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1740 S. Shin et al. / European Journal <strong>of</strong> Operational Research 207 (2010) 1728–1741<br />

Pro<strong>of</strong>. See Corless et al. (1996). h<br />

Proposition 1. If g2 =(v + g1)e v where g1 <strong>and</strong> g2 are not functions <strong>of</strong><br />

v, <strong>the</strong>n v ¼ Lambert W g2eg ð 1Þ<br />

g1 .<br />

Pro<strong>of</strong>. Consider <strong>the</strong> following equation:<br />

g 2 ¼ðv þ g 1 Þe v : ðA-1Þ<br />

Let v + g1 = w so Eq. (A-1) becomes<br />

g 2 ¼ we w g 1: ðA-2Þ<br />

To convert Eq. (A-2) in <strong>the</strong> st<strong>and</strong>ard form g = ve v , we first modify<br />

Eq. (A-2) as follows:<br />

g 2 e g 1 ¼ we w : ðA-3Þ<br />

Next, substitute g 2 e g 1 ¼ x to <strong>the</strong> right h<strong>and</strong> side <strong>of</strong> Eq. (A-3)<br />

<strong>the</strong>n we obtain x = we w . From Lemma 1, w is given by:<br />

w ¼ Lambert WðxÞ: ðA-4Þ<br />

Therefore, v is obtained as<br />

v ¼ Lambert W g2e g ð 1Þ<br />

g1 :<br />

Proposition 2. If g4 ¼ g1 v2 þ g2 eg3v2 , where g1, g2, g3, <strong>and</strong> g4 are<br />

not functions <strong>of</strong> v, <strong>the</strong>n<br />

v ¼<br />

ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi<br />

Lambert W g3g4 e g2g v<br />

u<br />

3<br />

u<br />

t<br />

g1 :<br />

g 3<br />

g 2<br />

Pro<strong>of</strong>. In order to prove Proposition 2 using Lemma 1, we first consider<br />

<strong>the</strong> equation<br />

g4 ¼ g1 v2 þ g2 e g3v2 : ðA-5Þ<br />

g 3g 4<br />

g 1<br />

Multiplied both sides with g3/g1, Eq. (A-5) becomes<br />

¼ g3 v2 þ g2 e g3v2 : ðA-6Þ<br />

Let w = g 3(v 2 + g 2), Eq. (A-6) can be written as<br />

g 3g 4 e g 2g 3<br />

g 1<br />

¼ we w : ðA-7Þ<br />

Fur<strong>the</strong>r, substituted g3g4 e g2g3 g1 dard form g = ve v .<br />

¼ x, Eq. (A-7) is now in <strong>the</strong> stan-<br />

w ¼ Lambert WðxÞ: ðA-8Þ<br />

Replaced x ¼ g3g4 e g2g3 g back into Eq. (A-8), <strong>the</strong> st<strong>and</strong>ard form in<br />

1<br />

Eq. (A-8) can be written as w ¼ Lambert W g3g4 e g2g3 g . Eq. (A-9)<br />

1<br />

can be exp<strong>and</strong>ed to express <strong>the</strong> solution in terms <strong>of</strong> v by replacing<br />

w with g3(v + g2). Thus, <strong>the</strong> solution for v is given by<br />

ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi<br />

Lambert W<br />

v ¼<br />

g3g4 e g2g v<br />

u<br />

3<br />

u<br />

t<br />

g1 : ðA-9Þ<br />

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