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The problem statement:
What I have managed to do:
This problem seems a bit tricky at first because it is talking about rotating a crystal while also changing the voltage - changing two variables at the same time makes no sense to me. This is why I assumed that while we change the voltage we do it at a constant angle ##\vartheta##! Distance ##d## between crystal planes which is a material property is also constant so I can write two equations which I can equate and solve for a number ##N_1## (which I don't know yet):
\begin{align}
\left.
\begin{aligned}
\substack{\text{Brag's law for voltage $U_1$}}\longrightarrow\quad2d\sin\vartheta &= N_1 \lambda_1\\
\substack{\text{Brag's law for voltage $U_2$}}\longrightarrow\quad2d\sin\vartheta&=\!\!\!\! \smash{\underbrace{(N_1+1)}_{\substack{\text{At voltage $U_2$}\\\text{I get an extra}\\\text{mirror reflection}}}}\!\!\!\lambda_1\\
\end{aligned}
\quad
\right\}
\qquad
N_1 \lambda_1 &= (N_1+1) \lambda_2\\
\frac{N_1+1}{N_1} &= \frac{\lambda_1}{\lambda_2}\\
1+\frac{1}{N_1} &= \frac{\lambda_1}{\lambda_2}\\
\frac{1}{N_1} &= \frac{\lambda_1}{\lambda_2} - 1\\
N_1 &= \frac{1}{\lambda_1/\lambda_2 -1}
\end{align}
Ok so I can calculate ##N_1## if i know the ratio ##\lambda_1/\lambda_2## which I can get from voltages (with a litle help of Lorentz invariant):
\begin{align}
\substack{\text{Lorentz invariance}}\longrightarrow p^2c^2 &= E^2 - {E_0}^2\\
p^2c^2 &= (E_k + E_0)^2 - {E_0}^2\\
p^2c^2 &= {E_k}^2 + 2E_kE_0 + {E_0}^2 - {E_0}^2\\
p^2c^2 &= {E_k}^2 + 2E_kE_0\\
p &= \frac{\sqrt{{E_k}^2 + 2E_kE_0}}{c}\\
~\\
~\\
~\\
\substack{\text{I use Lorentz invariance}\\\text{and De Broglie's hypothesis}\\\text{to calculate ratio $\lambda_1/\lambda_2$}} \longrightarrow \frac{\lambda_1}{\lambda_2} &= \frac{h p_2}{p_1 h} = \frac{p_2}{p_1} = \frac{\sqrt{{E_{k2}}^2 + 2E_{k2}E_0}}{\sqrt{{E_{k1}}^2 + 2E_{k1}E_0}} = \sqrt{\frac{e^2{U_{2}}^2 + 2eU_{2}E_0}{e^2{U_{1}}^2 + 2eU_{1}E_0}}= \\
&= \sqrt{\frac{e^2\cdot 214^2V^2 + 2e\cdot 214V\cdot0.51\times10^6eV}{e^2\cdot 137^2V^2 + 2e\cdot 137V\cdot0.51\times10^6eV}} = 1.25
\end{align}
If I use this ratio I can calculate that ##\boxed{N_1=4}##.
What I haven't managed to figure out:
Question 1:
Does my result ##N_1 = 4## mean that at voltage ##U_1=137V## we get the fourth maximum or does it mean that If I change angle ##\vartheta## I will get maximums at ##4## different angles? Is it both? Please explain!
Question 2:
I used De Broglie relation and Lorentz invariant to calculate
\begin{align}
\lambda_1&=1.04\times10^{-10}m\\
\lambda_2&=8.37\times10^{-11}m
\end{align}
but I have absolutely no idea on how to calculate the distance between the crystal planes ##d##. Can anyone give me a hint?
We are observing an electron diffraction on a "Ni" crystall. We point
the narrow beam of electrons on a crystall which can be rotated so that
we are changing the angle ##\vartheta## between an incomming beam and a crystal
planes.
We are also increasing the the voltage which accelerates the
electrons. By increasing the voltage the number of angles at which we
get mirror reflection also increases.
An extra mirror reflection on a same set of crystal planes appears
when we accelerate electrons with a voltage ##U_1=137V##, while next one
appears at voltage ##U_2=214V##.
How many angles, at which we get a mirror reflection, we get when
using voltage ##U_1=137V##? What is the distance ##d## between crystal planes?
What I have managed to do:
This problem seems a bit tricky at first because it is talking about rotating a crystal while also changing the voltage - changing two variables at the same time makes no sense to me. This is why I assumed that while we change the voltage we do it at a constant angle ##\vartheta##! Distance ##d## between crystal planes which is a material property is also constant so I can write two equations which I can equate and solve for a number ##N_1## (which I don't know yet):
\begin{align}
\left.
\begin{aligned}
\substack{\text{Brag's law for voltage $U_1$}}\longrightarrow\quad2d\sin\vartheta &= N_1 \lambda_1\\
\substack{\text{Brag's law for voltage $U_2$}}\longrightarrow\quad2d\sin\vartheta&=\!\!\!\! \smash{\underbrace{(N_1+1)}_{\substack{\text{At voltage $U_2$}\\\text{I get an extra}\\\text{mirror reflection}}}}\!\!\!\lambda_1\\
\end{aligned}
\quad
\right\}
\qquad
N_1 \lambda_1 &= (N_1+1) \lambda_2\\
\frac{N_1+1}{N_1} &= \frac{\lambda_1}{\lambda_2}\\
1+\frac{1}{N_1} &= \frac{\lambda_1}{\lambda_2}\\
\frac{1}{N_1} &= \frac{\lambda_1}{\lambda_2} - 1\\
N_1 &= \frac{1}{\lambda_1/\lambda_2 -1}
\end{align}
Ok so I can calculate ##N_1## if i know the ratio ##\lambda_1/\lambda_2## which I can get from voltages (with a litle help of Lorentz invariant):
\begin{align}
\substack{\text{Lorentz invariance}}\longrightarrow p^2c^2 &= E^2 - {E_0}^2\\
p^2c^2 &= (E_k + E_0)^2 - {E_0}^2\\
p^2c^2 &= {E_k}^2 + 2E_kE_0 + {E_0}^2 - {E_0}^2\\
p^2c^2 &= {E_k}^2 + 2E_kE_0\\
p &= \frac{\sqrt{{E_k}^2 + 2E_kE_0}}{c}\\
~\\
~\\
~\\
\substack{\text{I use Lorentz invariance}\\\text{and De Broglie's hypothesis}\\\text{to calculate ratio $\lambda_1/\lambda_2$}} \longrightarrow \frac{\lambda_1}{\lambda_2} &= \frac{h p_2}{p_1 h} = \frac{p_2}{p_1} = \frac{\sqrt{{E_{k2}}^2 + 2E_{k2}E_0}}{\sqrt{{E_{k1}}^2 + 2E_{k1}E_0}} = \sqrt{\frac{e^2{U_{2}}^2 + 2eU_{2}E_0}{e^2{U_{1}}^2 + 2eU_{1}E_0}}= \\
&= \sqrt{\frac{e^2\cdot 214^2V^2 + 2e\cdot 214V\cdot0.51\times10^6eV}{e^2\cdot 137^2V^2 + 2e\cdot 137V\cdot0.51\times10^6eV}} = 1.25
\end{align}
If I use this ratio I can calculate that ##\boxed{N_1=4}##.
What I haven't managed to figure out:
Question 1:
Does my result ##N_1 = 4## mean that at voltage ##U_1=137V## we get the fourth maximum or does it mean that If I change angle ##\vartheta## I will get maximums at ##4## different angles? Is it both? Please explain!
Question 2:
I used De Broglie relation and Lorentz invariant to calculate
\begin{align}
\lambda_1&=1.04\times10^{-10}m\\
\lambda_2&=8.37\times10^{-11}m
\end{align}
but I have absolutely no idea on how to calculate the distance between the crystal planes ##d##. Can anyone give me a hint?
Last edited: