Solving Electron Acceleration and Reflection Problems

In summary, we calculated the speed of the accelerated electrons to be 4.55 x 10^6 m/s, their De Broglie wavelength to be 0.16 nm, and their angle of reflection to be approximately 44.7 degrees.
  • #1
hayowazzup
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Homework Statement


Electrons are accelerated from rest by a voltage of 59.0 V. After that acceleration:
1.What is their speed?
2.What is their De Broglie wavelength?
3.The accelerated electrons are then reflected by a crystal with crystal spacing d of 0.085 nm. Through which angle are they reflected?

h = 6.63 × 10–34 J.s, c = 3 × 108 m/s, Mass of e = 9.11 × 10–31 kg, e = 1.6 × 10–19 C.

Homework Equations





The Attempt at a Solution


1. √((2*e*V)/massofe) = √((2*1.6 × 10–19 *59)/9.11 × 10–31 ) = 4552414.59 m/s
2. λ = h/p = h / √(2*h*e*massofe) = 6.63 × 10–34 / √((2*1.6 × 10–19 * 9.11 × 10–31 ) * (1E-9) = 0.16 nm
3. 2dsin (θ) = m λ
= sin-1 (1* 0.16 / (2 * 0.085)) = 70 ...<=== i m stuck because the answer in the book is 39.8
i really need help
 
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  • #2


Hello! I can help you with your questions.

1. Your calculation for the speed of the electrons is correct. However, it is given in m/s, not in nm/s. So the correct answer would be 4.55 x 10^6 m/s.

2. Your calculation for the De Broglie wavelength is also correct. However, the crystal spacing is given in nm, so the wavelength should also be in nm. Therefore, the correct answer would be 0.16 nm.

3. The formula you used for the angle of reflection is correct, but you made a mistake in your calculation. The angle of reflection should be in radians, not degrees. So the correct calculation would be sin-1 (1* 0.16 / (2 * 0.085)) = 0.78 radians. To convert this to degrees, you can multiply by 180/π, which gives an angle of 44.7 degrees. This is closer to the answer given in the book (39.8 degrees) but may still be slightly off due to rounding errors.

I hope this helps! Let me know if you have any other questions or need further clarification.
 

Related to Solving Electron Acceleration and Reflection Problems

1. What is the purpose of solving electron acceleration and reflection problems?

The purpose of solving electron acceleration and reflection problems is to understand and control the movement of electrons in various systems and devices such as particle accelerators, plasma reactors, and electron microscopes. This knowledge is crucial in advancing technologies in fields such as energy, medicine, and communications.

2. How do you calculate electron acceleration and reflection?

Electron acceleration and reflection can be calculated using principles of classical and quantum mechanics, as well as electromagnetic theory. The equations used to calculate these processes depend on the specific system and conditions, and may involve factors such as electric fields, magnetic fields, and particle interactions.

3. What are some common challenges in solving electron acceleration and reflection problems?

Some common challenges in solving electron acceleration and reflection problems include accurately modeling the complex interactions between particles and fields, accounting for the effects of relativity and quantum mechanics, and incorporating the effects of external factors such as temperature and pressure. Additionally, obtaining precise experimental data to validate theoretical calculations can also be a challenge.

4. How can electron acceleration and reflection be optimized?

Electron acceleration and reflection can be optimized by carefully designing and adjusting the parameters of the system, such as the strength and direction of applied fields, the geometry of the device, and the properties of the particles themselves. Computer simulations can also aid in optimizing these processes by allowing for virtual testing and analysis of different scenarios.

5. What are the real-world applications of solving electron acceleration and reflection problems?

Solving electron acceleration and reflection problems has numerous real-world applications, such as in medical imaging and treatment, where electron beams are used to generate X-rays for imaging and to target and destroy cancer cells. It is also crucial in the development of particle accelerators for scientific research, and in the manufacturing of microchips and other electronic devices.

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