Reed Thorne

“A Young Persons Guide to Tracking
Elements in Offsets and Highlines”
Presented by:
Reed Thorne
“A Young Persons Guide to Tracking Elements
in Offsets and Highlines”
Many times I am asked when a track line becomes a tracking line or a guiding line.
While the answer is not cut and dry, nor black and white, there are things going on in
the tracking elements that bear mention. This presentation goes into a diagrammatic
explanation using force vector analysis of steep highlines and the subtle symbiosis
as it were between the upper tag line and the track line. As the highlines track line
increases in steepness the tracking elements tensile force drops off significantly
until it becomes basically a tracking line or guiding line within the realm of the high
angle offset (see presentation #1). Conversely, as the highline becomes less steep it
takes on more of the tension force between the anchors and the tag lines see less
and less. In the case of a horizontal highline, this can then explain why we see more
force in the centre of a highline than at each end as we begin to see the taglines
holding some of this whilst the suspended mass is near each side.
This presentation will provide some informative base line understanding and critical
thinking on what is going on with respect to tracking element tension at various
angles within highlines and high angle offsets.
About the Presenter
Reed Thörne grew up in Southern California where he became involved with the
Sierra Club Rock Climbing and Mountaineering Sections as an instructor/leader. He
now runs Ropes That Rescue Ltd., a rigging school in the rugged highland regions
of northern Arizona near the town of Sedona. RTR teaches roped disciplines
including rope rescue, rope access and general rigging to emergency providers and
industry however, their specialty is energized power transmission line rescue. RTR’s
work was featured in the History Channel “Suicide Missions” special HIGH
VOLTAGE in 2000 with Georgia Power Company. Reed comes from a 1970’s
California lineman background where he learned rigging from various master
mechanics of the trade. Later, after moving to Arizona with his wife in 1979, Reed
became involved with Butch “Charles” Farabee or the National Park Service who
worked at the Grand Canyon National Park in the early 80’s. Beginning in 1981,
Reed became instrumental in the foundation of the Sedona Fire Department
Mountain Rescue Team and eventually Battalion Chief for the Special Ops Section
(helicopter, swiftwater and rope rescue). For one week in 1989, Reed, John Dill or
Yosemite SAR, and Arnor Larson of the BCCTR performed the “Sedona Drop Tests”
at the Sedona Fire Department. These tests formed some of the initial foundation for
the use of the tandem prusik belay around the world today.
Reed Thorne regularly holds rigging and rescue programs in the USA, Canada,
Australia and New Zealand each year. At this years ITRS, RTR has three of its
instructors attending: Len Batley from Australia, Kevin Frye from Los Angeles
County Fire, Dave Van Holstyn from Grand Rapids (MI) Fire and Eric Ulner from
Vertical Heartland Climbing School.
Presentation #2 for the 2007
International Technical Rescue Symposium
A Young Persons Guide to
Tracking Elements in
Offsets and Highlines
A Presentation by Reed Thorne
1
A Young Persons Guide to
Tracking Elements in Offsets and Highlines
By Reed Thorne: Ropes That Rescue Ltd. Sedona, AZ USA
Many times I am asked when a track line becomes a tracking line or a guiding line.
While the answer is not cut and dry, nor black and white, there are things going on
in the tracking elements that bear mention. This presentation goes into a
diagrammatic explanation using force vector analysis of steep highlines and the
subtle symbiosis as it were between the upper tag line and the track line. As the
highlines track line increases in steepness the tracking elements tensile force drops
off significantly until it becomes basically a tracking line or guiding line within the
realm of the high angle offset (see my presentation #3). Conversely, as the highline
becomes less steep it takes on more of the tension force between the anchors and
the tag lines see less and less. In the case of a horizontal highline, this can then
explain why we see more force in the centre of a highline than at each end as we
begin to see the taglines holding some of this whilst the suspended mass is near
each side.
This presentation will provide some informative base line understanding and critical
thinking on what is going on with respect to tracking element tension at various
angles within highlines and high angle offsets.
2
k
Trac
Line
ine
L
Tag
per
Up Line
lay
Be
Track Lines:
Force delivered by mass is shared
between the main line and the
track line
Carriage
100 kg
Lo
we
rT
ag
Tr
a
ck
Lin
e
Lin
e
3
k
Trac
Line
ine
L
Tag
per
Up Line
lay
Be
Track Lines:
Force delivered by mass is shared
between the main line and the
track line
Carriage
100 kg
1000 N
force vector
Lo
we
rT
ag
Tr
a
ck
Lin
Lin
e
e
4
k
Trac
Tag
per
Up Line
lay
Be
Line
e
Lin
1000 N
force vector
Carriage
100 kg
1000 N
force vector
Lo
we
rT
ag
Tr
a
ck
Lin
Lin
e
e
5
k
Trac
Line
ine
L
Tag
per
Up Line
lay
Be
1000 N
force vector
Carriage
1000 N
force vector
100 kg
Lo
we
rT
ag
Tr
a
ck
Lin
e
Lin
e
6
k
Trac
Line
ine
L
Tag
per
Up Line
lay
Be
1000 N
force vector
550 N
force vector
Carriage
100 kg
1000 N
force vector
Lo
we
rT
ag
Tr
a
ck
Lin
Lin
e
e
7
k
Trac
Tag
per
Up Line
lay
Be
Line
e
Lin
1450 N
force vector
1000 N
force vector
550 N
force vector
Carriage
100 kg
1000 N
force vector
Lo
we
rT
ag
Tr
a
ck
Lin
Lin
e
e
8
k
Trac
Line
ine
L
Tag
per
Up Line
lay
Be
1450 N
force vector
Must
Be
Equal
1000 N
force vector
550 N
force vector
100 kg
Tension on one side of a pulley must
be the same on the other
Lo
we
rT
ag
Tr
a
ck
Lin
e
Lin
e
9
k
Trac
Line
ine
L
Tag
per
Up Line
lay
Be
1450 N
force vector
Must
Be
Equal
1000 N
force vector
550 N
force vector
1450 N
– 550 N
100 kg
Lo
we
rT
ag
Tr
a
ck
Lin
Lin
e
e
10
k
Trac
e
Lin
Line
Tag
per
Up Line
lay
Be
1450 N
force vector
Must
Be
Equal
1000 N
force vector
900 N
force vector
550 N
force vector
1450 N
– 550 N
100 kg
= 900 N
Lo
we
rT
ag
Tr
a
ck
Lin
Lin
e
e
11
k
Trac
Line
ine
L
Tag
per
Up Line
lay
Be
550 N
force vector
Now are
Equal!
1000 N
force vector
900 N
force vector
550 N
force vector
100 kg
Lo
we
rT
ag
Tr
a
ck
Lin
e
Lin
e
12
k
Trac
Line
ine
L
Tag
per
Up Line
lay
Be
Track Lines:
As angle increases, track line
force increases
Carriage
100 kg
Tr
a
ck
Lin
e
13
k
Trac
Tag
per
Up Line
lay
Be
Line
e
Lin
Track Lines:
As angle increases, track line
force increases
Carriage
100 kg
Tr
a
ck
Lin
e
14
k
Trac
Line
ine
L
Tag
per
Up Line
lay
Be
Track Lines:
As angle increases, track line
force increases
Carriage
BEWARE!
100 kg
w
Ne
ck
a
Tr
eP
Lin
n
itio
os
15
k
Trac
Line
ine
L
Tag
per
Up Line
lay
Be
Carriage
100 kg
1000 N
force vector
ine
kL
ac
Tr
16
k
Trac
Tag
per
Up Line
lay
Be
Line
e
Lin
1000 N
force vector
Carriage
1000 N
force vector
100 kg
ck
a
Tr
e
e
Lin
Lin
18
ine
L
Tag
per
Up Line
lay
Be
17
1000 N
force vector
Carriage
1000 N
force vector
100 kg
k
ac
Tr
ine
L
Tag
per
Up Line
lay
Be
1000 N
force vector
Carriage
950 N
force vector
1000 N
force vector
100 kg
kL
ac
Tr
ine
19
Tag
per
Up Line
lay
Be
e
Lin
1850 N
force vector
1000 N
force vector
Carriage
950 N
force vector
1000 N
force vector
100 kg
ck
a
Tr
Lin
e
20
ine
L
Tag
per
Up Line
lay
Be
1850 N
force vector
Must
Be
Equal
1000 N
force vector
Carriage
950 N
force vector
100 kg
k
ac
Tr
e
Lin
21
ine
L
Tag
per
Up Line
lay
Be
1850 N
force vector
Must
Be
Equal
1000 N
force vector
Carriage
950 N
force vector
1850 N
– 950 N
100 kg
kL
ac
Tr
ine
22
Tag
per
Up Line
lay
Be
e
Lin
1850 N
force vector
Must
Be
Equal
1000 N
force vector
900 N
force vector
950 N
force vector
1850 N
– 950 N
100 kg
= 900 N
ck
a
Tr
Lin
e
23
ine
L
Tag
per
Up Line
lay
Be
950 N
force vector
Now are
Equal!
1000 N
force vector
900 N
force vector
950 N
force vector
100 kg
k
ac
Tr
e
Lin
24
Compare Forces?
1000 N
force vector
1000 N
force vector
900 N
force vector
900 N
force vector
950 N
force vector
550 N
force vector
25
Compare Forces?
Upper taglines: Tension remains
relatively constant
1000 N
force vector
1000 N
force vector
900 N
force vector
900 N
force vector
950 N
force vector
550 N
force vector
26
Compare Forces?
Trackline: Tension increases
with greater angle
1000 N
force vector
1000 N
force vector
900 N
force vector
900 N
force vector
950 N
force vector
550 N
force vector
Really, this is the inherent difference between
steep highlines and the tracking line offset....
27
comparisons w/offsets
28
comparisons w/offsets
Guiding Lines
Tracking Lines
Steep Highlines
29
l)
ine
na
kL
tio
ac
Tr Line (op
g
ne
Ta Li
lay
Be
Line
king
Trac Line
Main ine
yL
Bela
Line
Guiding e
in
Main L e
Lin
Belay
Principle differences between
the Offsets and the Highline
Tension Differences in
Guiding, Tracking and
Track lines
Ta
g
Guiding Line
Tracking Line
Steep Highline
Li
ne
30
ine
ine
ine
ing L
kL
ac
Tr
k
Trac
L
Guiding
Guiding Line
Principle differences between
the Offsets and the Highline
Tension Differences in
Guiding, Tracking and
Track lines
Tracking Line
Steep Highline
31
l)
ine
na
kL
tio
ac
Tr Line (op
g
ne
Ta Li
lay
Be
Line
king
Trac Line
Main ine
yL
Bela
Line
Guiding e
in
Main L e
Lin
Belay
Principle differences between
the Offsets and the Highline
Tension Differences in
Main Lines and Upper
Tagline
Ta
g
Guiding Line
g
Ta
Main
e
Lin
Line
ine
Main L
Guiding Line
Tracking Line
Steep Highline
Li
ne
32
Principle differences between
the Offsets and the Highline
Tension Differences in
Main Lines and Upper
Tagline
Tracking Line
Steep Highline
33
l)
ine
na
kL
tio
ac
Tr Line (op
g
ne
Ta Li
lay
Be
Line
king
Trac Line
Main ine
yL
Bela
Line
Guiding e
in
Main L e
Lin
Belay
Doubled longtailed bowline
Optional guiding
line tether
Principle differences between
the Offsets and the Highline
Doubled longtailed bowline with
belay, otherwise
single long-tailed
bowline
Single long-tailed
bowline
Ta
g
Guiding Line
Tracking Line
Steep Highline
l)
ine
na
kL
tio
ac
Tr Line (op
g
ne
Ta Li
lay
Be
Line
king
Trac Line
Main ine
yL
Bela
Line
Guiding e
in
Main L e
Lin
Belay
Kootenay
Carriage
Ta
g
Tracking Line
34
Principle differences between
the Offsets and the Highline
Small Pulley
Guiding Line
Li
ne
Steep Highline
Li
ne
35
comparisons w/offsets
Two rope Offsets
Drooping Highlines
36
Principle differences between
ft
the Offsets and the Highline
Le
M
ft
ain
Be
Lin
lay
At mid-span
e
Le
Lin
e
tM
gh Be
i
R ht
g
Ri
Tr Offset
Two Rope
ac
k
Lin
Le
e
Lin e
Lin
lay
ain
ine
kL
c
a
e
Tr
lin
ag
T
t
gh
Ri
e
ft T
ag
li
ne
Drooping Highline
37
Principle differences between
ft
the Offsets and the Highline
Le
M
ft
ain
Be
Lin
lay
At mid-span
e
Le
Lin
e
Two Rope Offset
Tr
ac
kL
ft T
ine
ag
lin
e
Drooping Highline
e
Lin e
Lin
lay
tM
gh Be
i
R ht
g
Ri
Multi directional
ring with doubled
long-tailed
bowlines each
side
Le
ain
ine
kL
c
a
e
Tr
lin
ag
T
t
gh
Ri
Single long-tailed
bowlines each
side
Kootenay
Carriage
Two Rope Offset
Lef
tM
a
Lef
t Be in Lin
lay
e
Line
Tra
c
Left
kL
ine
Tag
li
Rig
Principle differences between
the Offsets and the Highline
Near each station
Rig Rig
T
ht B ht M
ht T rack
ela
agl Lin
y L ain Li
ine e
ine ne
38
ne
Drooping Highline
39