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In Compton scattering, a photon scatters elastically off an electron initially at rest. Suppose the incoming photon has momentum of \(1.0 \times 10^{-21} \mathrm{~kg} \cdot \mathrm{m} / \mathrm{s} \hat{\imath}\). The scattered photon's momentum is \(1.8 \times 10^{-22} \mathrm{~kg} \cdot \mathrm{m} / \mathrm{s} \hat{\imath}-3.1 \times 10^{-28} \mathrm{~kg} \cdot \mathrm{m} / \mathrm{s} \hat{\jmath}\). Find the mo- mentum of the recoiling electron.

Short Answer

Expert verified
The electron's momentum is \(8.2 \times 10^{-22} \hat{\imath} + 3.1 \times 10^{-28} \hat{\jmath} \ \mathrm{kg} \cdot \mathrm{m}/\mathrm{s}\).

Step by step solution

01

Identify Initial and Final Momentums

The initial momentum of the system is the momentum of the incoming photon, which is given as \(1.0 \times 10^{-21} \ \mathrm{kg} \cdot \mathrm{m}/\mathrm{s} \ \hat{\imath}\). The momentum of the scattered photon after the collision is \(1.8 \times 10^{-22} \ \mathrm{kg} \cdot \mathrm{m}/\mathrm{s} \ \hat{\imath} - 3.1 \times 10^{-28} \ \mathrm{kg} \cdot \mathrm{m}/\mathrm{s} \ \hat{\jmath}\). The electron is initially at rest, so its initial momentum is \(0\).
02

Apply Conservation of Momentum

Since momentum is conserved, the total initial momentum must equal the total final momentum. We have:\[\vec{p}_{\text{initial}} = \vec{p}_{\text{photon final}} + \vec{p}_{\text{electron final}}\]Where \(\vec{p}_{\text{electron final}}\) is the momentum of the recoiling electron we are trying to find. Thus,\[1.0 \times 10^{-21} \ \hat{\imath} = (1.8 \times 10^{-22} \ \hat{\imath} - 3.1 \times 10^{-28} \ \hat{\jmath}) + \vec{p}_{\text{electron final}}\]
03

Solve for the Electron's Momentum in Each Direction

We solve for \(\vec{p}_{\text{electron final}}\) by separating it into \(\hat{\imath}\) and \(\hat{\jmath}\) components. For \(\hat{\imath}\):\[p_{e,x} = 1.0 \times 10^{-21} - 1.8 \times 10^{-22}= 8.2 \times 10^{-22} \ \mathrm{kg} \cdot \mathrm{m}/\mathrm{s}\]For \(\hat{\jmath}\):\[p_{e,y} = - ( -3.1 \times 10^{-28})= 3.1 \times 10^{-28} \ \mathrm{kg} \cdot \mathrm{m}/\mathrm{s}\]
04

Combine Components to Find Electron's Total Momentum

The total momentum of the electron is the vector sum of its \(\hat{\imath}\) and \(\hat{\jmath}\) components:\[\vec{p}_{\text{electron final}} = 8.2 \times 10^{-22} \ \hat{\imath} + 3.1 \times 10^{-28} \ \hat{\jmath} \ \mathrm{kg} \cdot \mathrm{m}/\mathrm{s}\]

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Key Concepts

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

Momentum Conservation
In the phenomenon of Compton scattering, momentum conservation plays a crucial role. Think of momentum as the 'oomph' an object has when it's moving, which depends on both its mass and velocity. The conservation of momentum states that in an isolated system, the total momentum before an event is equal to the total momentum after the event. This is particularly vital in Compton scattering, where a photon, a particle of light, interacts with an electron.
- Before the collision, the total momentum is that of the incoming photon since the electron is initially at rest. - As the photon strikes the electron, the momentum is redistributed between the scattered photon and the now-moving electron. This conservation law allows us to set up equations that account for all momentum components before and after the interaction. By using these, we can find unknown values like the momentum of recoiling particles, such as the electron after it has interacted with the photon.
Photon Interactions
Photons are remarkable particles of light that don't have mass, yet they carry momentum. In the context of Compton scattering, photon interactions are central because they showcase how light can influence particles like electrons, which do have mass.
- When a photon approaches an electron, its energy and momentum can be transferred to the electron upon collision. - This interaction alters the photon's path and reduces its momentum, a phenomenon described by the principles of quantum mechanics. The photon's change in direction and momentum is evidence of the interaction. By measuring this change, scientists can deduce valuable information about the internal structure of materials and the properties of photons themselves. The decreased momentum of the photon after scattering results in an increase in wavelength, a concept known as the Compton effect.
Recoiling Electron
When a photon and an electron interact through Compton scattering, the electron doesn't just stay put; it recoils, gaining the momentum initially carried by the photon. This recoiling electron is a key part of understanding momentum conservation in these interactions.
- Initially, the electron is stationary, waiting for the photon to arrive. - Once struck, it gains kinetic energy and moves away with newfound momentum. To calculate the electron's momentum after the collision, we consider the momentum transferred from the photon, factoring in its new direction and speed. This calculation involves decomposing the momentum conservation equation into components, typically along the x and y axes. The electron's acquired momentum demonstrates how energy and momentum are shared between particles during such quantum interactions. Understanding these concepts helps explain how energy can be transferred in atomic-scale processes, shedding light on fundamental physical theories.

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