Basics of Biomechanics [Mechanical engineering]

Basics of Biomechanics

Newton's Laws of Motion

1) How Inertia Applies to Biomechanics

Consider the late swing phase of gait and the forces going forward with the lower extremity. Just prior to heel-strike there are almost no muscles activated that bring the extremity forward, yet it is still proceeding to travel forward in space. This is inertia. To deal with this inertia the body deploys an eccentric contraction of the hamstrings to slow down the extremity to prepare for heel-strike and to reduce harsh reactionary forces.

The net force applied to a body (mass) produces a proportional acceleration. This law describes the relationship between an object’s mass, acceleration, and the applied force. Both acceleration and force must have the same vector direction.

This can also be viewed in different terms:

Momentum = mass x velocity. The change of momentum of a body is proportional to the impulse impressed on the body, and happens along the straight line on which that impulse is impressed. Momentum cannot be changed unless acted upon by an outside force; it can only be conserved.

Acceleration is proportional to the unbalanced forces acting on it and inversely proportional to the mass of the object (a = F/m)

How F=ma Applies to Biomechanics

Pretty much every static and dynamic movement has a force. Muscles are the tissues that contract and create force on the body’s levers (connective tissue, bones). With any human movement, F=ma can be used to create a simplified calculation of force. This equation can even be used with static positions. Consider the static forward head posture. Gravity and the mass of the head imposes an antero-inferior force. To counter this force and prevent your neck from snapping off at your desk, you have to constantly contract your levator scapulae, upper trapezius, and posterior cervical muscles to counter this force. By calculating the acceleration of gravity and mass of the head, you can begin to calculate the muscle forces necessary to prevent movement.

For every action there is an equal and opposite reaction. This law describes how forces always come in pairs, meaning that anytime objects are contacting each other, they are exerting a force. An important consideration here is the concept that gravity is ALWAYS touching every object.

How Action-Reaction Applies to Biomechanics

Putting that ankle weight on a patients leg will create an increase in the force of the mass and downward pull with gravity, the reaction is that the opposing muscle will have to create a force to overcome this mass. Another example of this law is with ground reaction forces. Running on soft ground will result in much less impact forces than running on hard concrete.

Newton’s 3 laws of motion are the basis for understanding motion and the correlative force systems. Each law can be applied to biomechanics in it’s own way.

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