Title: Applied Biomedical Engineering
1Applied Biomedical Engineering AMME4981 Lecture
2 Musculoskeletal Biomechanics (Statics and
Dynamics of Muscle and Joint Loads)
2Objectives
- It is important to determine the
internal/external undergone in the body before we
carry out biomechanical analysis. Hence, we need
to discuss the biomechanics issues related to
body first. - Calculate the joint reaction force for a defined
situation - Estimate muscle forces for a defined situation
- Discuss the relationship between muscle
performance and anatomic and physiologic
constraints
3Mechanics Concepts
- Forces and moments
- Degrees of freedom
- Displacement, velocity, and acceleration
- Inertia
- Static/dynamic equilibrium
- Newtons laws
- Free body diagrams/Kinetic diagram
- Vectors and algebraic analysis of vectors
- Linear and angular momentum
- Work and energy
4Anatomical Position
- Movements of the body are taken from the neutral
anatomical position - Legs straight with feet pointed forward
- Arms at side with palms facing forward
Transverse Plane
Sagittal Plane
Coronal Plane
Neutral anatomical position
5The Musculoskeletal System
6Musculoskeletal Biomechanics
How do we perform movement and/or apply forces?
7Forces in the Musculoskeletal Systems
- System experiences both internal and external
loads - Internal
- Active muscle forces
- Reaction forces of joints and ligaments
- External
- Inertial force due to acceleration of a segment
- Loads directly applied to a body segment
- Muscles transmit a load to the distally attached
body segment
8Musculoskeletal Dynamics
- Kinematics motion relationship
- Linear and angular displacement
- Linear and angular velocity
- Linear and angular acceleration
- Kinetics motion-load relationship
- Newtons second law
- Work-energy principle
- Impluse-momentum principle
- Anatomical concepts (rigid body)
- Body segments
- Thigh - leg - foot
- Arm - forearm - hand
9Forces in the Musculoskeletal Systems Contd
- Most static and dynamic systems
- Forces (internal/external) generally are given
- Solve for deformation or rigid body motion
- For musculoskeletal system
- Internal forces are not generally known
(Transducers can be inserted within tendons, but
only in laboratory animals) - Motion is relatively easy to measure
- Solve an inverse problem to determine muscle and
joint forces from motion (displacement, velcotiy,
acceleration)
10Muscle Force Constraints
- Each individual muscle must have a force such
that - Maximum muscle force is dependent on
- The physiological cross-sectional area (PCSA)
- Muscle stress limit (?)
- Active force correction for length-tension and
force-velocity relationships (?a) - Passive force correction (?p)
11Inverse and Direct Dynamic Problems
F
r
Known forces
Equations of motion
Double integration
Displacement
r
F
Known forces
Double differentiation
Equations of motion
Displacement
12Solving the Inverse Problems
- To calculate internal forces, need
- Full description of movement
- Accurate anthropomorphic measurements
- Knowledge of external forces
- Moment balance done at the center of rotation of
a joint eliminates the effect of the unknown
joint reaction force
13Body Segments and Model
- Body segments can be modeled as rigid bodies,
- e.g. foot, leg, forearm, thigh,
- Free body diagrams can be drawn for each segment
- Intersegmental forces and moments acting at
joint centers - Gravitational forces acting at the centers of
mass - Accurate measurements are needed of
- Segment masses (m)
- Centers of mass
- Joint centers
- Mass moment of inertia (I)
14Model Assumptions
- Rigid body motion - deformation is small
relative to overall motion - Body segments interconnected at joints and
length of each segment is constant - Each segment has a fixed mass located at its
center of gravity - The location of a segments center of mass is
fixed during any movement - Joints are considered to be hinge (2D motion) or
ball and socket (3D motion) - Moment of inertia of each segment about any
point is constant during any movement
15Forces
- Gravitational forces
- Act downward through center of mass of each
segment - Equal mass ? acceleration due to gravity (mg)
- Ground reaction force
- Distributed over an area of the foot
- To represent as a vector, assume it acts at a
point, the center of pressure - Calculated from force plate data
- Externally applied forces
- Any restraining or accelerating force that acts
outside of the body - Obstacle being tripped over
- Mass being lifted
- Muscle Forces
- Net effect of agonists and antagonists on body
segments - True muscle forces are slightly underestimated
due to frictional losses in joint - Ligament forces
- Influence muscle and joint loads at extremes of
motion
16Analyse Trajectories of Motion
Determine displacement, velocity and acceleration
as a function of time t
17Analyse Angular Motion
Determine angular displacement, velocities and
angular accelerations
18Document Kinematics
19Document the Motion (Kinematics) Contd
Data Presentation
20Measurement of Sagittal motion
21Kinematic Studies
- Segment angles
- Calculated based on the position of two segment
markers placed along long axis of segment in
plane of angle - Segment linear velocities and accelerations
- Use two data intervals to minimize error
- Segment angular velocities and accelerations
22Anthropometry
Use Anthropometry (physical parameters of the
human body) to model human body
Data are per single limb Relative distance
of C.M. (measured from the lower numbered joint)
23Anthropometry Diagram
0.130H
0.186H
0.146H
0.108H
0.129H
0.520H
H
0.259H
0.174H
0.936H
0.191H
0.870H
0.720H
0.530H
0.818H
0.485H
HHeight of standing subject
0.285H
0.377H
0.630H
0.039H
Foot Breadth
Foot Length
0.152H
0.055H
Modified from Drillis and Contini, 1966
24Type of Motions and Equation of Motions
- Translation When all the particles of the body
move in parallel trajectories
- Rotational (Angular motion)
- General Motion When the body performs
simultaneous translation and rotation
25Example 1.1 Muscle/Tendon Force
Flexed arm holding a ball of W20N with a
distance of 30cm to the elbow center. What is the
biceps force required (B) if the forearm weighs
15N and the center of mass for forearm is 15cm
from the elbow center of rotation? The biceps
tendon is inserted 3cm from elbow center.
B
Ry
Rx0
mg
W
3
15cm
30cm
Anatomical schematic
Statics model
26Example 1.1 Contd
Step 1 If the arm is in static equilibrium
Step 2 Scalar equation in x and y directions
Step 3 Solve for the equations ( - means
opposite direction to positive sense)
27Example 1.2 Joint Reaction Load
A person stands statically on one foot. Ground
reaction force acts 4cm anterior to ankle center
of rotation. The body mass is 60kg and foot mass
0.9kg. Center of mass of foot is 6cm from the
center of rotation. Determine the forces and
moment in the ankle.
Rotation center
Mass center
28Example 1.2 Contd
More general equation of motion (Newtons 2nd law)
29Example 1.3
A person exercises his left shoulder rotators.
Show how would you go about calculating the
forces and moments exerted on his shoulder.
Consider a quasi-equilibrium
Motion of equation
a
Fjy-F
b
F200 N, a25 cm, b30 cm.
FBD
Answer
30Tutorial 1
A weight lifter raises a barbell to his chest.
Determine the torque developed by the back and
the hip extensor muscles (Mj) when the barbell is
about the knee height (as shown in the
illustration). Weight of barbell Wb1003 N,
Weight of upper body Fw,u525 N a38
cm, b32 cm, d64 cm IG7.43 kg-m2, ?8.7
rad/s2, aGx0.2 m/s2, aGy - 0.1 m/s2.
O
31Solution to Tutorial Problem
Step 0 Newtons 2nd law
Step 1 Mass moment of inertia about O
Step 2 Dynamic equilibrium of forces
Step 3 Dynamic equilibrium of moments
32Other example
A man walks in the platform with test markers in
his right limb as shown. Determine the forces and
moments (1) at the ankle and (2) at the knee,
based upon the following measurements. Determine
force/moment in the ankle and knee.
33Summary
- Measurement of motion
- Kinematic analysis to determine linear/angular
displacement, velocity and acceleration - Kinetic analysis to determine the force and
moment in muscle and joints
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