RESULTS
Reconstructed topography of pneumatic diverticula in sauropod necks
The distribution of pneumatic diverticula in
sauropod necks has been reconstructed in detail for Sauroposeidon,
Brachiosaurus, diplodocids and dicraeosaurids (Wedel et al. 2000;
Wedel and
Cifelli 2005;
Schwarz and Fritsch 2006;
Schwarz et al. 2007). The topography of osteological correlates for pneumatic diverticula is similar in these and other
sauropods, suggesting a similar distribution of pneumatic diverticula. The
following pneumatic diverticula subsystems are likely to have been present in
all eusauropods (Figure 3): lateral vertebral diverticula (LVDv) laterally
adjacent to the vertebral bodies, infradiapophyseal diverticula (IDDv) ventral
to the diapophyses, infrapostzygapophyseal diverticula (IPDv) ventral to the
postzygapophyses, lateral spinal diverticula (LSDv) lateral to the neural arch
and neural spine, supravertebral diverticula (SVDv) cranial and caudal to the
neural spines, and supramedullary diverticula (SMDv) within the neural canal
(Wedel et al. 2000;
Wedel 2005;
Schwarz and Fritsch 2006;
Schwarz et al. 2007).
Size and depth of the pneumatic fossae and
foramina in the lateral surface of the vertebral bodies, and comparisons with
extant birds indicate large LVDv along the entire lateral surface of the
cervical centra (Figure 3). The LVDv passed through the intertransversal
foramina, forming a lateral vertebral pneumatic diverticula system similar to
the canalis intertransversarius in birds (Müller 1908;
Landolt and Zweers 1985).
The lumen of the intertransversal foramina was most likely completely occupied
by pneumatic diverticula, therefore the diameters of these foramina hint to the
cross-section of the whole unit of LVDv. The LVDv were laterally bounded by the
cervical ribs, connective tissue, and lateral epaxial and laterocostal cervical
muscles, which inserted on the diapophyses and cervical ribs (Wedel and Sanders
2002;
Schwarz et al. 2007). Like in birds (Müller 1908;
Duncker 1971;
O'Connor
2006), the pneumatic diverticula of sauropods were most probably connected with
each other by a network of pneumatic ducts, although fossil evidence for
pneumatic ducts is rare (Wedel et al. 2000). Pneumatic fossae in the external
vertebral surface of many sauropod taxa, such as Diplodocus,
Apatosaurus, Barosaurus, Camarasaurus or Brachiosaurus,
are internally divided into subfossae, which indicates a segmentation of the
respective pneumatic diverticula into subunits (Wilson 1999;
Wedel 2005). Most
likely, these diverticula anastomozed at least occasionally with one another,
similar to birds (O'Connor 2006). It is likely that corresponding to extant
birds, adjacent pneumatic diverticula were bundled together to "aggregates of
narrow tubes rather than large, simple sacs" (Wedel 2003a,
figure 5 caption).
Rare pneumatic foramina and depressions on the medial surface of the
metapophyses and within the postspinal cavity of the cervical vertebrae indicate
that SVDv filled the gap between these metapophyses and the postspinal cavity,
respectively (Figure 3.2-3.3) (Schwarz and Fritsch 2006;
Schwarz et al. 2007).
In sauropods with single neural spines in the neck, pneumatic diverticula formed
large evulsions in the interarticular gaps, as is seen in extant birds (Müller
1908; Britt 1993;
O'Connor 2001;
Wedel 2003a;
O'Connor 2006). Median tuberosities within the postspinal cavity and between the metapophyses of
bifurcate neural spines provide osteological evidence for large elastic
ligaments inserting cranially and caudally on the neural spines of sauropods
(Tsuihiji 2004;
Schwarz et al. 2007). Therefore, pneumatic diverticula between
the metapophyses and within the postspinal cavity must have been medially in
direct contact with these elastic ligaments, proliferating around the latter
(Figure 3.2-3.3). Additionally, thin laminae on the cranial and caudal margin of
the metapophyses, and the well-developed postzygapophyseal laminae suggest the
presence of a paired interspinal septum like in extant Crocodylia (Frey 1988a;
Schwarz et al. 2007). Between single neural spines, the left and right sheet of
the interspinal septum probably enclosed the elastic ligament and the SVDv,
which both filled also the postspinal fossa (Schwarz and Fritsch 2006;
Schwarz et al. 2007). In bifurcate neural spines, the interspinal septum probably
adjoined the SVDv around the elastic ligaments and dorsally contacted the
supraspinal ligament. Such an arrangement of spinal ligament sheaths would have
provided a hose-like envelope for the dorsal pneumatic diverticula. The width of
the area between the metapophyses indicates the volume of the SVDv including
their ligamentary envelope.
According to the distribution of pneumatic
diverticula along the neck of sauropods, a tripartite arrangement can be
distinguished from a dual one (Figure 3). Sauropods with a tripartite
arrangement of pneumatic diverticula have bifurcate neural spines in at least
half the cervical vertebrae, such as Apatosaurus, Diplodocus,
Dicraeosaurus or Amargasaurus. In the area of bifurcate neural
spines, the entity of SVDv formed a dorsal median pneumatic canal around the
elastic ligaments (Figure 3.2). Additionally, a pair of LVDv units at the
vertebral centra, assembled in an intertransversar canal, would have been
present. In sauropods with a dual arrangement of pneumatic diverticula,
bifurcate neural spines occurred in less than half of the cervical vertebrae,
like in Camarasaurus, or were completely missing like in
Mamenchisaurus or Euhelopus. In the first case, single SVDv formed a
dorsal pneumatic canal in the caudal region of the neck only (Figure 3.3). In
the second case, SVDv filled the interarticular space and the postspinal cavity.
Similar to the tripartite arrangement, the LVDv formed a paired, voluminous,
hose-like intertransversar canal.
Results of the Experiment - Pneumatic Stabilization of a Chain Beam
The experiment was carried out with those
configurations of balloons corresponding to the arrangement of pneumatic
diverticula reconstructed for sauropod necks. Each experimental approach (E1-E8)
followed a specific question that is outlined below. In the following
description, proximal refers to the end of the chain fixed at the pivot board,
whereas distal refers to the opposite end bearing the plastic cup with iron
powder. The sagging index (si; in mm) indicates the holding point
of the distal end of the chain beam aboveground in a vertical plane. The
bending index (bi; in mm) is the dislocation of the distal end of the
chain beam from the straight line in a horizontal plane.
E1: Calibration of the unbraced chain beam.
Objective: What is the maximum si of the system without pneumatic bodies and
with other bracing elements?
As a calibration base for all following
experiments, the intrinsic curvature of the system with and without a bracing
element was determined. The chain beam was fixed with its proximalmost segment
at the pivot board and loaded by its own weight in the absence of any bracing
structure. The chain beam hung vertically down in its basal joint (Figure 4.1).
A small intersegmental wedge of Styrodur™ was then placed in the gap between
each segment. This arrangement yielded an intrinsic curvature siE1 of the
chain beam, which was 265 mm above-ground (Figure 4.2). For all following
experiments, siE1 represents the intrinsic reference curvature of the
plain coil chain with a bracing element.
E2: One median ventral pneumatic tube
Objective 1: What is the bracing and deformation effect of one median ventral
pneumatic tube?
One inflated balloon with a pressure of 0.15 bar
was tied with gauze bandages ventral to the chain beam. The si of the
chain beam with this arrangement was 370 mm. The curvature of the beam was
strongest between both proximalmost segments, whereas the other segments formed
nearly a straight line (Figure 5.1). At an increase of the pressure to 0.3 bar,
the chain beam curved slightly dorsally (Figure 5.2). In contrast, the decrease
of the pressure to 0.1 bar resulted in a sagging of the chain beam with the
balloon buckling up between the two proximal segments. The insertion of a
ventral intersegmental wedge between both proximalmost segments resulted in the
curvature siE1 at a pressure of 0.1 bar.
Objective 2: How does the median ventral pneumatic tube influence the load
capacity of the chain beam and what effect has a pressure increase to the load
capacity?
An empty cup was attached to the distal end of
the chain beam and filled with iron powder until siE1 was reached. No
ventral intersegmental wedges were used. At a pressure of 0.15 bar, 45 g of iron
powder was necessary to produce siE1, which is 122.5% of the weight of
the chain beam itself. At a pressure of 0.25 bar, 230 g of iron powder was
necessary to deflect the chain to siE1 (Figure 5.3). This corresponds to
215% of the weight of the chain beam. As a result, a pressure increase of 0.1
bar only increased the load capacity of the system by five times. In both load
cases, the chain beam tended to twist around its long axis due to torque
moments.
E3: One pair of ventral or lateral pneumatic tubes
Objective 1: What is the bracing effect with a pair of lateral or ventral
pneumatic bodies respectively?
Two inflated balloons were tied with gauze
bandage lateral to each side of the chain beam. The lateral arrangement of the
balloons yielded no support effect for the chain beam, which sagged completely
(Figure 6.1). The two inflated balloons were then tied ventral to the chain
beam. This configuration yielded a si of 410 mm (Figure 6.2), which is
10% less than with one ventral balloon. With the ventral pair of balloons, the
chain beam was stable with respect to torque.
Objective 2: How does the configuration influence the load capacity of the chain
beam?
An empty cup was attached to the distal end of
the chain beam and filled with iron powder until the curvature siE1 was
reached. At a pressure of 0.15 bar, 80g of iron powder were needed to reach
siE1, corresponding to 140% of the weight of the chain beam.
E4: One pair of ventral and a median dorsal pneumatic tube
Objective 1: What is the bracing effect with two ventral and one dorsal
pneumatic body?
Two inflated balloons were tied ventral and one dorsal to the chain beam with
gauze bandages. The pressure in all balloons was 0.15 bar. The tripartite
arrangement of pneumatic bodies led to a si of 435 mm aboveground. The
dorsally positioned balloon was under tension, whereas the two ventral balloons
were under pressure and pushed proximally towards the pivot board (Figure 7.1).
When an intersegmental wedge was inserted ventrally between the two proximal
segments (Figure 7.2), the si decreased to 475 mm.
Objective 2: How does the configuration influence the load capacity of the chain
beam?
An empty cup was attached to the distal end of the chain beam and filled with
iron powder until siE1 was reached. The pressure of the balloons was 0.15
bar, and no intersegmental wedge was inserted. With this arrangement, 54 g of
iron powder were necessary to achieve siE1 (Figure 7.3), corresponding to
127% of the inertial weight of the chain beam. Inserting an intersegmental wedge
ventrally between the two proximal segments increased the load capacity to bear
136 g until reaching siE1, which is 168% of the inertial weight of the
chain beam.
E5: One median dorsal pneumatic tube
Objective 1: What is the bracing effect with one dorsal pneumatic body?
One balloon was tied to the dorsal side of the chain beam with gauze bandages,
but not fixed at its proximal end. The unfixed balloon generated no bracing
effect, instead, the chain beam sagged (Figure 8.1), and the balloon was drawn
in a distal direction (Figure 8.2). The balloon was then fixed at its proximal
end with a clothespin (8.3). With this arrangement, the chain beam exposed a
si of 265 mm (Figure 8.4), similar to siE1. The dorsal balloon was
tensed proximally, but distally kept the segmented chain in a straight line.
Following, the combination of a ventral intersegmental wedge and a proximal
fixation of the balloon yielded an si of 405 mm (Figures 8.5, 8.6). The
combination of an unfixed dorsal balloon, but a ventral intersegmental wedge
yielded a si of 320 mm aboveground.
Objective 2: How does the configuration influence the load capacity of the chain
beam and what influence has the basal pivot?
An empty cup was attached to the distal end of the chain beam and filled with
iron powder until siE1 was reached. In the arrangement with one ventral
intersegmental wedge and the proximally unfixed balloon with a pressure 0.15
bar, 34 g of iron powder were necessary to achieve siE1. This corresponds
to 117% of the intrinsic weight of the chain beam. In the arrangement with one
ventral intersegmental wedge and an additional proximal fixation of the balloon,
54 g of iron powder were necessary to achieve siE1. This was 127% of the
intrinsic weight of the chain beam. At this load, the balloon buckled
proximally.
E6: One median dorsal or ventral pneumatic tube fixed to the segments
Objective: What is the influence of a segmentally fixed median pneumatic body on
the bracing of the chain beam?
A party balloon was tied to the dorsal side of the chain beam with gauze
bandages and fixed to the segments by a patch of double-sided tape (Figures 9.1,
9.2). The achieved curvature of the chain beam with this arrangement and a
pressure of 0.15 bar was si=405 mm (Figure 9.1). Both proxim almost
segments approached each other (Figure 9.2), and the dorsal balloon bulged at
the articulation between two segments (Figure 9.3).
In a second test, one balloon was tied to the ventral side of the chain beam
with gauze bandages and fixed to the segments by a patch of double-sided tape.
At a pressure of 0.15 bar, the si was 420 mm aboveground (Figure 9.4).
The ventral balloon was compressed, and the chain beam exposed a deflection at
its base only. Distally, the chain beam formed a nearly straight line. Applying
extra load to this system, 115 g of iron powder were necessary to achieve siE1.
This is 157.5% of the weight of the chain beam.
For the third test, the gauze bandages were removed, the balloon being held only
by double-sided tape. This resulted in an si of 350 mm, and 22 g of iron
powder were necessary to produce siE1.
E7: Segmented dorsal pneumatic tube
Objective: How do pneumatic segments connected with each other influence the
bracing of a chain beam?
A balloon was segmented by twisting it according to the distances of the
segments of the chain beam. The balloon was tied to the dorsal side of the chain
beam with a gauze bandage. When the intersegmental parts of the pneumatic tube
were positioned level with the intersegmental gaps of the chain beam, no bracing
effect occurred. When the intersegmental parts of the pneumatic tube were
positioned mediodorsally to the Styrodur™ segments and thus bridged the intersegmental gaps of the
chain beam, the achieved si was 125 mm. By placing ventral intersegmental
wedges between the proximal three segments, the si of the chain beam
increased to 270 mm (Figure 9.5).
E8: Mobility by asymmetrical pressure changes
Objective: Is there an option to move the chain beam pressure increase in one
pneumatic tube in a triple system of pneumatic bodies?
The chain beam was positioned with the belt joints standing vertically to allow
lateral movements. One pair of balloons was tied ventrally and one balloon
dorsally to the chain beam with a gauze bandage. At a pressure of 0.15 bar in
all balloons, the chain beam formed a straight line (Figure 10.1). If the
pressure in the right ventral balloon was increased to 0.25 bar, this resulted
in a bi of 405 mm to the right side (Figures 10.2, 10.3).
|