JP3383874B2 - Diesel engine combustion simulation method - Google Patents
Diesel engine combustion simulation methodInfo
- Publication number
- JP3383874B2 JP3383874B2 JP19883593A JP19883593A JP3383874B2 JP 3383874 B2 JP3383874 B2 JP 3383874B2 JP 19883593 A JP19883593 A JP 19883593A JP 19883593 A JP19883593 A JP 19883593A JP 3383874 B2 JP3383874 B2 JP 3383874B2
- Authority
- JP
- Japan
- Prior art keywords
- combustion
- fuel
- diesel engine
- evaporation
- calculated
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Fee Related
Links
- 238000002485 combustion reaction Methods 0.000 title claims description 56
- 238000000034 method Methods 0.000 title claims description 9
- 238000004088 simulation Methods 0.000 title claims description 9
- 239000000446 fuel Substances 0.000 claims description 39
- 238000001704 evaporation Methods 0.000 claims description 24
- 230000008020 evaporation Effects 0.000 claims description 22
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 claims description 12
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 claims description 10
- 229910052799 carbon Inorganic materials 0.000 claims description 10
- 238000009792 diffusion process Methods 0.000 claims description 7
- 238000004458 analytical method Methods 0.000 claims description 6
- 239000007787 solid Substances 0.000 claims description 5
- 239000007788 liquid Substances 0.000 claims description 4
- 238000004364 calculation method Methods 0.000 description 8
- 238000002347 injection Methods 0.000 description 7
- 239000007924 injection Substances 0.000 description 7
- 238000002474 experimental method Methods 0.000 description 6
- 230000002000 scavenging effect Effects 0.000 description 6
- 239000007921 spray Substances 0.000 description 6
- 238000006243 chemical reaction Methods 0.000 description 4
- 239000000498 cooling water Substances 0.000 description 4
- 239000007789 gas Substances 0.000 description 4
- 239000003921 oil Substances 0.000 description 4
- 238000010586 diagram Methods 0.000 description 3
- 230000020169 heat generation Effects 0.000 description 3
- 239000000203 mixture Substances 0.000 description 3
- 230000033228 biological regulation Effects 0.000 description 2
- 230000015572 biosynthetic process Effects 0.000 description 2
- 239000000295 fuel oil Substances 0.000 description 2
- 239000010763 heavy fuel oil Substances 0.000 description 2
- 239000004071 soot Substances 0.000 description 2
- 238000003915 air pollution Methods 0.000 description 1
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 239000013626 chemical specie Substances 0.000 description 1
- 239000000567 combustion gas Substances 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000003647 oxidation Effects 0.000 description 1
- 238000007254 oxidation reaction Methods 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 230000000704 physical effect Effects 0.000 description 1
- 238000007670 refining Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
- 238000006557 surface reaction Methods 0.000 description 1
- 238000011144 upstream manufacturing Methods 0.000 description 1
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F02—COMBUSTION ENGINES; HOT-GAS OR COMBUSTION-PRODUCT ENGINE PLANTS
- F02B—INTERNAL-COMBUSTION PISTON ENGINES; COMBUSTION ENGINES IN GENERAL
- F02B3/00—Engines characterised by air compression and subsequent fuel addition
- F02B3/06—Engines characterised by air compression and subsequent fuel addition with compression ignition
Landscapes
- Testing Of Engines (AREA)
- Management, Administration, Business Operations System, And Electronic Commerce (AREA)
Description
【発明の詳細な説明】
【0001】
【産業上の利用分野】本発明はディーゼル機関の燃焼状
態をコンピュータを用いてシミュレートするためのディ
ーゼル機関の燃焼シミュレーション方法に関するもので
ある。
【0002】
【従来の技術】大型船舶では、一般に、燃料油として、
石油精製過程で生じる残渣油に粘度調整のために若干の
軽質油を混合したC重油と呼ばれるブレンド油が使用さ
れており、石油精製設備の性能が上がれば上がるほど、
それにつれて低質化し主機の燃焼障害や大気汚染問題が
惹起される。
【0003】したがって、このような問題を改善するた
めには、燃料の性状に基づいて、状況に合った最適な運
転状態が得られるように燃料を燃焼させることが必要と
なる。
【0004】
【発明が解決しようとする課題】ところが、燃料の性状
に基づいた機関の最適な運転状態を指標するには、予
め、ディーゼル機関の実機を用いて、あらゆる性状の燃
料について、各種の燃焼条件を設定して広角度な燃焼実
験を行う必要があるが、その場合、多大な労力及び費用
がかかるばかりでなく、大型舶用ディーゼル機関による
C重油の燃焼実験については、公害規制上陸上では実験
が困難である、という問題がある。そのため、あらゆる
種類の燃料に対して簡単に燃焼実験結果が得られるよう
な技術の開発が要望されているが、現時点では開発され
ていないのが実情である。
【0005】そこで、本発明は、ディーゼル機関の燃焼
を、種々の簡略化モデルの採用によりシミュレートして
燃料の性状に応じた機関の最適運転状態を簡単に指標す
ることができるようなディーゼル機関の燃焼シミュレー
ション方法を提供しようとするものである。
【0006】
【課題を解決するための手段】本発明は、上記課題を解
決するために、対象となるディーゼル機関の機関形状や
燃料噴射タイミング、冷却水温度、掃気温度、燃料への
水分混合率の各パラメータ等の各種既存値と対象となる
燃料の分析値とを基に、先ず、燃料液滴を液体燃焼成分
・水分蒸発層と水分蒸発層と固体炭素表面燃焼層との3
つの層に分けて燃料液滴の蒸発を計算し、次に、火炎伝
播を計算し、更に、燃料液滴の蒸発、予混合燃焼、拡散
燃焼、残留炭素燃焼の4項目についての熱発生率を計算
してトータル的な熱発生率を求め、その結果を出力させ
るようにすることを特徴とするディーゼル機関の燃焼シ
ミュレーション方法とする。
【0007】
【作用】燃料液滴を3つの層に分けて液滴の蒸発を計算
するので、燃料蒸発量、水分蒸発量、炭素燃焼量等が正
確に求められる。又、火炎伝播が計算された後、燃料液
滴の蒸発、予混合燃焼、拡散燃焼、残留炭素燃焼の4項
目を計算してトータルな熱発生率を求めるので、実測値
に極めて近い値が得られる。
【0008】
【実施例】以下、本発明の実施例を図面を参照して説明
する。
【0009】図1は本発明のディーゼル機関の燃焼シミ
ュレーション方法を実施するためのフローチャートを示
すもので、パソコンの如きコンピュータを用い、データ
ベースに蓄えておいた各種の燃料分析値のうち、対象燃
料の分析値と、対象機関の各種既存値(機関形状や、燃
料噴射タイミング(FQS)、冷却水温度、掃気温度、
燃料への水分混合率の各パラメータ)を入力し、先ず、
燃料液滴の蒸発計算を行い、次に、火炎伝播を計算し、
続いて、液滴の蒸発、予混合燃焼、拡散燃焼、残留炭素
燃焼の4項目についての熱発生率を計算してトータル的
な熱発生率を求め、更に、NOx生成の計算、すす生成
の計算、燃焼室の壁面温度の決定等を行い、正味熱発生
率を求めてディスプレイ上に表示して出力させるように
したものである。なお、上記各計算のプログラムはハー
ドディスクあるいは基板などにソフトとして取り込ませ
ておくようにする。
【0010】以下、詳述する。
【0011】先ず、ステップ1として、機関スペック、
物性値、初期値等の各種既存値の読み込みを行わせ、し
かる後、ステップ2として、対象とする燃料の分析値を
読み込ませる。
【0012】次に、ステップ3として、下死点から排気
弁閉までの掃気圧力や温度を固定し、続いて、ステップ
4として、排気弁閉から燃料噴射開始までのシリンダ内
圧力や温度を計算する。
【0013】次いで、本発明の特徴をなすステップ5と
して、燃料噴射開始から終了までを、上記燃料分析値
と、既存値としての機関形状や燃料噴射タイミング、ジ
ャケット冷却温度、掃気温度、燃料への水分混合率のパ
ラメータ等とにより、所定の計算を下記の如く行わせ
る。
【0014】すなわち、図2は燃料液滴の蒸発モデルを
示すもので、この際、液滴は、液体燃焼成分・水分蒸発
層としての第I層と、水分蒸発層としての第II層と、固
形炭素表面燃焼層としての第III 層との3つの層を考え
る。
【0015】液滴は常に球形とし、液体燃料及び水の蒸
発は次式に従うものとする。
【0016】
【数1】
但し、Dd は液滴直径、kf は蒸発係数である。
【0017】固形炭素分は次式で示される表面燃焼によ
り、直径が減少するものとする。
【0018】
mc ′=ks P02 …(2)
但し、ks は表面反応速度定数、P02は酸素分圧であ
る。排気弁が開くときに燃焼が終了していない未燃量を
燃焼残渣とする。
【0019】又、図3は噴霧燃焼モデルを示し、計算刻
み毎に噴射される液滴の集団を燃料噴霧ユニットとし、
ユニット内のみで液滴の蒸発及び燃焼が起こるものとす
る。ユニット内の燃焼ガスは瞬時に拡散し、周囲ガスと
混合する。
【0020】噴霧の到達距離は噴射時のユニット内の運
動量が保存されるものとして、次式の関係から計算す
る。
【0021】
噴射時の燃料の運動量=液滴の運動量+ユニット内ガスの運動量 …(3)
噴霧先端で燃焼が開始すると、上流側に予混合燃焼によ
る火炎面が伝播する。この際、予混合気の燃焼速度は次
式で計算する。
【0022】
【数2】
但し、su0は基準圧力P0 及び基準温度T0 における燃
焼速度である。火炎伝播速度は燃料噴霧ユニットの速度
と燃焼速度の差として計算される。
【0023】予混合燃焼終了後のユニットは、蒸発律則
による拡散燃焼をする。
【0024】又、NOxの生成については、次式に示す
拡大Zeldovich機構を採用した。
【0025】
【数3】
反応速度は次式で計算する。但し、化学種Aのモル濃度
を[A]、反応速度定数をkで表す。化学種の濃度には
ユニット内の化学平衡濃度を用いる。
【0026】
【数4】
反応後、ユニット内外のガスは瞬時に相互拡散によって
混合するものとする。
【0027】一方、すすの生成と酸化はアレニウス形の
反応式で記述し、実際の生成量は両者の差として次式で
計算する。
【0028】
【数5】
又、燃焼室壁面温度の決定には、燃焼室壁面をシリンダ
カバー、ライナー、ピストンの3つの部分に分け、冷却
水入口温度と流量を与えて準定常伝熱計算を行う。これ
により各部の冷却水出口温度と燃焼室壁面温度を計算す
る。壁面熱伝達率にはWoschniの式を使用した。
【0029】更に、シリンダ内での正味の熱発生率は次
式で計算する。
【0030】
【数6】
但し、右辺第1〜3項はそれぞれ予混合燃焼、拡散燃
焼、固形炭素の燃焼による熱発生であり、右辺第4と5
項はそれぞれ燃料の蒸発及び水の蒸発による熱損失であ
り、右辺第6項は壁面熱損失である。
【0031】上記の如くしてステップ5が終了すると、
次に、ステップ6として、燃焼終了から排気弁開までの
シリンダ内圧力や温度を計算し、続いて、ステップ7と
して、排気弁開から掃気ポート開までのシリンダ内圧力
の直線近似化やシリンダ内温度の計算を行い、更に、ス
テップ8として、掃気ポート開から下死点までのシリン
ダ内圧力を固定すると共に、シリンダ内温度の直線近似
化を行い、終了とする。
【0032】これらのシミュレーションの結果は、図4
に一例を示す如くディスプレイ上に表示して出力させ
る。なお、図4において、イはシリンダ内圧、ロはシリ
ンダ内温度、ハは熱発生率のそれぞれ予測値としての計
算値を、又、ニはシリンダ内圧の実測値を示し、イとニ
がほとんど一致する結果が得られた。
【0033】なお、本発明は舶用ディーゼル機関に限ら
ず、あらゆる分野で用いられているディーゼル機関の燃
焼をシミュレーションすることができること、その他本
発明の要旨を逸脱しない範囲内において種々変更を加え
得ることは勿論である。
【0034】
【発明の効果】以上述べた如く、本発明のディーゼル機
関の燃焼シミュレーション方法によれば、対象となるデ
ィーゼル機関の既存値と燃料の分析値を基に、燃焼によ
る熱発生率を計算により求めて出力させるようにするの
で、実機による燃焼実験を行うことなく、燃料の性状に
応じたディーゼル機関の最適運転状態を簡単に指標する
ことができ、特に、公害規制上陸上では実験が困難な大
型舶用ディーゼル機関によるC重油についても容易に実
施することができる、という優れた効果を発揮する。Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a diesel engine combustion simulation method for simulating the combustion state of a diesel engine using a computer. [0002] In a large ship, generally, as fuel oil,
Blend oil called C heavy oil, which is a mixture of residual oil generated in the oil refining process with some light oil for viscosity adjustment, is used.
As a result, the quality of the engine deteriorates, causing a combustion failure of the main engine and an air pollution problem. [0003] Therefore, in order to improve such a problem, it is necessary to burn the fuel based on the properties of the fuel so as to obtain an optimal operating state suitable for the situation. [0004] However, in order to indicate the optimum operating state of the engine based on the properties of the fuel, various types of fuels of various properties were previously determined using an actual diesel engine. It is necessary to set a combustion condition and conduct a wide-angle combustion experiment.In that case, not only is it labor and cost intensive, but also about the combustion experiment of heavy fuel oil C with a large marine diesel engine, the pollution regulation land There is a problem that the experiment is difficult. For this reason, there is a demand for the development of a technology that can easily obtain the results of combustion experiments for all types of fuels, but at present it has not been developed. Accordingly, the present invention provides a diesel engine in which combustion of a diesel engine is simulated by employing various simplified models to easily indicate the optimum operating state of the engine according to the properties of the fuel. It is intended to provide a combustion simulation method. SUMMARY OF THE INVENTION In order to solve the above problems, the present invention provides an engine shape, fuel injection timing, cooling water temperature, scavenging temperature, and water mixing ratio of a target diesel engine. First, based on the various existing values such as the above parameters and the analysis values of the target fuel, the fuel droplets are first divided into a liquid combustion component / water evaporation layer, a water evaporation layer, and a solid carbon surface combustion layer.
Calculate the evaporation of the fuel droplets in two layers, then calculate the flame propagation, and further calculate the heat release rates for the four items of fuel droplet evaporation, premixed combustion, diffusion combustion, and residual carbon combustion. A combustion simulation method for a diesel engine is characterized in that a total heat release rate is obtained by calculation and the result is output. Since the evaporation of the droplet is calculated by dividing the fuel droplet into three layers, the amount of fuel evaporation, the amount of water evaporation, the amount of carbon combustion, and the like can be accurately obtained. After the flame propagation is calculated, the total heat release rate is calculated by calculating the four items of fuel droplet evaporation, premixed combustion, diffusion combustion, and residual carbon combustion, so that a value very close to the measured value is obtained. Can be An embodiment of the present invention will be described below with reference to the drawings. FIG. 1 shows a flow chart for carrying out the method for simulating combustion of a diesel engine according to the present invention, wherein a computer such as a personal computer is used to analyze a target fuel among various fuel analysis values stored in a database. The analysis values and various existing values of the target engine (engine shape, fuel injection timing (FQS), cooling water temperature, scavenging temperature,
Parameters of the water mixing ratio into the fuel)
Calculate the evaporation of the fuel droplets, then calculate the flame propagation,
Next, the total heat release rate is calculated by calculating the heat release rates for the four items of droplet evaporation, premixed combustion, diffusion combustion, and residual carbon combustion, and further, the calculation of NOx generation and the calculation of soot generation In addition, the wall temperature of the combustion chamber is determined, and the net heat generation rate is obtained and displayed on a display for output. In addition, the program for each of the above calculations is loaded as software on a hard disk or a substrate. The details will be described below. First, as step 1, the engine specifications,
Various existing values, such as physical property values and initial values, are read. Thereafter, as step 2, the analysis values of the target fuel are read. Next, in step 3, the scavenging pressure and temperature from the bottom dead center to the closing of the exhaust valve are fixed, and then in step 4, the pressure and temperature in the cylinder from the closing of the exhaust valve to the start of fuel injection are calculated. I do. Next, as a step 5 which is a feature of the present invention, from the start to the end of the fuel injection, the fuel analysis value and the existing values of the engine shape, fuel injection timing, jacket cooling temperature, scavenging temperature, fuel Predetermined calculation is performed as follows based on the parameters of the water mixing ratio and the like. That is, FIG. 2 shows an evaporation model of a fuel droplet. At this time, the droplet is composed of a first layer as a liquid combustion component / water evaporation layer, a second layer as a water evaporation layer, and a second layer as a water evaporation layer. Consider three layers, the third layer as a solid carbon surface combustion layer. The droplets are always spherical and the evaporation of liquid fuel and water follows the formula: ## EQU1 ## Here, D d is the droplet diameter, and k f is the evaporation coefficient. The diameter of the solid carbon content is reduced by surface combustion represented by the following formula. M c ′ = k s P 02 (2) where k s is a surface reaction rate constant and P 02 is an oxygen partial pressure. The unburned amount of the combustion that has not been completed when the exhaust valve is opened is defined as a combustion residue. FIG. 3 shows a spray combustion model, in which a group of droplets injected at each calculation step is defined as a fuel spray unit.
It is assumed that evaporation and burning of droplets occur only in the unit. The combustion gases in the unit diffuse instantaneously and mix with the surrounding gases. The reach of the spray is calculated from the following equation, assuming that the momentum in the unit at the time of injection is preserved. Momentum of fuel at the time of injection = Momentum of droplet + Momentum of gas in unit ... (3) When combustion starts at the spray tip, a flame surface due to premix combustion propagates to the upstream side. At this time, the combustion speed of the premixed gas is calculated by the following equation. ## EQU2 ## However, s u0 is the burn rate of the reference pressure P 0 and the reference temperature T 0. The flame propagation speed is calculated as the difference between the speed of the fuel spray unit and the burning speed. After completion of the premixed combustion, the unit performs diffusion combustion according to the evaporation rule. For the generation of NOx, an extended Zeldovich mechanism shown in the following equation was adopted. [Equation 3] The reaction rate is calculated by the following equation. Here, the molar concentration of the species A is represented by [A], and the reaction rate constant is represented by k. The chemical equilibrium concentration in the unit is used for the concentration of the chemical species. [Mathematical formula-see original document] After the reaction, the gas inside and outside the unit is instantaneously mixed by mutual diffusion. On the other hand, soot formation and oxidation are described by an Arrhenius type reaction equation, and the actual amount of formation is calculated by the following equation as the difference between the two. (Equation 5) To determine the temperature of the combustion chamber wall surface, the combustion chamber wall surface is divided into three parts, a cylinder cover, a liner, and a piston, and a quasi-stationary heat transfer calculation is performed by giving a cooling water inlet temperature and a flow rate. Thereby, the cooling water outlet temperature and the combustion chamber wall surface temperature of each part are calculated. The Wosni equation was used for the wall heat transfer coefficient. Further, the net heat release rate in the cylinder is calculated by the following equation. (Equation 6) However, the first to third terms on the right side represent heat generation by premixed combustion, diffusion combustion, and solid carbon combustion, respectively.
The terms are heat loss due to fuel evaporation and water evaporation, respectively, and the sixth term on the right side is wall heat loss. When step 5 is completed as described above,
Next, in Step 6, the pressure and temperature in the cylinder from the end of combustion to the opening of the exhaust valve are calculated. Subsequently, in Step 7, linear approximation of the pressure in the cylinder from the opening of the exhaust valve to the opening of the scavenging port, and the calculation in the cylinder are performed. The temperature is calculated, and in step 8, the pressure in the cylinder from the scavenging port opening to the bottom dead center is fixed, and the temperature in the cylinder is linearly approximated. The results of these simulations are shown in FIG.
Is displayed on a display as shown in FIG. In FIG. 4, A indicates the cylinder pressure, B indicates the cylinder temperature, C indicates the calculated value of the heat release rate as a predicted value, and D indicates the actual measured value of the cylinder pressure. Results were obtained. The present invention is not limited to marine diesel engines, but can simulate the combustion of diesel engines used in various fields, and can make various changes without departing from the gist of the present invention. Of course. As described above, according to the combustion simulation method for a diesel engine of the present invention, the heat generation rate due to combustion is calculated based on the existing values of the target diesel engine and the analyzed values of the fuel. It is possible to easily determine the optimal operating condition of the diesel engine according to the properties of the fuel without conducting a combustion experiment with an actual machine, and it is particularly difficult to perform an experiment on land with pollution regulations. An excellent effect is exhibited in that it is easy to carry out heavy fuel oil C by a large marine diesel engine.
【図面の簡単な説明】
【図1】本発明のディーゼル機関の燃焼シミュレーショ
ン方法のフローチャートである。
【図2】燃料液滴の蒸発モデルを示す概略図である。
【図3】燃料の噴霧燃焼モデルを示す概略図である。
【図4】得られた結果の一例を示すシミュレーション出
力図である。
【符号の説明】
1 ステップ1
2 ステップ2
3 ステップ3
4 ステップ4
5 ステップ5
6 ステップ6
7 ステップ7
8 ステップ8BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a flowchart of a combustion simulation method for a diesel engine according to the present invention. FIG. 2 is a schematic diagram showing an evaporation model of a fuel droplet. FIG. 3 is a schematic diagram showing a fuel spray combustion model. FIG. 4 is a simulation output diagram showing an example of the obtained result. [Description of Signs] 1 Step 1 2 Step 2 3 Step 3 4 Step 4 5 Step 5 6 Step 6 7 Step 7 8 Step 8
フロントページの続き (72)発明者 中島 利幸 東京都江東区豊洲二丁目1番1号 石川 島播磨重工業株式会社 東京第一工場内 (56)参考文献 特表 平3−504042(JP,A) (58)調査した分野(Int.Cl.7,DB名) G06F 17/00 G01M 15/00 Continuation of front page (72) Inventor Toshiyuki Nakajima 2-1-1, Toyosu, Koto-ku, Tokyo Ishikawa Shima-Harima Heavy Industries Co., Ltd. Tokyo 1st Factory (56) References 58) Fields surveyed (Int. Cl. 7 , DB name) G06F 17/00 G01M 15/00
Claims (1)
と対象となる燃料の分析値を基に、先ず、燃料液滴を液
体燃焼成分・水分蒸発層と水分蒸発層と固体炭素表面燃
焼層との3つの層に分けて燃料液滴の蒸発を計算し、次
に、火炎伝播を計算し、更に、燃料液滴の蒸発、予混合
燃焼、拡散燃焼、残留炭素燃焼の4項目についての熱発
生率を計算してトータル的な熱発生率を求め、その結果
を出力させるようにすることを特徴とするディーゼル機
関の燃焼シミュレーション方法。(57) [Claims] [Claim 1] First, based on various existing values of a target diesel engine and analysis values of a target fuel, a fuel droplet is first formed into a liquid combustion component / moisture evaporating layer and water. Calculate the evaporation of fuel droplets in three layers, evaporating layer and solid carbon surface combustion layer, then calculate flame propagation, further evaporate fuel droplets, premix combustion, diffusion combustion, residual combustion A combustion simulation method for a diesel engine, wherein a total heat release rate is calculated by calculating heat release rates for four items of carbon combustion, and the result is output.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19883593A JP3383874B2 (en) | 1993-07-19 | 1993-07-19 | Diesel engine combustion simulation method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19883593A JP3383874B2 (en) | 1993-07-19 | 1993-07-19 | Diesel engine combustion simulation method |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH0734894A JPH0734894A (en) | 1995-02-03 |
JP3383874B2 true JP3383874B2 (en) | 2003-03-10 |
Family
ID=16397712
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP19883593A Expired - Fee Related JP3383874B2 (en) | 1993-07-19 | 1993-07-19 | Diesel engine combustion simulation method |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP3383874B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP2860380A4 (en) * | 2012-06-08 | 2016-01-06 | Toyota Motor Co Ltd | Device for diagnosing combustion states in internal combustion engines |
Families Citing this family (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6464585B1 (en) * | 1997-11-20 | 2002-10-15 | Nintendo Co., Ltd. | Sound generating device and video game device using the same |
JP4158747B2 (en) * | 2004-06-28 | 2008-10-01 | 日産自動車株式会社 | Ignition timing control device for internal combustion engine |
JP4424242B2 (en) | 2005-03-30 | 2010-03-03 | トヨタ自動車株式会社 | Mixture state estimation device and emission generation amount estimation device for internal combustion engine |
JP5413874B2 (en) * | 2008-08-01 | 2014-02-12 | 学校法人立命館 | Combustion analysis method, combustion analysis apparatus, and computer program |
US8353196B2 (en) | 2008-09-24 | 2013-01-15 | Toyota Jidosha Kabushiki Kaisha | Gas-mixture-nonuniformity acquisition apparatus and gas-mixture-state acquisition apparatus for internal combustion engine |
JP5330932B2 (en) * | 2009-08-24 | 2013-10-30 | 富士重工業株式会社 | Spray measurement method and spray measurement device |
JP6813163B2 (en) * | 2016-04-25 | 2021-01-13 | 国立研究開発法人 海上・港湾・航空技術研究所 | Fuel evaporation process analysis method, evaporation process analysis program and fuel injection control system using it |
CN107269408B (en) * | 2017-05-15 | 2022-08-05 | 吉林大学 | Diesel engine optimized combustion controller and simulation model control method |
CN108998112B (en) * | 2018-07-20 | 2020-09-25 | 太原理工大学 | F-T diesel oil characterization fuel skeleton mechanism model construction method |
-
1993
- 1993-07-19 JP JP19883593A patent/JP3383874B2/en not_active Expired - Fee Related
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP2860380A4 (en) * | 2012-06-08 | 2016-01-06 | Toyota Motor Co Ltd | Device for diagnosing combustion states in internal combustion engines |
Also Published As
Publication number | Publication date |
---|---|
JPH0734894A (en) | 1995-02-03 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
Duclos et al. | 3D modeling of combustion for DI-SI engines | |
JP3383874B2 (en) | Diesel engine combustion simulation method | |
Karaky et al. | Development and validation of a new zero-dimensional semi-physical NOx emission model for a DI diesel engine using simulated combustion process | |
Ismail et al. | Numerical investigations on the performance and emissions of a turbocharged engine using an ethanol-gasoline blend | |
Subramanian et al. | New developments in turbulent combustion modeling for engine design: ECFM-CLEH combustion submodel | |
Puduppakkam et al. | Accurate and dynamic accounting of fuel composition in flame propagation during engine simulations | |
Bordet et al. | A physical 0D combustion model using tabulated chemistry with presumed probability density function approach for multi-injection diesel engines | |
Oppenheim et al. | Refinement of heat release analysis | |
Krenn et al. | A new approach for combustion modeling of large dual-fuel engines | |
Regner et al. | Analysis of transient drive cycles using CRUISE-BOOST co-simulation techniques | |
Murthy et al. | Modeling and prediction of NOx emission in an LPG–diesel dual‐fuel CI engine | |
Chan et al. | Prediction of transient nitric oxide in diesel exhaust | |
Falfari et al. | Hydrogen Application as a Fuel in Internal Combustion Engines. Energies 2023, 16, 2545 | |
Leman et al. | Engine modelling of a single cylinder diesel engine fuelled by diesel-methanol blend | |
Alizadeh Attar | Optimization and knock modeling of a gas fueled spark ignition engine. | |
Bozza et al. | Experimental investigation and numerical modelling of an advanced turbocharged DI diesel engine | |
Subramanian et al. | Modeling engine turbulent auto-ignition using tabulated detailed chemistry | |
Karaky et al. | Semi-empirical 0D modeling for engine-out soot emission prediction in DI diesel engines | |
Tavakoli et al. | Natural gas engine thermodynamic modeling concerning offshore dynamic condition | |
Poetsch et al. | A Real-Time Capable and Modular Modeling Concept for Virtual SI Engine Development | |
Tromellini | Investigation of post-oxidation by means of 3D-CFD virtual engine development | |
Liu et al. | Numerical Investigation of Different Combustion Models for Dual‐Fuel Engine Combustion Processes | |
Bohbot et al. | Multiscale engine simulations using a coupling of 0-d/1-dmodel with a 3-d combustion code | |
Held et al. | A 3D computational study of the formation, growth and oxidation of soot particles in an optically accessible direct-injection spark-ignition engine using quadrature-based methods of moments | |
Schnapp et al. | A Phenomenological Unburned Hydrocarbon Model for Diesel Engines |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20071227 Year of fee payment: 5 |
|
S531 | Written request for registration of change of domicile |
Free format text: JAPANESE INTERMEDIATE CODE: R313531 |
|
S533 | Written request for registration of change of name |
Free format text: JAPANESE INTERMEDIATE CODE: R313533 |
|
FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20071227 Year of fee payment: 5 |
|
R350 | Written notification of registration of transfer |
Free format text: JAPANESE INTERMEDIATE CODE: R350 |
|
FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20081227 Year of fee payment: 6 |
|
FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20091227 Year of fee payment: 7 |
|
FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20091227 Year of fee payment: 7 |
|
FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20101227 Year of fee payment: 8 |
|
FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20101227 Year of fee payment: 8 |
|
S111 | Request for change of ownership or part of ownership |
Free format text: JAPANESE INTERMEDIATE CODE: R313115 |
|
FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20101227 Year of fee payment: 8 |
|
R350 | Written notification of registration of transfer |
Free format text: JAPANESE INTERMEDIATE CODE: R350 |
|
FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20111227 Year of fee payment: 9 |
|
FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20121227 Year of fee payment: 10 |
|
LAPS | Cancellation because of no payment of annual fees |