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The Mechanics of Swing
The Tangent-Release Principle

  
August 24, 2010
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The Mechanics of Swing
   Dr. Gerald George
Dr. George
From a mechanical standpoint, swing is essentially a form of rotary or angular motion. It can be defined as circular movement of an object about an axial line in a fashion such that all parts of the object travel through the same angle, in the same direction, in the same amount of time. This line, often referred to as the "axis of rotation," always lies at a right angle to the object's plane of motion.
 
The human anatomy, with its numerous joints and segments, can be thought of as an articulated system of swinging levers that circle about one another in a properly coordinated sequence to produce a desired movement. To qualify as swing, the movement need not necessarily be complex. Any joint of motion of one body segment about another can be considered an elementary form of swing.

In my new book, Championship Gymnastics, I discuss all of the aspects of swing: internal swing, external swing, optimizing swing mechanics, and fundamental concepts of swing. But today I want to focus on one aspect of optimizing swing mechanics: The Tangent-Release Principle.

CLICK HERE to view Table of Contents
of Championship Gymnastics

The Tangent-Release Principle
Force always acts in the precise straight-line direction in which it is applied. Consequently, any body in motion as a result of applied force tends to travel its same straight-line path, and speeds up (accelerates) at a rate proportional to that force's magnitude. The only factor which can alter this state of affairs is the introduction of one or more additional forces. If, for example, force is applied in a direction opposite the already-existing motion, the body slows down (decelerates). The relationship between the magnitude of force and the direction of the applied force determines whether the body will move, and if so, at what rate of speed and in which direction.
 Descent of Overgrip Giant Swing
For example, during the descent phase of the Overgrip Giant Swing, the force of gravity tends to accelerate the performer's mass downward in a straight line. The body's mass center, however, does not travel straight downward. Rather, it continuously changes direction, circling relative to its fixed axis of rotation (bar). Because the performer's hands are firmly anchored to the apparatus, the body tends to follow a circular path equal in length to its radius of rotation.
 
This circular movement pattern is due to the mutual force relationship between the gymnast and the bar. The action of the performer pulling against the bar causes a simultaneous reaction of the bar pulling against the performer. Because this action-reaction relationship is equal in magnitude and opposite in direction, the effects would seem to cancel out. Yet this is not the case, for the action of the performer pulling against the bar cannot possibly move the apparatus, as it is firmly attached to the colossal mass of the earth! However, the reaction of the bar pulling against the performer does possess sufficient magnitude to produce a continuous change in direction of the performer's light mass. The observed effect of this action-reaction scenario is a circular pattern of the total body unit about the bar. As long as this mutual force relationship is maintained, the performer's external swing motion is preserved.
 Tangent-Release Illus
However, if the performer were to release her hand-grasp at any time while circling about the bar, this mutual force relationship would cease to exist, and her body would be projected away from the bar in a straight-line at an angle perpendicular to its radius of rotation. Once airborne, the body's mass center would then travel a perfectly regular, curved path (parabolic trajectory). This is precisely what occurs in the Double Backward Somersault Dismount presented in the illustration on the right. The performer's pulling does bend the bar in the direction of the pull. The only exception to the parabolic trajectory outcome would be if the performer's center of mass were at either the 3 o'clock or 9 o'clock position when the hand-release occurred, in which case her body would be projected either straight up or straight down. At the instant of release, notice how the performer's body is projected in a straight line at a 90° angle to its radius of rotation, and how, once airborne, her center of mass follows its predetermined parabolic trajectory.
 
Every release from any external-swing movement always results in
the center of mass being projected at a right angle to its radius.

Summary of Tangent-Release Principle
Because the body's mass center exits from any external swing at a 90° angle to its radius of rotation (tangent to the swing), the gymnast can confidently take advantage of the Tangent-Release Principle to direct the flight pattern properly for any dismount or release-grip skill on the uneven bars. Effective use of this principle, however, requires a clear understanding of the intended direction and objective of the skill's airborne phase, so the release phase can be timed accordingly. Simply put, proper timing of the release is critical to success in all airborne movements generated by external swing.The wise gymnast becomes well aware that:
 
Just as the archer's bow establishes the flight direction of the arrow,
so too
 does the tangent release establish the flight direction of the gymnast.

Information excerpted from Championship Gymnastics: Biomechanical Techniques for Shaping Winners, by Gerald S. George, Ph.D.

I invite you to send me your questions regarding coaching mechanics and techniques. Go to my website and click on the  "Contact Us" button (at the top of each page) and submit your question. Questions having the broadest application will be addressed in each eNewsletter. Click HERE for past eNewsletter Archive.

Thanks for your participation and continued support!

Gerald S. George, Ph.D.
WinningGymnastics.com
888-796-5229 (Toll-free in U.S.)
760 458-4993
(M-F 9-5 PST)


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