hours Distance (d) 15.53428 miles
d= 0 miles t= 5.835485 hours
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7.3.2 ModelResults–PetersReserve–ScenarioP‐2
The following model output depicts the times required for spilled crude oil to reach key
receptors and/or locations from a spill originating at location 2 (creek immediately south of the
pond).
Figure 7.7 – Scenario P‐2 Results
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Figure 7.8 – Time to Reach the Pond
Figure 7.9 – Time to Exit the Pond
Planning Distance Calculation Worksheet
Segment # 3
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 99 ft 0 m Stream desctiption n
Elevation (end) 67 ft 0 m Minor Streams (top width <100 ft)
Segment Distance 207 ft 0.04 miles Clean Straight 0.03
Slope (s ) 0.154589 ft/ft Winding 0.04
Stream Type (n) 0.1 Sluggish No trees or brush 0.06
Water depth (if open channel) 0.5 ft Trees and/or brush 0.1
Wetted radius (r ) 0.3335 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 2.816314 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) hours stance (d) 0.04 miles
d= 0 miles t= 0.020887 hours
Planning Distance Calculation Worksheet
Segment # 4
Segment type Still Water
Volume (V) 1,000.00 gallons
A=105*V
3/4*C= 2,921,713.07 ft
2
C=0.1643
A=(pi)*r2
r=(A/3.14)1/2= 964.61 ft
0.18 miles
Wind speed (v) 5.00 mph
Hours (t) 0.40 hours
Distance= D=r+(v*0.03*t)= 0.24 miles
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Figure 7.10 – Time from the Pond to the Fraser
Figure 7.11 – Time to the Mission Bridge
Planning Distance Calculation Worksheet
Segment # 3
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 67 ft 0 m Stream desctiption n
Elevation (end) 66 ft 0 m Minor Streams (top width <100 ft)
Segment Distance 2428.8 ft 0.46 miles Clean Straight 0.03
Slope (s ) 0.000412 ft/ft Winding 0.04
Stream Type (n) 0.1 Sluggish No trees or brush 0.06
Water depth (if open channel) 0.5 ft Trees and/or brush 0.1
Wetted radius (r ) 0.3335 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 0.145343 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) hours Distance (d) 0.46 miles
d= 0 miles t= 4.6542918 hours
Planning Distance Calculation Worksheet
Segment # 2
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 66 ft m Stream desctiption n
Elevation (end) 33 ft m Minor Streams (top width <100 ft)
Segment Distance 82021 ft 15.53428 miles Clean Straight 0.03
Slope (s ) 0.000402 ft/ft Winding 0.04
Stream Type (n) 0.035 Sluggish No trees or brush 0.06
Water depth (if open channel) 14.7 ft Trees and/or brush 0.1
Wetted radius (r ) 9.8049 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 3.914761 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) hours Distance (d) 37.304 miles
d= 0 miles t= 14.013326 hours
EmergWest Consulting Trans Mountain Expansion Project
Draft Report 55 March 2015
7.3.3 ModelResults–PetersReserve–ScenarioP‐3
The following model output depicts the times required for spilled crude oil to reach key
receptors and/or locations from a spill originating at location 3 (un‐named creek above the
Hwy).
Figure 7.12 – Scenario P‐3 Results
EmergWest Consulting Trans Mountain Expansion Project
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Figure 7.13 – Time to the Fraser River
Figure 7.14 – Time to the Mission Bridge
Planning Distance Calculation Worksheet
Segment # 3
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 141 ft 42.9768 m Stream desctiption n
Elevation (end) 66 ft 20.11 m Minor Streams (top width <100 ft)
Segment Distance 2376 ft 0.45 miles Clean Straight 0.03
Slope (s ) 0.031566 ft/ft Winding 0.04
Stream Type (n) 0.1 Sluggish No trees or brush 0.06
Water depth (if open channel) 0.5 ft Trees and/or brush 0.1
Wetted radius (r ) 0.3335 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 1.27262 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) hours Distance (d) 0.45 miles
d= 0 miles t= 0.520002 hours
Planning Distance Calculation Worksheet
Segment # 2
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 66 ft 691.4 m Stream desctiption n
Elevation (end) 33 ft 564.8 m Minor Streams (top width <100 ft)
Segment Distance 82021 ft 15.53428 miles Clean Straight 0.03
Slope (s ) 0.000402 ft/ft Winding 0.04
Stream Type (n) 0.035 Sluggish No trees or brush 0.06
Water depth (if open channel) 14.7 ft Trees and/or brush 0.1
Wetted radius (r ) 9.8049 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 3.914761 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) 24 hours Distance (d) 37.304 miles
d= 63.8889 miles t= 14.013326 hours
EmergWest Consulting Trans Mountain Expansion Project
Draft Report 57 March 2015
7.3.4 ModelResults–PetersReserve–ScenarioP‐4
The following model output depicts the times required for spilled crude oil to reach key
receptors and/or locations from a spill originating at location 4 (un‐named creek above the
Hwy).
Figure 7.15 – Scenario P‐4 Results
EmergWest Consulting Trans Mountain Expansion Project
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Figure 7.16 – Time to the Fraser River
Figure 7.16 – Time to the Mission Bridge
Planning Distance Calculation Worksheet
Segment # 3
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 99 ft 0 m Stream desctiption n
Elevation (end) 66 ft 0 m Minor Streams (top width <100 ft)
Segment Distance 1296 ft 0.19545 miles Clean Straight 0.03
Slope (s ) 0.025463 ft/ft Winding 0.04
Stream Type (n) 0.1 Sluggish No trees or brush 0.06
Water depth (if open channel) 0.5 ft Trees and/or brush 0.1
Wetted radius (r ) 0.3335 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 1.142999 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) hours Distance (d) 0.19545 miles
d= 0 miles t= 0.2514671 hours
Planning Distance Calculation Worksheet
Segment # 2
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 66 ft 691.4 m Stream desctiption n
Elevation (end) 33 ft 564.8 m Minor Streams (top width <100 ft)
Segment Distance 82021 ft 15.53428 miles Clean Straight 0.03
Slope (s ) 0.000402 ft/ft Winding 0.04
Stream Type (n) 0.035 Sluggish No trees or brush 0.06
Water depth (if open channel) 14.7 ft Trees and/or brush 0.1
Wetted radius (r ) 9.8049 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 3.914761 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) 24 hours Distance (d) 37.304 miles
d= 63.8889 miles t= 14.013326 hours
EmergWest Consulting Trans Mountain Expansion Project
Draft Report 59 March 2015
7.3.5 ModelResults–PetersReserve–ScenarioP‐5
The following model output depicts the times required for spilled crude oil to reach key
receptors and/or locations from a spill originating at location 5 (un‐named creek at the west
end of the IR).
Figure 7.17 – Scenario P‐5 Results
EmergWest Consulting Trans Mountain Expansion Project
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Figure 7.18 – Time to the Fraser River
Figure 7.19 – Time to the Mission Bridge
Planning Distance Calculation Worksheet
Segment # 3
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 109.9456 ft 33.52 m Stream desctiption n
Elevation (end) 66 ft 20 m Minor Streams (top width <100 ft)
Segment Distance 239.712 ft 0.0454 miles Clean Straight 0.03
Slope (s ) 0.183327 ft/ft Winding 0.04
Stream Type (n) 0.1 Sluggish No trees or brush 0.06
Water depth (if open channel) 0.5 ft Trees and/or brush 0.1
Wetted radius (r ) 0.3335 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 3.066931 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) hours Distance (d) 0.0454 miles
d= 0 miles t= 0.0217692 hours
Planning Distance Calculation Worksheet
Segment # 2
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 66 ft 691.4 m Stream desctiption n
Elevation (end) 33 ft 564.8 m Minor Streams (top width <100 ft)
Segment Distance 82021 ft 15.53428 miles Clean Straight 0.03
Slope (s ) 0.000402 ft/ft Winding 0.04
Stream Type (n) 0.035 Sluggish No trees or brush 0.06
Water depth (if open channel) 14.7 ft Trees and/or brush 0.1
Wetted radius (r ) 9.8049 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 3.914761 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) 24 hours Distance (d) 37.304 miles
d= 63.8889 miles t= 14.013326 hours
EmergWest Consulting Trans Mountain Expansion Project
Draft Report 61 March 2015
7.3.6 ModelResults–Shxw'owhámelReserve–ScenarioS‐1
The following model output depicts the times required for spilled crude oil to reach key
receptors and/or locations from a spill originating at location 5 (un‐named ditch at the
northeast end of the IR).
Figure 7.20 – Scenario S‐1 Results
EmergWest Consulting Trans Mountain Expansion Project
Draft Report 62 March 2015
Figure 7.21 – Time to Fraser River
Figure 7.22 – Fraser River Segment 1
Planning Distance Calculation Worksheet
Segment # 2
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 95 ft m Stream desctiption n
Elevation (end) 66 ft m Minor Streams (top width <100 ft)
Segment Distance 27076 ft miles Clean Straight 0.03
Slope (s ) 0.001071 ft/ft Winding 0.04
Stream Type (n) 0.035 Sluggish No trees or brush 0.06
Water depth (if open channel) 14.7 ft Trees and/or brush 0.1
Wetted radius (r ) 9.8049 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 6.387304 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) hours Distance (d) 5.13 miles
d= 0 miles t= 1.1811115 hours
EmergWest Consulting Trans Mountain Expansion Project
Draft Report 63 March 2015
Figure 7.23 – Fraser River Segment 2
Planning Distance Calculation Worksheet
Segment # 3
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 66 ft m Stream desctiption n
Elevation (end) 33 ft m Minor Streams (top width <100 ft)
Segment Distance 82021 ft miles Clean Straight 0.03
Slope (s ) 0.000402 ft/ft Winding 0.04
Stream Type (n) 0.035 Sluggish No trees or brush 0.06
Water depth (if open channel) 14.7 ft Trees and/or brush 0.1
Wetted radius (r ) 9.8049 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 3.914761 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) hours Distance (d) 37.304 miles
d= 0 miles t= 14.013326 hours
EmergWest Consulting Trans Mountain Expansion Project
Draft Report 64 March 2015
7.3.7 ModelResults–Shxw'owhámelReserve–ScenarioS‐2
The following model output depicts the times required for spilled crude oil to reach key
receptors and/or locations from a spill originating at location 5 (un‐named ditch at the east end
of the IR).
Figure 7.24 – Scenario S‐2 Results
EmergWest Consulting Trans Mountain Expansion Project
Draft Report 65 March 2015
Figure 7.25 – Time to Fraser River
Figure 7.26 – Fraser River Segment 1
Planning Distance Calculation Worksheet
Segment # 2
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 95 ft m Stream desctiption n
Elevation (end) 66 ft 0 m Minor Streams (top width <100 ft)
Segment Distance 27067 ft miles Clean Straight 0.03
Slope (s ) 0.001071 ft/ft Winding 0.04
Stream Type (n) 0.035 Sluggish No trees or brush 0.06
Water depth (if open channel) 14.7 ft Trees and/or brush 0.1
Wetted radius (r ) 9.8049 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 6.388365 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) hours Distance (d) 5.13 miles
d= 0 miles t= 1.1809152 hours
EmergWest Consulting Trans Mountain Expansion Project
Draft Report 66 March 2015
Figure 7.27 – Fraser River Segment 2
Planning Distance Calculation Worksheet
Segment # 3
Segment type Open Channel
Open Channel n values
Roughness
Coefficient
Elevation (start) 66 ft m Stream desctiption n
Elevation (end) 33 ft m Minor Streams (top width <100 ft)
Segment Distance 82021 ft miles Clean Straight 0.03
Slope (s ) 0.000402 ft/ft Winding 0.04
Stream Type (n) 0.035 Sluggish No trees or brush 0.06
Water depth (if open channel) 14.7 ft Trees and/or brush 0.1
Wetted radius (r ) 9.8049 ft Major Streams (top width >100 ft)
Regular Section (no boulders/brush) 0.035
Vx=1.49/n * r2/3 * s
1/2 = 3.914761 ft/sec Irregular Section (Brush) 0.05
d=v*t*c
c=0.68
Finding for Distance (d) Finding for Time(t)
Time (t) hours Distance (d) 37.304 miles
d= 0 miles t= 14.013326 hours
EmergWest Consulting Trans Mountain Expansion Project
Draft Report 67 March 2015
8 Submerged/SinkingOils
The TMEP materials include a discussion of the fate (sometimes called weathering) of spilled
crude oil. However, there is a limited discussion on the mechanisms of sinking and/or
submergence.
The following discussion includes:
Predicting the Submerging and Sinking of Oil
Oil Submergence or “Over‐Washing”
Oil Density
A case study of the Line 6b (Enbridge spill) in Marshall, MI
Finally, since there are numerous references throughout the TMEP submission(s) to the
“Gainford Study”, conducted in 2013 In Gainford, Alberta, there is a discussion of the Study and
its applicability to this project.
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8.1 PredictingtheSubmergingandSinkingofOil
As is the case for all oil spills, every incident of submerged oil is a unique set of conditions based
on the type of oil, the environment in which it’s spilled, and other physical processes (Michel,
2008). Sunken oil is spilled oil which has negative buoyancy and will sink to the sea/riverbed.
Submerged oil is spilled oil that has near‐neutral buoyancy and has been submerged below the
surface (Rymell, 2009). Several main processes have been identified which could cause oil to
sink or become submerged.
Where the oil has an inherent density greater than the water in which it’s spilled, the oil will
sink to the sea/riverbed. Should the oil then move to an area with higher water densities, it
may rise again (Rymell, 2009).
Where the oil has a density close to the water in which its spilled, wave action and currents can
cause it to become submerged for periods and even trapped in the water column. This
emulsification and weathering can also cause lighter oils to increase in density and become
closer to that of the water. SL Ross conducted tank tests to develop a model for when oil may
submerge. It was determined that the oil must be viscous enough to break into fragments
small enough to become over washed. There must also be sufficient wave energy to push these
fragments below the water’s surface (Rymell, 2009).
Where floating oil is spilled or enters into an area with high concentrations of suspended
sediment, it can mix with the sediment increasing its density causing it to sink or become
submerged. Experiments in 1987 for the Integration of Suspended Particulate Matter and Oil
Transportation Study by Payne et al provide a “rule of thumb” regarding suspended sediment
concentrations leading to sinking oil (Rymell, 2009).
When stranded oil on a beach remobilizes, it can pick up sediment causing it to sink close to the
shore. This process requires that the oil have a suitably‐high viscosity and a shoreline substrate
consisting of sand or other coarse material. A short time period is also necessary for the oil to
incorporate the sediment. A rule of thumb is proposed that if the oil has a viscosity greater
than 20,000 cP and on a sand or shingle beach, it will have a high probability of sinking upon
remobilization (Rymell, 2009).
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Figure 8.1 ‐ General approach to modeling oil sinking or submerging. Photo from, RP595 Sunken and Submerged
Oils, 2009.
In the riverine waters near the Shxw'owhámel and Peters Reserves, the density and subsequent
movement of viscous oils will be affected by multiple factors, including emulsification,
sedimentation, tidal and other currents, waves generated by wind, low temperatures and
salinity anomalies. It is therefore likely that some percentage (10‐20%) of the bitumen‐blends
could sink within 10 days, or could be over washed easily by wave action in the turbulent
waters (Counterspil, 2011).
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8.2 OilSubmergenceor“Over‐Washing”
Large masses of oil that have a density close to that of water may be submerged for periods
from surface turbulence. This phenomenon is called over‐washing. Investigation has
discovered that oil will become over‐washed with densities as low as 0.90 g/ml, and over
washing time increases with oil density and wave size (Rymell, 2009).
Lab testing has shown that high‐viscosity, high‐density oils do not spread as a coherent slick but
rather formed “rafts” or “blobs” under the effect of waves. These blobs can be pushed rather
deep into the water and take a long time to resurface. Studies also revealed that in moderate
sea states, emulsified oil could be almost permanently covered in a layer of water (Rymell,
2009).
In a more recent analysis, it was found that the buoyancy behaviour of dilbits in marine
conditions depends most‐strongly on the presence of medium‐to‐fine sediment in the water
column. Evaporative weathering alone and evaporative and photo‐oxidation weathering in
combination all resulted in products that were buoyant in marine conditions. Mixing with
water generally increased the density of the products, but all oils tested remained buoyant in
seawater even when saturated with water. When mixed with fine‐ and moderate‐sized
sediments however, the fresh‐ to moderately‐weathered dilbits sank in saltwater…..this work
demonstrates that, in waters where fine‐ to moderate‐sized sediment is present, these oils are
at risk to sink, when there is a high degree of mixing energy available (Environment Canada,
2014).
During many parts of the year, the Fraser River delta has been found to have sediment
concentrations approaching 1 g/L during the highest annual flows (Kostaschuk et al., 1993),
thus creating an environment in which, when combined with sufficient mixing energy
(turbulence), could certainly sink.
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8.3 OilDensity
If the density of oil is greater than the water in which it’s spilled, it will sink. The American
petroleum institute’s “API gravity” is the standard measure of “heaviness” or density of oils
when compared to water.
When coupled with viscosity, it creates four categories for crude oil (Rymell, 2009).
1. Light Oil: is also known as “conventional oil”, with an API gravity of at least 22° and a
viscosity less than 100 cP.
2. Heavy Oil: described as above, the upper API gravity limit being set at 22° and a viscosity
of less than 100 cP.
3. Extra‐Heavy Oil: like Heavy Oil but with an API gravity of less than 10°.
4. Natural Bitumen: also known as “oil sands”, is like Heavy Oil but even more dense and
viscous with a viscosity greater than say 10,000 cP.
Freshwater has a density of 1.000 g/ml, and seawater typically has a density of 1.025 g/ml. The
salinity and density of water are proportional (Rymell, 2009).
*Density vs. Sinking behavior of oil, from RP595 Sunken and Submerged Oils, 2009.
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Few oils have densities greater than full‐salinity seawater. These are highly‐cracked oils are
also known as slurry oils or black carbon. Depending on the speed of current, the sinking oil
may be sheared into small droplets and spread over a vast area, or pool in depressions in the
seabed (Rymell, 2009).
If the density of the oil is close to but less than the water into which it’s spilled, it will initially
float, but sit very low in the water. Low‐viscosity oils will be naturally dispersed by wave action,
but if the viscosity is high, the oil will be broken into blobs of spilled oil (Rymell, 2009).
EmergWest Consulting Trans Mountain Expansion Project
Draft Report 73 March 2015
8.4 CaseStudy–EnbridgeLine6bRelease,Marshall,MI
On July 26, 2010, 20,084 US Barrels (bbls) of crude oil released near Marshall, Michigan from
Enbridge’s Line 6b near Marshall, MI. The crude (reported by Enbridge) released was a
combination of (77.5%) Cold Lake a heavy dilbit, and (22.5%) MacKay River Heavy, a heavy
synbit (USEPA, May, 2013).
Of the 20,080 bbls (843,360 gallons) of crude released from the pipeline, it is estimated that
only 8,333 bbls (350,000 US gallons) reached Talmadge Creek, and eventually the Kalamazoo
River. The river was in a flood condition at time of release (USEPA, May, 2013).
It is unclear at which point it was realized that some percentage of the oil had submerged/sunk,
however it would soon become clear that a considerable amount of oil was on the bottom, in
the sediments of the creek and river.
It would eventually be determined by EPA officials that primary mechanisms of submergence
were (USEPA, May, 2013):
– volatilization of light ends
– Emulsification, and
– interactions and agglomeration onto sediment (dominant)
The EPA (USEPA, May, 2013) would later estimate that, as of July/August 2012 (2 years after the
spill, and much of the cleanup) that:
The total submerged Line 6B oil volume for the discharge site is estimated to have been 180,000 gallons ± 100,000 gallons when summed over all sampling strata.
In summary, the calculated estimate of submerged Line 6B oil quantified in sediment supports other assessment and monitoring results. These multiple lines of evidence indicate that submerged Line 6B oil is present and has migrated into depositional areas along the entire 38-mile-long reach of the Kalamazoo River affected by the July 2010 Line 6B oil discharge.
Since the spill occurred in July, in relatively warm temperatures, it can be conservatively
estimated that 10% (35,000 gallons) of the crude entering the creek would have evaporated,
thus only around 315,000 gallons remained, at least for a while, on the water surface.
Based on the EPA’s numbers, the range of percentages of the oil that entered the creek that
would ultimately sink or submerge would be from 25% (at the low end of the EPA’s estimate) to
89% (at the high end). Based on the EPA’s best estimate, some 57% of the oil that entered
Talmadge Creek would ultimately find its way to the sediments on the bottom.
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8.5 GainfordStudy
8.5.1 General
In June 2012, Trans Mountain Pipeline ULC (TMPL) asked O’Brien’s Response Management to
organize a study on diluted bitumen (dilbit) products to support their application for the TMEP.
The stated purpose of the study was to further the knowledge of dilbit in general and, more
specifically, to investigate the behavior of dilbit when spilled into a marine environment.
Unfortunately, the Gainford Study was extremely limited in scope, in that only two crude oils
were tested, and an environment was chosen in which it was highly unlikely that any of the oil
would sink. The tests were conducted only using a salt water environment. Also, oil
thicknesses and wind apparatus were used that were unlikely to create small oil droplet
formation. Also, no suspended sediments, clays, or plant matter were present, which would
have increased the likelihood of the oil sinking. Finally, the study was limited in time to stop at
a point in time when the oils might have sunk.
The Study was also not designed to test current capability of recovering sunken/submerged oil:
Page vii “Is the performance of the equipment currently stockpiled by North American oil
spill recovery organizations adequate to mechanically remove diluted bitumens off the
surface of the water?”
Unfortunately, as a result of these limitations, the results of the study cannot be reasonably
used to represent many of the conditions in which crude oil could be spilled. It is even more
unfortunate that the study designers, knowing that a considerable percentage of the crude oil
spilled in the Enbridge (Marshall) incident did sink, did not design the study to determine at
which point the key variables, i.e., water density, sediment load, and turbulence, would cause
these crude oils to sink.
EmergWest Consulting Trans Mountain Expansion Project
Draft Report 75 March 2015
8.5.2 StudyAppropriatenessasaPredictorforRiverineSpills
The Gainford Study was not designed to test fate of oil spilled into fresh (river) water, where it
is more likely to sink/submerge (due to the less‐dense fresh water, and the presence of
suspended sediments, clays, or plant matter):
Page vii “This team was tasked with designing and executing a controlled test to
evaluate the fate and behavior of dilbit discharged into a simulated marine environment
similar to that of Burrard Inlet (Vancouver, BC, Canada) where the Westridge Terminal is
located”
Although the Gainford Study refers to the freshwater lens (the layer of lighter fresh water that
floats above the salt water layer) from rivers and in high‐rain periods often found in the Burrard
Inlet, the Study did not allow for the potential effects that the lens might have on the buoyancy
of spilled oil:
Page 5 “Most of Burrard Inlet is characterized by an upper surface layer of brackish
water subject to runoff and river inputs, predominantly the Fraser River for the outer
harbor and the Indian, Seymour, and Capilano rivers for the inner harbor. The surface
water layer temperatures are dependent on local weather conditions and precipitation,
generally ranging from a mean near 7 ˚Celsius (˚C) in February to approximately 17 ˚C in
July. On average, salinities decrease from approximately 20‐25 ppt (parts per thousand)
at First Narrows to approximately 15 ppt near the south end of Indian Arm.”
Instead the study assumed a homogenous salt‐water mixture, with an average salinity:
Page 5 “On average, salinities decrease from approximately 20‐25 ppt (parts per
thousand) at First Narrows to approximately 15 ppt near the south end of Indian Arm.”
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8.5.3 StudyLength
Unfortunately, the tests were stopped at the point where submerging/sinking was possible:
Page 6 “The objectives of the applied research were multifaceted. One objective was to
better understand and characterize the changes in physical and chemical properties of
dilbit in an estuarine simulated condition over a 10‐day period.“
Hopefully, no one is suggesting that all of the oil from a large, uncontained spill would be
recovered within 10 days.
Also, while it is unknown when oil began to sink during the Enbridge (Marshall) spill, it took
approximately 2 weeks before it was determined that oil had sunk. It is unfortunate that the
tests, which were carried out after the Marshall spill (the Marshall spill was referenced in the
literature review) did not include a time‐frame taking advantage of the lessons learned from
Marshall.
Page 5 “Two documented spills of dilbit into an aquatic setting are the 2010 Marshall
Spill (Kalamazoo, MI) from the Enbridge Pipeline (NTSB 2012; see also Enbridge Line 6B
Response)”
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8.5.4 SalinityofTestWater
The tests used a single water salinity of 20 ppt, even though it is recognized that salinity in
many parts of the Burrard Inlet are lower:
Page 8 “The scientific study tanks were filled with water at a prepared salinity, using
SolarSalt, of 20 ppt.”
Page 6 “On average, salinities decrease from approximately 20‐25 ppt (parts per
thousand) at First Narrows to approximately 15 ppt near the south end of Indian Arm.”
Again, it is unfortunate that the tests did not include a range of salinities to determine at which
salinity/densities the oils did submerge/sink.
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Draft Report 78 March 2015
8.5.5 CrudeOilsTested
Only two crude oils were tested, thus representing only a small fraction of the range of crude
oils that would likely be transported. This is especially important given the fact that many
crude oils, when weathered, are likely to reach specific gravities close to, or over 1.0 (see
Section 6.1).
Page 6 “A Cold Lake Winter Blend (CLWB) dilbit was selected to provide a “standard”
dilbit, with the winter blend representing more diluent initially. The slightly higher
diluent is expected to result in higher hydrocarbon flux to atmosphere and to the water
column (dissolution of acutely toxic low molecular weight hydrocarbons). The summer
blend has fewer lighter end hydrocarbons and hence a slightly higher initial density than
CLWB. More research has been completed with CLB dilbit than other blends; thus, it was
expected that results from these tests would provide a basis for comparison with a
broader range of prior research.
Winter specification Access Western Blend (AWB) was the second oil tested for physical
and chemical properties under similar weathering scenarios as the tests on CLWB. AWB
is a dilbit from the Athabasca region south of Fort McMurray, Alberta.”
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8.5.6 StudyConditions
Unfortunately, the Gainford Study used conditions that did not adequately mimic real life
situations/conditions.
Page 8 ‐ The night of May 17 (after approximately 48 hours of weathering without
cover), these tanks were covered with a tent (Figure 3‐3) in preparation for forecasted
windy and rainy weather.
As it often rains and is windy in BC, it would have been useful to see if these, real‐life conditions
might have some impact on the tendency of oil to sink. At least one test did include the effects
of wind and rain (see Section 8.5.7), which resulted in the oil becoming neutrally buoyant much
more quickly.
Also, the oil thicknesses employed in the tests (over 1 cm) greatly reduced the potential for oil
to sink.
Page 13 ‐ Containment by the tank configuration limited what would be the natural
spreading of oil in an unconfined condition.
In open water conditions, oil will spread to a very thin layer (often microns thick). A thicker oil
layer (as was the case in the tests) will tend to greatly reduce the effects of wind in the creation
of wind‐induced waves. The areas with the thickest oil layer will attenuate (flatten) the waves
(see Figure 8.2), thus greatly reducing the creation of wave‐induced droplets (see Figure 8.3).
Figure 8.2 – Wave Attenuation (photo credit OSRL)
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Figure 8.3 – Wave‐Induced Droplets (photo credit Boston Globe)
The study used what were described as “static”, “Mild” and “Moderate” wave conditions (see
Figure 8.4). These agitation levels, combined with the unrealistically‐high oil thickness
contributed to the conditions in which oil sinking was unlikely.
Figure 8.4 – Agitation Levels Used on Gainford Study
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The apparatus used to create wind (and turbulence) appears to be from a single, relatively
discrete source (see Figure 8.5). While it is possible that the wind created by the device shown
would have created local waves in the immediate area in which the blown air sheared over the
oil, it also appears that much of the tank would have unaffected by the moving air.
Figure 8.5 – Wind Apparatus
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8.5.7 GainfordStudyFindings
The study findings showed that, in spite of the relatively favourable design parameters, that the
crude oils tested became essentially neutrally buoyant with 4‐5 days (see Figures 8.6 – 8.8).
Test S1 results showed AWB becoming essentially neutrally buoyant (under static condition,
i.e., no induced waves) within 144 hours, thus becoming a candidate for sinking or at least
submergence (and thus interaction with suspended sediments), especially under more‐realistic
conditions.
Figure 8.6 ‐ AWB in Tank S1 Weathered Under Static Conditions
Test S2 showed AWB becoming essentially neutrally buoyant (under mild agitation) within 96
hours, thus becoming a candidate for sinking or at least submergence (and thus interaction
with suspended sediments), especially under more‐realistic conditions.
Figure 8.7 ‐ AWB in Tank S2 Weathered Under “Mild” Conditions
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Test S4 showed CLB becoming essentially neutrally buoyant (under “moderate” agitation)
within 96 hours, thus becoming a candidate for sinking or at least submergence (and thus
interaction with suspended sediments), especially under more‐realistic conditions.
Figure 8.8 ‐ CLWB in Tank S9A Weathered Under “Moderate” Agitation Conditions
Test S4 showed CLWB becoming essentially neutrally buoyant (under “moderate” agitation)
within 72 hours, thus becoming a candidate for sinking or at least submergence (and thus
interaction with suspended sediments), especially under more‐realistic conditions.
Figure 8.9 ‐ CLWB in tank S4 (oil reservoir tank) – weathered under mild agitation conditions,
sun light, and local weather conditions (wind and rain)
The Study concludes that:
Page 63 ‐ Fresh dilbit oil is much like most medium to heavy crude oils and can be
recovered using a variety of skimmer systems, ranging from weirs to oleophilic units. As
dilbit weathers, the oil viscosity increases significantly but skimmers designed for more
viscous oils, including brush, belt, and mechanical systems, can continue to effectively
recover weathered oil (demonstrated in up to 10 days of weathering in tank tests).
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However, it must be remembered that the primary problem in recovering spilled oil is not
removing oil from the water’s surface, but instead the challenge in encountering the oil. In
real‐world spill conditions, spilled oil will spread very quickly, covering potentially enormous
areas very quickly, greatly exceeding any existing technologies’ ability to apprehend it. The
Gainford study proved that existing oil skimmers can recover oil spilled into a tank with areas
ranging from 1 to 19 m2.
One useful outcome of the Gainford Study found that the alternative countermeasures tested
all had extremely short effectiveness windows, essentially making all of them useless on a large,
wide‐scale release (i.e., in open water), where it would be next‐to‐impossible to execute within
the necessary window.
Page 2 “Three non‐mechanical countermeasures were investigated for their ability to
mitigate spilled CLB dilbit under specific conditions. In‐situ burning was found to be
effective on oil that had only weathered for 24 hours or less. Chemical dispersants were
marginally effective for up to a 6 hour weathering window.”
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10 Conclusions
Based on the previous discussions and model findings, there are a number of issues which
should remain of concern to both the Shxw'owhámel First Nation and Peters Band.
Due to the close proximity of the proposed pipeline to their Reserves, there is a risk that a spill
from the pipeline could directly affect the immediate health and safety of the Shxw'owhámel
First Nation and Peters Band. There could also be long‐term affects to both their traditional
territories and Reserves.
There remain a number of unanswered questions about how the communities would be
protected from potentially toxic or flammable vapours, and, how they would even know if the
vapours were present.
The question of the safe and timely evacuation of residents, and the problems associated with
emergency responders entering the affected areas also remain unanswered.
If there is a spill, there is essentially no chance that the spread of oil would be stopped before it
reached the Reserves. And, because crude oils can sink and/or submerge, there is a significant
likelihood that some percentage of the oil would make its way to the river bottom sediments.
If this occurs, history has shown that the techniques available to spill responders are extremely
limited, time‐consuming, and in many cases ineffective.
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10 References
Clark, B. J. Parsons, C. Yen, B. Ahier, J. Alexander, D. Mackay, 1987. A STUDY OF FACTORS
INFLUENCING OIL SUBMERGENCE, Report EE‐90 prepared for Conservation and Protection,
Environment Canada.
Counterspil Research Inc., November 2011, A Review of Countermeasures Technologies for
Viscous Oils that Submerge.
Eastern Canada Response Corporation (ECRC), May 2013. Subsurface Oil Spill Conference.
Entrix, 2010. Tank Barge DBL 152 Incident Response, Environmental Unit Report.
Environment Canada, 2014. Properties, Composition and Marine Spill Behaviour, Fate and
Transport of Two Diluted Bitumen Products from the Canadian Oil Sands.
Hansen, K.A., Guidroz, L., Hazel, B., and G.W.Johnsen, TESTING SUBMERGED OIL RECOVERY
SYSTEMS, Interspill 2012
Kostaschuk et al., 1993. Suspended sediment concentration in a buoyant plume.
Michel, 2008. Spills of Nonfloating Oil: Evaluation of Response Technologies.
Rymell, M., BMT Cordah Limited, RP595 Sunken and Submerged Oils – Behaviour and Response,
prepared for Maritime and Coastguard Agency (UK), 27 February 2009.
SL Ross, October, 2012. Meso‐scale Weathering of Cold Lake Bitumen/Condensate Blend.
USEPA, May, 2013. U.S. EPA Volume Estimate for Submerged Line 6B Oil in the Kalamazoo
River.
Usher, D., Marine Pollution Control, Responding to Submerged Oils in Freshwater
Environments, slide presentation, Freshwater Spills Symposium, 2006.