Polymer Glass Transition

Interactive demonstration of glass transition temperature (T_g), molecular motion, and mechanical property changes

Polymer Types

Specific Volume vs Temperature

Current Temperature: 25°C
Current State: -
Glass Transition Temperature:: 100°C

Molecular Motion

Elastic Modulus vs Temperature

Current Modulus: - GPa
Modulus Change at T_g: Drastic drop (10³-10⁴×)

Parameters

Temperature Control

Molecular Factors

Display Options

Property Comparison

Property Glassy State (T < T_g) Rubbery State (T > T_g)
Mechanical Behavior Brittle, rigid Tough, flexible
Elastic Modulus 10³-10⁴ GPa 1-10 GPa
Molecular Motion Frozen (vibrational only) Segmental motion
Thermal Expansion Low coefficient High coefficient
Applications Plastics, glasses Rubbers, elastomers

Physical Principles

Glass Transition Temperature: T_g
Glassy State: T < T_g (Brittle, high modulus)
Rubbery State: T > T_g (Tough, low modulus)
V-T Relation: Slope change at T_g

Instructions

  • Select different polymer types to see their T_g values
  • Adjust temperature to cross T_g and observe state changes
  • Watch molecular motion animation - frozen in glassy state, active in rubbery state
  • Modify molecular factors to see how they affect T_g
  • Use heating animation to observe continuous transition

What is Glass Transition?

The glass transition is a reversible transition in amorphous polymers from a hard and relatively brittle glassy state into a viscous or rubbery state as temperature increases. The glass transition temperature (T_g) is where this transition occurs. Unlike melting (first-order transition), glass transition is second-order, characterized by changes in heat capacity, thermal expansion, and mechanical properties.

Specific Volume vs Temperature

The volume-temperature (V-T) curve shows specific volume vs temperature. Below T_g: glassy state with low thermal expansion. Above T_g: rubbery state with high expansion. Slope change at T_g indicates increased free volume and chain mobility.

Molecular Motion

In glassy state (T < T_g): polymer chains frozen, only small vibrational motions possible. Lack of large-scale motion makes material brittle and stiff. Above T_g: sufficient thermal energy enables segmental motion - chain portions can rotate and move. This mobility transforms mechanical properties from rigid to flexible.

Elastic Modulus vs Temperature

Elastic modulus decreases dramatically at T_g by factor of 10³-10⁴. Glassy: high modulus (GPa) due to restricted mobility. Rubbery: low modulus (MPa) as chains gain mobility. This drastic change determines useful temperature range: plastics below T_g for rigidity, rubbers above T_g for flexibility.

Factors Affecting T_g

Molecular weight: higher MW increases T_g due to chain entanglement. Cross-linking: creates covalent bonds between chains, restricts mobility, raises T_g. Plasticizers: small molecules that increase free volume and mobility, lower T_g. Chain flexibility, side groups, intermolecular forces also influence T_g.

Applications

Understanding glass transition is crucial for: selecting materials for specific temperature ranges, designing processing conditions, predicting material behavior, developing polymer blends, and optimizing formulations. Examples: polystyrene cups (T_g ≈ 100°C), rubber tires (T_g ≈ -70°C), impact-modified plastics.