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Joint International Conference on Long-term Experiments ...

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It was marked with AI the area of the leaking secti<strong>on</strong> near the needle top of injector with<br />

c<strong>on</strong>ic top.<br />

Ai = f(sa, β, d) = ct;<br />

Ai = π(dp - 0,5 sa sinβ)sa sin β/2;<br />

sa = 0,15 mm; dp = 1…1,2 mm; β = 60 0 .<br />

Figure 2: The calculati<strong>on</strong> scheme of electromagnetic injector<br />

Discharge of gasoline which passes the injector leaking secti<strong>on</strong> is calculated by the<br />

relati<strong>on</strong>:<br />

2(<br />

pb<br />

− pga<br />

)<br />

Q = μ ⋅ A<br />

; (4)<br />

b i i<br />

ρb<br />

where μI coefficient of discharge in the secti<strong>on</strong> offered by the needle; μi = 0,8 - 0,93 ;<br />

Taking in c<strong>on</strong>siderati<strong>on</strong> relati<strong>on</strong> (2):<br />

Q<br />

2K<br />

= μ ⋅ A<br />

(5)<br />

r<br />

b i i<br />

ρb<br />

where: Ai is the leaking secti<strong>on</strong> at the injector; pb – gasoline pressure at the entrance of<br />

injector; pga – air pressure from the manifold; ρb – gasoline density; Kr - c<strong>on</strong>stant<br />

regulator pressure; Qb- discharge of the gasoline.<br />

In the other hands it is lanown from the relati<strong>on</strong> of the discharge definiti<strong>on</strong>, that is<br />

the leaking fuel volume during a time unit.<br />

We obtain<br />

Q<br />

b<br />

V<br />

=<br />

t<br />

b<br />

i<br />

mcb<br />

=<br />

ρ ⋅t<br />

b<br />

i<br />

From the equality of relati<strong>on</strong> (5) and (6) results un durati<strong>on</strong> of the injecti<strong>on</strong>, ti:<br />

mcb<br />

1<br />

ti<br />

= ⋅<br />

ρb<br />

μ ⋅ A ⋅<br />

2K<br />

r<br />

mcb<br />

=<br />

;<br />

μi<br />

⋅ Ai<br />

⋅ 2K<br />

r ⋅ ρb<br />

1<br />

d =<br />

λ ⋅ Lo<br />

m<br />

=<br />

m<br />

i<br />

i<br />

ρ<br />

b<br />

429<br />

(6)<br />

cb<br />

aer<br />

;

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