| @@ -1,136 +1,125 @@ |
| | − | Speed of sound in different media |
| | | |
| | − | Given: |
| | + | Условие: |
| | | |
| | − | $$\beta_{\mathrm{Hg}}=3\cdot10^{-5}\,\mathrm{atm}^{-1},\qquad |
| | − | \rho_{\mathrm{Hg}}=13.6\cdot10^3\,\mathrm{kg/m^3}$$ |
| | + | Сжимаемость ртути, воды и воздуха равна соответственно 3 · 10⁻⁵, 5 · 10⁻⁵ и 0,71 атм⁻¹, а их плотность — соответственно 13,6 · 10³, 1 · 10³ и 1,2 кг/м³. |
| | + | Определите скорость звука в этих средах. |
| | | |
| | − | $$\beta_{\mathrm{water}}=5\cdot10^{-5}\,\mathrm{atm}^{-1},\qquad |
| | − | \rho_{\mathrm{water}}=1.0\cdot10^3\,\mathrm{kg/m^3}$$ |
| | | |
| | − | $$\beta_{\mathrm{air}}=0.71\,\mathrm{atm}^{-1},\qquad |
| | − | \rho_{\mathrm{air}}=1.2\,\mathrm{kg/m^3}$$ |
| | + | \[Дано: |
| | + | \beta_{\mathrm{Hg}}=3\cdot10^{-5}\,\mathrm{атм}^{-1},\qquad \rho_{\mathrm{Hg}}=13.6\cdot10^3\,\mathrm{кг/м^3} |
| | + | \] |
| | + | \[ |
| | + | \beta_{\mathrm{H_2O}}=5\cdot10^{-5}\,\mathrm{атм}^{-1},\qquad \rho_{\mathrm{H_2O}}=1.0\cdot10^3\,\mathrm{кг/м^3} |
| | + | \] |
| | + | \[ |
| | + | \beta_{\text{воздух}}=0.71\,\mathrm{атм}^{-1},\qquad \rho_{\text{воздух}}=1.2\,\mathrm{кг/м^3} |
| | + | \] |
| | | |
| | − | Main formula: |
| | + | Основная формула: |
| | + | \[ |
| | + | v=\sqrt{\frac{1}{\beta\rho}} |
| | + | \] |
| | + | где $\beta$ — сжимаемость среды, а $\rho$ — плотность среды. |
| | | |
| | − | $$v=\sqrt{\frac{1}{\beta\rho}}$$ |
| | + | Переведём сжимаемость из $\mathrm{атм}^{-1}$ в $\mathrm{Па}^{-1}$: |
| | + | \[ |
| | + | 1\,\mathrm{атм}=101325\,\mathrm{Па} \implies 1\,\mathrm{атм}^{-1}=\frac{1}{101325}\,\mathrm{Па}^{-1} |
| | + | \] |
| | | |
| | − | where $\beta$ is the compressibility of the medium, and $\rho$ is the density of the medium. |
| | + | 1. Ртуть |
| | | |
| | − | We convert the compressibility from $\mathrm{atm}^{-1}$ to $\mathrm{Pa}^{-1}$. |
| | + | \[ |
| | + | \beta_{\mathrm{Hg}}=\frac{3\cdot10^{-5}}{101325} \approx 2.96\cdot10^{-10}\,\mathrm{Па}^{-1} |
| | + | \] |
| | | |
| | − | $$1\,\mathrm{atm}=101325\,\mathrm{Pa}$$ |
| | + | Используем формулу: |
| | + | \[ |
| | + | v_{\mathrm{Hg}}=\sqrt{\frac{1}{\beta_{\mathrm{Hg}}\rho_{\mathrm{Hg}}}} |
| | + | \] |
| | | |
| | − | Therefore, |
| | + | Подставляем значения: |
| | + | \[ |
| | + | v_{\mathrm{Hg}}=\sqrt{\frac{1}{(2.96\cdot10^{-10})(13.6\cdot10^3)}} |
| | + | \] |
| | | |
| | − | $$1\,\mathrm{atm}^{-1}=\frac{1}{101325}\,\mathrm{Pa}^{-1}$$ |
| | + | Вычисляем знаменатель: |
| | + | \[ |
| | + | (2.96\cdot10^{-10})(13.6\cdot10^3) \approx 4.0256\cdot10^{-6} |
| | + | \] |
| | | |
| | − | 1. Mercury |
| | + | Следовательно: |
| | + | \[ |
| | + | v_{\mathrm{Hg}}=\sqrt{\frac{1}{4.0256\cdot10^{-6}}} \approx 498\,\mathrm{м/с} |
| | + | \] |
| | | |
| | − | $$\beta_{\mathrm{Hg}}= |
| | − | \frac{3\cdot10^{-5}}{101325} |
| | − | \approx2.96\cdot10^{-10}\,\mathrm{Pa}^{-1}$$ |
| | + | Ответ для ртути: |
| | + | \[ |
| | + | v_{\mathrm{Hg}}\approx 500\,\mathrm{м/с} |
| | + | \] |
| | | |
| | − | We use the formula: |
| | + | 2. Вода ($\mathrm{H_2O}$) |
| | | |
| | − | $$v_{\mathrm{Hg}}= |
| | − | \sqrt{\frac{1}{\beta_{\mathrm{Hg}}\rho_{\mathrm{Hg}}}}$$ |
| | + | \[ |
| | + | \beta_{\mathrm{H_2O}}=\frac{5\cdot10^{-5}}{101325} \approx 4.93\cdot10^{-10}\,\mathrm{Па}^{-1} |
| | + | \] |
| | | |
| | − | Substituting the values: |
| | + | Используем формулу: |
| | + | \[ |
| | + | v_{\mathrm{H_2O}}=\sqrt{\frac{1}{\beta_{\mathrm{H_2O}}\rho_{\mathrm{H_2O}}}} |
| | + | \] |
| | | |
| | − | $$v_{\mathrm{Hg}}= |
| | − | \sqrt{\frac{1} |
| | − | {(2.96\cdot10^{-10})(13.6\cdot10^3)}}$$ |
| | + | Подставляем значения: |
| | + | \[ |
| | + | v_{\mathrm{H_2O}}=\sqrt{\frac{1}{(4.93\cdot10^{-10})(1.0\cdot10^3)}} |
| | + | \] |
| | | |
| | − | First, we calculate the denominator: |
| | + | Вычисляем знаменатель: |
| | + | \[ |
| | + | (4.93\cdot10^{-10})(1.0\cdot10^3) = 4.93\cdot10^{-7} |
| | + | \] |
| | | |
| | − | $$(2.96\cdot10^{-10})(13.6\cdot10^3) |
| | − | \approx4.0256\cdot10^{-6}$$ |
| | + | Следовательно: |
| | + | \[ |
| | + | v_{\mathrm{H_2O}}=\sqrt{\frac{1}{4.93\cdot10^{-7}}} \approx 1424\,\mathrm{м/с} |
| | + | \] |
| | | |
| | − | Therefore: |
| | + | Ответ для воды: |
| | + | \[ |
| | + | v_{\mathrm{H_2O}}\approx 1420\,\mathrm{м/с} |
| | + | \] |
| | | |
| | − | $$v_{\mathrm{Hg}}= |
| | − | \sqrt{\frac{1}{4.0256\cdot10^{-6}}}$$ |
| | + | 3. Воздух |
| | | |
| | − | $$v_{\mathrm{Hg}}\approx498\,\mathrm{m/s}$$ |
| | + | \[ |
| | + | \beta_{\text{воздух}}=\frac{0.71}{101325} \approx 7.01\cdot10^{-6}\,\mathrm{Па}^{-1} |
| | + | \] |
| | | |
| | − | Answer for mercury: |
| | + | Используем формулу: |
| | + | \[ |
| | + | v_{\text{воздух}}=\sqrt{\frac{1}{\beta_{\text{воздух}}\rho_{\text{воздух}}}} |
| | + | \] |
| | | |
| | − | $$\boxed{v_{\mathrm{Hg}}\approx500\,\mathrm{m/s}}$$ |
| | + | Подставляем значения: |
| | + | \[ |
| | + | v_{\text{воздух}}=\sqrt{\frac{1}{(7.01\cdot10^{-6})(1.2)}} |
| | + | \] |
| | | |
| | + | Вычисляем знаменатель: |
| | + | \[ |
| | + | (7.01\cdot10^{-6})(1.2) = 8.412\cdot10^{-6} |
| | + | \] |
| | | |
| | − | 2. Water |
| | + | Следовательно: |
| | + | \[ |
| | + | v_{\text{воздух}}=\sqrt{\frac{1}{8.412\cdot10^{-6}}} \approx 345\,\mathrm{м/с} |
| | + | \] |
| | | |
| | − | $$\beta_{\mathrm{water}}= |
| | − | \frac{5\cdot10^{-5}}{101325} |
| | − | \approx4.93\cdot10^{-10}\,\mathrm{Pa}^{-1}$$ |
| | + | Ответ для воздуха: |
| | + | \[ |
| | + | v_{\text{воздух}}\approx 345\,\mathrm{м/с} |
| | + | \] |
| | | |
| | − | We use the formula: |
| | − | |
| | − | $$v_{\mathrm{water}}= |
| | − | \sqrt{\frac{1}{\beta_{\mathrm{water}}\rho_{\mathrm{water}}}}$$ |
| | − | |
| | − | Substituting the values: |
| | − | |
| | − | $$v_{\mathrm{water}}= |
| | − | \sqrt{\frac{1} |
| | − | {(4.93\cdot10^{-10})(1.0\cdot10^3)}}$$ |
| | − | |
| | − | We calculate the denominator: |
| | − | |
| | − | $$(4.93\cdot10^{-10})(1.0\cdot10^3) |
| | − | =4.93\cdot10^{-7}$$ |
| | − | |
| | − | Therefore: |
| | − | |
| | − | $$v_{\mathrm{water}}= |
| | − | \sqrt{\frac{1}{4.93\cdot10^{-7}}}$$ |
| | − | |
| | − | $$v_{\mathrm{water}}\approx1424\,\mathrm{m/s}$$ |
| | − | |
| | − | Answer for water: |
| | − | |
| | − | $$\boxed{v_{\mathrm{water}}\approx1420\,\mathrm{m/s}}$$ |
| | − | |
| | − | |
| | − | 3. Air |
| | − | |
| | − | $$\beta_{\mathrm{air}}= |
| | − | \frac{0.71}{101325} |
| | − | \approx7.01\cdot10^{-6}\,\mathrm{Pa}^{-1}$$ |
| | − | |
| | − | We use the formula: |
| | − | |
| | − | $$v_{\mathrm{air}}= |
| | − | \sqrt{\frac{1}{\beta_{\mathrm{air}}\rho_{\mathrm{air}}}}$$ |
| | − | |
| | − | Substituting the values: |
| | − | |
| | − | $$v_{\mathrm{air}}= |
| | − | \sqrt{\frac{1} |
| | − | {(7.01\cdot10^{-6})(1.2)}}$$ |
| | − | |
| | − | We calculate the denominator: |
| | − | |
| | − | $$(7.01\cdot10^{-6})(1.2) |
| | − | =8.412\cdot10^{-6}$$ |
| | − | |
| | − | Therefore: |
| | − | |
| | − | $$v_{\mathrm{air}}= |
| | − | \sqrt{\frac{1}{8.412\cdot10^{-6}}}$$ |
| | − | |
| | − | $$v_{\mathrm{air}}\approx345\,\mathrm{m/s}$$ |
| | − | |
| | − | Answer for air: |
| | − | |
| | − | $$\boxed{v_{\mathrm{air}}\approx345\,\mathrm{m/s}}$$ |
| | − | |
| | − | |
| | − | Final answer: |
| | − | |
| | − | $$\boxed{ |
| | − | v_{\mathrm{Hg}}\approx500\,\mathrm{m/s},\qquad |
| | − | v_{\mathrm{water}}\approx1420\,\mathrm{m/s},\qquad |
| | − | v_{\mathrm{air}}\approx345\,\mathrm{m/s} |
| | − | }$$ |
| | + | Ответ: |
| | + | \[ |
| | + | v_{\mathrm{Hg}}\approx500\,\mathrm{м/с},\qquad v_{\mathrm{H_2O}}\approx1420\,\mathrm{м/с},\qquad v_{\text{воздух}}\approx345\,\mathrm{м/с} |
| | + | \] |