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The negative pion \(\left(\pi^{-}\right)\) is an unstable particle with an average lifetime of \(2.60 \times 10^{-8}\) s (measured in the rest frame of the pion). (a) If the pion is made to travel at very high speed relative to a laboratory, its average lifetime is measured in the laboratory to be \(4.20 \times 10^{-7} \mathrm{s}\) . Calculate the speed of the pion expressed as a fraction of \(c .\) (b) What distance, measured in the laboratory, does the pion travel during its average lifetime?

Short Answer

Expert verified
The speed of the pion is 0.998c, and it travels 125.3 meters.

Step by step solution

01

Understanding Time Dilation

When an object moves at high speed, time experienced by it is different from that observed in the stationary frame. This phenomenon is explained by the theory of relativity and is known as time dilation. The relationship can be expressed by the formula:\[ t = \frac{t_0}{\sqrt{1 - \frac{v^2}{c^2}}} \] where \( t \) is the time measured in the lab, \( t_0 \) is the proper time (pion's rest frame), \( v \) is the speed of the pion, and \( c \) is the speed of light.
02

Plugging Known Values Into Time Dilation Equation

Given \( t = 4.20 \times 10^{-7} \) s (lab frame) and \( t_0 = 2.60 \times 10^{-8} \) s (pion's rest frame), we plug these into the time dilation equation:\[ 4.20 \times 10^{-7} = \frac{2.60 \times 10^{-8}}{\sqrt{1 - \frac{v^2}{c^2}}} \]
03

Solving Time Dilation Equation for v/c

To find \( v/c \), we first isolate \( \sqrt{1 - \frac{v^2}{c^2}} \):\[ \sqrt{1 - \frac{v^2}{c^2}} = \frac{2.60 \times 10^{-8}}{4.20 \times 10^{-7}} \]Calculate the right side:\[ \frac{2.60 \times 10^{-8}}{4.20 \times 10^{-7}} = \frac{1}{16.15} \]Now square both sides to solve for \( \frac{v^2}{c^2} \):\[ 1 - \frac{v^2}{c^2} = \left( \frac{1}{16.15} \right)^2 \]\[ 1 - \frac{v^2}{c^2} = 0.00384 \]\[ \frac{v^2}{c^2} = 1 - 0.00384 = 0.99616 \]
04

Calculate the Pion's Speed as a Fraction of c

Taking the square root gives us \( \frac{v}{c} \):\[ \frac{v}{c} = \sqrt{0.99616} = 0.99808 \]
05

Calculate Distance Traveled in the Lab Frame

To find the distance, we use the formula \( d = v \times t \), where \( t \) is the time in the lab frame. First, convert \( \frac{v}{c} \) to \( v \):\( v = 0.99808 \times c \).Now calculate \( d \) as:\[ d = (0.99808 \cdot c) \times 4.20 \times 10^{-7} \]\[ d = 0.99808 \cdot 3 \times 10^8 \times 4.20 \times 10^{-7} \]\[ d = 1.253 \times 10^2 \text{ m} \]
06

Final Summary

The speed of the pion as a fraction of the speed of light is approximately \( 0.998 \), and it travels a distance of approximately \( 125.3 \) meters in the lab frame during its average lifetime.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Relativity
Relativity is a fundamental theory in physics developed by Albert Einstein. It introduces the concept that the laws of physics are the same for all non-accelerating observers, which revolutionized our understanding of space, time, and motion. One of its most famous aspects is time dilation, which occurs when an object moves at a significant fraction of the speed of light.
Time dilation means that time passes at different rates depending on the observer's frame of reference. When an object, like a pion, travels at high speeds relative to an observer in a stationary frame (such as a lab), the time experienced by the object appears to slow down.
The time dilation effect is mathematically expressed by the equation:
  • \( t = \frac{t_0}{\sqrt{1 - \frac{v^2}{c^2}}} \)
Here, \( t \) is the time measured in the stationary frame (lab), \( t_0 \) is the proper time experienced by the moving object, \( v \) is the object's speed, and \( c \) is the speed of light. This formula shows how time and speed are interrelated, demonstrating the profound effects of relativity.
Pions
Pions are subatomic particles and a part of the meson family, which are essential in particle physics. They play a critical role in mediating the strong nuclear force, the fundamental force responsible for holding atomic nuclei together.
These particles, often denoted as \( \pi^+ \), \( \pi^- \), and \( \pi^0 \), have different charges and lifetimes. The lifetime of the pion is usually very short, in the order of nanoseconds, particularly in a pion's rest frame.
Understanding pions provides insight into the complex interactions within atomic nuclei and the forces that govern the universe at a fundamental level. Their behavior, studied in high-energy physics experiments, can reveal unknown aspects of particle interactions and contribute to the development of theoretical models in particle physics.
Speed of Light
The speed of light, denoted as \( c \), is a universal constant crucial in the field of physics. Its value is approximately \( 3 \times 10^8 \) meters per second \( (m/s) \). This constant is significant because it represents the maximum speed at which information and matter can travel in the universe.
In the context of relativity and particle physics, the speed of light acts as a benchmark for measuring the speeds of fast-moving particles like pions. When particles approach fractions of the speed of light, relativistic effects such as time dilation become increasingly prominent.
The concept that nothing can travel faster than light is central to our understanding of the universe, influencing everything from the movement of galaxies to the fleeting existence of subatomic particles. Its role is pivotal in calculations and theories that seek to explain the universe's fundamental workings.
Particle Physics
Particle physics is the branch of physics that investigates the smallest known building blocks of the universe and the fundamental forces acting upon them. It explores the interactions and behaviors of elementary particles like quarks, leptons, bosons, and mesons including pions.
In experiments, high-energy particles are often used to collide with each other at nearly the speed of light, producing new particles in the process. This helps scientists explore and verify the laws of physics on a quantum level.
The study of particle physics has led to groundbreaking discoveries, like the Higgs boson, and helps us understand the conditions of the early universe, particularly after the Big Bang. Pions and their interactions are an integral part of ongoing research in this field, contributing to the exploration of unanswered questions about matter and energy.

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Most popular questions from this chapter

After being produced in a collision between elementary particles, a positive pion \(\left(\pi^{+}\right)\) must travel down a 1.90 -km-long tube to reach an experimental area. A \(\pi^{+}\) particle has an average lifetime (measured in its rest frame) of \(2.60 \times 10^{-8} \mathrm{s}\) ; the \(\pi^{+}\) we are considering has this lifetime. How fast must the \(\pi^{+}\) travel if it is not to decay before it reaches the end of the tube? (Since \(u\) will be very close to \(c,\) write \(u=(1-\Delta) c\) and give your answer in terms of \(\Delta\) rather than \(u .\) (b) The \(\pi^{+}\) has a rest energy of 139.6 \(\mathrm{MeV} .\) What is the total energy of the \(\pi^{+}\) at the speed calculated in part (a)?

Space pilot Mavis zips past Stanley at a constant speed relative to him of 0.800\(c .\) Mavis and Stanley start timers at zero when the front of Mavis's ship is directly above Stanley. When Mavis reads 5.00 s on her timer, she turns on a bright light under the front of her spaceship. (a) Use the Lorentz coordinate transformation derived in Example 37.6 to calculate \(x\) and \(t\) as measured by Stanley for the event of turning on the light. (b) Use the time dilation formula, Eq. \((37.6),\) to calculate the time interval between the two events (the front of the spaceship passing overhead and turning on the light) as measured by Stanley. Compare to the value of \(t\) you calculated in part (a). (c) Multiply the time interval by Mavis's speed, both as measured by Stanley, to calculate the distance she has traveled as measured by him when the light turns on. Compare to the value of \(x\) you calculated in part (a).

Measuring Speed by Radar. A baseball coach uses a radar device to measure the speed of an approaching pitched base-ball. This device sends out electromagnetic waves with frequency \(f_{0}\) and then measures the shift in frequency \(\Delta f\) of the waves reflected from the moving baseball. If the fractional frequency shift produced by a baseball is \(\Delta f / f_{0}=2.86 \times 10^{-7}\) , what is the baseball's speed in \(\mathrm{km} / \mathrm{h} ?\) (Hint: Are the waves Doppler- shifted a second time when reflected off the ball?

A source of electromagnetic radiation is moving in a radial direction relative to you. The frequency you measure is 1.25 times the frequency measured in the rest frame of the source. What is the speed of the source relative to you? Is the source moving toward you or away from you?

A spaceship moving at constant speed \(u\) relative to us broadcasts a radio signal at constant frequency \(f_{0 .}\) As the spaceship approaches us, we receive a higher frequency \(f ;\) after it has passed, we receive a lower frequency. (a) As the spaceship passes by, so it is instantaneously moving neither toward nor away from us, show that the frequency we receive is not \(f_{0}\) , and derive an expression for the frequency we do receive. Is the frequency we receive higher or lower than \(f_{0} ?\) (Hint: In this case, successive wave crests move the same distance to the observer and so they have the same transit time. Thus \(f\) equals 1\(/ T .\) Use the time dilation formula to relate the periods in the stationary and moving frames.) (b) A spaceship emits electromagnetic waves of frequency \(f_{0}=345 \mathrm{MHz}\) as measured in a frame moving with the ship. The spaceship is moving at a constant speed 0.758\(c\) relative to us. What frequency \(f\) do we receive when the spaceship is approaching us? When it is moving away? In each case what is the shift in frequency, \(f-f_{0} ?(\mathrm{c})\) Use the result of part (a) to calculate the frequency \(f\) and the frequency shift \(\left(f-f_{0}\right)\) we receive at the instant that the ship passes by us. How does the shift in frequency calculated here compare to the shifts calculated in part (b)?

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