Use Stefan's law to calculate how much less energy is emitted per unit area of a 4500-K sunspot.

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**Physics Problem Solving with Stefan's Law**
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**Problem Statement:**

Use Stefan’s law to calculate how much less energy is emitted per unit area of a 4500-K sunspot.

**Explanation:**

Stefan's Law, also known as the Stefan-Boltzmann Law, is fundamental in understanding the radiation emitted by a blackbody. The law states that the total energy radiated per unit surface area of a blackbody across all wavelengths per unit time \( (E) \) is directly proportional to the fourth power of the blackbody's absolute temperature \( (T) \). Mathematically, it is expressed as:

\[ E = \sigma T^{4} \]

where:
- \( E \) is the radiant energy emitted per unit area.
- \( \sigma \) (sigma) is the Stefan-Boltzmann constant, approximately \( 5.67 × 10^{-8} \, W \, m^{-2} \, K^{-4} \).
- \( T \) is the absolute temperature of the blackbody in Kelvin (K).

To determine how much less energy is emitted per unit area by a sunspot with a temperature of 4500 K, apply Stefan’s Law to compare it with the energy emitted by the Sun's photosphere (typically around 5778 K).

**Steps:**

1. **Calculate the Energy Emitted by the Sun’s Photosphere:**

   Let \( T_{sun} \) be the temperature of the Sun’s photosphere.
   
   \( E_{sun} = \sigma T_{sun}^{4} \)

   \( E_{sun} = (5.67 \times 10^{-8} \, W \, m^{-2} \, K^{-4}) \times (5778 \, K)^{4} \)

2. **Calculate the Energy Emitted by the Sunspot:**

   Let \( T_{sunspot} \) be the temperature of the sunspot.
   
   \( E_{sunspot} = \sigma T_{sunspot}^{4} \)

   \( E_{sunspot} = (5.67 \times 10^{-8} \, W \, m^{-2} \, K^{-4}) \times (4500 \, K)^{4} \)

3. **Determine the Difference:**

   The difference in emitted energy per unit area:

   \( \Delta E = E
Transcribed Image Text:**Physics Problem Solving with Stefan's Law** --- **Problem Statement:** Use Stefan’s law to calculate how much less energy is emitted per unit area of a 4500-K sunspot. **Explanation:** Stefan's Law, also known as the Stefan-Boltzmann Law, is fundamental in understanding the radiation emitted by a blackbody. The law states that the total energy radiated per unit surface area of a blackbody across all wavelengths per unit time \( (E) \) is directly proportional to the fourth power of the blackbody's absolute temperature \( (T) \). Mathematically, it is expressed as: \[ E = \sigma T^{4} \] where: - \( E \) is the radiant energy emitted per unit area. - \( \sigma \) (sigma) is the Stefan-Boltzmann constant, approximately \( 5.67 × 10^{-8} \, W \, m^{-2} \, K^{-4} \). - \( T \) is the absolute temperature of the blackbody in Kelvin (K). To determine how much less energy is emitted per unit area by a sunspot with a temperature of 4500 K, apply Stefan’s Law to compare it with the energy emitted by the Sun's photosphere (typically around 5778 K). **Steps:** 1. **Calculate the Energy Emitted by the Sun’s Photosphere:** Let \( T_{sun} \) be the temperature of the Sun’s photosphere. \( E_{sun} = \sigma T_{sun}^{4} \) \( E_{sun} = (5.67 \times 10^{-8} \, W \, m^{-2} \, K^{-4}) \times (5778 \, K)^{4} \) 2. **Calculate the Energy Emitted by the Sunspot:** Let \( T_{sunspot} \) be the temperature of the sunspot. \( E_{sunspot} = \sigma T_{sunspot}^{4} \) \( E_{sunspot} = (5.67 \times 10^{-8} \, W \, m^{-2} \, K^{-4}) \times (4500 \, K)^{4} \) 3. **Determine the Difference:** The difference in emitted energy per unit area: \( \Delta E = E
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