13. Heat conduction, diffusion, fluids Flashcards
What is heat conduction
- the flow of energy to eliminate temperature differences
* ie. the constant heat loss from our bodies through our skin at moderate temperatures
How do you calculate the number of accessible microstates of the system?
• S = Kb*ln(W)
S - entropy
Kb - botzmann’s constant
W = number of accessible microstates of the system
When is the entropy of a system highest? Why?
When at equilibrium
•In an isolated system, when the system’s entropy reaches the maximum, the system stays there
•because any further change would reduce entropy
What can closed and open systems exchange?
Closed:
• exchange heat
Open
• heat and matter
What is the material constant λ? Unit?
λ is the thermal conductivity coefficient
•unit - J/(m.s.K)
Why is λ always positive?
λ (Thermal conductivity coefficient) always positive as heat always flows from an area of high temperature to one with lower temperature
Why is it easier to cut an ice cube using copper than aluminium?
- copper has a higher thermal conductivity
* gains heat more easily and speeds up the melting process
Passive diffusion
Allows small ions and molecules to penetrate the membrane in the direction from higher to lower concentration
Active ion transport
These processes require energy, typically via ATP, to transport ions such as sodium and potassium across cell membranes
What is observed in Fick’s law of diffusion?
The rate of a gas passing through a membrane of contact area A and width L is proportional to A, and the density difference on both sides of the membrane
What is an ideal stationary fluid?
A fluid that has
•no internal friction or viscosity and is •incompressible (both volume and its density are constant)
What are the forces acting on an ideal stationary fluid?
• the weight of the fluid directed downward
• contact forces
- fluid below the element pushes the fluid element upwards
- fluid above the element pushes the fluid element downwards
What is Pascal’s law?
States that the difference between pressures at two different positions in a fluid of constant density is proportional to the vertical distance between these 2 positions
p2 - p1 = -pg (y2-y1)