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Consider the following decay process: \(\pi^{+} \rightarrow \mu^{+}+v .\) The mass of the pion \(\left(\pi^{+}\right)\) is \(139.6 \mathrm{MeV} / c^{2},\) the mass of the muon \(\left(\mu^{+}\right)\) is \(105.7 \mathrm{MeV} / c^{2},\) and the mass of the neutrino \((v)\) is negligible. If the pion is initially at rest, what is the total kinetic energy of the decay products?

Short Answer

Expert verified
Answer: The total kinetic energy of the decay products is 33.9 MeV.

Step by step solution

01

Conservation of Energy

We'll start by applying the conservation of energy. In this decay process, the total energy must be conserved. This means that the initial energy of the pion at rest is equal to the final combined energy of the muon and neutrino: \(E_{initial} = E_{final}\) Since the pion is initially at rest, its energy is just its rest mass energy, given by \(E_{\pi} = m_{\pi}c^2\). The energies of the muon and neutrino after the decay are denoted as \(E_{\mu}\) and \(E_{\nu}\), respectively. So, we can write the energy conservation equation as: \(m_{\pi}c^2 = E_{\mu} + E_{\nu}\)
02

Conservation of Momentum

Since the pion is initially at rest, its momentum is zero. After the decay, the total momentum of the decay products, muon and neutrino, must also be zero to conserve momentum: \(p_{\pi} = p_{\mu} + p_{\nu} = 0\)
03

Relativistic Energy-Momentum Relation

We can use the relativistic energy-momentum relation to express the energies and momenta of the decay products in terms of their masses and velocities. The relation for each particle is given by: \(E^2 = (mc^2)^2 + (pc)^2\) Applying this relation for the muon and neutrino, we get: \(E_{\mu}^2 = (m_{\mu}c^2)^2 + (p_{\mu}c)^2\) \(E_{\nu}^2 = (p_{\nu}c)^2\) Note that we didn't include a mass term for the neutrino, since the mass of the neutrino \((v)\) is negligible.
04

Total Kinetic Energy

We want to find the total kinetic energy of the decay products. This is given by the sum of the kinetic energies of the muon and neutrino: \(K_{total} = K_{\mu} + K_{\nu}\) Remember that the kinetic energy of a particle is given by \(K = E - mc^2\). Therefore, we can write: \(K_{total} = (E_{\mu} - m_{\mu}c^2) + (E_{\nu})\) We can substitute the expressions for \(E_{\mu}\) and \(E_{\nu}\) from the energy conservation equation: \(K_{total} = (m_{\pi}c^2 - E_{\nu}) - m_{\mu}c^2 + E_{\nu} = m_{\pi}c^2 - m_{\mu}c^2\) Now, we can plug in the given values for the masses of the pion and muon: \(K_{total} = (139.6 \mathrm{MeV} - 105.7 \mathrm{MeV})\) Calculating the difference, we get: \(K_{total} = 33.9 \text{ MeV}\) Therefore, the total kinetic energy of the decay products (muon and neutrino) is \(\boxed{33.9\text{ MeV}}\).

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Most popular questions from this chapter

Octavio, traveling at a speed of \(0.60 c,\) passes Tracy and her barn. Tracy, who is at rest with respect to her barn, says that the barn is 16 m long in the direction in which Octavio is traveling, \(4.5 \mathrm{m}\) high, and $12 \mathrm{m}$ deep. (a) What does Tracy say is the volume of her barn? (b) What volume does Octavio measure?
A rectangular plate of glass, measured at rest, has sides \(30.0 \mathrm{cm}\) and \(60.0 \mathrm{cm} .\) (a) As measured in a reference frame moving parallel to the 60.0 -cm edge at speed \(0.25 c\) with respect to the glass, what are the lengths of the sides? (b) How fast would a reference frame have to move in the same direction so that the plate of glass viewed in that frame is square?
Starting with the energy-momentum relation \(E^{2}=E_{0}^{2}+\) \((p c)^{2}\) and the definition of total energy, show that $(p c)^{2}=K^{2}+2 K E_{0}[\mathrm{Eq} .(26-11)]$.
A futuristic train moving in a straight line with a uniform speed of \(0.80 c\) passes a series of communications towers. The spacing between the towers, according to an observer on the ground, is \(3.0 \mathrm{km} .\) A passenger on the train uses an accurate stopwatch to see how often a tower passes him. (a) What is the time interval the passenger measures between the passing of one tower and the next? (b) What is the time interval an observer on the ground measures for the train to pass from one tower to the next?
Show that Eq. \((26-11)\) reduces to the nonrelativistic relationship between momentum and kinetic energy, \(K \approx p^{2} /(2 m),\) for \(K<E_{0}\).
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