LAST Problem from the International Physics Olympiad

ZPhysics
19 Mar 202308:26
EducationalLearning
32 Likes 10 Comments

TLDRThis script tackles the intriguing problem of a black hole's mass change rate in the context of the universe, considering both Hawking radiation and cosmic microwave background radiation. It explains the application of fundamental physics constants and Stefan-Boltzmann's law to derive the rate of mass change. The script further explores the concept of thermal equilibrium for black holes, revealing a fascinating symmetry where the black hole's temperature matches the cosmic microwave background temperature at equilibrium. The explanation is rich with mathematical derivations, showcasing the beauty of physics in understanding the cosmos.

Takeaways
  • ๐Ÿ“š The script discusses a problem from the International Physics Olympiad related to black holes and their interaction with cosmic microwave background radiation.
  • ๐ŸŒก๏ธ The Hawking temperature of a black hole is derived using fundamental constants and the area of the event horizon, which is related to the black hole's mass.
  • โšซ The black hole is considered as part of the universe, receiving cosmic microwave background radiation, which contributes to its mass.
  • ๐ŸŒŒ The cosmic microwave background radiation has a temperature of approximately 2.7 Kelvin and affects the black hole's mass.
  • ๐Ÿ”ข The rate of change of the black hole's mass is calculated by considering the difference between the power emitted due to Hawking radiation and the power absorbed from cosmic microwave background radiation.
  • โ„Ž The use of Einstein's mass-energy equivalence principle (E=mcยฒ) simplifies the calculation of the rate of change of mass.
  • ๐Ÿ”„ Stefan-Boltzmann's law is applied to find the power emitted by the black hole due to Hawking radiation and the power absorbed from the cosmic microwave background.
  • ๐Ÿงฎ The algebraic manipulation of the equations leads to an expression for the rate of change of the black hole's mass in terms of fundamental constants and the black hole's mass.
  • โญ The black hole reaches thermal equilibrium when the rate of change of its mass is zero, which is derived by setting the derivative equal to zero and solving for the mass.
  • ๐ŸŒก๏ธ At thermal equilibrium, the temperature of the black hole is found to be equal to the temperature of the cosmic microwave background radiation.
  • ๐Ÿค” The script ends with a hint to explore the derivation of the temperature of a black hole, suggesting a deeper understanding of Hawking radiation.
Q & A
  • What is the topic of the discussion in the provided script?

    -The topic of the discussion is the calculation of the rate of change of a black hole's mass considering both Hawking radiation and the absorption of cosmic microwave background radiation.

  • What is the Hawking temperature of a black hole?

    -The Hawking temperature of a black hole is a theoretical temperature at which black holes emit radiation due to quantum effects near the event horizon. It is given by an expression involving fundamental constants such as the Planck constant, the speed of light, and the gravitational constant.

  • What is the significance of Stefan Boltzmann's constant in this context?

    -Stefan Boltzmann's constant is used to describe the power emitted by a black hole due to Hawking radiation, which is proportional to the fourth power of the temperature and the surface area of the black hole.

  • What is the role of the cosmic microwave background radiation in the black hole's mass change?

    -The cosmic microwave background radiation contributes to the mass of the black hole by being absorbed, which counteracts the mass loss due to Hawking radiation.

  • How does the black hole's mass change over time?

    -The black hole's mass changes over time due to the difference between the power emitted as Hawking radiation and the power absorbed from the cosmic microwave background radiation.

  • What is the relationship between the rate of change of energy and the rate of change of mass in the context of a black hole?

    -The rate of change of energy (dE/dt) is related to the rate of change of mass (dM/dt) through the equation dE/dt = c^2 * dM/dt, where c is the speed of light.

  • What is the significance of setting the rate of change of mass to zero?

    -Setting the rate of change of mass to zero signifies the point at which the black hole is in thermal equilibrium, neither gaining nor losing mass overall.

  • What is the expression for the mass of a black hole at thermal equilibrium?

    -The mass of a black hole at thermal equilibrium (M*) is given by an expression involving the speed of light, the Planck constant, the gravitational constant, Boltzmann's constant, and the temperature of the cosmic microwave background radiation.

  • What is the temperature of a black hole at thermal equilibrium?

    -At thermal equilibrium, the temperature of the black hole is equal to the temperature of the cosmic microwave background radiation.

  • How does the derivation of the temperature of a black hole relate to the concept of Hawking radiation?

    -The derivation of the temperature of a black hole is directly related to Hawking radiation, as it describes the temperature at which black holes emit this radiation due to quantum effects.

Outlines
00:00
๐ŸŒŒ Black Hole Mass Change Analysis

This paragraph delves into the complex dynamics of a black hole's mass change, considering it as part of the universe and its interaction with cosmic microwave background radiation. The script introduces the concept of Hawking temperature and Stefan Boltzmann's constant to calculate the rate of change of the black hole's mass. It outlines the algebraic process to determine the net energy change by considering both the emitted radiation due to Hawking and the absorbed cosmic microwave background radiation. The ultimate goal is to find the rate of change of the black hole's mass, which involves intricate calculations with fundamental constants and the area of the black hole's event horizon.

05:01
๐Ÿ”ญ Thermal Equilibrium of Black Holes

The second paragraph continues the exploration of black hole physics by examining the scenario where a black hole reaches thermal equilibrium with the cosmic microwave background radiation. It discusses the condition where the rate of mass change of the black hole becomes zero, leading to a state of balance between the radiation emitted due to Hawking temperature and the radiation absorbed from the background. The script provides a mathematical derivation to find the mass of the black hole at this equilibrium and reveals an intriguing result: the black hole's temperature matches the temperature of the background radiation. This section also touches upon the derivation of the temperature of a black hole, hinting at the profound implications of Hawking radiation.

Mindmap
Keywords
๐Ÿ’กHawking Temperature
Hawking Temperature refers to the theoretical temperature of a black hole, which is a result of quantum effects near the event horizon. It is named after physicist Stephen Hawking who first predicted this phenomenon. In the video, the concept is used to discuss the black hole's emission of radiation, which is a key factor in determining its rate of change in mass.
๐Ÿ’กStefan-Boltzmann Constant
The Stefan-Boltzmann Constant is a fundamental constant in physics that relates the total energy radiated from a black body in unit time to its temperature. In the script, it is used in the context of calculating the power emitted by the black hole due to Hawking radiation and the power absorbed from the cosmic microwave background radiation.
๐Ÿ’กEvent Horizon
The Event Horizon is the boundary around a black hole beyond which nothing can escape, not even light. The area of the event horizon is used in the script to calculate the power emitted by the black hole, as it is directly related to the black hole's size and the amount of radiation it emits.
๐Ÿ’กCosmic Microwave Background Radiation
Cosmic Microwave Background Radiation is the remnant thermal radiation from the early universe after the Big Bang. In the video, it is mentioned as a source of energy that contributes to the mass of the black hole, affecting its rate of change.
๐Ÿ’กEinstein's Mass-Energy Equivalence
Einstein's Mass-Energy Equivalence, represented by the equation E=mc^2, states that mass can be converted into energy and vice versa. In the script, this principle is applied to express the rate of change of the black hole's mass in terms of the power emitted and absorbed.
๐Ÿ’กThermal Equilibrium
Thermal Equilibrium is a state where the rate of change of mass of a black hole becomes zero, meaning the black hole is neither gaining nor losing energy. The script discusses the conditions under which a black hole would reach this state and how to calculate the corresponding mass.
๐Ÿ’กBlack Hole Mass
Black Hole Mass is a measure of the amount of matter that has been compressed into a black hole. The script explores how the mass of a black hole changes over time due to the emission of Hawking radiation and the absorption of cosmic microwave background radiation.
๐Ÿ’กHawking Radiation
Hawking Radiation is a theoretical process by which black holes lose mass over time due to quantum effects near the event horizon. The script discusses the calculation of the power emitted by a black hole through this process and its impact on the black hole's mass.
๐Ÿ’กPlanck Constant
The Planck Constant is a fundamental constant in quantum mechanics that relates the energy of a photon to its frequency. In the script, it is used in the derivation of the Hawking temperature formula and the calculation of the power emitted by the black hole.
๐Ÿ’กBoltzmann Constant
The Boltzmann Constant is a fundamental constant in physics that relates the temperature of a system to the average kinetic energy of its particles. In the script, it is used in the Stefan-Boltzmann law to calculate the power emitted by the black hole.
๐Ÿ’กGravitational Constant
The Gravitational Constant, denoted as G, is a fundamental constant in physics that quantifies the force of gravity between two bodies. In the script, it is used in the calculation of the area of the event horizon and the mass of the black hole at thermal equilibrium.
Highlights

Solving the black hole question from the International Physics Olympiad using the Hawking temperature formula.

Hawking temperature of a black hole is derived using fundamental constants and the area of the Event Horizon.

Considering the black hole as part of the universe, receiving cosmic microwave background radiation.

The black hole's mass change rate is influenced by both Hawking radiation emission and cosmic microwave background radiation absorption.

Using the equation E=mc^2 to relate the rate of change of energy to the rate of change of mass.

Applying Stefan-Boltzmann's law to calculate the power output due to Hawking radiation.

Deriving an algebraic expression for the rate of change of mass (dM/dt) in terms of fundamental constants.

The expression for dM/dt includes terms for both the emitted power due to Hawking radiation and the absorbed power from cosmic microwave background.

Simplifying the expression to isolate the rate of change of mass, showing a balance between emitted and absorbed power.

Setting the derivative equal to zero to find the black hole's mass at thermal equilibrium.

Rearranging the equation to solve for the mass of the black hole at thermal equilibrium (M*).

Finding an expression for M* that includes the cosmic microwave background temperature.

Demonstrating that at thermal equilibrium, the black hole's temperature equals the cosmic microwave background temperature.

The derivation of the temperature of a black hole at thermal equilibrium from the mass expression.

The surprising result that the black hole's temperature matches the cosmic microwave background temperature at equilibrium.

The importance of understanding the derivation of Hawking radiation for the temperature of a black hole.

The significance of the theoretical contribution to the understanding of black hole thermodynamics.

Transcripts
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