<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">EPE</journal-id><journal-title-group><journal-title>Energy and Power Engineering</journal-title></journal-title-group><issn pub-type="epub">1949-243X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/epe.2017.98027</article-id><article-id pub-id-type="publisher-id">EPE-78154</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Engineering</subject></subj-group></article-categories><title-group><article-title>
 
 
  Modeling the Effect of Thermal Diffusion Process from Nuclear Power Plants in Vietnam
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Tran</surname><given-names>H. Thai</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Doan</surname><given-names>Q. Tri</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>International Association of Lowland Technology, Saga City, Japan</addr-line></aff><aff id="aff1"><addr-line>National Hydrometeorological Service, Hanoi City, Vietnam</addr-line></aff><pub-date pub-type="epub"><day>04</day><month>08</month><year>2017</year></pub-date><volume>09</volume><issue>08</issue><fpage>403</fpage><lpage>418</lpage><history><date date-type="received"><day>June</day>	<month>1,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>August</month>	<year>1,</year>	</date><date date-type="accepted"><day>August</day>	<month>4,</month>	<year>2017</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In this study, we evaluate the ecological impact of effluent cooling water from the Ninh Thuan nuclear power plant II, using a two-dimensional hydraulic model to simulate thermal diffusion from the effluent outfall. Sites selected for this study were Ninh Thuan nuclear power plant and Vinh Hai seawater in four different scenarios. This paper utilized the relationship between surface water temperature and the water temperature at a depth of -15 m to calculate the water temperature at intake and outlet at a depth of -14 m. A combination between the results of interpolated and results of model showed that effluent cooling water from Ninh Thuan plant affected the largest incidence about 2450 m in the North, 880 m in the South and 960 m in the West. It can be considered as safe distance to not to affect the coral reefs ecosystem in the North and sea turtle conservation area in the South. This study was first in this region to have an integrated approach using two-dimensional model.
 
</p></abstract><kwd-group><kwd>Ninh Thuan Nuclear Power Plant</kwd><kwd> Effluent Cooling Water</kwd><kwd> Ecological System</kwd><kwd> MIKE 21</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The increasing global demand for energy has hitherto been met to an increasing extent by the use of fossil fuels and hydropower. Nuclear energy has been developed and used commercially for about two decades to meet a fraction of the electrical energy needs. Statistical data on energy consumption of the world in recent years showed that world consumption has increased by about 50% in less than ten years. Vietnam has considered establishing nuclear power generation since 1995, and firm surfaced proposals in 2006. In July 2014, the government issued a master plan specifying Ninhthuan- I &amp; II nuclear power plants with a total of capacity 1000 MW e-class reactors [<xref ref-type="bibr" rid="scirp.78154-ref1">1</xref>] . Thermal pollution is the change in the water temperatures of lakes, rivers, and oceans caused by made-man industries or practices. These temperature changes may adversely affect ecosystems by contributing to the decline of wildlife populations and habitat destruction. Any practice that affects the equilibrium of an aquatic environment may alter the temperature of that environment and subsequently cause thermal pollution. Thermal pollution is one parameter of the broader subject of water pollution. The adverse effects of thermal pollution are often conjoined with other forms of water pollution such as chemical contamination or biological contamination [<xref ref-type="bibr" rid="scirp.78154-ref2">2</xref>] . The cooling water discharge from nuclear power plants (NPPs) is among the greatest local sources of thermal pollution due to the high levels of energy produced per plant. In addition, nuclear power plants require 30% - 100% more cooling water than other types of plant with a comparable power output [<xref ref-type="bibr" rid="scirp.78154-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.78154-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.78154-ref5">5</xref>] . Regulation of thermal pollution has been more elusive than for other forms of water pollution, although straightforward mitigation measures are available, especially in the case of elevated temperature discharges. Some countries and even individual states and provinces require limits on discharges that lead to thermal pollution of receiving waters. This aspect of water pollution has proven to be more elusive than conventional chemical discharge [<xref ref-type="bibr" rid="scirp.78154-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.78154-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.78154-ref8">8</xref>] . Numerical models are simplified mathematical representations of physical systems and processes. A numerical model can be constructed as a one-, two-, or three-dimensional model in accordance with the dominant spatial directions of the physical processes [<xref ref-type="bibr" rid="scirp.78154-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.78154-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.78154-ref11">11</xref>] . There are several methodologies to study thermal plume behavior, ranging from physical models [<xref ref-type="bibr" rid="scirp.78154-ref12">12</xref>] , to in situ data analysis [<xref ref-type="bibr" rid="scirp.78154-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.78154-ref14">14</xref>] to the use of numerical models [<xref ref-type="bibr" rid="scirp.78154-ref15">15</xref>] . The objectives of this paper were as follows: 1) to simulate the transport of temperature process and thermal diffusion of effluent cooling water of Ninh Thuan nuclear power plant, 2) to impact assessment of effluent cooling water to environment and ecological ecosystem around areas.</p></sec><sec id="s2"><title>2. Methodology</title><sec id="s2_1"><title>2.1. Description of Study Site</title><p>The Ninh Thuan nuclear power is located in Vinh Hai commune, Ninh Hai district, Ninh Thuan province, far from the center of Ninh Thuan 10 km in the Southeast of Vietnam (<xref ref-type="fig" rid="fig1">Figure 1</xref>). Ninh Thuan plant fits into the buffer zone of Nui Chua National Park, marine protected areas and within a radius of 1 km inland boundary of the National Park [<xref ref-type="bibr" rid="scirp.78154-ref16">16</xref>] . Ninh Thuan plant is reported on Environmental Impact Assessment (EIA) of the project Ninh Thuan Nuclear Power plant.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> The study location area</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x2.png"/></fig></sec><sec id="s2_2"><title>2.2. Methods</title><p>MIKE 21 FM flow model (HD), a general 2D hydrodynamic modeling system for simulation of flows in estuaries, bays and coastal areas, and in oceans. The MIKE21 FM flow model (HD) solves vertically integrated equations of continuity and momentum in two horizontal dimensions. The discretization in solution domain is performed using a finite volume method. The spatial domain is discretized by subdivision of the continuum into non-overlapping cells [<xref ref-type="bibr" rid="scirp.78154-ref17">17</xref>] . The numerical model Mike 21 solves in two dimensions (in the horizontal plane) stationary/non-stationary flow of incompressible Reynolds averaged Navier-Stokes equations, subject to the assumption of Boussinesq and of a hydrostatic distribution of pressure.</p><p>The continuity equation is written as:</p><disp-formula id="scirp.78154-formula42"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-6201944x3.png"  xlink:type="simple"/></disp-formula><p>And the two horizontal momentum equations for the x and y component, respectively</p><disp-formula id="scirp.78154-formula43"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-6201944x4.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.78154-formula44"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-6201944x5.png"  xlink:type="simple"/></disp-formula><p>where: t: time,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-6201944x6.png" xlink:type="simple"/></inline-formula>: velocities in x, y, z directions,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-6201944x7.png" xlink:type="simple"/></inline-formula>: elevation above mean sea level,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-6201944x8.png" xlink:type="simple"/></inline-formula>: vertical transformed co-ordinate, d: water depth,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-6201944x9.png" xlink:type="simple"/></inline-formula>: density, g: acceleration due to gravity,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-6201944x10.png" xlink:type="simple"/></inline-formula>: Coriolis parameter,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-6201944x11.png" xlink:type="simple"/></inline-formula>: turbulent eddy viscosity, P<sub>A</sub>: atmospheric pressure, S: the magnitude of the flow due to the point source<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-6201944x12.png" xlink:type="simple"/></inline-formula>: speed.</p><disp-formula id="scirp.78154-formula45"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-6201944x13.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.78154-formula46"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-6201944x14.png"  xlink:type="simple"/></disp-formula><p>where A is a horizontal eddy viscosity; the state of surface and bottom boundary with u, v and w are calculated as follows:</p><p>At <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-6201944x15.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.78154-formula47"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-6201944x16.png"  xlink:type="simple"/></disp-formula><p>At <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-6201944x17.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.78154-formula48"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-6201944x18.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.78154-formula49"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-6201944x19.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-6201944x20.png" xlink:type="simple"/></inline-formula> are wind surface stress and bottom stress.</p><p>The transports of temperature follow the general transport diffusion equation as:</p><disp-formula id="scirp.78154-formula50"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-6201944x21.png"  xlink:type="simple"/></disp-formula><p>where: Q<sub>H</sub> is transport of temperature, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-6201944x22.png" xlink:type="simple"/></inline-formula>is a number of Prandtl/Schmidt.</p></sec></sec><sec id="s3"><title>3. Model Setup</title><sec id="s3_1"><title>3.1. Computation Mesh</title><p>The study scope of the factory has sized 5500 &#215; 10,000 m with coordinates: Longitude (1,283,324 - 1,290,889), Latitude (604,155 - 602,341) (<xref ref-type="fig" rid="fig2">Figure 2</xref>). The topography and bathymetry data used in the model were provided by survey project from May 23 to June 19, 2014 according to the coordinate system VN 2000 with scale 1:1000. In this paper we used unstructured grid, triangular grid to solve problem (<xref ref-type="fig" rid="fig3">Figure 3</xref>(a)). Due to thermal diffusion calculation at intake and outlet area should divide smaller computation grid in this area than the external area to save computation time. The maximum mesh area of the triangular</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> The cross-sectional structure of Ninh Thuan II nuclear power plant</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x23.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> (a) Computation grid-Triangular mesh; (b) Calculated boundaries (C1, TS1 and TS2 are the test positions)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x24.png"/></fig><p>grids is 2000 m<sup>2</sup>, the sea regional in front of intake effluent cooling water and outlet has sized of 2000 &#215; 3000 m. The maximum triangular grid of the offshore area can reach to 50,000 m<sup>2</sup>. The total number of mesh is 11,200 and the number of nodes is 5718 and 4 boundaries including one land boundary, three open boundaries in North, East and South (<xref ref-type="fig" rid="fig3">Figure 3</xref>(b)).</p></sec><sec id="s3_2"><title>3.2. Boundary Condition</title><p>Water level boundary is extracted from the calculation model Dynasty China Sea (Global Forecast System (GFS) of the US National Environment Forecast Center). Temperature boundary used the measure data of the project at the TE1, TE2, TE3, TE4, TE5, TE6 in the northern boundary; TE6, TE12, TE18, TE24, TE30 in the eastern boundary; TE25, TE25, TE27, TE28, TE29, TE30 in the southern boundary in the period from June 2014 to July 2015 (<xref ref-type="fig" rid="fig3">Figure 3</xref>(b)). The measured data will be interpolated along the boundary and the chain computation time. Salinity boundary was used from the survey results at a position distance of 1km to inland in 2014-2015. The salinity of study area ranged from 32% - 33% during rising tide phase. Average salinity has not changed much in years. Average salinity in the dry and rainy season is about 33 ppt. Hence the paper used constant values of salinity in the caculated time series for each season.</p></sec></sec><sec id="s4"><title>4. Results and Discussion</title><sec id="s4_1"><title>4.1. The Calibration</title><p>The calibration parameters of model are conducted primarily by changes to the hydraulic roughness and diffusion coefficient changes. This paper used measure data at C1 position on June 19-26, 2014 and on December 18-26, 2014 for the water level calibration, on December 18-26, 2014 for the temperature calibration at TS1 and TS2 positions in the model. The results of water level calibration in summer and winter are shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>(a) and <xref ref-type="fig" rid="fig4">Figure 4</xref>(b). The results of temperature calibration at TS1 and TS2 positions are shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>(c) and <xref ref-type="fig" rid="fig4">Figure 4</xref>(d). <xref ref-type="fig" rid="fig4">Figure 4</xref>(c) and <xref ref-type="fig" rid="fig4">Figure 4</xref>(d) showed that the variation tendency of calculated temperature was decreasing at TS1 position from 25.1 to 24.2 degree, at TS2 position from above 25 to 24.1 degree. The results of water level calibration in summer and winter showed a high conformity about phase and water level amplitude between calculated and observed data. By editing Nash-Sutclifee criterion [<xref ref-type="bibr" rid="scirp.78154-ref18">18</xref>] we have the results of water level and temperature calibration (<xref ref-type="fig" rid="fig4">Figure 4</xref>). It means that model was edited well with hydraulic parameters. These parameters are used as the basic for validation model and thermal diffusion process.</p></sec><sec id="s4_2"><title>4.2. The Validation</title><p>Validation model was used water level data at C1 position in summer from August 04-12, 2014 and in winter from December 03-11, 2014. Temperature validation was used observed temperature data at TS1 and TS2 positions from December 03-11, 2014. The results of water level validation at C1 position in summer and winter are shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>(a) and <xref ref-type="fig" rid="fig5">Figure 5</xref>(b). The results of temperature validation at TS1 and TS2 position are shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>(c) and</p><fig-group id="fig4"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> (a) The calculated and observed of water level calibration at C1 on June 19-26, 2014 with NASH = 0.82; (b) on December 18-26, 2014 with NASH = 0.85; (c) The calculated and observed of temperature calibration at TS1 position on December 18-26, 2014 with NASH = 0.76; (d) The calculated and observed of temperature calibration at TS2 position in winter on December 18-26, 2014 with NASH = 0.78.</title></caption><fig id ="fig4_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x26.png"/></fig><fig id ="fig4_2"><label>(c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x25.png"/></fig><fig id ="fig4_3"><label> (d)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x28.png"/></fig><fig id ="fig4_4"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x27.png"/></fig></fig-group><p><xref ref-type="fig" rid="fig5">Figure 5</xref>(d). The variation tendency of temperature validation at TS1 and TS2 positions showed that the simulated temperature involving a tendency was smaller than observed temperature with the maximum peak error about 0.25 degree. The results revealed that in the validation case, the water lever between calculated and observed have a high conformity about phase and water amplitude with Nash-Sutcliffe criterion (<xref ref-type="fig" rid="fig5">Figure 5</xref>). The temperature process simulations from calibration and validation model are not really coinciding with the measurement process. The results of calibration and validation showed that the observed line is quite undulating and the simulated line is quite smooth. However, there are quite similar about trajectories. According to analysis above, we can use the parameters in calibration and validation process to apply for the problem of calculating thermal diffusion from effluent cooling water of Ninhthuan-II nuclear power plant in Vinh Hai by using MIKE 21 FM model.</p></sec><sec id="s4_3"><title>4.3. Development of Scenarios</title><p>The scenarios were built based on climate characteristics, the computational requirements as follows:</p><fig-group id="fig5"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> (a) The calculated and observed of water level validation at C1 position in summer on August 4-12, 2014 with NASH = 0.84; (b) The calculated and observed of water level validation at C1 position in winter on December 3-11, 2014 with NASH = 0.79; (c) The calculated and observed of temperature validation at TS1 position in winter on December 3-11, 2014 with NASH = 0.72; (d) The calculated and observed of temperature validation at TS2 position in winter on December 3-11, 2014 with NASH = 0.75.</title></caption><fig id ="fig5_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x30.png"/></fig><fig id ="fig5_2"><label>(c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x29.png"/></fig><fig id ="fig5_3"><label> (d)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x32.png"/></fig><fig id ="fig5_4"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x31.png"/></fig></fig-group><p>Scenario 1, 2 (S1, S2): with the period time from 0 h 5/9/2014 to 0 h 19/09/ 2014; regime of rising tide; velocity of flow is 5.1 m/s; temperature is 28.8˚C; effluent cooling water temperature is 35.8˚C; wind speed is 4.8 m/s; wind direction is southwest.</p><p>Calculation results showed that the changes cycle of water temperature is about 25 hours in the summer. This paper used tidal cycle from 7:00 pm on 8/9/ 2014 to 8:00 pm on 9/9/2014 at falling tide to analyze the temperature’s change cycle and determine the greatest impact area.</p><p>Calculation results of thermal diffusion by the effluent cooling water at Ninhthuan-II nuclear power plant in scenarios S1, S2 showed that the areas affected by the effluent cooling water is very small; the region has a temperature greater than 1˚C ambient temperature about 0.114 km<sup>2</sup> with distance from the outlet to the south about 880 m and 290 m to the west in S1. Scenario S2 with dead tide has an affected area about 0.072 km<sup>2</sup> with the distance from the outlet to the North about 920 m and to the West about 160 m. Initially influenced by the flow, hot water flow moves in southward. When there are southwest winds, effluent cooling water gradually move to the Northeast, meet the flow, move closer to the shore and temperature is decreased. A hot flow does not affect to the intake gate of plant. The maximum temperature field in S1 at 15:00 pm on 8/9/ 2014 is shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>(a). The maximum temperature field in S2 at 15:00 pm on 9/9/2014 is shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>(b). Finally, effluent thermal flow in two scenarios S1, S2 do not affect effluent cooling water intake area of the plant.</p><p>Scenario 3, 4 (W1, W2): with the period time from 0 h 5/11/2014 to 0 h 21/11/2014; regime of rising tide; velocity of flow is 5.1 m/s; temperature is 27.1˚C; effluent cooling water temperature is 34.1˚C; wind speed is 6 m/s; wind direction is northeast.</p><p>Calculation results showed that the changes cycle of water temperature about 25 hours in the summer. This paper used tidal cycle from 23 h on 12/11/2014 to 0 h on 14/11/2014 at falling tide to analyze the temperature’s change cycle and determine the greatest impact area.</p><fig-group id="fig6"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> (a) The maximum temperature field in S1 scenario; (b) The maximum temperature field in S2 scenario.</title></caption><fig id ="fig6_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x33.png"/></fig><fig id ="fig6_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x34.png"/></fig></fig-group><p>Calculation results of thermal diffusion by the effluent cooling water at Ninhthuan-II nuclear power plant in scenarios W1, W2 showed that the area affected by the effluent cooling water is very small; the region area has a temperature greater than 1˚C ambient temperature about 1.54 km<sup>2</sup> with distance from the outlet to the north about 1950 m and 550 m to the west. Scenario W2 with dead tide has an affected area about 1.68 km<sup>2</sup> with the distance from the outlet to the North about 2450 m and to the West about 960 m. Initially influenced by the northeast wind, hot water flow moves in southward. After flow affected by the tide, it moves to Vinhhy bay again. The maximum temperature field in W1 at 2:00 am on 13/11/2014 showed in <xref ref-type="fig" rid="fig7">Figure 7</xref>(a). The maximum temperature field in W2 at 19:00 pm on 13/11/2014 showed in <xref ref-type="fig" rid="fig7">Figure 7</xref>(b). Finally, effluent thermal flow in two scenarios W1, W2 do not affect the intake effluent cooling water area of the plant.</p><fig-group id="fig7"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> (a) The maximum temperature field in W1 scenario; (b) The maximum temperature field in W2 scenario.</title></caption><fig id ="fig7_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x35.png"/></fig><fig id ="fig7_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x36.png"/></fig></fig-group></sec><sec id="s4_4"><title>4.4. Interpolated Calculated Results Follow Depth</title><p>There are not data measuring the depth of water temperature across the study site. This paper used correlation between surface water temperature and water temperature at a depth of −15 m at TS1 position to calculate the water temperature at a depth of −14 m in placement of intake and outlet of effluent cooling water. Based on the measured data on water temperature at TS1 position on 9/2014, 10/2014-1/2015 and 4-5/2015, we built the relationship between surface water temperature and water temperature at a depth of −15 m. This relationship lines will be used to interpolate the water temperature at the effluent cooling water outlet location in the above scenarios.</p><sec id="s4_4_1"><title>4.4.1. Application for S1 and S2 Scenario</title><p>The scenarios S1, S2 calculated for the period from on September 5-19, 2014. Therefore, we can use the relationship between surface water temperature and water temperature at a depth of −15 m measured on September 03, 2011 to interpolate the water temperature at intake and outlet effluent cooling water at a depth of −14 m for two scenarios S1 and S2 (<xref ref-type="fig" rid="fig8">Figure 8</xref>(a)). Mean square error is 0.743. It represents a good correlation so it can be used for the temperature interpolation process at two positions intake and outlet of effluent cooling water. The results of calculation in <xref ref-type="fig" rid="fig8">Figure 8</xref> showed that in the surface layer and a depth of −14 m in the summer thermal of Ninhthuan-II nuclear power plant only ranged from 24.8˚C to 27.5˚C at the intake and 23.8˚C - 26.8˚C at the outlet. It does not affect the taking effluent cooling water of plant.</p></sec><sec id="s4_4_2"><title>4.4.2. Application for W1 and W2 Scenario</title><p>The scenarios W1, W2 calculated for the period on November 5-21, 2014. Therefore, we can use the relationship between surface water temperature and water temperature at a depth of −15 m measured on October 9, 2014 to November 15, 2015 to interpolate the water temperature at intake and outlet effluent cooling water at a depth of −14 m for two scenarios W1 and W2 (<xref ref-type="fig" rid="fig8">Figure 8</xref>(b)). Mean square error is 0.983. It indicates a very good correlation so it can be used for the temperature interpolation process at two positions intake and outlet of effluent cooling water in above two scenarios W1, W2. The results of calculation showed that the surface layer and a depth layer of −14 m in the summer thermal of Ninhthuan-II nuclear power plant only ranged from 25.8˚C to 26.5˚C at the intake and 25.7˚C - 27.3˚C at the outlet. It does not affect the taking effluent cooling water of factory.</p></sec></sec><sec id="s4_5"><title>4.5. Impact Assessment of Effluent Cooling Water on Environmental and Ecological System</title><p>It is now generally acknowledged that coral reefs are among the most threatened global ecosystems, and among the most vital [<xref ref-type="bibr" rid="scirp.78154-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.78154-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.78154-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.78154-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.78154-ref23">23</xref>] . Reefs are of critical importance to human survival because they provide subsistence food for a substantial portion of the population, serve as the principle coastal protection</p><fig-group id="fig8"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> (a) Correlation between surface water temperature and water temperature at a depth layer of −15 m on September 2011; (b) Correlation between surface water temperature and water temperature at a depth layer of −15 m on November 2011 to January 2012.</title></caption><fig id ="fig8_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x37.png"/></fig><fig id ="fig8_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x38.png"/></fig></fig-group><p>structures for most tropical islands, and contribute major income and foreign exchange earnings from tourism [<xref ref-type="bibr" rid="scirp.78154-ref24">24</xref>] [<xref ref-type="bibr" rid="scirp.78154-ref25">25</xref>] . The field survey in this place the most notable is the coral reefs in Thai An about 200 ha wide area. Outside the region has a sand and coral (65% sand, 35% coral), inside region is the dead coral areas account for 60%, 40% living coral. Oviparity of turtle beaches concentrated in the northern of the plant from Mong Tay to Ngang beach and sea turtle conservation concentrated in the southern (<xref ref-type="fig" rid="fig9">Figure 9</xref>).</p><p>The condition of marine life depends on: water level and water level fluctuations, flow rate, water clarity, salinity, etc. In fact, biological living in the water affected by many environmental factors such as: light, temperature, pH, dissolved oxygen, CO<sub>2</sub>, etc. The environmental factors impact on the organism living referred to as the ecological factors. Each organism can only withstand the impact of a certain limit of a factor, called ecological limitation. Each species has own ecological threshold so they are distributed in the areas of climate (temperature) characteristics. The distribution is often limited by the condition above and below the range polarization lead to decrease of growth and reproductive or increase mortality level of the species. Water temperature conditions outside the range polarization usually have a relationship with other factors (humidity, dissolved oxygen concentration, the solubility of the substance, etc.); create the aggregate impact on the organisms.</p><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> A combination map between ecosystem and results of model</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-6201944x39.png"/></fig><p>According to the biological characteristics of coral reefs temperature for normal development is about 20˚C - 32˚C. When the water temperature is higher than 2˚C, over 29˚C exceeding 1 - 2 weeks, corals will start exhausted and dead. The sex of sea turtles depends greatly on the environmental temperature. Specifically, when the high around environmental temperature sea turtle eggs will be hatched females, while low temperature will be hatched males. If the ambient temperature increased about 4˚C, all eggs will be hatched females. This gender will be imbalance and lead to the extinction of sea turtles species. The simulation results of the scenarios showed that the effluent thermal water from Ninhthuan-II nuclear power plant has the trajectories moving to North and it does not affect the intake gate and sea turtle beach. Area of higher temperature 1˚C is quite small, non-pollution thermal for the study area. According to the National Technical Regulation on industrial wastewater quality NTR 40:2011/MONRE, the maximum limitation value allow of the industrial wastewater temperature is 40˚C. Finally, the impact of cooling water discharges of Ninh Thuan-II nuclear power plant does not affect large environment and within the permissible limits. The results of the thermal diffusion simulation combined the model and ecosystem maps give us an overview of the impact to the Ninh Thuan ecosystem.</p></sec></sec><sec id="s5"><title>5. Conclusion</title><p>The affected areas by the effluent cooling water in four simulation scenarios are very small, ranging about 0.072 - 1.68 km<sup>2</sup>, the largest incidence about 2450 m in the North, 880 m in the South, 960 m in the West. It does not affect the intake gate of plant. In addition, this paper also builds the relationships between surface water temperature and the water temperature at a depth of −15 m to calculate the water temperature at intake and outlet at a depth of −14 m. The combination between this results and results of MIKE 21 FM model can assess the magnitude of effluent cooling water to the environmental and marine ecosystem. The influence area and temperature of effluent cooling water do not affect the coral reefs area in the North and sea turtle conservation in the southern of the plant.</p></sec><sec id="s6"><title>Acknowledgements</title><p>We are grateful to thank Le Hoang Anh, Trinh Hoang Long and Ha Trong Ngoc for their assistance with the collection of land use, topography, meteorological, salinity, temperature and oceanographic data. We are thankful to Institute of Energy Consulting for Thermal, Nuclear Power and Environment for this research opportunity and for the facilities that were used to perform the study.</p></sec><sec id="s7"><title>Cite this paper</title><p>Thai, T.H. and Tri, D.Q. (2017) Modeling the Effect of Thermal Diffusion Process from Nuclear Power Plants in Vietnam. 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