8/12/2019 Traverse Computations

1/42

8/12/2019 Traverse Computations

2/42

8/12/2019 Traverse Computations

3/42

8/12/2019 Traverse Computations

4/42

8/12/2019 Traverse Computations

5/42

8/12/2019 Traverse Computations

6/42

8/12/2019 Traverse Computations

7/42

8/12/2019 Traverse Computations

8/42

8/12/2019 Traverse Computations

9/42

8/12/2019 Traverse Computations

10/42

8/12/2019 Traverse Computations

11/42

8/12/2019 Traverse Computations

12/42

8/12/2019 Traverse Computations

13/42

8/12/2019 Traverse Computations

14/42

8/12/2019 Traverse Computations

15/42

8/12/2019 Traverse Computations

16/42

8/12/2019 Traverse Computations

17/42

8/12/2019 Traverse Computations

18/42

8/12/2019 Traverse Computations

19/42

8/12/2019 Traverse Computations

20/42

8/12/2019 Traverse Computations

21/42

8/12/2019 Traverse Computations

22/42

8/12/2019 Traverse Computations

23/42

8/12/2019 Traverse Computations

24/42

8/12/2019 Traverse Computations

25/42

8/12/2019 Traverse Computations

26/42

8/12/2019 Traverse Computations

27/42

8/12/2019 Traverse Computations

28/42

8/12/2019 Traverse Computations

29/42

8/12/2019 Traverse Computations

30/42

8/12/2019 Traverse Computations

31/42

8/12/2019 Traverse Computations

32/42

8/12/2019 Traverse Computations

33/42

8/12/2019 Traverse Computations

34/42

8/12/2019 Traverse Computations

35/42

8/12/2019 Traverse Computations

36/42

8/12/2019 Traverse Computations

37/42

8/12/2019 Traverse Computations

38/42

8/12/2019 Traverse Computations

39/42

8/12/2019 Traverse Computations

40/42

8/12/2019 Traverse Computations

41/42

8/12/2019 Traverse Computations

42/42