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Marketing vs. Physics

The truth about axis migration and core dynamics

By Nick Siefers, USBC research engineer



Many theories about why and how a bowling ball rolls down a lane have been discussion
topics within the bowling industry in recent years, including at the United States Bowling
Congress, where a ball motion study is a major research focus.


With key trends appearing in the data, the significant factors that affect bowling ball
motion are becoming scientifically apparent. A separate study relating to how and why
the ball rolls the way it does has been conducted. In the following discussion, an attempt
will be made to explain the physics that govern bowling ball motion relating to core
dynamics.


Of the many theories available to explain the motion of a bowling ball, different
companies take a wide variety of stances on this subject. Several beliefs include the
following:
    1) Core dominates cover
    2) Cover dominates core
    3) Core and cover have a delicate balance with each other
    4) Mass bias strength governs axis migration
    5) Asymmetrical vs. symmetrical cores determine bowling ball motion
    6) RG, differential and cover stock work together to affect the roll
    7) Other(s)


To the average bowler, these different theories provided by the industry can be confusing.
Which one is correct? Is more than one theory useful in determining why a ball rolls as it
does? At the USBC, we set out to discover the truth regarding these theories, as they
relate to core dynamics and the roll of the ball.


Before describing the testing parameters, it is important to understand the facts and
certain physics principles used in this research. First, the radius of gyration (RG) is
defined as the square root of the moment of inertia divided by the mass of the object.
Therefore, the radius of gyration is the distance that, if the entire mass of the object were
together at only that specific radius, would yield the same moment of inertia. The
moment of inertia for an object is the ratio of applied torque and the resultant angular
acceleration of the object. Translating the physics definition, the moment of inertia
measures how easy an object will rotate when a force is applied. Thus, in simple terms,
the radius of gyration determines how easy it is for the bowling ball of particular weight
to rotate about a given axis and is a measurement of where the weight is located inside
the ball, relative to the center. Second, Sir Isaac Newton’s laws of motion state that
energy is neither created nor destroyed, but rather conserved and all matter in the
universe had a natural tendency to go from an unstable state to a stable state in which
forces are balanced. This is called equilibrium. To reverse the process and move from a
stable state to an unstable state whereas forces are not balanced, work or energy must be
added to the system.


With these concepts in mind, when a bowler releases a ball during delivery, the ball will
first begin rotating about what is called his or her positive axis point (PAP). Simply
defined, the positive axis point serves as the initial point of rotation. Then, due to the
influence of ball properties, bowler attributes, lane conditions and the laws of physics
(unstable to stable), new axis of rotation will exist as the ball travels down the lane. This
change from the initial point of rotation to each subsequent point of rotation is called
“Axis Migration.” The migration of axis points can be determined and traced for a bowler
by using an armadillo® to locate the axis of rotation for each flare ring as the ball rolls
down the lane. Each flare ring will have an individual axis that the ball has rotated about
to create that particular flare ring. The armadillo® is able to measure and find the rotation
axis. Thus, for each flare ring, there is an axis point. The migration of axis points can be
plotted on the ball and, depending upon certain characteristics, will yield different shapes
(curved vs. straight line) due to the drilling pattern used. The plots will be at different
distances away from the pin of the bowling ball.


It is at this point, the many theories come into play. In regards to performance, does
having a straight line axis migration path differ than having a curved path? Does an axis
migration path closer to the pin affect the roll different than a path further away from the
pin? Does the ball’s path migrate toward the high RG or Mass Bias spot? Does the ball’s
path migrate toward the low RG or pin? Is the axis migration path dependant upon the
core’s orientation inside the ball? Is the path due to RG differences or similarities? Is the
migration path a combination of any of these theories or does the path not depend on any
of these theories? What does the axis migration path have to do with ball performance at
all? These are some of the questions that have been asked and now for the first time
answers are being found.


In order to dig into these questions, five major types of tests were completed. Several
types of bowling balls, drillings, and bowlers in the USBC Equipment Specifications and
Certification department were selected for measuring axis migration and the results were
used to determine the trends in axis migration. The chart below lists all of the balls that
were tested:

TEST I – Standard and Unconventional Drillings


Test I used both normal/standard and unconventional drillings. The balls used for this test
were all approved for USBC competition prior to drilling (balls nos. 1-19). This first set
of test balls were subject to one of four designed oil patterns ranging from a 38-foot
house pattern to a 44-foot PBA pattern. For each ball tested, the bowler threw enough
shots to accurately portray all possible flare rings in both the oil and dry part of the lane
on the surface of the ball. Each flare ring was then traced with a grease pencil and the
armadillo® was used to locate the axis of rotation. An example of this process is shown
below in Picture 1.


Picture 1: Marking the PAP


Depending on the bowler’s rev rate and actual flare of the ball, different numbers of rings
were traced for each ball. Once the axis migration points were plotted, the path was seen
to be either straight or curved. At this point, the distance of each migration point from the
pin was also recorded. This distance describes the core’s orientation (standing up or
laying down) as the ball traveled down lane. Finally, the RG value about each axis
migration point was measured to investigate the motion of the bowling ball. The RG was
recorded to the third decimal but rounded to the second decimal point, due to the
accuracy of the RG device and process used to measure. The following pictures show a
portion of the different migratory paths that were observed.



Picture 2: Different migratory paths (conventional layouts)



Picture 3: Pin or MB on PAP (unconventional layouts)


The figures below show a graphical representation of each axis point on all balls in all
tests as it relates to distance away from the pin. The next figure shows the RG value for
each axis point.


Figure 2 shows the axis migration as it occurred on the surface of each bowling ball. The
center of the “spider web” graph is labeled 0. Imagine this as being the location of the
pin on the bowling ball. As you move upward the numbers range from 0 to 7 and
represent the distance, in inches, away from the pin. The numbers on the outside portion
of the graph that move in a circular notation represent an individual axis point as the
flared down the lane. Thus, the overall plot is a function of the distance each axis point in
the migratory path is away from the pin.



Figure 3 is the same type of “spider web” graph as previously noted. However, the center
of this graph represents a low RG value of 2.45’’. Moving upward on the chart, the RG
values range from 2.45’’ to 2.58’’. The numbers going around the outside of the graph
are again, just as in Figure 2, representing each axis point in the migratory path as the ball
flares down lane. This figure graphically shows the RG value at each axis point in the
path.


The graphs for Test I show that despite having different distances or migratory paths, a
trend is noticed. The most important overall factor that was consistent through out this
test was noticed:


    “While on the lane, RG values of the migratory path remained
    approximately constant at each migratory axis point for all core geometries
    and drillings.”


Based on the variety of ball tested, an accurate analysis concluded that the axis migration
path was INDEPENDENT (not dependant) of the following:
    1) Core shape
    2) Core angle/orientation
    3) Cover stock
    4) Asymmetry
    5) Symmetry
    6) Mass bias strength/intermediate differential
    7) Spin time
    8) Oil Pattern
    9) Mass Distribution of the Core
    10) Ratio of the Intermediate to Total Differential


Regardless of the above factors, the same trend in axis migration occurred. While the
approved ball is on the lane, the bowling ball flared and created an axis migration to yield
approximately the same RG value that the ball was initially rotating on from the bowlers
PAP.


TEST II – Large Differential Test Ball



Next, in Test II a particular case study was conducted. In this case study, a ball was made
outside the limits of the total differential specification set forth by the USBC (ball no.
23). The maximum allowable limit on differential is currently .060’’. Differential directly
relates to the flare potential of the ball. The test ball was designed to have three times the
legal limit of total differential. The drilling used was 3 3/8’’ (pin to pap) x 4’’ (pap to cg).
After drilling, the low radius of gyration was 2.43’’ and the total differential was .190’’.
This ball also had an intermediate differential of .005’’. Subject to multiple lane
conditions, this test ball flare around the entire ball. Because of the large amount of flare,
a greater axis migration plot was obtained.


In this particular case, as shown in Figure 4 below, the ball initially started rolling around
the bowler’s PAP (green circle). As flaring occurred, the axis of rotation transgressed
through the red circle, then the yellow circle and finally the white circle. Since this ball
was able to flare a great deal more than a standard USBC approved ball, a greater
detailed picture of axis migration was found. As in Test I, the RG values were obtained
for each of the colored axis points. Picture 4 below shows the actual ball and colored
axis migration points.




Picture 4: Large differential test ball


The interesting trend in this test actually coincides with the results of Test I. If this test
ball flared within USBC specifications, the path would start on the green axis point and
end up down lane approximately on the red axis point. After looking at the data, the
green axis and the red axis point exhibit the virtually same RG value, which directly
matches the trend results of Test I. However, since the ball flares more and no energy is
added to the ball as it travels down lane, an important trend it noticed in the subsequent
RG axis points. The RG value at the yellow and white axis points actually decrease
compared to the first two rotation axis. As in Test I, with energy being lost as the ball
rolls down the lane, the migration is controlled by physics and the conservation of
energy. The test ball loses energy and migrates toward a lower energy and lower RG
values. Also as in Test I, the on lane migration does not seek a higher RG state or the
mass bias spot (the highest RG of the ball).


TEST III – High Speed Camera



Test III was conducted on a dry/stripped lane with no oil applied. A high speed camera
was set up at approximately 53 feet down lane to capture the axis migration after the ball
stopped hooking. It is important to understand that friction causes the ball to stop hooking
but axis migration is a function of RPM and total differential RG of the ball. Thus, the
axis of rotation will continue to migrate after the ball has reached its final directional
rolling phase.


Several of the balls in Test I were subject to Test III - high speed camera testing. A few
freeze frame examples are shown below in Pictures 4, 5 and 6. In each of these video
segments, it is certain that the axis of rotation is not the high RG axis of the ball
(regardless of strength of intermediate differential). However, in each video segment, it
can be seen that the axis of rotation is in a region near the low Rg axis of the ball. The
low RG axis is located near the pin, which can be seen in the pictures below. It is the
round/circular dot near the center of the ball in the pictures. This trend, would again,
show the same result as both Test I and II.


Picture 4: Sahara axis of rotation at 53 feet on dry lane


Picture 5: Black MoRich test ball axis of rotation at 53 feet on dry lane


Picture 6: Beetle core test ball axis of rotation at 53 feet on dry lane


TEST IV – Standard Drilling without/with Balance Hole



An Ebonite NVS was used for Test IV. The ball was drilled in a 4 ½’’ x 4’’ (pin X Mass
Bias) with no balance hole and the axis migration was traced. Again, just as the previous
tests, the migration path was shaped in way that each axis point had an approximate equal
RG value. The axis points were plotted in the above charts (Figures 2 and 3) as well.
Next an inch and a quarter weight hole was placed 4 inches deep on the bowler’s PAP.
Due to the removal of core weight, the RG value about the same PAP was increased.
This step was done to determine and verify what the effect on migration would be. Would
it follow the original path before the weight hole or would the path be generated in the
same since as all other testing and therefore create a second migratory path of same RG
values? The ball was tested and sure enough a second path was created that followed the
same trend in RG values. The PAP (with weight hole) had a higher RG, and a new path
that had the same higher RG as the PAP was traced. The picture below illustrates this
test.


Picture 7: Ebonite NVS – No balance hole/balance hole on PAP


TEST V – Mass Bias Marking on Traditional Migratory Path



Lastly, in Test 5, a Columbia Ten was drilled in an unconventional manner with the Mass
Bias marking beneath the ring finger and approximately 2-1/2 inches towards the PAP.
The picture below shows the layout. The thought behind this test was to place the mass
bias spot in a location along a normal migratory path that was traced in several previous
test balls.


While on the lane, if the ball wanted to show an axis of migration path toward the highest
RG, this drilling layout would present prime opportunity to do so. However, as in all
previous testing, the migration points plotted a path with the same trend. The ball created
a migratory path such that each axis rotation point was equal to the initial RG value of the
PAP.


Picture 8: Columbia 10 – Mass bias in “normal” migration path


Testing Results



What does all of this mean in the practical world of bowling? For starters, many
marketing tactics have been employed by companies to explain how and why a bowling
ball rolls down the lane. The research presented here shows USBC testing results, which
may differ from others in the industry. It is important to remember that the research was
conducted in a non-bias and neutral atmosphere. This test was not comparing cover stock
strengths, but concentrated on core dynamics and how the core behaves in motion on the
lane. All testing shows the same trends and indicates that on-lane Axis migration is
DEPENDENT upon the following two things:

    1) Physics
    a. While on the lane, the bowling ball did not migrate to an axis that had
    a higher RG value (ball did not end up rotating about the mass bias
    spot or high RG axis).
    b. Newton’s Law of Energy Conservation and Work still applied.
    2) Radius of Gyration
    a. While on the lane, the USBC approved ball always flared and migrated
    toward an axis of rotation that was approximately equal in the RG
    value of the starting PAP (measured and rounded to the second
    decimal point).
    b. RG is measured for the entire bowling ball as a “system” and not on
    the core alone.
The laws of physics stay intact and have not been broken. Physics terms such as Radius
of Gyration, Moment of Inertia, Conservation of Energy, Work and Equilibrium have
proven to be applied in the motion of a bowling ball. Certain terms and ideas that are not
found in physics books and principles show little affect on true core dynamics.
In short, an asymmetrical core ball drilled with the same layout as a symmetric ball
merely has a different initial RG value on a bowlers PAP (of same low RG and Diff.
RG). Thus, in proving that all asymmetrical or symmetrical cores have the same RG
progression as the ball rolls down the lane, testing now in progress will attempt to answer
another highly debated question:


“Assuming the same coverstock, Differential RG, and the same starting RG value on
the bowlers PAP with the same flare potential, will an asymmetrical core exhibit the
same on-lane core dynamics and ball motion as a symmetrical core?”


Hopefully, this in depth analysis on bowling ball motion and core dynamics help sort
through the marketing campaigns and distinguish the “real” factors that influence how
and why a ball rolls as it does. Remember, though, changes in cover stock technology are
separate and will influence ball motion separately. Integrating the concepts of cover stock
options with the balls radius of gyration and total differential should help a bowler
become more successful in choosing an arsenal. USBC would like to thank MoRich
Bowling Company for supplying some of the test balls used in this investigation.


If there are any questions regarding any of the above information presented, please send
an e-mail to Nick.Siefers@bowl.com.