All Topics
physics-9702 | as-a-level
Responsive Image
10. Magnetic Fields
27. Quantum Physics
Recall and use the first law of thermodynamics: ∆U = q + W

Topic 2/3

left-arrow
left-arrow
archive-add download share

Your Flashcards are Ready!

15 Flashcards in this deck.

or
NavTopLeftBtn
NavTopRightBtn
3
Still Learning
I know
12

Recall and Use the First Law of Thermodynamics: ∆U = q + W

Introduction

The First Law of Thermodynamics is a fundamental principle in physics that establishes the relationship between internal energy, heat, and work. For AS & A Level students studying Physics - 9702, understanding this law is crucial as it forms the foundation for various applications in energy transfer and conservation. This article delves into the intricacies of the First Law, providing a comprehensive overview tailored to the curriculum requirements.

Key Concepts

Understanding the First Law of Thermodynamics

The First Law of Thermodynamics, often referred to as the Law of Energy Conservation, states that energy cannot be created or destroyed in an isolated system. Instead, energy can only be transformed from one form to another. Mathematically, it is expressed as:
$$\Delta U = q + W$$
Where:
  • ∆U represents the change in internal energy of the system.
  • q denotes the heat exchanged between the system and its surroundings.
  • W stands for the work done on or by the system.

Internal Energy (∆U)

Internal energy is the total energy contained within a system, encompassing both kinetic and potential energies of the particles. It is a state function, meaning it depends only on the current state of the system, not on how the system arrived at that state.

Heat (q)

Heat is a form of energy transfer due to temperature difference. When a system absorbs heat, \( q \) is positive, and when it releases heat, \( q \) is negative.

Work (W)

Work in thermodynamics is defined as the energy transfer when an external force acts on the system's boundary. If work is done on the system, \( W \) is positive; if work is done by the system, \( W \) is negative.

Types of Work

There are various types of work in thermodynamics, including:
  • Pressure-Volume Work: The most common form, calculated as \( W = -P \Delta V \).
  • Electrical Work: Involving the transfer of charge through an electrical potential difference.
  • Surface Work: Related to changes in surface area under surface tension.

Sign Conventions

Consistent sign conventions are essential for correctly applying the First Law:
  • Heat (q): Positive when absorbed, negative when released.
  • Work (W): Positive when done on the system, negative when done by the system.

Applications of the First Law

The First Law applies to various real-world scenarios, such as:
  • Calorimetry: Measuring the heat of chemical reactions or physical changes.
  • Thermal Engines: Understanding energy conversion in engines and refrigerators.
  • Phase Transitions: Analyzing energy changes during changes in state.

Mathematical Derivations

Deriving the First Law involves understanding the conservation of energy principle. For instance, in a closed system with no mass transfer:
$$\Delta U = Q - W$$
Here, \( Q \) is the heat added to the system and \( W \) is the work done by the system, aligning with the sign conventions mentioned earlier.

Examples and Problem-Solving

Consider a gas in a piston where heat \( q \) is added, and the gas does work \( W \) by expanding. The change in internal energy can be calculated using \( \Delta U = q - W \). If \( q = 500 \, \text{J} \) and \( W = 200 \, \text{J} \), then:
$$\Delta U = 500 \, \text{J} - 200 \, \text{J} = 300 \, \text{J}$$

Energy Conservation in Isolated Systems

In isolated systems, where no heat or work is exchanged with the surroundings, the internal energy remains constant (\( \Delta U = 0 \)). This highlights the conservation principle integral to the First Law.

Heat Capacity and Specific Heat

Heat capacity (\( C \)) is the amount of heat required to change a system's temperature by one degree. Specific heat (\( c \)) is the heat capacity per unit mass. These concepts are vital for calculating heat transfer in various processes:
$$q = mc\Delta T$$
Where:
  • m is mass.
  • c is specific heat capacity.
  • ∆T is the temperature change.

First Law in Thermodynamic Cycles

In cyclic processes, the change in internal energy over one complete cycle is zero (\( \Delta U = 0 \)), implying that the net heat added equals the net work done by the system.

Heat Engines and the First Law

Heat engines operate based on the First Law, converting heat into work. The efficiency of a heat engine is determined by the ratio of work output to heat input, constrained by the First Law and the Second Law of Thermodynamics.

Internal Energy and Temperature

The internal energy of an ideal gas is directly proportional to its temperature. For an ideal monoatomic gas, internal energy can be expressed as:
$$U = \frac{3}{2}nRT$$
Where:
  • n is the number of moles.
  • R is the gas constant.
  • T is temperature in Kelvin.

Real-World Implications

The First Law has significant implications in various fields, including engineering, chemistry, and environmental science. It aids in designing efficient energy systems, understanding chemical reactions, and analyzing energy flows in ecosystems.

Advanced Concepts

Detailed Theoretical Explanations

Delving deeper into the First Law, we explore the microscopic perspective of internal energy. Internal energy comprises translational, rotational, vibrational, and electronic energies of molecules. For ideal gases, the internal energy depends solely on temperature, whereas real gases also account for intermolecular forces and molecular sizes.

Mathematical Derivations and Proofs

To derive the First Law from classical mechanics, consider a system of particles. The total work done on the system is equivalent to the change in kinetic energy plus the change in potential energy within the system. This aligns with the conservation of energy, leading to the formulation \( \Delta U = q + W \).

Complex Problem-Solving

Consider a scenario where a gas undergoes a two-step process: isothermal expansion followed by adiabatic compression. Using the First Law, we can calculate the overall change in internal energy by analyzing each step separately and applying \( \Delta U = q + W \) accordingly.
  • Isothermal Process: \( \Delta U = 0 \) (for ideal gas), so \( q = -W \).
  • Adiabatic Process: \( q = 0 \), hence \( \Delta U = W \).
By solving each step, we can determine the net internal energy change over the complete cycle.

Interdisciplinary Connections

The First Law bridges physics with chemistry and engineering. In chemistry, it is fundamental to thermochemistry, dictating energy changes in reactions. In engineering, it underpins the design of engines, refrigerators, and energy systems, ensuring efficient energy conversion and utilization.

Energy Transfer Mechanisms

Beyond heat and work, advanced studies consider other energy transfer mechanisms such as mass flow. In open systems, mass transfer can carry energy into or out of the system, modifying the basic First Law equation to include enthalpy changes.

Entropy and the First Law

While the First Law focuses on energy conservation, the concept of entropy relates to the quality of energy. The Second Law of Thermodynamics introduces entropy, highlighting that while energy is conserved, its availability for work decreases in natural processes.

Thermodynamic Potentials

Advanced studies introduce thermodynamic potentials like Helmholtz and Gibbs free energies, which extend the First Law to predict the spontaneity of processes and equilibrium states under various conditions.

Phase Equilibria and the First Law

Understanding phase changes involves applying the First Law to account for latent heats during transitions between solid, liquid, and gas phases. This is crucial in fields like meteorology and materials science.

Statistical Thermodynamics

At a microscopic level, statistical thermodynamics connects the First Law to the behavior of particles, using probabilities to describe energy distribution and internal energy fluctuations in systems.

Energy Efficiency and Sustainability

The First Law informs discussions on energy efficiency and sustainability. By quantifying energy inputs and outputs, it aids in optimizing processes to minimize energy loss and enhance sustainable practices.

Advanced Calculations and Numerical Methods

Complex systems often require numerical methods to solve the First Law equations, especially when dealing with variable pressures, temperatures, and non-ideal conditions. Computational tools and simulations play a vital role in these calculations.

Comparison Table

Aspect First Law of Thermodynamics Second Law of Thermodynamics
Fundamental Principle Energy conservation: ∆U = q + W Entropy increase: Energy quality degrades
Focus Quantitative energy changes Directionality of processes
Applications Energy transfer calculations, calorimetry Heat engines efficiency, spontaneous process criteria
State Function Yes (Internal Energy) Yes (Entropy)
Equation ∆U = q + W ∆S ≥ 0

Summary and Key Takeaways

  • The First Law of Thermodynamics establishes energy conservation in systems.
  • Internal energy changes are governed by heat exchange and work done.
  • Understanding sign conventions is crucial for accurate calculations.
  • Advanced applications include thermodynamic cycles and statistical mechanics.
  • The First Law forms the foundation for further thermodynamic principles and real-world energy applications.

Coming Soon!

coming soon
Examiner Tip
star

Tips

To remember the First Law equation \( \Delta U = q + W \), think of "U" as your "Energy Update" from heat and work. Use the mnemonic "Q WILD" where Q is heat and W is work, both influencing the internal energy. Additionally, always double-check your sign conventions: positive for heat absorbed and work done on the system, negative otherwise. Practice with diverse problems to reinforce these concepts and enhance retention for exams.

Did You Know
star

Did You Know

The First Law of Thermodynamics not only governs physical systems but also plays a pivotal role in biological processes. For instance, in human metabolism, the conversion of food into energy follows this law, ensuring that the energy intake equals energy expenditure. Additionally, this law was instrumental in the development of the steam engine during the Industrial Revolution, revolutionizing transportation and manufacturing.

Common Mistakes
star

Common Mistakes

One common mistake is confusing the sign convention for work. Students often mix up whether work done by the system is positive or negative. Remember, work done by the system is negative (\( W < 0 \)). Another error is neglecting to account for all forms of energy transfer, especially in complex systems where both heat and work are involved. Lastly, misapplying the internal energy change by forgetting that it is a state function, leading to incorrect calculations based on the process path.

FAQ

What is the First Law of Thermodynamics?
The First Law of Thermodynamics states that energy cannot be created or destroyed in an isolated system. It is expressed as ∆U = q + W, where ∆U is the change in internal energy, q is heat added to the system, and W is work done on the system.
How is internal energy defined in the First Law?
Internal energy (∆U) is the total energy contained within a system, including both kinetic and potential energies of its particles. It is a state function, dependent only on the system's current state.
What is the significance of sign conventions in the First Law?
Sign conventions are crucial for correctly applying the First Law. Heat (q) is positive when absorbed and negative when released. Work (W) is positive when done on the system and negative when done by the system.
Can you provide an example of the First Law in action?
Sure! If 500 J of heat is added to a gas and the gas does 200 J of work by expanding, the change in internal energy is calculated as ∆U = 500 J - 200 J = 300 J.
How does the First Law apply to isolated systems?
In isolated systems, no heat or work is exchanged with the surroundings, so the internal energy remains constant (∆U = 0), illustrating the conservation of energy.
What is the relationship between the First Law and thermodynamic cycles?
In thermodynamic cycles, the total change in internal energy over one complete cycle is zero (∆U = 0). This means the net heat added to the system equals the net work done by the system.
10. Magnetic Fields
27. Quantum Physics
Download PDF
Get PDF
Download PDF
PDF
Share
Share
Explore
Explore
How would you like to practise?
close