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Article

Numerical Investigation of Sediment Flushing and Morphological Changes in Tamsui River Estuary through Monsoons and Typhoons

1
Disaster Prevention and Water Environment Research Center, National Yang Ming Chiao Tung University, Hsinchu 30010, Taiwan
2
National Center for Computational Hydroscience and Engineering, University of Mississippi, Oxford, MS 38677, USA
*
Author to whom correspondence should be addressed.
Current Address: U. S. Army Engineer Research and Development Center, Coastal and Hydraulics Laboratory, Vicksburg, MS 39180, USA.
Water 2022, 14(11), 1802; https://doi.org/10.3390/w14111802
Submission received: 13 April 2022 / Revised: 26 May 2022 / Accepted: 31 May 2022 / Published: 2 June 2022
(This article belongs to the Special Issue Hydrodynamics in Ocean Environment: Experiment and Simulation)

Abstract

:
The removal of reservoir silt and the restoration of existing reservoir capacities through land excavation and hydraulic sediment flushing have become necessary. Hydraulic sediment flushing discharge changes flow and sediment conditions of the downstream river channel. In the Tamsui River estuary in Taiwan, sediment flushing from the Shihmen reservoir upstream has potential impacts on the morphology of the navigation channels and the adjacent coasts. This study employed a validated coastal and estuarine processes model to investigate: (1) the influence of sediment flushing and tidal levels on morphological changes during flood and flushing-discharge operations of the reservoir, and (2) the differences in morphological changes on the estuary between monsoon and typhoon seasons. The prediction of the morphological changes was carried out by simulating hydrodynamic and morphodynamic processes under multi-year synthetic conditions combined by northeast monsoon and three historical typhoon events. The simulation results reveal that during the operation of sediment flushing when the peak discharge of river flood flow reaches the estuary section at ebb tides, more sediment can be transported to the open sea than that at flood tides. Additionally, the nature reserve area on the left bank of the estuary is eroded during monsoon and silted in typhoon seasons.

1. Introduction

Estuaries are ununiformed waters influenced by interactions between seawater and freshwater masses, which makes the ecological and hydrodynamic systems relatively complex. This complex ecosystem provides abundant fishery resources and promotes social and economic development; the complicated hydrodynamic system makes the estuary region rich in landforms [1,2,3]. However, influenced by tropical depressions and cyclones and natural hydrodynamic processes, landforms and coastlines of estuaries change dynamically, affecting the ecological environment, social economy, ship transportation, and flood defenses. Therefore, a proper understanding of the water movement behavior of estuaries will be beneficial for flood control and disaster reduction, coastal erosion protection, and the preservation of coastal structures [4,5,6].
An estuary’s flow field is mainly controlled by physical parameters, such as river runoff, waves, tidal current, estuary topography, and salinity. When river sediment is transported to an estuary, it is affected by the transport effects of tidal or coastal currents, and longshore drift is formed. If river sediment supply is greater than the sediment transport capacity of waves and tidal currents, then features such as deltas, sandspits, and other accumulative landforms can develop. If the sediment supply is less than the sediment transport capacity of waves and tidal currents, the beach line will retreat, forming an eroded coast [7,8]. The Tamsui River is the largest river in northern Taiwan, and its erosion-deposition balance is closely related to hydrology and sediment transport behaviors in the adjacent sea area. The lower river’s main sediment contributions come from longshore drift and sediment transport from upstream sources (Figure 1). However, since the completion of the Shihmen reservoir in 1964, the reservoir intercepted part of the sediment, and sand mining became prevalent in the river channel. Consequently, total sediment transport of the Tamsui River decreased, some reaches experienced downcutting of deep grooves, and the estuary and coast retreated. After completing Taipei Port in 1998, the longshore drift behavior between the estuary and the adjacent coast changed further, impacting the topography and landscape of the adjacent coast. The topography of the Tamsui River estuary to the North breakwater at Taipei port changed from erosion to siltation because the North breakwater blocked part of alongshore sediment transport [9]. Studies report that the total siltation of the Shihmen reservoir will reach 1.05 million m3 by 2020, accounting for 34% of the designed storage capacity of the reservoir [10]. To meet the demand for water resources in northern Taiwan and prolong the life of the reservoir, the Water Resources Agency of the Ministry of Economic Affairs put forward three strategies, including (1) construction of the Zhongzhuang Adjustment Pool of Dahan River to increase the amount of reserve water for 6.2 days, so that the reservoir’s sediment discharge time of the reservoir can be more concentrated and continuous; (2) construction of Amuping tunnel in the reservoir area for hydraulic scouring and silting and land transportation; (3) construction of the Dawanping Tunnel to remove the density current fine silt [11,12]. The Zhongzhuang adjustment pool was completed and put into use at the end of 2017, while the completion and use of the Amuping anti-silt tunnel are expected by the end of 2022, which will change the sediment supply of the Tamsui River and indirectly affect the balance of the supply and demand of silt between rivers and seas.
To effectively manage the sediment in the estuary area, the use of appropriate numerical tools is necessary to clarify changes in riverbed erosion and deposition in the estuary and adjacent coast. The models used to describe the dynamic changes in silt in coastal areas can be divided into sediment transport and morphodynamic models. Morphological models can be divided into process or behavior-based models. The first method is based on the sediment transport process, while the second method is based on geology, which describes the large-scale morphological system through simple parameters, and is continuously corrected by long-term observation data [13]. To simulate morphological changes in the Tamsui estuary, a process-based model is employed to drive sedimentation under the combined influence of longshore drift and downstream transport.
Longshore and cross-shore drift is a phenomenon of nearshore sediment movement caused by waves and currents. The high shear velocity of the boundary layer at the bottom of waves produces strong turbulence and shear stress that further affects the current and increases resistance at the bottom of the mixed flow, affecting the transport and spread of sediment [14]. Therefore, some scholars analyzed wave propagation under smooth and rough beds through experiments and numerical methods [15,16]. Moreover, the incident angle of waves and interactions between waves and currents also affect sediment movement behavior in offshore areas. Therefore, some researchers developed numerical models to explore sediment movement processes in river channels under the action of waves and currents, the influences of tides on sandpits, and the effect of beach nourishment by sediment sources in offshore areas [17,18,19].
To reproduce the morphological change behavior caused by river runoff, waves, tidal currents, and topography using a numerical model, a hydrodynamic model is usually taken as the core framework, and then wave, turbulence, and morphological change models are added. This can be called an integrated coastal model to simulate dynamic changes in coastal types, including shoreline changes, erosion, barrier breaching, and dam breaks [20,21,22,23]. Presently, common commercial models include Delft3D [24], ROMS [25], POLCOMS [26], the MIKE suite of models [27], TELEMAC [28], FVCOM [29], and CCHE2D-Coast [30].
Among them, CCHE2D-Coast is an integrated river/coastal/estuarine/ocean process modeling system [30]. It is applicable for simulating multi-scale hydrodynamic and morphodynamic processes of free-surface water flows, such as river flows, tidal currents, waves, and storm surges, induced by tropical cyclones, longshore and cross-shore sediment transport, and morphological changes. This model has been successfully applied to simulate processes in the Touchien [31,32] and Tamsui River estuaries [33]. The validated CCHE2D-Coast has been used for further simulations and predictions of the morphological changes and impact of reservoir sediment flushing in this study.
The rest of the paper is organized as follows: Section 2 provides a brief introduction of the integrated coastal and estuarine processes model, CCHE2D-Coast. Section 3 gives more information on the study area and the settings of relevant model parameters. Section 4 provides simulation results and discussions on the tidal levels and monsoon and typhoon seasons on the morphological changes in the estuary area. Finally, Section 5 concludes the paper and provides some preliminary suggestions on the management of flood and sediment in the estuary.

2. Brief Description of Integrated Coastal and Estuarine Model

CCHE2D-Coast is an integrated model that takes river, estuary, and coastal processes into account. It can be used to simulate hydrodynamic and morphological changes under hydrological conditions, such as waves, tides, storm surges, and river floods. Therefore, relevant units can make protection planning and engineering layout of estuaries and coasts according to numerical simulation results. The numerical model was developed by the National Center for Computational Hydroscience and Engineering at the University of Mississippi, USA, and has been verified by several studies [30,31,32,33,34]. CCHE2D-Coast consists of four main sub-modules, namely (1) the wave action model; which calculates the multi-directional and irregular deformation transformation process of waves from deep oceans to shallow water areas, (2) the tropical cyclone parametric wind model; which simulates the atmospheric pressure and wind field along the landing line of tropical cyclones and storms, (3) the flow (current) model; which simulates the hydrodynamic process, including astronomical tide, storm surge, waves, river runoff, coastal current, and Coriolis force, and (4) the morphodynamic model; which simulates the sediment transport rate and morphological changes in estuaries and coastal areas. The interconnections between the models are shown in Figure 2.
In the wave action model, the multi-directional wave spectrum transmission equation was adopted, which calculates the statistical characteristics of irregular waves, such as significant wave height, average period, and average wave direction. Based on the characteristics of the wave energy balance equation, various wave deformation states were further described, including refraction, diffraction, shallowing, and wave breaking. Additionally, the model can faithfully reflect effects, such as run-up, overtopping, and energy dissipation, when waves pass through permeable and impermeable structures.
The tropical cyclone parametric wind model adopts the tropical cyclone parametric cyclonic hurricane wind model proposed by Holland [35]. The model assumes that a typhoon is an ideal circular storm and estimates the atmospheric pressure and wind field along the line by setting parameters, such as atmospheric pressure, maximum wind speed, and maximum wind speed radius, at the center of the typhoon.
The current module is governed by the two-dimensional (2-D) depth, and shortwave˗averaged shallow water equations with wave forcing represented by the radiation stress to simulate currents, tides, storm surges, river inflows, the Coriolis force, and turbulence in coastal zones, tidal estuaries, and ocean waters. The wave model provides two options to calculate the wave radiation stresses for driving the flow module: one is the traditional wave stress formulations using the linear small-amplitude wave theory; another is the improved radiation stresses formulae derived from the non-sinusoidal wave assumption, which allows consideration for some dispersion effects of vertical-current structures (e.g., surface rollers or undertow currents) in the surf zone.
In the sediment transport submodel, empirical sediment transport models were used to calculate the sediment transport rates of bed materials and the suspended sediment under the conditions of combined waves and currents. For morphodynamic process modeling in an estuary with a strong impact from the river and coastal waves, such as the Tamsui River estuary, a unified sediment transport model was developed to estimate sediment fluxes from upstream rivers to estuaries and coasts to consider the sediment transport from the non-wave environment at a river to the wave-current coexisting area at an estuary and a wave-dominant coastal zone. Morphological changes are computed on the basis of the mass conservation of sediments, and the flows are simulated by iteratively updating the computed bed changes. Moreover, wetting and drying processes were modeled to simulate the inundation and retreat of tidal flows together with bed changes in an inter-tidal zone.

3. Study Area and Mode Setting

3.1. Study Area

The study area is the Tamsui River, which is the largest river in northern Taiwan, with a total length of 24 km. It is composed of main tributaries, such as the Dahan River, Xindian River, Keelung River, and Sanxia River, with a basin area of 2726 square kilometers (Figure 1). Prior to human interventions, the volume of sediment moving through the Tamsui River was sufficient to maintain and expand the footprint of estuarine deposits. Since the completion of the Shihmen reservoir in the upper reaches of the Dahan River in 1964, sediment was blocked in the upper reaches of the reservoir, and the Tamsui River estuary and Bali coast to its south gradually retreated. From 1977 to 1979, sand mining prevailed in the lower reaches of the Tamsui River. In 1986, the Feitsui Reservoir in the upper reaches of the Xindian River was completed, which led to the intensification of coastal retreat. Sand mining in 1989 was banned in the Tamsui River, and channel erosion changed to siltation, especially in the region between the Guandu Bridge and the Chongyang Bridge. The construction of Taipei port began in 1993, and the North breakwater at Taipei port blocked part of the north–south longshore sediment transport. Therefore, the topography of the Tamsui River estuary to the North breakwater Taipei port changed from erosion to siltation, but the region between the Taipei port and the Linkou Power Plant has changed from siltation to erosion. In recent years, the sediment release from the Shihmen reservoir has influenced the downstream morphological change of the Tamsui River estuary. To conclude, these data suggest that changes in the sediment transport capacity of the Tamsui River and the construction of large hydraulic structures have contributed to erosion and deposition of the coastal topography at the Tamsui River estuary [36,37].
The average daily discharge of the Tamsui River is 400–500 m3/s in the dry season, and 800 m3/s when it rains. The peak discharge at the Tamsui River estuary can reach more than 2000 m3/s under typhoon rainstorms, and the water flow also carries abundant sediment downstream at this time, which is one of the major sediment sources in the coastal waters of the Tamsui River. Moreover, the estuary to the Xinhai Bridge of the Dahan River (Figure 1) is a tidal reach, which belongs to a typical semi-diurnal tide. Water levels of this reach change with the tide levels in the open sea, and the water flow direction reciprocates that of the tide, which affects the sediment transport at the estuary. Therefore, the mechanism of sediment transport in the Tamsui River estuary is complicated, and processes, such as waves, river runoff, tides, construction of hydraulic structures, flood discharge, and sediment discharge operation of reservoirs during the flood season, affect the morphological changes in the Tamsui River estuary.
In this study, the jurisdiction of the 10th River Bureau of the Water Resources Agency of the Ministry of Economic Affairs was selected as the research area (Figure 3). The total length of the coastline is approximately 21 km from the northern boundary at the TN08 section to the southern boundary at the TS035 section, as measured by the Water Resources Agency. The whole coast is mostly sandstone mixed terrain, and there are many concave bays on the northern side of the Tamsui River estuary. When marine drift sediment accumulates in bays, pocket beaches, such as Qianshui Bay, Zhouzi Bay, and Shalun, are formed. From the southern part of the Tamsui River estuary to the North breakwater of Taipei port, the Bali sections of the coast on the northern side of the port are currently silting because of the influences of floating sediments blocked by hydraulic structures. Meanwhile, from the south of Taipei port to the TS035 section, the floating sediment in the ocean is blocked, leading to erosion of the coastal topography.

3.2. Mode Parameter Setting

To further clarify the influences of flood and sediment discharges from the Shihmen Reservoir on the morphological changes in the Tamsui River estuary, this study used CCHE2D-Coast as a numerical simulation tool to explore the hydrodynamic force, bed erosion, and deposition change process of the coast and estuary. In the numerical elevation part, the measurement data of Harbor and Marine Technology Center, Institute of Transportation, Ministry of Transportation and Communications was adopted, and the river ranges between the Guandu Bridge and the estuary. The sea area ranges from the northern boundary at the large section (with measurement number of TN08 of the Tenth River Management Office) to the southern boundary at the TS035 section and extends outward to a water-depth elevation of −20 m (approximately 3–5 km outside the estuary). To further improve the model’s accuracy, this study extended the northern boundary of the sea area to the Linshanbi (the topographic data measured by the Tenth River Management Office) and generated non-orthogonal grids with CCHE-GUI. The total grid numbers were 156,349 points (289 × 541), the grid resolution at the estuary and river channel was approximately 20 m, and the grid resolution on the open sea was approximately 500 m to improve the calculation efficiency of the model.
In the coastal boundary of CCHE2D-Coast, the spectral energy density was set according to the observation pile data outside Taipei port. Regarding wave direction, the study divided −180–180 degrees into 37 sections, and each section provided 10 degrees of directivity; the spectrum of 0.02–2 Hz was divided into 21 sections; the wind field part was reproduced using observation pile data outside Taipei port; and the eddy viscosity required by the flow field module was calculated using the average depth parabolic eddy viscosity model. Tide level data required for the east and west sides were the ones monitored for a long time at the Linshanbi and Zhuwei Fishing Port by the Central Weather Bureau, respectively. River discharge and sediment flux were obtained by simulating the hydrograph of flow and sediment flux at Guandu Bridge with the verified one-dimensional mobile-bed model (CCHE1D). The upstream boundary of CCHE1D adopted the hydrograph of measured discharge and sediment concentration of the Shihmen Reservoir; the downstream boundary adopted the measured tidal level of the Tamsui River estuary.
Additionally, the median particle size of d50 = 0.2 mm was set, and sediment transport was calculated by the total load. Manning’s roughness on the open sea was set at 0.02, and that of the river area was set at 0.025 [9,37]. The model topographic data were measured in May 2013.

4. Situation Case Simulation Results and Discussion

In this study, the CCHE2D-Coast model is applied to investigate the influence of tides and waves on morphological changes in the Tamsui River estuary during flood and flushing-discharge operations of the reservoir. Numerical simulations of flows and sediment transport were performed to quantify the differences in morphological changes between monsoon and typhoon seasons. This model has been validated by comparing the simulated tidal levels and significant wave heights with those measured in the Tamsui River estuary during periods of the Fung-Wong, Sinlaku, and Jangmi typhoons in 2008. For a detailed discussion of the validation of the CCHE2D-Coast model and the related analysis of statistical errors, the readers can refer to our previous work [33].
Furthermore, in order to better predict the morphological changes, this study refined the empirical coefficient of the Watanabe sediment transport model in CCHE2D-Coast [38]. The coefficient BW, a non-dimensional coefficient of the wave-induced sediment transport rate formula by Watanabe (1986), is an empirical scaling parameter of sediment transport flux, which needs to be calibrated at the study site. Figure 4a presents the measured topographic changes in the study area from May to November 2008; moreover, Figure 4b,c show that the simulation results of BW was 2 and 3, respectively. It suggests that the numerical simulation results are similar to the measured topographic changes. There were significant siltation occurrences in the main deep channel between the Guandu Bridge and the estuary, as well as the isobaths from the estuary to −10 m, and the same scouring phenomenon also occurred at the center of the river. Figure 4d depicts the longitudinal profiles of bed elevations along the transect through the middle of the river, from the Guandu Bridge to 1500 m of the outer sea of the estuary (dotted line A–A’ in Figure 4a). It confirms that the simulation results with BW = 2 are closer to the measured topographic changes, so the situation simulation with BW = 2 will be carried out later. Additionally, the measured topography outside the North breakwater was eroded, and the simulation result was silting, possibly caused by artificial dredging. The right bank of the river mouth showed significant erosion in the simulation result, which was mainly due to coastal currents caused by tides and waves. However, due to the lack of relevant measured data, this study still assumed that the coast at this point was erosive. To conclude, CCHE2D-Coast can reproduce the morphological change behaviors at the Tamsui River estuary.

4.1. Influences of Downstream Tidal Level on Scouring and Silting of Estuary Bed

The rivers in Taiwan have the characteristics of short flow paths, steep slopes, high flow rates, and large differences in flow rates of wet and dry seasons. During a typhoon flood period, the mountain flank is washed by heavy rain, and the river bed is washed by high speed flow. The sediment supply capacity of the river increases sharply, and the estuary area is influenced by the interactions of ocean forces and high river flow. Consequently, the topography of the estuary and its adjacent coast change substantially in a short time. During a non-typhoon flood period, the river flow and sediment supply decrease considerably, and the sediment transport behavior derived from waves and tides induces the morphological changes in the estuary and adjacent coast. However, the tidal reach of the Tamsui River basin is very long, reaching as far as the Xinhai Bridge of the Dahan River (Figure 1), and the downstream tidal level state during the typhoon flood period is bound to affect changes, such as bed erosion and deposition in the estuary. Therefore, this study takes Typhoon Aere of 2004 as a situational case and discusses the influences of the peak and trough of tidal levels on changes to bed erosion and deposition when the peak discharge reaches the estuary [12].
Typhoon Aere of 2004 is the largest recorded typhoon flood event in the study area; it hit the study area at 2:00 on 23 August 2004. To maintain the safety of the Shihmen Reservoir, the management unit carried out flood and sediment discharge operations. At 5:00 on 25 August 2004, the maximum flood discharge of the Shihmen Reservoir was 8366 m3/s, which was the flow between 50 and 100-year return periods. Notice the 50 and 100-year return flows at cross-section No. T075 were 7800 and 8400 m3/s, respectively, and the cross-section No. T075 is located about 10.6 km downstream of the Shihmen Reservoir (Figure 1). The total flood and sediment discharges of Typhoon Aere were 890.23 million m3 and 7.01 million tons, respectively. Therefore, in this study, the scenario from 00:00 on 9 August 2004 to 00:00 on 23 August 2004 was considered here to serve as a starting scenario; the time steps of the flow field and wave field calculations were 30 and 7200 s, respectively. From 01:00 on 24 August to 00:00 on 27 August 2004, for the situational case (case 1), the time steps of the flow field and wave field calculations were 30 and 7200 s, respectively, and the time step of bottom bed calculation was 100 s. The model topographic data were measured in May 2013.
Figure 5 shows the time series of flow and sediment flux at the Guandu Bridge from 23 August to 29 August 2004, including tidal levels at Linshanbi and Zhuwei Fishing Port, which were used as boundary conditions at the river upstream and the tidal conditions on the two cross-shore boundaries. Influenced by flood and sediment discharges of the Shihmen Reservoir, the Guandu Bridge had a maximum flood discharge of 11,069 m3/s at 12:00 on 25 August, when the sediment flux could reach 144,656 kg/s. Moreover, the peak discharge reached the downstream estuary; the downstream tidal level was the low tide level exactly. The sediment was carried to the estuary by the upstream flood, which could reach a water depth of −25 m. Sediment fluxes at the estuary and river channel could reach 0.11 and 0.05 m3/s/m, respectively, as shown in Figure 6a St. 1 and St. 2. Figure 6b is the change chart of bed erosion and deposition after Typhoon Aere (case 1). The changes in river erosion and deposition were mostly influenced by the flood discharge of the Shihmen Reservoir and its flow path characteristics, and it was silted between the Guandu Bridge and 2500 downstream, with an average height of 2.6 m. The 2500–4000 m downstream of the Guandu Bridge (adjacent to the Tamsui mangrove reserve) was the main erosion section, and the river channel had been scoured down by an average of 1 m. From the Tamsui Ferryboat Wharf to 1500 m upstream and affected by the widening of the river width, the flow velocity gradually decreased, and the average aggradation height was approximately 1.0 m. The Tamsui Ferryboat Wharf was affected by the narrowing of the river and deep channels, and the average brushing depth in this area could reach −2.0 m. The average aggradation height was 1.3 m from the Tamsui River estuary to 2500 m out to sea.
To further clarify the influences of downstream tidal levels on bed scouring and silting, this study adjusted the time points of flood discharge and discharges of the Shihmen Reservoir. Consequently, when the peak discharge reached the downstream estuary, the downstream tidal level was just the high tide level (06:00 on 25 August), and it was defined as case 2 (Figure 7). Figure 8a shows the distribution map of sediment flux at the flood peak. Influenced by the downstream tidal level, sediment flux at the estuary (St. 1) decreased to 0.04 m3/s/m, while sediment flux at the river channel (St. 2) increased to 0.06 m3/s/m. However, silt can still be transported to a water depth of −25 m due to the heavy flood of the river. Figure 8b is the change chart of bed erosion and deposition after Typhoon Aere (case 2). It was confirmed that the area of sediment deposition slightly expanded from Tamsui Wharf to 1500 m upstream, and the average deposition height increased to 1.2 m. The sediment silting area was slightly reduced from the Tamsui River estuary to 2500 m out to sea, while the average aggradation height was reduced to 1.1 m. Figure 9 depicts the longitudinal profiles of accumulative bed changes and bed elevations along the transect through the middle of the river, from the Guandu Bridge to 2500 m out to sea from the estuary (dotted line A–A’ in Figure 6b). It is confirmed that the downstream tidal level had a great influence on the scouring and silting of the bottom bed at 700–1700, 2800–5400, and 7200–9600 m downstream of the Guandu Bridge, and there was no significant difference in other locations.

4.2. Influences of Typhoon Flood Period and Monsoon Season on Scouring and Silting of the Estuary Bed

An estuary is the intersection of river, coast, and ocean, and its flow field is mainly controlled by physical processes, such as river runoff, waves, tidal current, estuary topography, and salinity. When river sediment is transported to the estuary, it is affected by the transport effect of tidal or coastal currents, and longshore drift is formed. If the river sediment supply is greater than the sediment transport capacity of waves and tidal currents, it is easy to form morphological elements on the estuary, such as a riparian delta, sandspit, and accumulative coast. If the sediment supply is less than the sediment transport capacity of waves and tidal currents, the shorelines will retreat, forming an eroded coast.
Marine sediment drift and morphological changes at the Tamsui River estuary are affected by northeast monsoons in winter, southwest monsoons in summer, and 2–3 annual typhoon flood events.To further investigate the influences of long-term monsoon seasons and typhoon flood bed scouring and silting, this study used the long-term monitoring data for wave, wind, and tides to simulate. We assumed that a typical one-year morphological change on the Tamsui River estuary is composed of the three-month monsoon season and three typhoon flood events. Figure 10 shows the synthetic time series (hydrographs) of flow and sediment flux at the Guandu Bridge as a combination of monsoon and typhoons. Table 1 shows the start and end time of each event. The simulation time of the monsoon season was from 1 December 2009 to 28 February 2010. The typhoon flood events were Typhoon Aere in 2004, Typhoon Jangmi in 2008, and Typhoon Saola in 2012. The peak discharge of each typhoon event was 11,069, 7438 and 8407 m3/s, respectively. Moreover, we simulation was repeated four times to explore the change in behavior of bed erosion and deposition in the Tamsui River estuary area over four years. The calculation time step of flow field was 40 s, the calculation time steps of wave field in monsoon and typhoon seasons were 10,800 and 7200 s, respectively, and the calculation time step of the bottom bed was 100 s.
Figure 11a shows the simulation results of bed changes from the initial time (t = 0 h) to the end of the first year’s monsoon season (t = 2160 h), which are induced only by the monsoon of the first year. Because of the small runoff and weak sediment supply capacity of rivers during the monsoon season (Figure 10), the morphological changes at the estuary are dominated by nearshore drift sediments. Influenced by the northeast monsoon, the marine drift sediment will form a northeast-southwest belt of silt outside the second fishing port, and influenced by the tide; the silt will gradually move into the second fishing port. Moreover, when the current flows through the North breakwater of Taipei port, it will be blocked by the dike, and a backflow will be generated, which will carry the sediment at the Wazihwei spit mouth of the excavator to the left bank of the estuary. Figure 11b shows the simulation bed changes after the simulations went through the entire first-year hydrographs, as shown in Figure 10, including the first year’s monsoon season and three typhoon events. Influenced by flood and sediment discharges of the Shihmen Reservoir during Typhoons Aere, Jangmi, and Saola, large amounts of floods washed away the river sediment, and the 2500–4000 m downstream of the Guandu Bridge was a concave bank with fast velocity, which was the main erosion area. At 6000–7000 m, it was influenced by the morphology of the bottom bed and was also eroded. However, the Guandu Bridge to 2500 m downstream and the estuary to 2500 m out to sea (7500–10,000 m downstream of the Guandu Bridge) were the main silting areas. The sediment in the outer sea was affected by sea currents, and part of the sediment was carried by the coastal current and diffused to the Wazihwei sandy ground.
Figure 12a shows the simulation results of bed changes at the end of the second year’s monsoon season. It can be found that tides and coastal currents were still the main forces influencing the morphological changes in the estuary, and the sediment transport along the coast was southwest. However, the backflow at the estuary continuously carried the sediment at the Wazihwei spit to the left bank of the estuary. When the monsoon season and typhoon flood period in the second year were over, it was confirmed that the amount of sediment brought by the typhoon flood event was largely deposited in the estuary area, while the Wazihwei spit was recharged by the sediment from the river channel, with slight back siltation, but its overall change trend remains erosion (Figure 12b). Eventually, at the end of the fourth monsoon season (Figure 13a), the siltation height at the second fishing port of the Tamsui River possibly reached approximately 1.0 m. The silted sediments were all over the estuary area, and only places near the North breakwater and Wazihwei spit remained eroded. At the end of the fourth year’s monsoon and typhoons (Figure 13b), it was confirmed that the main erosion areas were the Wazihwei spit, the left bank of the outlet of the Tamsui River, and the outer side of the North breakwater. The siltation phenomenon began to appear at a corner of the North breakwater after the fourth year of monsoons.
Figure 14 depicts the longitudinal profiles of bed elevations along the transect through the middle of the river, from the Guandu Bridge to 2500 m out to sea from the estuary (dotted line A–A’ in Figure 11a). It was confirmed that the main influence range was located at 8500–9500 m downstream of the Guandu Bridge during the monsoon season, while the silted sediment in this area was disturbed by the river flood and moved out to sea (approximately 9500–10,000 m downstream of the Guandu Bridge). During the typhoon flood period, the river flood would erode the riverbed at 2500–7000 m downstream of the Guandu Bridge, among which there was a relatively substantial erosion occurrence at 2500–4500 m, and the range of sediment deposition was located at 2100 m and 7000–10,000 m downstream of the Guandu Bridge.

5. Conclusions and Suggestions

To investigate the influences of hydrodynamic forcing, such as tides, waves, and river discharge, on sediment flushing and morphological changes in the Tamsui River estuary, the study employed a validated CCHE2D-Coast model [33]. This model has been validated by simulating flow and sediment transport in the Tamsui River estuary during the periods of multiple typhoons, such as Fung-Wong, Sinlaku, and Jangmi in 2008. This site-specifically validated coastal and estuarine processes model can reproduce the complex flow fields and sediment migration behaviors of the Tamsui River estuary, such as the erosion and siltation processes of estuaries, rivers and shoals, and the overflow phenomenon along the coast.
Using this model, this study simulated the sediment transport and morphological changes in the estuary due to sediment flushing at the upstream reservoir. The synthetic hydrodynamic conditions for the simulations include historical events such as a three-month-long monsoon from December 2009 to February 2010 and three typhoons (Aere in 2004, Jangmi in 2008, and Saola in 2012). Meanwhile, Typhoon Aere (2004) represents the strongest storm event in the region.
Analyses of the simulation results reveal that when the peak discharge of the river flood flow reaches the estuary section at ebb tides; more sediment can be transported to the open sea than that at flood tides. The location of the maximum deposition height is predicted to be 9400 m downstream of the Guandu Bridge. However, when the peak discharge reaches the estuary section at high tidal levels, owing to flood tide currents against river flow, the amount of silt transported to the open sea will decrease. For this case, the maximum deposition height occurs at 8400 m downstream of the Guandu Bridge. The amount of siltation increases significantly at 7200–8500 and 4800–5300 m downstream of the Guandu Bridge. Additionally, owing to the influences of the northeast monsoon, there would be significant zonal siltation at the exit of the second fishing port of the Tamsui River (8500–9500 m downstream of the Guandu Bridge). At the beginning of the typhoon flood season, a large flood amount caused by heavy rain moves the silted sediment to the outer sea (approximately 9500–10,000 m downstream of the Guandu Bridge). The Wazihwei spit would be influenced by backflow during the monsoon season; the sediments are taken to the freshwater channel, the shoal gradually retreats, and it will be recharged by sediment from the channel during the typhoon flood season, with slight back siltation.
The Shihmen Reservoir in the upper reaches of the Tamsui River is affected by the reservoir sediment, and its storage capacity will be gradually decreasing. In recent years, relevant sediment discharge facilities have been completed, and the sediment supply of the Tamsui River will experience more changes in the future. Because the tidal level of the Tamsui River estuary belongs to the semi-diurnal tide, adjusting the operation timing of flood and sediment discharges of the Shihmen Reservoir can further reduce the amount of sediment deposition outside the river channel and the second fishing port of Tamsui, under the influence of flood control safety. In addition, as the Wazihwei spit is a nature reserve, it is also possible to continuously manage sediment using numerical models in the future to maintain the shoal area.
By using the site-specifically validated coastal model CCHE2D-Coast, this study quantifies the dynamic behavior of morphology in seasons of monsoon and typhoons in the Tamsui River estuary. The validated model and simulated results are conducive to managing the sediment transport and reservoir flushing driven by waves, tides and river runoffs and stabilizing the Tamsui River Estuary and the adjacent coasts.

Author Contributions

Conceptualization, T.-C.H. and Y.D.; methodology, T.-C.H. and Y.D.; software, T.-C.H., R.-K.J. and Y.D.; validation, T.-C.H., R.-K.J. and Y.D.; formal analysis, T.-C.H.; investigation, T.-C.H.; resources, T.-C.H. and K.-C.Y.; data curation, T.-C.H. and Y.D.; writing—original draft preparation, T.-C.H. and R.-K.J.; writing—review and editing, Y.D. and K.-C.Y.; visualization, T.-C.H.; supervision, K.-C.Y.; project administration, K.-C.Y. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Not applicable.

Acknowledgments

Parts of the contents in this study are derived from the outcomes of a commissioned project of the Tenth River Management Office of the Ministry of Economic Affairs. The authors are grateful to the Tenth River Management Office for providing relevant information for this study.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. (a) Taiwan and (b) geographical location map of the Tamsui River basin.
Figure 1. (a) Taiwan and (b) geographical location map of the Tamsui River basin.
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Figure 2. Flow chart of CCHE2D-Coast calculation.
Figure 2. Flow chart of CCHE2D-Coast calculation.
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Figure 3. Relative position diagram of the study area and related monitoring stations.
Figure 3. Relative position diagram of the study area and related monitoring stations.
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Figure 4. Comparison between measured and simulated bed changes in the Tamsui River estuary. (a) Measured bed changes from May to October 2008. (b) Simulation results with BW = 2. (c) Simulation results with BW = 3. (d) Longitudinal profiles of bed elevations along the transect through the middle of the river from the Guandu Bridge to 1500 m of the outer sea of the estuary (dotted line A–A’ in (a)).
Figure 4. Comparison between measured and simulated bed changes in the Tamsui River estuary. (a) Measured bed changes from May to October 2008. (b) Simulation results with BW = 2. (c) Simulation results with BW = 3. (d) Longitudinal profiles of bed elevations along the transect through the middle of the river from the Guandu Bridge to 1500 m of the outer sea of the estuary (dotted line A–A’ in (a)).
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Figure 5. Upstream conditions of river discharge and sediment fluxes at the Guandu Bridge (Case 1) and tidal levels on the two cross-shore boundaries (Linshanbi and Zhuwei Fishing Port stations).
Figure 5. Upstream conditions of river discharge and sediment fluxes at the Guandu Bridge (Case 1) and tidal levels on the two cross-shore boundaries (Linshanbi and Zhuwei Fishing Port stations).
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Figure 6. Sediment flux distribution and changes in bed scouring and deposition of Case 1 (DZ = bed change, the contour line is bed elevation. The unit is meters for both). (a) Distribution diagram of sediment flux at peak time. (b) Simulation results of bed scouring and deposition.
Figure 6. Sediment flux distribution and changes in bed scouring and deposition of Case 1 (DZ = bed change, the contour line is bed elevation. The unit is meters for both). (a) Distribution diagram of sediment flux at peak time. (b) Simulation results of bed scouring and deposition.
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Figure 7. Upstream conditions of river discharge and sediment fluxes at the Guandu Bridge (Case 2) and tidal levels on the two cross-shore boundaries (Linshanbi and Zhuwei Fishing Port stations).
Figure 7. Upstream conditions of river discharge and sediment fluxes at the Guandu Bridge (Case 2) and tidal levels on the two cross-shore boundaries (Linshanbi and Zhuwei Fishing Port stations).
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Figure 8. Sediment flux distribution and changes in bed scouring and deposition of Case 2 (DZ = bed change, the contour line is bed elevation. The unit is meters for both). (a) Distribution diagram of sediment flux at peak time. (b) Simulation results of bed scouring and deposition.
Figure 8. Sediment flux distribution and changes in bed scouring and deposition of Case 2 (DZ = bed change, the contour line is bed elevation. The unit is meters for both). (a) Distribution diagram of sediment flux at peak time. (b) Simulation results of bed scouring and deposition.
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Figure 9. Longitudinal profiles of accumulative bed changes and bed elevations along the transect through the middle of the river from the Guandu Bridge to 2500 m of the outer sea of the estuary (dotted line A–A’ in Figure 6b).
Figure 9. Longitudinal profiles of accumulative bed changes and bed elevations along the transect through the middle of the river from the Guandu Bridge to 2500 m of the outer sea of the estuary (dotted line A–A’ in Figure 6b).
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Figure 10. Time series of river discharge and sediment fluxes at the Guandu Bridge.
Figure 10. Time series of river discharge and sediment fluxes at the Guandu Bridge.
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Figure 11. Changes in topographical erosion and deposition in the Tamsui River estuary after the end of the first year’s monsoon and typhoon seasons (DZ = bed change, the contour line is bed elevation. The unit is meters for both). (a) At the end of monsoon season of the first year. (b) At the end of the first-year hydrographs.
Figure 11. Changes in topographical erosion and deposition in the Tamsui River estuary after the end of the first year’s monsoon and typhoon seasons (DZ = bed change, the contour line is bed elevation. The unit is meters for both). (a) At the end of monsoon season of the first year. (b) At the end of the first-year hydrographs.
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Figure 12. Changes in topographical erosion and deposition at the Tamsui River estuary after the end of monsoon and typhoon seasons in the second year (DZ = bed change, the contour line is bed elevation. The unit is meters for both). (a) At the end of monsoon season of the second year. (b) At the end of monsoon season and typhoon flood period of the second year.
Figure 12. Changes in topographical erosion and deposition at the Tamsui River estuary after the end of monsoon and typhoon seasons in the second year (DZ = bed change, the contour line is bed elevation. The unit is meters for both). (a) At the end of monsoon season of the second year. (b) At the end of monsoon season and typhoon flood period of the second year.
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Figure 13. Changes in topographical erosion and deposition in the Tamsui River estuary after the end of monsoon and typhoon seasons in the fourth year (DZ = bed change, the contour line is bed elevation. The unit is meters for both). (a) At the end of monsoon season of the fourth year. (b) At the end of monsoon season and typhoon flood period of the fourth year.
Figure 13. Changes in topographical erosion and deposition in the Tamsui River estuary after the end of monsoon and typhoon seasons in the fourth year (DZ = bed change, the contour line is bed elevation. The unit is meters for both). (a) At the end of monsoon season of the fourth year. (b) At the end of monsoon season and typhoon flood period of the fourth year.
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Figure 14. Profiles of bed elevations from the Guandu Bridge to 2500 m out to sea from the estuary (dotted line A–A’ in Figure 11a).
Figure 14. Profiles of bed elevations from the Guandu Bridge to 2500 m out to sea from the estuary (dotted line A–A’ in Figure 11a).
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Table 1. Interval from the beginning to the end of each event, and the peak discharge and sediment flux of each event.
Table 1. Interval from the beginning to the end of each event, and the peak discharge and sediment flux of each event.
Event NameStart TimeEnd TimeDaysDuration (Hour)
Monsoon season1 December 2009 0:0028 February 2010 23:00902160
Typhoon Aere24 August 2004 1:0027 August 2004 0:002.9671
Typhoon Jangmi28 September 2008 10:0030 September 2008 23:002.5461
Typhoon Saola30 July 2012 21:004 August 2012 13:004.67112
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Hsieh, T.-C.; Ding, Y.; Yeh, K.-C.; Jhong, R.-K. Numerical Investigation of Sediment Flushing and Morphological Changes in Tamsui River Estuary through Monsoons and Typhoons. Water 2022, 14, 1802. https://doi.org/10.3390/w14111802

AMA Style

Hsieh T-C, Ding Y, Yeh K-C, Jhong R-K. Numerical Investigation of Sediment Flushing and Morphological Changes in Tamsui River Estuary through Monsoons and Typhoons. Water. 2022; 14(11):1802. https://doi.org/10.3390/w14111802

Chicago/Turabian Style

Hsieh, Tung-Chou, Yan Ding, Keh-Chia Yeh, and Ren-Kai Jhong. 2022. "Numerical Investigation of Sediment Flushing and Morphological Changes in Tamsui River Estuary through Monsoons and Typhoons" Water 14, no. 11: 1802. https://doi.org/10.3390/w14111802

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