Правка разделов «Problem», «Solution», «0. Write down the given data (a purely f»
en/6.6.3.md
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| − | ### | ||
| + | ### Problem | ||
| − | $6.6.3.$ | ||
| + | $6.6.3.$ | ||
| + | The saturated vapor pressure of water at $18^{\circ}C$ is $2 \cdot 10^{3} \ Pa$, and its dielectric constant is 1.0078. From these data, find the average dipole moment of a water molecule in an electric field of strength $10^{3}$ V/m. Reference books give the dipole moment of water as $-0.61 \cdot 10^{-29} C \cdot m$. How can the discrepancy in the results be explained? | ||
| + | |||
| ### Solution | |||
| − | 12 | ||
| + | Before looking at the solution, you can review the first solution method (the second one is also possible, for broadening your knowledge) of problem $6.6.2$ and then try to solve this one. | ||
| − | #### Answer | ||
| + | #### 0. Write down the given data (a purely formal step to make the solution clear). | ||
| − | |||
| + | $\varepsilon = 1.0078$ | ||
| + | |||
| + | $E = 10^{3} \ V/m$ | ||
| + | |||
| + | $T = 18^{\circ}C = 291 \ K$ | ||
| + | |||
| + | $\varepsilon_{0} = 8.85 \cdot 10^{-12} \ F/m$ | ||
| + | |||
| + | $P = 2 \cdot 10^{3} \ Pa$ | ||
| + | |||
| + | $p' = -0.61 \cdot 10^{-29} \ C \cdot m$ | ||
| + | |||
| + | $K = 1.38 \cdot 10^{-23} \ J/K$ | ||
| + | |||
| + | #### 1. Find the answer to the first question. | ||
| + | |||
| + | We will find the answer by working backwards, that is, we write the formula for the dipole moment and start from there. | ||
| + | |||
| + | \[ | ||
| + | \boxed{p=\frac{P_{pol}}{n}} | ||
| + | \] | ||
| + | |||
| + | where $P_{pol}$ is the polarization vector, but since our dielectric is isotropic (the same in all directions), the vector concept does not play a role here, and $n$ is the concentration of molecules; we find it from the basic MKT equation. | ||
| + | |||
| + | $P = nKT \Rightarrow n = \frac{P}{KT}$ | ||
| + | |||
| + | $P_{pol}$ is found from the polarization vector formula: | ||
| + | |||
| + | $P_{pol} = \varepsilon_{0}(\varepsilon - 1)E$ | ||
| + | |||
| + | Now we find the dipole moment: | ||
| + | |||
| + | \[ | ||
| + | \boxed{p = \frac{\varepsilon_{0}(\varepsilon - 1)EKT}{P}} | ||
| + | \] | ||
| + | |||
| + | $p = \frac{8.85 \cdot 10^{-12} \cdot (1.0078 - 1) \cdot 10^{3} \cdot 1.38 \cdot 10^{-23} \cdot 291}{2 \cdot 10^{3}} \approx 1.4 \cdot 10^{-34} \ C \cdot m$ | ||
| + | |||
| + | #### 2. Reasoning for the answer to the second question. | ||
| + | |||
| + | First of all, we need to understand what we found and what is given in reference materials. | ||
| + | |||
| + | We found the induced dipole moment, while reference books give the permanent dipole moment of the molecule. | ||
| + | |||
| + | What is the difference between the induced and the permanent dipole moment? | ||
| + | |||
| + | The induced dipole moment is a temporary dipole moment that arises in a particle under the influence of an external electric field. | ||
| + | |||
| + | The permanent dipole moment remains with the molecule forever (as the name suggests), even at $E = 0$, in our equations. | ||
| + | |||
| + | If we speak quantitatively about the difference, the Langevin-Debye formula helps, which has the form: | ||
| + | |||
| + | \[ | ||
| + | \boxed{\frac{\varepsilon - 1}{\varepsilon + 2} = \frac{n}{3\varepsilon_{0}}\left(\alpha + \frac{p_{0}^{2}}{3KT}\right)} | ||
| + | \] | ||
| + | |||
| + | Here $p_{0}^{2}$ is precisely that permanent dipole moment, and $\alpha$ is the electronic polarizability. | ||
| + | |||
| + | More detailed information about this formula can be read here: https://www.sciencedirect.com/topics/pharmacology-toxicology-and-pharmaceutical-science/lachesine | ||
| + | ### Answer | ||
| + | |||
| + | \[ | ||
| + | \boxed{p = 1.4 \cdot 10^{-34} \ C \cdot m} | ||
| + | \] | ||
| @@ -1,11 +1,76 @@ | |||
| ### |
### Problem | ||
| $6.6.3.$ |
$6.6.3.$ | ||
| The saturated vapor pressure of water at $18^{\circ}C$ is $2 \cdot 10^{3} \ Pa$, and its dielectric constant is 1.0078. From these data, find the average dipole moment of a water molecule in an electric field of strength $10^{3}$ V/m. Reference books give the dipole moment of water as $-0.61 \cdot 10^{-29} C \cdot m$. How can the discrepancy in the results be explained? | |||
| ### Solution | ### Solution | ||
| 12 | Before looking at the solution, you can review the first solution method (the second one is also possible, for broadening your knowledge) of problem $6.6.2$ and then try to solve this one. | ||
| #### Answer | #### 0. Write down the given data (a purely formal step to make the solution clear). | ||
| $\varepsilon = 1.0078$ | |||
| $E = 10^{3} \ V/m$ | |||
| $T = 18^{\circ}C = 291 \ K$ | |||
| $\varepsilon_{0} = 8.85 \cdot 10^{-12} \ F/m$ | |||
| $P = 2 \cdot 10^{3} \ Pa$ | |||
| $p' = -0.61 \cdot 10^{-29} \ C \cdot m$ | |||
| $K = 1.38 \cdot 10^{-23} \ J/K$ | |||
| #### 1. Find the answer to the first question. | |||
| We will find the answer by working backwards, that is, we write the formula for the dipole moment and start from there. | |||
| \[ | |||
| \boxed{p=\frac{P_{pol}}{n}} | |||
| \] | |||
| where $P_{pol}$ is the polarization vector, but since our dielectric is isotropic (the same in all directions), the vector concept does not play a role here, and $n$ is the concentration of molecules; we find it from the basic MKT equation. | |||
| $P = nKT \Rightarrow n = \frac{P}{KT}$ | |||
| $P_{pol}$ is found from the polarization vector formula: | |||
| $P_{pol} = \varepsilon_{0}(\varepsilon - 1)E$ | |||
| Now we find the dipole moment: | |||
| \[ | |||
| \boxed{p = \frac{\varepsilon_{0}(\varepsilon - 1)EKT}{P}} | |||
| \] | |||
| $p = \frac{8.85 \cdot 10^{-12} \cdot (1.0078 - 1) \cdot 10^{3} \cdot 1.38 \cdot 10^{-23} \cdot 291}{2 \cdot 10^{3}} \approx 1.4 \cdot 10^{-34} \ C \cdot m$ | |||
| #### 2. Reasoning for the answer to the second question. | |||
| First of all, we need to understand what we found and what is given in reference materials. | |||
| We found the induced dipole moment, while reference books give the permanent dipole moment of the molecule. | |||
| What is the difference between the induced and the permanent dipole moment? | |||
| The induced dipole moment is a temporary dipole moment that arises in a particle under the influence of an external electric field. | |||
| The permanent dipole moment remains with the molecule forever (as the name suggests), even at $E = 0$, in our equations. | |||
| If we speak quantitatively about the difference, the Langevin-Debye formula helps, which has the form: | |||
| \[ | |||
| \boxed{\frac{\varepsilon - 1}{\varepsilon + 2} = \frac{n}{3\varepsilon_{0}}\left(\alpha + \frac{p_{0}^{2}}{3KT}\right)} | |||
| \] | |||
| Here $p_{0}^{2}$ is precisely that permanent dipole moment, and $\alpha$ is the electronic polarizability. | |||
| More detailed information about this formula can be read here: https://www.sciencedirect.com/topics/pharmacology-toxicology-and-pharmaceutical-science/lachesine | |||
| ### Answer | |||
| \[ | |||
| \boxed{p = 1.4 \cdot 10^{-34} \ C \cdot m} | |||
| \] | |||