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event B or in uences the way B happens, or (2) knowing the value of A changes the probability or probability distribution of B (i.e. A and B are probabilistically dependent, and A or the knowledge of A occurs rst in time). Two events A and B can be probabilistically correlated and yet not be joined by a directed arc, for example, if they share common dependence upon some third variable C (Figure 20.11). Knowing the value of C, the uncertainties A and B are assumed probabilistically independent in this in uence diagram (because they are not directly joined by an arc); but if C is unknown, A and B are probabilistically dependent, because each depends on the realization of C. Two events A and B can also be statistically correlated and yet not joined by a directed arc, for example, if estimates of their values are based on the same set of experimental observations. Estimating the Mohr-Coulomb strength parameters c and from a single set of tests introduces correlation because the parameters are effectively regression coef cients.

If you look closely at the address that the JMP at 004041F4 is going to you ll notice that it s very far from where you are at the moment right at the beginning of this function actually. To refresh your memory, here s the code at that location:

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You may or may not remember this, but the line immediately preceding 00403401 was setting [EBP-8] to 1, which seemed a bit funny considering it was immediately checked. Well, here s the answer there is encrypted code at the end of the function that sets this variable to zero and jumps back to that same position. Since the conditional jump is taken this time, you land at 40346D, which is a sequence that appears to be very similar to the decryption sequence you studied in the beginning. Still, it is somewhat different, and observing its effect in the debugger reveals the obvious: it is reencrypting the code in this function. There s no reason to get into the details of this logic, but there are several details that are worth mentioning. After the encryption sequence ends, the following code is executed:

Downwind, your tactics as the lead boat are usually heavily dictated by the boat behind you. Often it is simpler to try and keep your air clean and sail as fast as you can! Where possible, encourage those boats around you to work with you to get away

The typical procedure for creating an in uence diagram is: 1. Identify the events and uncertain quantities whose outcomes could be important to the safety of the system. 2. For each uncertain quantity, assign a name and a unit of measure; if decision variables are involved, de ne speci c, quantitative alternatives. 3. Identify in uences or dependencies among the uncertain quantities, and between each decision and each uncertain quantity; then represent each uncertain quantity and each decision by a node in a graph, aligning them in order of occurrence, if time is relevant. 4. Assign directed arcs among uncertainty nodes and between decision and uncertainty nodes, with the direction of the arcs indicating the direction of presumed in uence. 5. In constructing the in uence diagram, there should be no closed loops or cycles among the nodes. That is, there should be no connected path along the directed arcs that leads back to an earlier node. We earlier introduced the system states and uncertainties associated with a simple oodway levee. These can be combined in an in uence diagram to begin to show the interrelationship among the various elements and considerations in beginning a risk analysis of the levee. A rst attempt at such an in uence diagram is shown in Figure 20.12. This diagram consists both of system states and uncertainties affecting those states.

004034D0 004034D5 004034DA 004034DB MOV DWORD PTR DS:[406008],EAX PUSH Defender.004041FD POP EBX JMP EBX

The first line saves the value in EAX into a global variable. EAX seems to contain some kind of a checksum of the encrypted code. Also, the PUSH, POP, JMP sequence is the exact same code that originally jumped into the decrypted code, only it has been modified to jump to the end of the function.

Figure 20.12 In uence diagram for levee failure. (Canadian Electricity Association, Guide to Dam Safety Risk Management, forthcoming.)

After the huge function you ve just dissected returns, the entry point routine makes the traditional call into NtDelayExecution and calls into another internal function, at 404202. The following is a full listing for this function:

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