TY - JOUR
T1 - Macroscopic diesel fuel spray shadowgraphy using high speed digital imaging in a high pressure cell
AU - Klein-Douwel, R.J.H.
AU - Frijters, P.J.M.
AU - Somers, L.M.T.
AU - Boer, de, W.A.
AU - Baert, R.S.G.
PY - 2007
Y1 - 2007
N2 - Spray formation from diesel fuel injection through a realistic heavy-duty multi-hole common rail injector is studied in a newly developed high pressure, high temperature cell, using digital high speed shadowgraphy at 4500 frames per second. Care is taken to establish accurate synchronisation between camera and injection system and because of the relatively large exposure time, an effective camera image time is calculated for every frame. Further emphasis is given to determining the actual start of fuel mass injection by comparing (for each injection) a predetermined, rail pressure dependent needle relaxation distance to the actual needle lift signal. The spatiotemporal evolution of the spray is found to reproduce well in general, but often sprays suffer from short-lived, small, laterally moving anomalies, which influence axial motion and the spray cone angle. High speed shadowgraphy allows this to be observed and taken into account. After an overview of methods found in the literature, an algorithm for geometrical analysis is presented, which is based on an extension of a combination of those methods. In this algorithm, a local spray angle i(x) is determined from lateral cross-sections at 80% of the shadow level in order to encompass most of the spray without being too sensitive to background noise. The macroscopic cone angle cone is derived from the approximate constancy of i(x) over a relatively long axial distance. Spray penetration is obtained by lateral integration of the spray shadow. A procedure for accurate correlation of spray growth with time shows that the growth is proportional to tb with b = 0.57 ± 0.02 for a common rail pressure of 150 MPa and a gas density 33 kg/m3 (N2 at room temperature). The exact value of b is very sensitive to uncertainties in synchronisation and the start of injection determination. The spray cone angle cone is not constant, but varies with time during an injection, mainly as a result of spray shape changes.
AB - Spray formation from diesel fuel injection through a realistic heavy-duty multi-hole common rail injector is studied in a newly developed high pressure, high temperature cell, using digital high speed shadowgraphy at 4500 frames per second. Care is taken to establish accurate synchronisation between camera and injection system and because of the relatively large exposure time, an effective camera image time is calculated for every frame. Further emphasis is given to determining the actual start of fuel mass injection by comparing (for each injection) a predetermined, rail pressure dependent needle relaxation distance to the actual needle lift signal. The spatiotemporal evolution of the spray is found to reproduce well in general, but often sprays suffer from short-lived, small, laterally moving anomalies, which influence axial motion and the spray cone angle. High speed shadowgraphy allows this to be observed and taken into account. After an overview of methods found in the literature, an algorithm for geometrical analysis is presented, which is based on an extension of a combination of those methods. In this algorithm, a local spray angle i(x) is determined from lateral cross-sections at 80% of the shadow level in order to encompass most of the spray without being too sensitive to background noise. The macroscopic cone angle cone is derived from the approximate constancy of i(x) over a relatively long axial distance. Spray penetration is obtained by lateral integration of the spray shadow. A procedure for accurate correlation of spray growth with time shows that the growth is proportional to tb with b = 0.57 ± 0.02 for a common rail pressure of 150 MPa and a gas density 33 kg/m3 (N2 at room temperature). The exact value of b is very sensitive to uncertainties in synchronisation and the start of injection determination. The spray cone angle cone is not constant, but varies with time during an injection, mainly as a result of spray shape changes.
U2 - 10.1016/j.fuel.2006.11.039
DO - 10.1016/j.fuel.2006.11.039
M3 - Article
SN - 0016-2361
VL - 86
SP - 1994
EP - 2007
JO - Fuel
JF - Fuel
IS - 12-13
ER -