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A pion is an elementary particle that, on average, disintegrates \(2.6 \times 10^{-8} \mathrm{~s}\) after creation in a frame at rest relative to the pion. An experimenter finds that pions created in the laboratory travel 13 m on average before disintegrating. How \(f\) ast are the pions traveling through the lab?

Short Answer

Expert verified
The speed of the pions traveling through the lab is \(5 \times 10^{7}\) m/s.

Step by step solution

01

Calculate the time need for a pion to travel 13m at rest

First, convert the given pion life, \(2.6 \times 10^{-8}\) s, into a time rate that can be used to determine the time it would take the pion to travel a distance of 13m at rest. This is calculated by dividing the distance the pion travels by its average rest lifespan, which gives the time in the frame moving with the pions. We represent the distance as \(d\) and the lifespan as \(T\). Therefore \(d/T = 13m / 2.6 \times 10^{-8}\) s.
02

Calculate the pions' speed

Given that speed (v) is distance divided by time, after finding the time required for pions to travel 13m in step 1, we can substitute the same into the speed formula \(v=d/t\) to find the pion speed. So \(v = d/t = 13m / (13m / 2.6 \times 10^{-8}\) s.

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Key Concepts

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

Elementary Particles
Elementary particles are the smallest known building blocks of the universe. Unlike atoms, which have complex structures consisting of a nucleus and orbiting electrons, elementary particles are not composed of other particles; they are fundamental in nature. The Standard Model of particle physics categorizes these particles into quarks, leptons, and bosons. Within this framework, a pion is a type of meson, which is a hadron created by the strong force interactions between quarks and antiquarks.

Pions play a significant role in explaining the forces that hold the atomic nucleus together. There are three types of pions: positive, negative, and neutral, each characterized by different charges and mass properties. Pions are unstable particles, which means they decay into lighter particles quite rapidly after their creation, typically on the order of nanoseconds. This rapid disintegration makes studying pions challenging but also provides insights into the fundamental forces and symmetries of the universe.
Relativistic Effects
Relativistic effects come into play when particles are traveling at speeds close to the speed of light, denoted by the symbol 'c'. At these high velocities, the rules of Newtonian mechanics no longer apply, and we must look to Einstein's theory of relativity to describe the motion and interactions of particles. In this context, we often find that time, mass, and length seem to change when measured from different frames of reference.

For pions traveling through a lab, relativistic effects will manifest if their speed is a significant fraction of the speed of light. This can result in phenomena such as length contraction and time dilation, which we'll discuss more in the next section. Relativistic effects are crucial for understanding how particles like pions behave at high speeds and also for ensuring that experimental measurements align with theoretical predictions.
Time Dilation
Time dilation is a relativistic effect whereby time, as measured by a clock moving relative to an observer, appears to pass more slowly when compared to a clock at rest with respect to the observer. This concept is a cornerstone of Einstein's theory of special relativity and has profound implications for high-velocity particles, such as pions in our exercise.

In the context of the exercise, time dilation explains why pions, which disintegrate after an average lifespan of approximately 26 nanoseconds when at rest, can travel a distance of 13 meters in the laboratory frame before decaying. The high speed causes time in the moving (pion) frame to stretch out, or dilate, relative to the time in the laboratory frame. When experiments such as these are performed, and pions are found to travel further than they should, given their brief existence, it confirms the effects predicted by relativity. Additionally, it highlights the importance of considering both the velocity of particles and their relativistic effects when conducting high-energy physics experiments.

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Most popular questions from this chapter

A plank. fixed ro a sled at rest in frame \(S\), is of length \({L}_{0}\) and makes an angle of \(L_{0}\) with the \(x\) -axis. Later. the sled zooms through frame \(S\) at constant speed \(v\) parallel to the r-axis. Show that according to an observer who remains at rest in frame \(S\). the length of the plank is now\(L=L_{0} \sqrt{1-\frac{v^{2}}{c^{2}} \cos \theta_{0}}\) and the angle it makes with the \(x\) -axis is $$ \theta=\tan ^{-1}\left(\gamma_{v} \tan \theta_{0}\right) $$.

A chin plate has a round hole whose diameter in its rest frame is \(D\). The plate is parallel to the ground and moving upward, in the \(+y\) direction, relative to the ground. A thin round disk whose diameter in its rest frame is \(D\) is also parallel to the ground but moving in the \(+x\) direction relative to it. In the frame of the ground, the plate and disk are on course so that the centers of the hole and disk will at some point coincide. The disk is contracted, but the hole in the plate is not, so the disk will pass through the hole. Now consider the frame of the disk. The disk is of diameter \(D\). but the hole is contracted. Can the disk pass through the hole, and if so, how?

You stand at the center of your. \(100 \mathrm{~m}\) spaceship and watch Anna's identical ship pass at \(0.6 \mathrm{c} .\) At \(t=0\) on your wristwatch. Anna, at the center of her ship, is directly across from you and her wristwatch also reads \(0 .\) (a) A friend on your ship, \(24 \mathrm{~m}\) from you in a direction toward the tail of Anna's passing ship, looks at a clock directly across from him on Anna's ship. What does it read? (b) Your friend now steps onto Anna's ship. By this very act, he moves from a frame where Anna is one age to a frame where she is another. What is the difference in these ages? Explain. (Hint: Your friend moves to Anna's frame, where the time is whatever the clock at the location reads.) (c) Answer parts (a) and (b) for a friend \(24 \mathrm{~m}\) from you but in a direction toward the front of Anna's passing ship. (d) What happens to the reading on a clock when you accelerate toward it? Away from it?

In the collision shown, energy is conserved. because both objects have the same speed and mass after as before the collision. Since the collision merely reverses the velocities, the final (total) momentum is opposite the initial. Thus, momentum can be conserved ooly if it is zero. (a) Using the relativistically correct expression for momentum, show that the total momentum is zero that momentum is conserved. (Masses are in arbitrary units.) (b) Using the relativistic velocity transformation, find the four velocities in a frame moving to the right at \(0.6 c\) (c) Verify that momentum is conserved in che new frame.

You are floating in space when you notice a flying saucer circling you. Each time it passes in front of you, you note the reading on its clock. Do you see its clock advancing faster or slower than your wristwatch? Does the space alien see your wristwatch advancing faster or slower than his clock? Explain.

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