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For a cartain metal, the K obsorption ed...

For a cartain metal, the `K` obsorption edge is at `0.72 Å`. The wavelength of `K_(alpha), K_(beta). And K_(gamma)` lines of of `K` series are `0.210 Å , 0.192 Å, and 0.180 Å, respectively. The eneggies of `K, L and M` orbit are `E_(K), E_(L) and E_(M)`, respectively. Then

A

`E_(K) = - 13.04 keV`

B

`E_(L) = - 7.52 keV`

C

`E_(M) = - 3.21 keV`

D

`E_(K) = - 13.04 keV`

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To solve the problem, we need to calculate the energies of the K, L, and M orbits based on the given absorption edge and the wavelengths of the K series lines. Here's a step-by-step solution: ### Step 1: Calculate the Energy of the K Absorption Edge The energy corresponding to the K absorption edge can be calculated using the formula: \[ E = \frac{hc}{\lambda} \] where: - \( h \) is Planck's constant (\( 4.1357 \times 10^{-15} \, \text{eV s} \)) - \( c \) is the speed of light (\( 3 \times 10^8 \, \text{m/s} \)) - \( \lambda \) is the wavelength in meters. Given that the K absorption edge is at \( 0.72 \, \text{Å} = 0.072 \, \text{nm} \), we convert this to nanometers: \[ \lambda = 0.072 \, \text{nm} \] Now, substituting the values into the equation: \[ E_K = \frac{(4.1357 \times 10^{-15} \, \text{eV s})(3 \times 10^8 \, \text{m/s})}{0.072 \, \text{nm}} = \frac{1240 \, \text{eV nm}}{0.072 \, \text{nm}} \approx 72.09 \, \text{keV} \] ### Step 2: Calculate the Energy of Kα, Kβ, and Kγ Lines Using the same formula for the Kα, Kβ, and Kγ lines: 1. **For Kα (0.210 Å = 0.0210 nm)**: \[ E_{K\alpha} = \frac{1240 \, \text{eV nm}}{0.0210 \, \text{nm}} \approx 59.04 \, \text{keV} \] 2. **For Kβ (0.192 Å = 0.0192 nm)**: \[ E_{K\beta} = \frac{1240 \, \text{eV nm}}{0.0192 \, \text{nm}} \approx 64.58 \, \text{keV} \] 3. **For Kγ (0.180 Å = 0.0180 nm)**: \[ E_{K\gamma} = \frac{1240 \, \text{eV nm}}{0.0180 \, \text{nm}} \approx 68.88 \, \text{keV} \] ### Step 3: Calculate the Energies of the K, L, and M Orbits Now we can find the energies of the K, L, and M orbits using the previously calculated energies: 1. **Energy of K shell (\( E_K \))**: \[ E_K = E_{K\alpha} - E_K = 59.04 \, \text{keV} - 72.09 \, \text{keV} = -13.05 \, \text{keV} \] 2. **Energy of L shell (\( E_L \))**: \[ E_L = E_{K\beta} - E_K = 64.58 \, \text{keV} - 72.09 \, \text{keV} = -7.51 \, \text{keV} \] 3. **Energy of M shell (\( E_M \))**: \[ E_M = E_{K\gamma} - E_K = 68.88 \, \text{keV} - 72.09 \, \text{keV} = -3.21 \, \text{keV} \] ### Summary of Results - \( E_K \approx -13.05 \, \text{keV} \) - \( E_L \approx -7.51 \, \text{keV} \) - \( E_M \approx -3.21 \, \text{keV} \) ### Final Answer The energies of the K, L, and M orbits are approximately: - \( E_K = -13.05 \, \text{keV} \) - \( E_L = -7.51 \, \text{keV} \) - \( E_M = -3.21 \, \text{keV} \)

To solve the problem, we need to calculate the energies of the K, L, and M orbits based on the given absorption edge and the wavelengths of the K series lines. Here's a step-by-step solution: ### Step 1: Calculate the Energy of the K Absorption Edge The energy corresponding to the K absorption edge can be calculated using the formula: \[ E = \frac{hc}{\lambda} \] where: ...
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