1. Fundamentals of Biomechanics
Biomechanics applies mechanical principles to biological systems to understand how living organisms move and interact with their environments.
Core Concepts
- Kinematics: Description of motion without considering forces
- Kinetics: Study of forces that cause or result from motion
- Statics: Analysis of systems in equilibrium (no acceleration)
- Dynamics: Analysis of systems in motion
- Mechanics of materials: Study of how materials deform under loads
Coordinate Systems in Biomechanics
Different coordinate systems are used to describe body movements:
- Global (laboratory) coordinate system: Fixed reference frame
- Local (segment) coordinate system: Attached to body segments
- Anatomical coordinate system: Based on anatomical planes (sagittal, frontal, transverse)
2. Statics in Biomechanics
Statics involves analyzing systems in equilibrium where the sum of forces and moments is zero.
∑M = 0 (Sum of moments equals zero)
Free Body Diagrams (FBD)
Essential tool for solving biomechanics problems:
- Isolate the body or segment of interest
- Identify all external forces and moments acting on the body
- Draw the body with all forces represented as vectors
- Establish coordinate system
- Apply equilibrium equations
Example: Elbow Joint Force
Calculate the joint reaction force at the elbow when holding a 10kg weight in hand. Assume the forearm weight is 2kg, distance from elbow to weight is 30cm, and distance from elbow to forearm center of mass is 15cm.
Solution approach: Create FBD of forearm, apply ∑M = 0 about elbow to find muscle force, then apply ∑F = 0 to find joint reaction force.
3. Dynamics: Kinematics and Kinetics
Kinematic Variables
| Variable | Description | Units |
|---|---|---|
| Position | Location in space relative to reference point | m |
| Displacement | Change in position (vector) | m |
| Velocity | Rate of change of position | m/s |
| Acceleration | Rate of change of velocity | m/s² |
| Angular position | Orientation angle | rad |
| Angular velocity | Rate of change of angular position | rad/s |
Newton's Laws Applied to Biomechanics
- First Law (Inertia): A body remains at rest or in uniform motion unless acted upon by a net external force.
- Second Law (F=ma): The acceleration of a body is proportional to the net force acting on it and inversely proportional to its mass.
- Third Law (Action-Reaction): For every action force, there is an equal and opposite reaction force.
4. Mechanics of Materials in Biological Tissues
Stress and Strain
Strain (ε) = Change in length / Original length (unitless)
Material Properties
| Property | Description | Formula |
|---|---|---|
| Young's Modulus (E) | Stiffness in tension/compression | E = σ/ε |
| Shear Modulus (G) | Stiffness in shear | G = τ/γ |
| Poisson's Ratio (ν) | Ratio of transverse to axial strain | ν = -εtransverse/εaxial |
| Ultimate Strength | Maximum stress before failure | - |
| Yield Strength | Stress at which permanent deformation begins | - |
Viscoelasticity
Biological tissues exhibit time-dependent mechanical behavior:
- Creep: Continued deformation under constant load
- Stress relaxation: Decrease in stress under constant deformation
- Hysteresis: Energy loss during loading-unloading cycles