Use special relativity and Newton’s law of gravitation to show that a photon of mass m = E/c² just grazing the Sun will be deflected by an angle ∆θ given by ∆θ = 2GM/c²R, where G is the gravitational constant, R and M are the radius and mass of the Sun, and c is the speed of light. Put in values and show ∆θ = 0.87". (General Relativity predicts an angle twice as large, 1.74".)
Ch. 44 - Astrophysics and Cosmology
Giancoli Douglas5th editionPhysics for Scientists and EngineersISBN: 9780137488179Not the one you use?Change textbook
Chapter 39, Problem 42
At approximately what time had the universe cooled below the threshold temperature for producing (a) kaons (M ≈ 500 MeV/ c²), (b) Y (M ≈ 9500 MeV/c²), and (c) muons (M ≈ 100 MeV/c²)?
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Understand the relationship between temperature and energy: The energy of particles in the early universe is related to the temperature by the equation \( E \approx k_B T \), where \( E \) is the energy, \( k_B \) is the Boltzmann constant, and \( T \) is the temperature. For relativistic particles, \( E \) can also be approximated as \( mc^2 \), where \( m \) is the particle's mass and \( c \) is the speed of light.
Convert the mass of each particle into energy: Use the given masses of the particles (in \( \text{MeV}/c^2 \)) to calculate their corresponding energy thresholds. For example, for kaons, \( E_{kaon} = 500 \text{ MeV} \), for \( \Upsilon \), \( E_{\Upsilon} = 9500 \text{ MeV} \), and for muons, \( E_{muon} = 100 \text{ MeV} \).
Relate the energy to temperature: Use the equation \( T = \frac{E}{k_B} \) to find the temperature threshold for each particle. Here, \( k_B \) is the Boltzmann constant, which in natural units is approximately \( 1 \text{ MeV}/\text{K} \). This simplifies the calculation to \( T \approx E \) (in MeV) when using natural units.
Determine the time-temperature relationship: In the early universe, the temperature \( T \) is related to time \( t \) by the equation \( T \propto \frac{1}{\sqrt{t}} \). This means that as the universe expands and time increases, the temperature decreases. Rearrange this relationship to express time as \( t \propto \frac{1}{T^2} \).
Calculate the approximate time for each particle: Substitute the temperature thresholds for kaons, \( \Upsilon \), and muons into the time-temperature relationship to estimate the time at which the universe cooled below the threshold for producing each particle. Ensure the units are consistent when performing this calculation.

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Key Concepts
Here are the essential concepts you must grasp in order to answer the question correctly.
Temperature and Particle Production
In the early universe, temperature played a crucial role in determining which particles could be produced. As the universe expanded, it cooled, and only particles with masses lower than the thermal energy available could be created. The threshold temperature for producing a particle is directly related to its mass, as described by the equation E = mc², where E is the energy equivalent of the mass.
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Cosmic Timeline
The cosmic timeline refers to the sequence of events in the history of the universe, from the Big Bang to the present. Key milestones include the formation of fundamental particles, nucleosynthesis, and the emergence of atoms. Understanding this timeline helps in estimating when specific particles could form based on the universe's temperature at various stages.
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Mass-Energy Equivalence
Mass-energy equivalence, encapsulated in Einstein's famous equation E = mc², indicates that mass can be converted into energy and vice versa. This principle is fundamental in particle physics, as it allows us to calculate the energy required to create particles with specific masses. For instance, to produce a kaon, the universe must have cooled to a temperature corresponding to its mass-energy threshold.
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