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Stochastic Programming - Index of

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294 STOCHASTIC PROGRAMMING<br />

[-1,1]<br />

[1,3]<br />

1<br />

2<br />

2<br />

1<br />

(0,[2,4]) 3<br />

(0,[2,4])<br />

(0,[2,6])<br />

1<br />

3<br />

3<br />

4 6<br />

4<br />

(0,[2,4])<br />

2<br />

(0,[4,8])<br />

8<br />

1<br />

(0,[2,6])<br />

4 7 5<br />

5 [-2,0]<br />

2<br />

1<br />

(0,[6,8])<br />

2<br />

(0,[0,2])<br />

Slack<br />

Figure 11<br />

[3,3]<br />

Network illustrating the different bounds.<br />

6.5 Bounds<br />

We discussed some bounds for general LPs in Chapter 3. These <strong>of</strong> course<br />

also apply to networks, since networks are nothing but special cases <strong>of</strong> linear<br />

programs. The Jensen lower bound can be found by replacing each random<br />

variable (external flow or arc capacity) by its mean and solving the resulting<br />

deterministic network flow problem. The Edmundson–Madansky upper bound<br />

is found by evaluating the network flow problem at all extreme points <strong>of</strong> the<br />

support. (If the randomness sits in the objective function, the methods give<br />

opposite bounds, just as we discussed for the LP case.)<br />

Figure 11 shows an example that will be used in this section to illustrate<br />

bounds. The terminology is as follows. Square brackets, for example [a, b], are<br />

used to denote supports <strong>of</strong> random variables. Placed next to a node, they<br />

show the size <strong>of</strong> the random external flow. Placed in a setting like (c, [a, b]),<br />

the square bracket shows the support <strong>of</strong> the upper bound on the arc flow for<br />

the arc next to which it is placed. In this setting, c is the lower bound on<br />

the flow. It can become negative in some <strong>of</strong> the methods. The circled number<br />

next to an arc is the unit arc cost, and the number in a square on the arc is<br />

the arc number. For simplicity, we shall assume that all random variables are<br />

independent and uniformly distributed.<br />

Figure 12 shows the set-up for the Jensen lower bound for the example from<br />

Figure 11. We have now replaced each random variable by its mean, assuming<br />

that the distributions are symmetric. The optimal flow is<br />

f =(2, 0, 0, 0, 2, 2, 1, 1) T ,<br />

with a cost <strong>of</strong> 18.<br />

Although the Edmundson–Madansky distribution is very useful, it still has<br />

the problem that the objective function must be evaluated in an exponential

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