• 한국자동차공학회논문집
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• 제20권2호
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• pp.110-115
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• 2012

This study describes the characteristics of combustion and exhaust emission in the special engine applying a fuel reactivity controlled compression ignition (RCCI) concept with two different energizing type (solenoid and piezoelectric) injectors for diesel injection. A diesel-gasoline mixed dual-fuel reactivity controlled compression ignition concept is demonstrated as a promising method to achieve high thermal efficiency and low emission in internal combustion engines for transportation vehicles. For investigating the combustion characteristics of RCCI, engine experiments were performed in a light-duty diesel engine over a range of injection timing and mixing rate of gasoline in mass. It was investigated that by increasing the nozzle hole diameter, increasing the combustion pressure and the net indicated mean effective pressure. $NO_x$ and soot can be reduced by advancing start of injection in 84 mixing rate of gasoline in mass. The resulting operation showed that light duty engine could achieve 48 percent net indicated efficiency and 191[g/kW-hr] net indicated specific fuel consumption with lower levels of nitrogen oxides and soot.

• Journal of Mechanical Science and Technology
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• 제19권5호
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• pp.1194-1205
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• 2005

The common-rail injection systems, as a new diesel injection system for passenger car, have more degrees of freedom in controlling both the injection timing and injection rate with the high pressure. In this study, a piezo-driven injector was applied to a high pressure common-rail type fuel injection system for the control capability of the high pressure injector's needle and firstly examined the piezo-electric characteristics of a piezo-driven injector. Also in order to analyze the effect of injector's needle response driven by different driving method on the injection, we investigated the diesel spray characteristics in a constant volume chamber pressurized by nitrogen gas for two injectors, a solenoid-driven injector and a piezo-driven injector, both equipped with the same injection nozzle with sac type and 5-injection hole. The experimental method for spray visualization was based on back-light photography technique by utilizing a high speed framing camera. The macroscopic spray propagation was geometrically measured and characterized in term of the spray tip penetration, spray cone angle and spray tip speed. For the evaluation of the needle response of the above two injectors, we indirectly estimated the needle's behavior with an accelerometer and injection rate measurement employing Bosch's method was conducted. The experimental results show that the spray tip penetrations of piezo­driven injector were longer, on the whole, than that of the solenoid-driven injector. Besides we found that the piezo-driven injector have a higher injection flow rate by a fast needle response and it was possible to control the injection rate slope in piezo-driven injector by altering the induced current.

• 한국정밀공학회:학술대회논문집
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• 한국정밀공학회 2003년도 춘계학술대회 논문집
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• pp.764-767
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• 2003

The characteristics of diesel spray have much effect on the engine performances such as power. fuel consumption rate and emissions. Therefore, the measurement of fuel spray characteristics is very important for the improvement of heat engine. The factors which control diesel spray characteristics are injection pressure, ambient temperature and density etc. Spray behaviors are visualized by using the high speed video camera and spray angle, spray penetration are measured. Experimental equations of spray penetration and spray angle were derived by using the experimental results. 1) Ambient temperature and density influence on the characteristics of diesel spray. 2) Experimental equation of spray penetration is expressed as follows 0＜t＜ $t_{b}$ ; $S_1$=11.628$\Delta$ $P^{0.485}$ $\rho$$_{a}$ $^{-0.478}$ $t^{1.337}$, $t_{b}$ ＜t; $S_2$=7.457$\Delta$ $P^{0.523}$ $\rho$$_{a}$ $^{-0.382}$ $t^{0.548}$ 3) Experimental equation of spray Angie is expressed as follows $T_{a}$ =293K; Tan($\theta$/2)=059($\rho$$_{a}$ / $\rho$$_{f}$ )$^{0.437}$, $T_{a}$ =473K; Tan($\theta$/2)=0588($\rho$$_{a}$ / $\rho$$_{f}$ )$^{0.404}$_{f}$ )$^{0.404}$

• Journal of Biosystems Engineering
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• 제7권2호
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• pp.30-35
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• 1983

동력분무기(動力噴霧機)의 능률적(能率的)인 방제작업(防除作業)을 실시(實施)하기 위하여 호오스 길이 및 토출압력별(吐出壓力別)로 도달성(到達性)에 영향(影響)을 미치는 제인자(諸因子)를 구명(究明)하고자 균등분포율(均等分布率) 10%이상(以上)의 최대도달거리(最大到達距離), 균등분포율(均等分布率) 50%이상(以上)의 유효도달거리, 균등분포율(均等分布率)에 의한 최다낙하량분포중심위치(最多落下量分布中心位置)및 분무입자(噴霧粒子), 압력(壓力)의 변화등(變化等)을 측정(側定)하여 분석(分析)한 결과(結果)를 종합(綜合)하면 다음과 같다. 1. 분무(噴霧)호오스의 길이가 증가(增加)함에 따라 관마찰(管摩擦)에 의한 손실(損失)로 최다낙하량분포중심위치(最多落下量分布中心位置)가 100m 길이에서 0.5m 짧아지는 경향을 보였고, 최대도달거리(最大到達距離)는 100m 길이에서 13mm 호오스가 0.5m, 8.5mm 호오스가 1.0m, 유효도달거리는 각각(各各) 0.5m 감소(減所)하였다. 2. 상용압력(常用壓力)(28kg/$cm^2$)하(下)에서 분무(噴霧)호오스의 길이를 최소(最小)로 하더라도 유효도달거리는 14m이상(以上) 초과(超過)하기 어려울 것으로 판단(判斷)되며, 13mm 호오스가 8.5mm 호오스에 비(比)하여 1.0m정도(程度) 도달거리(到達距離)가 증가(增加)하였다. 3. 13mm 호오스에서는 토출압력(吐出壓力)이 8kg/$cm^2$ 상승(上昇)함에 따라 최다낙하량분포중심위치(最多落下量分布中心位置)가 0.5m(1kg/$cm^2$당(當) 약(約) 0.06m) 연장(延長)되었고 최대도달거리(最大到達距離)는 2.0m, 유효도달거리는 0.5m 증가(增加)하였다. 또 8.5mm 호오스에 있어서는 토출압력(吐出壓力) 변화(變化)가 도달성(到達性)에 거의 영향(影響)을 미치지 않았다. 4. 분무(噴霧)호오스 길이의 감소(減少) 및 토출압력(吐出壓力)의 증가(增加)가 분무입자(噴霧粒子)의 미립화효과에 크게 기여(寄與)하고, 분무입경(噴霧粒徑)은 분무압력(噴霧壓力)과 호오스 내경(內徑)의 크기에 상호관련성(相互關聯性)이 있는 것으로 생각된다. 5. 토출압력(吐出壓力) 25~33kg/$cm^2$에 대(對)한 분무(噴霧)호오스 끝에서의 압력강하(壓力降下)는 13mm 호오스가 100m 길이에서 3~7kg/$cm^2$로 10m 길이당(當) 2%정도(程度)의 비율(比率)로 압력(壓力)이 강하(降下)하였다.