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Rock Climbing and Differential Equations: The Fall-Factor Dr. Dan Curtis Central Washington University.

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Presentation on theme: "Rock Climbing and Differential Equations: The Fall-Factor Dr. Dan Curtis Central Washington University."— Presentation transcript:

1 Rock Climbing and Differential Equations: The Fall-Factor Dr. Dan Curtis Central Washington University

2 Based on my article: “Taking a Whipper : The Fall-Factor Concept in Rock-Climbing” The College Mathematics Journal, v.36, no.2, March, 2005, pp. 135-140.

3 Climbers use ropes and protection devices placed in the rock in order to minimize the consequences of a fall.

4

5

6

7 Intuition says: The force exerted on the climber by the rope to stop a long fall would be greater than for a short fall.

8 Intuition says: The force exerted on the climber by the rope to stop a long fall would be greater than for a short fall. According to the lore of climbing, this need not be so.

9 belayer climber protection point

10 belayer climber protection point

11 belayer climber protection point

12 L = un-stretched length of rope between climber and belayer.

13 DFDF DTDT

14 The Fall-Factor is defined as the ratio D T / L

15 The Fall-Factor is defined as the ratio D T / L Climbing folklore says: The maximum force exerted by the rope on the climber is not a function of the distance fallen, but rather, depends on the fall-factor.

16 Fall-factor about 2/3

17 Fall-factor 2 belay point

18 0 x DFDF DTDT position at start of fall position at end of free-fall position at end of fall

19 During free-fall

20

21

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23 whenso

24 whenso

25 whenso When

26 whenso When After the rope becomes taut, the differential equation changes, since the rope is now exerting a force.

27

28 The solution is

29 Maximum force felt by the climber occurs when and

30 Maximum force felt by the climber occurs when and

31 The maximum force is given by


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