(455) HL Thermodynamics 1st law and basics [IB Physics HL]
Thermodynamics Overview
Focus on the first law of thermodynamics.
Basic example: coffee cooling down from hot to cold.
Systems in Thermodynamics
Closed Systems
No mass transfer in or out.
Energy transfer (heat) is possible.
Isolated Systems
No mass or energy transfer.
First Law of Thermodynamics
Applies to closed systems.
Equation: Q = ΔU + W
Q: Heat transferred (joules)
ΔU: Change in internal energy (joules)
W: Work done (joules)
Significance: Describes how internal energy relates to energy transfer.
Work in Thermodynamics
Work Equation: W = P * ΔV
Work done (joules).
Pressure (pascals).
ΔV: Change in volume (cubic meters).
Area under the PV curve represents work.
Clausius Conventions
Work direction impacts sign:
Positive if volume expands (right arrow).
Negative if volume contracts (left arrow).
Heat and Energy Terms
Heat transferred to surroundings: Q is positive.
Internal energy change:
Positive ΔU: Internal energy increases.
Work done by a system: Positive work.
Work done on a system: Negative work.
Change in Internal Energy
Internal energy equation: ΔU = 3 * n * R * ΔT or ΔU = 3/2 * N * kB * ΔT.
Need to know units:
ΔU: joules
ΔT: kelvin
n: number of moles
R: gas constant
N: number of molecules
kB: Boltzmann's constant
Example Problem
Context
Gas undergoes isovolumetric change (volume stays constant).
Initial (A) and final (B) states known: pressure, volume, and temperature.
Query
Find thermal energy removed when transitioning from A to B.
Approach
Understand that thermal energy means finding Q.
From the first law: Q = ΔU + W
Work done is zero in isovolumetric process.
Therefore, Q = ΔU.
Calculate ΔU using: ΔU = 3 * nR * ΔT.
Utilize the ideal gas law to determine n:
PV = nRT implies n = PV/T.
Calculation
Substitute known values from state A into ΔU, taking care of temperature change (ΔT).
Example calculation yields: Q = -332,353 joules (or -332 joules for significant figures).
Summary
Key takeaways include understanding the first law of thermodynamics, conditions of closed vs. isolated systems, work definition, Clausius conventions, and applying these to problems involving internal energy and heat transfer.