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A copper sphere is suspended in an evacu...

A copper sphere is suspended in an evacuated chamber maintained at `300K`. The sphere is maintained at a constant temperature of `500K` by heating it electrically. A total of `210W` of electric power is needed to do it. When the surface of the copper sphere is completely blackened, `700W` is needed to maintain the same temperature of the sphere. Calculate the emissivity of copper.

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To solve the problem, we will use the concept of thermal radiation and the Stefan-Boltzmann law. The power radiated by a body is given by: \[ P = \varepsilon \sigma A (T^4 - T_0^4) \] where: - \( P \) is the power (in watts), - \( \varepsilon \) is the emissivity of the material, - \( \sigma \) is the Stefan-Boltzmann constant (\( 5.67 \times 10^{-8} \, \text{W/m}^2\text{K}^4 \)), - \( A \) is the surface area of the sphere, - \( T \) is the temperature of the sphere (in Kelvin), - \( T_0 \) is the temperature of the surroundings (in Kelvin). ### Step 1: Set up equations for both scenarios 1. **For the copper sphere (not blackened)**: - Given that \( P_1 = 210 \, \text{W} \), \( T = 500 \, \text{K} \), and \( T_0 = 300 \, \text{K} \): \[ 210 = \varepsilon \sigma A (500^4 - 300^4) \tag{1} \] 2. **For the blackened copper sphere**: - Given that \( P_2 = 700 \, \text{W} \): \[ 700 = 1 \cdot \sigma A (500^4 - 300^4) \tag{2} \] (Here, emissivity \( \varepsilon = 1 \) for a black body) ### Step 2: Calculate \( 500^4 - 300^4 \) We need to calculate \( 500^4 - 300^4 \): \[ 500^4 = 62500000000 \quad \text{and} \quad 300^4 = 8100000000 \] \[ 500^4 - 300^4 = 62500000000 - 8100000000 = 54499999999 \] ### Step 3: Substitute the value into equations Substituting this value into both equations: 1. From equation (1): \[ 210 = \varepsilon \sigma A (54499999999) \] 2. From equation (2): \[ 700 = \sigma A (54499999999) \] ### Step 4: Solve for \( \varepsilon \) Now, we can divide equation (1) by equation (2): \[ \frac{210}{700} = \frac{\varepsilon \sigma A (54499999999)}{\sigma A (54499999999)} \] This simplifies to: \[ \frac{3}{10} = \varepsilon \] Thus, the emissivity \( \varepsilon \) of copper is: \[ \varepsilon = 0.3 \] ### Final Answer The emissivity of copper is **0.3**. ---

To solve the problem, we will use the concept of thermal radiation and the Stefan-Boltzmann law. The power radiated by a body is given by: \[ P = \varepsilon \sigma A (T^4 - T_0^4) \] where: - \( P \) is the power (in watts), - \( \varepsilon \) is the emissivity of the material, - \( \sigma \) is the Stefan-Boltzmann constant (\( 5.67 \times 10^{-8} \, \text{W/m}^2\text{K}^4 \)), ...
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