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The Bungee Jump: potential energy at work

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Title: The Bungee Jump: potential energy at work


1
The Bungee Jump potential energy at work
  • AiS Challenge
  • Summer Teacher Institute
  • 2002
  • Richard Allen
  • ?

2
Bungee Jumping a short history
  • The origin of bungee jumping is quite recent, and
    probably related to the centuries-old,
    ritualistic practices of the "land divers" of
    Pentecost Island in the S Pacific.
  • In rites of passage, young
    men jump hundreds of feet,
    protected only by tree vines
    attached to their ankles

3
A Short History
Modern Bungee jumping began with a four-man team
from the Oxford Univ. Dangerous Sports Club
jumping off the Clifton Suspension Bridge in
Bristol, England, on April 1, 1979 dressed in
their customary top hat and tails
4
A Short History
  • During the late 1980's A.J. Hackett opened up the
    first commercial jump site in New Zealand and to
    publicize his site, per-formed an astounding
    bungee jump from the Eiffel Tower!
  • Sport flourished in New Zealand and France during
    1980s and brought to US by John and Peter
    Kockelman of CA in late 1980s.

5
A Short History
  • In 1990s facilities sprang up all over the US
    with cranes, towers, and hot-air balloons as
    jumping platforms.
  • Thousands have now experienced the ultimate
    adrenaline rush.
  • The virtual Bungee jumper

6
Bungee Jump Geometry
L (cord free length)

d (cord stretch length)
Schematic depiction of a jumper having fallen a
jump height, L d.
7
Potential Energy
  • Potential energy is the energy an object has
    stored as a result of its position, relative to a
    zero or equilibrium position.
  • The principle physics components of bungee
    jumping are the gravitational potential energy of
    the bungee jumper and the elastic potential
    energy of the bungee cord.

8
Examples Potential Energy
9
Gravitational Potential Energy
  • An object has gravitational potential energy if
    it is positioned at a height above its zero
    height position PEgrav mgh.
  • If the fall length of the bungee jumper is L
    d, the bungee jumper has gravitational
    potential energy,
  • PEgrav mg(L d)

10
Treating the Bungee Cord as a Linear Spring
  • Springs can store elastic potential energy
    resulting from compression or stretching.
  • A spring is called a linear spring if the amount
    of force, F, required to compress or stretch it a
    distance x is proportional to x F kx where
    k is the spring stiffness
  • Such springs are said to obey Hookes Law

11
Elastic Potential Energy
  • An object has elastic potential energy if its in
    a non-equilibrium position on an elastic medium
  • For a bungee cord with restoring force, F
    kx, the bungee jumper, at the cords limiting
    stretch d, has elastic potential energy,
  • PEelas F(0) F(d)/2d
  • 0 kd /2d kd2/2

12
Conservation of Energy
  • From energy considerations, the gravitational
    potential energy of the jumper in the initial
    state (height L D) is equal the elastic
    potential energy of the cord in the final state
    (bottom of the jump) where the jumpers velocity
    is 0
  • mg(L d) kd2/2
  • Gravitational potential energy at the top of the
    jump has been converted to elastic potential
    energy at the bottom of the jump.

13
Equations for d and k
  • When a given cord (k, L) is matched with a
    given person (m), the cords stretch length (d)
    is determined by
  • d mg/k m2g2/k2 2mgL/k1/2.
  • When a given jump height (L d) is matched
    with a given person (m), the cords stiffness (k)
    is determined by
  • k 2(mg)(L d)/d2.

14
Example a firm bungee ride
  • Suppose a jumper weighing 70 kg (686 N,154
    lbs) jumps using a 9m cord that stretches 18m.
    Then
  • k 2(m g) (L d)/d2 2 (7 0 9.8)
    (27/182) 114.3 N/m (7.8 lbs/ft)
  • The maximum force, F kx, exerted on the
    jumper occurs when x d
  • Fmax 114.3 N/m 18 m 2057.4 N (461.2
    lbs),
  • This produces a force 3 times the jumper
    weight
  • 2057.4N/686N 3.0 gs

15
Example a softer bungee ride
  • If the 9m cord stretches 27m (3 times its
    original length), its stiffness is
  • k 2(709.8)(36/272) 67.8 N/m (4.6
    lbs/ft)
  • producing a maximum force of
  • Fmax (67.8 N/ m)(27 m) 1830.6 N (411.5
    lbs)
  • This produces a force 2.7 times the jumpers
    weight,
  • 1830.6 N/686 N 2.7 gs,
  • and a softer ride.

16
Extensions
  • Incorporate variable stiffness in the bungee
    cord in practice, cords generally do not behave
    like linear springs over their entire range of
    use.
  • Add a static line to the bungee cord customize
    jump height to the individual.
  • Develop a mathematical model for jumpers position
    and speed as functions of time incorporate drag.

17
Work To Stretch a Piecewise Linear Spring
18
Evaluation
  • In designing a safe bungee cord facility, what
    issues must be addressed and why?
  • Formulate a hypothesis about the weight of the
    jumper compared to the stretch of
    the cord as the jumpers weight
    increases. Design an experiment to
    test your hypothesis.

19
Reference URLs
  • Constructivism and the Five E's
  • http//www.miamisci.org/ph/lpintro5e.html
  • Physics Teacher article on bungee jumping
    http//www.bungee.com/pressmore/press/pt.html
  • Hookes Law applet
  • www.sciencejoywagon.com/physicszone/lesson/02force
    s/hookeslaw.htm

20
Reference URLs
  • Jumpers weight vs stretch experiment
  • http//www.uvm.edu/vsta/sample11.html
  • Ultimate adrenalin rush movie
  • http//www-scf.usc.edu/operchuc/bungy.htm
  • Potential energy examples
  • www.glenbrook.k12.il.us/gbssci/phys/Class/energy/u
    5l1b.htm
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