New solution
en/11.1.30.md
+46 −0
| @@ -0,0 +1,46 @@ | |||
| + | ### Statement | ||
| + | |||
| + | $11.1.30.$ [Insert the problem statement] | ||
| + | |||
| + | ### Solution | ||
| + | |||
| + | First, we analyze the total power supplied to the rotor (50 W), which is distributed as: | ||
| + | |||
| + | · Friction losses: 4% of 50 W | ||
| + | P_{\text{friction}} = 0.04 \times 50 = 2\ \text{W} | ||
| + | · Mechanical power converted into electrical power: | ||
| + | P_{\text{electrical}} = 50\ \text{W} - 2\ \text{W} = 48\ \text{W} | ||
| + | |||
| + | Calculation of the EMF | ||
| + | |||
| + | Assuming the internal resistance of the dynamo is negligible (or that the 300 Ω already includes the entire circuit), all the generated electrical power is dissipated in the external resistance R: | ||
| + | |||
| + | P_{\text{electrical}} = \frac{\mathcal{E}^2}{R} | ||
| + | |||
| + | Solving for \mathcal{E}: | ||
| + | |||
| + | \mathcal{E} = \sqrt{P_{\text{electrical}} \cdot R} = \sqrt{48 \times 300} = \sqrt{14400} = 120\ \text{V} | ||
| + | |||
| + | \boxed{\mathcal{E} = 120\ \text{V}} | ||
| + | |||
| + | Finding the new resistance while keeping the same speed | ||
| + | |||
| + | The EMF depends only on the rotation speed (and the magnetic field). Since the rotation frequency remains the same, the EMF does not change: | ||
| + | |||
| + | \mathcal{E}' = \mathcal{E} = 120\ \text{V} | ||
| + | |||
| + | New resistance: R' = 60\ \Omega. | ||
| + | New generated electrical power: | ||
| + | |||
| + | P'_{\text{electrical}} = \frac{\mathcal{E}^2}{R'} = \frac{14400}{60} = 240\ \text{W} | ||
| + | |||
| + | Friction losses depend on speed, which does not change, so they remain at 2 W. | ||
| + | |||
| + | P_{\text{input}}' = P'_{\text{electrical}} + P_{\text{friction}} = 240\ \text{W} + 2\ \text{W} = 242\ \text{W} | ||
| + | |||
| + | \boxed{P_{\text{input}}' = 242\ \text{W}} | ||
| + | |||
| + | |||
| + | #### Answer | ||
| + | |||
| + | [Insert a concise answer or boxed result] | ||
| @@ -0,0 +1,46 @@ | |||
| ### Statement | |||
| $11.1.30.$ [Insert the problem statement] | |||
| ### Solution | |||
| First, we analyze the total power supplied to the rotor (50 W), which is distributed as: | |||
| · Friction losses: 4% of 50 W | |||
| P_{\text{friction}} = 0.04 \times 50 = 2\ \text{W} | |||
| · Mechanical power converted into electrical power: | |||
| P_{\text{electrical}} = 50\ \text{W} - 2\ \text{W} = 48\ \text{W} | |||
| Calculation of the EMF | |||
| Assuming the internal resistance of the dynamo is negligible (or that the 300 Ω already includes the entire circuit), all the generated electrical power is dissipated in the external resistance R: | |||
| P_{\text{electrical}} = \frac{\mathcal{E}^2}{R} | |||
| Solving for \mathcal{E}: | |||
| \mathcal{E} = \sqrt{P_{\text{electrical}} \cdot R} = \sqrt{48 \times 300} = \sqrt{14400} = 120\ \text{V} | |||
| \boxed{\mathcal{E} = 120\ \text{V}} | |||
| Finding the new resistance while keeping the same speed | |||
| The EMF depends only on the rotation speed (and the magnetic field). Since the rotation frequency remains the same, the EMF does not change: | |||
| \mathcal{E}' = \mathcal{E} = 120\ \text{V} | |||
| New resistance: R' = 60\ \Omega. | |||
| New generated electrical power: | |||
| P'_{\text{electrical}} = \frac{\mathcal{E}^2}{R'} = \frac{14400}{60} = 240\ \text{W} | |||
| Friction losses depend on speed, which does not change, so they remain at 2 W. | |||
| P_{\text{input}}' = P'_{\text{electrical}} + P_{\text{friction}} = 240\ \text{W} + 2\ \text{W} = 242\ \text{W} | |||
| \boxed{P_{\text{input}}' = 242\ \text{W}} | |||
| #### Answer | |||
| [Insert a concise answer or boxed result] | |||