Kinetics examines the forces that cause or influence movement, as well as forces that allow maintenance of equilibrium or balance.
Kinematics describes HOW movement occurs, while kinetics explains WHY movement occurs.
Force is described as the action of one body on another.
It is a vector quantity, possessing both magnitude and direction.
Like kinematics, force has linear and angular components.
Forces can be added together; the mathematical symbol for summation is \sum. Therefore, when looking at multiple forces, you pl see \sum F = Linear Forces.
Forces create linear or translatory action.
SI units: Newtons (N)
Generally known as 'moment' or 'torque'. For our purposes, moment = torque.
Just as a linear force is represented by an arrow, an angular force is represented by a curved arrow, still indicating direction.
Angular forces can be added if there is more than one.
SI Units for moments: Newton-meters (N.m)
To generate a moment or the potential for producing rotation or angular movement, three elements are needed:
Linear force
Axis (denoted by a circle with a point in the center, or a triangle \triangle, or by a \land)
A distance from the linear force to the axis. This distance is a perpendicular distance – the distance would be at right angles to the linear force.
Therefore, if a linear force is applied a distance from an axis, then there a potential exists for rotation or angular movement around that axis – there the potential exists for a moment to exist
External forces (linear and/or angular) are exerted on the body from outside sources: gravity, weights, backpacks, resistance.
Internal forces are usually in response to some external stimuli or external forces
Have different names for the effect of the directed force(s)
Equal and opposite loads extending outward from surface of structure; applied in parallel to long axis of object
Lengthens and narrows
A force that is perpendicular to a joint surface, is directed away from that joint surface, and allows for separation of the joint surfaces.
Equal and opposite loads are applied toward the surface of a structure.
Opposite of joint distraction.
Applying perpendicular forces to joint surfaces directed toward the surface in attempt to bring the surfaces together.
Any force (or component of a force) that has an action line parallel to contacting surfaces (or tangential to curved surfaces) that creates or limits movement between surfaces.
i.e., Two parallel forces applied in opposite directions – not in line with each other.
Tries to cause movement between those two contacting surfaces.
Load applied to structure in a manner that causes it to bend about an pivot point.
Combination of compression/tension.
Load applied to a structure in a manner that causes it to twist about the structure’s long axis.
Shear stresses distributed over the entire surface
Further stresses are from axis, higher their magnitude
Combination of more than one loading modes
Amount of matter of which a body is composed
Point at which a body’s mass is concentrated in equilibrium (evenly distributed).
Point where acceleration of gravity acts on the body (whole body and segment).
AKA Center of Gravity (CG, CoG).
Often represented by the symbols:. For single object or rigid body → CoM will not change regardless of orientation.
For segment → will not change location as the mass of a given segment is fixed for an individual (e.g. hand)
For linked systems → as the masses of the links move, orientation of masses also changes and the CoM for the entire system will move
CoM for the entire system will move.
May even lie outside of system
Move towards the added weight.
When external mass is removed, the CoM will move again more towards center of system
CoM for body is just anterior of S2
Defined as a force (typically denoted ‘g’ for gravity) on a mass pulled by earth’s mass causing object to accelerate toward the earth
This gravitational pull gives an object weight:
Weight = mass * g
Notice that this makes weight a force and is a vector quantity
Represents the orientation (internal and/or external) – or – the line along which a force acts – or – along the shaft of the vector
Look at the name – it is the line along which an action can occur
*
Usually related to some form of resistance (will tend to use the term resistance for external sources of force)
For gravity acting on segment//system//additional resistance – the line of action of gravity is usually vertical (with arrowhead pointing downward).
From other sources (weights, manual contact, etc) will vary according to the situation
Usually are forces created by muscle, but can be other tissues
The line of action is usually parallel to the direction of the muscle fibers (with the arrowhead directed toward the stabilizing segment to complete the vector)
So you can say that the line of action of the muscle is along or parallel to its fibers
When the vector is drawn, this is where the tip of the tail goes
Point of application is at the segment/system’s CoM
Point of application is the attachment site for the tissue on the bone that force is acting upon
Most of the time we will be referring to muscle so the point of application of a given muscle is at the attachment is the proximal or distal insertion site of the muscle with the arrow going from the moving segment towards the stabilizing segment
Typically represents effect of gravity on the body
In anatomical position, LoG is parallel to the trunk and extremities
If in supine (or prone), then LoG is perpendicular to the body
Define by contact of system to ground – may include assistive devices or other objects
Contact with the ground in turn results with the ground reacting or ‘pushing back’
Occurs with all 3 planes/axes
If orthogonal (at right angles or 90° to each other) – have 3 components:
Vertical force (Z in graphics below)
Front – back (anterior-posterior or Y in graphic)
Side-to-side (medial-lateral or X)
When add all 3 components together → GRFv
Linear and Angular Forces
Need to know the differences between linear and angular forces and their relationship to each other
Need to know the terminology and associated with linear and angular forces
Often use the term ‘translatory’ or ‘translation’ to describe linear forces. For example, you need to make sure that the force you are exerting is a translatory force to test and mobilize a joint. You do not want to create rotation at the joint.
Angular force → called a moment or torque
Internal and External Forces
Need to know the difference between internal and external forces
Be able to give examples of internal and external forces
Later need to be able to understand and discuss which forces can be changed or manipulated to change how much force an individual must exert to perform an action and the consequences if they cannot create sufficient force for a given activity.
The effect of a given force (compression, tensile, etc.) becomes important in understanding how the tissues of the body are loaded and the effect the load has on the tissues.
Later need to be able to understand which forces can be changed or manipulated and how they can be changed/manipulated for exercise objectives
To increase or decrease how much a muscle needs to contract for an exercise objective
Progression of exercises
CoM, Gravity, Line of Action, Point of Application
To be able to distinguish differences in segmental vs. system CoM
To be able to determine the general reaction of CoM to changes and added/subtracted weight
Understand the meaning and applications of the line of action
Be able to “see” the line of action visually on paper, in your actions, the actions of your patients and conceptual or ‘imaginary’ lines such as gravity
Understanding the line of action of muscles along with planes and axes helps determine the muscle actions on a joint.
For example, muscle fibers that do not run strictly horizontal or vertical cross more than one plane so the muscle will have more than one action
The line of action of a muscle may change its orientation to an axis – be superior to it in one position but then become inferior to the axis in another position changing its action on that joint
The point of application can have influence on how ‘hard’ or how ‘easy’ a muscle or a person may have to work. It can be involved in levers, moments, and helps standardize the depiction of forces on a body
LoG, GRFv
Applications of the information presented above – forces, line of action, point of application, etc.
They are specific depiction of linear forces that act on the body and are important in balance, gait, mechanism of injury, injury prevention and potential creation of moments
LoG involved with balance and stability as presented below
GRFv will be covered in detail with gait
BoS
Strongly involved in balance and stability as presented below
Can refer to the ability to maintain or return to a steady state in presence of perturbations
Degree to which one can stand still or move without falling (full body)
Assessed through CoM, LoG and BoS
Line of gravity within base of support
Larger the base of support, more stable
The lower the CoM is to the base of support, more stable
The closer to the center of the base of support that the LoG falls, the more stable
Can refer to the capability of a system to move without falling – control is lost and the “fall” is to the ground or supporting surface
The integration of systems whose ultimate goal is to maintain static or dynamic stability
Can be assessed through either CoM and/or CoP depending on application and instrumentation:
Force plates
Pressure mats
Biodex Balance System
Balance Master (etc.)
LoG falls outside of the base of support
Controlled mobility → alternates with LoG falling within and out of the BOS
Uncontrolled mobility → fall
Term used to mean angular forces
Also called torque
May create movement or may be in equilibrium
Named for action on joint or tissue (usually osteokinematic action, e.g., flexor moment, adduction moment)
Have both internal and external moments
Remember that there are 3 conditions (parts/components/items) necessary for a moment to be produced:
Linear force
Axis around which the angular motion can occur
A perpendicular distance from the linear force to the axis
So when taken together …Mathematically:
\sum M = \sum(F * \perp d)
where M is the sum of the moments generated, F are the applied linear forces, and d are the \perp distances between the axis of rotation and the line of action of the applied forces (called moment arms – more on this later)
Linear force – any tissue (tendon, ligament, etc.) but here the focus will be: Muscle Need to know:
As it is a linear force, it can be represented by a vector
Line of action → usually parallel to the direction of the muscle fibers
One vector can represent entire muscle so do not have to represent each muscle fiber
May need more than one vector if the muscle is a pennate (angled in which not all muscle fibers are parallel to each other (e.g. gastrocs)
Point of application → is at attachment of the muscle on the moving segment
Direction → is toward the stabilizing segment
Orientation → Angle of Application (Inclination)
Angle is created by: 1) line of action of the muscle (represented by the tendon) and 2) the long axis of the bone onto which the tendon inserts (on the side of the joint axis.)
Axis – can be
Fulcrum around which angular motion occurs
Pivot point for angular motion
Typically for the joint it is the “instantaneous center of joint rotation” (which can move as joint moves)
Perpendicular distance from line of action to the axis
Line that is perpendicular (at right angle to or is at 90°) to the line of action of internal force to joint axis of rotation
Goes by many names:
Moment arm
Force arm
Effort arm
Linear force – something external to the body (gravity//added resistance in the form of a weight or a person//object pushing against or pulling on the body )
Need to know:
As it is a linear force, it can be represented by a vector
Line of action:
Gravity is generally vertical with the arrow pointing down
If added resistance from a free weight → usually vertical with arrow pointing down
If added resistance from manual resistance or object → the orientation of however the force is being directed
Point of application:
Gravity is at the CoM of the segment being acted upon
Added resistance / free wt – also at the weight’s CoM
Added resistance / manual - at the point of contact
Direction and orientation→ as given above with line of action
Axis – same axis as for internal – can be
Fulcrum around which angular motion occurs
Pivot point for angular motion
Typically for the joint it is the “instantaneous center of joint rotation” (which can move as joint moves)
Perpendicular distance from line of action to the axis
Line that is perpendicular (at right angle to or is at 90°) to the line of action of external force to joint axis of rotation
Goes by many names:
Moment arm
Resistance arm
Effort arm
Using what has been presented thus far:
Determining muscle action and type of internal moment produced at a joint
If line of action of muscle passes anterior to frontal axis, muscle will flex the joint (exception -- knee); It creates an internal flexion or flexor moment
If line of action of muscle passes posterior to frontal axis, muscle will extend the joint (exception -- knee); It creates an internal extension or extensor moment
If line of action of muscle passes superiorly to sagittal or A/P axis (thick line going front/back), muscle will abduct creating an abduction moment
If line of action of muscle passes inferiorly to sagittal or A/P axis (thick line going front/back), muscle will adduct creating an adduction moment
Location of muscle to longitudinal axis determines whether or not it will internally or externally rotate:
External moments follow the same concepts as for the internal moments above:
If the line of action of the external force is anterior to a frontal axis, it can create a flexor moment
If the line of action of the external force is posterior to the frontal axis, it can create an extensor moment
Line of action is superior to sagittal axis → abductor moment
Line of action is inferior to sagittal axis → adductor moment
Same relationship for longitudinal axis for internal and external rotator moments
Same exceptions as above
Relationship of internal ↔ external moments
When an external moment is acting on a joint, we usually want the body to respond by creating an opposing internal moment
For example, when going from sit-to-stand, gravity may try to flex the hip, flex the knee and dorsiflex the ankle joint such that if there is no opposing or countering force, the body will collapse
The muscles contract to try to overcome the effect of gravity creating extensor moments to allow the motion to be completed
Posture
Examine the effect of gravity on the joints of the body and what external moment(s) gravity can produce
This is one of the uses of the LoG
In ‘normal’ or ideal posture, slight moments will be created by gravity pulling down on the spinal segments and lower extremities
In postural deviations, these moments may increase or change directions
GRFv and Gait
When walking (or running or other forms of gait), the foot makes contact with the ground and the ground “pushes back” and creates a GRFv
Where the GRFv is located in relation to the joints can influence the immediate external moment created and subsequently, the internal moment that needs to be created to offset the external moment
For example, the GRFv at initial contact (heels strike) falls posterior to the ankle in the sagittal plane creating an external plantarflexion moment (graphic below on left); the muscles/tissues in the body then create an internal dorsiflexor moment (graphic on right)
In individuals with no impairments, this is done seemingly automatically
However, in individuals with some form of ankle impairment (restricted ROM, decreased strength in the dorsiflexors, etc.), it can be a problem and the PT needs to be aware of the possibilities that exist in this situation