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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 maitained at a constant temperature of 500K by heating it electrically. A total of 210W is electric power is needed to do it. When the surface of the copper sphere is completely blackned, 700W is needed to maintain the same temperature of the sphere. Calculate the emissivity of copper.

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To solve the problem of finding the emissivity of the copper sphere, we can follow these steps: ### Step 1: Understand the Problem We have a copper sphere at a constant temperature of 500 K in an evacuated chamber at 300 K. The power required to maintain this temperature when the sphere is in its natural state is 210 W. When the sphere is blackened, the power required increases to 700 W. We need to find the emissivity of the copper sphere. ### Step 2: Use the Stefan-Boltzmann Law According to the Stefan-Boltzmann Law, the power emitted by a body is given by: \[ P = \epsilon \sigma A (T_1^4 - T_0^4) \] where: - \( P \) is the power emitted, - \( \epsilon \) is the emissivity, - \( \sigma \) is the Stefan-Boltzmann constant, - \( A \) is the surface area, - \( T_1 \) is the temperature of the body (500 K), - \( T_0 \) is the temperature of the surroundings (300 K). ### Step 3: Set Up the Equations For the copper sphere when it is not blackened, the power equation can be written as: \[ P_c = \epsilon_c \sigma A (T_1^4 - T_0^4) \] Given \( P_c = 210 \, W \), we can write: \[ 210 = \epsilon_c \sigma A (500^4 - 300^4) \] (Equation 1) For the blackened sphere (acting as a black body), the emissivity is 1: \[ P_b = \sigma A (T_1^4 - T_0^4) \] Given \( P_b = 700 \, W \), we can write: \[ 700 = \sigma A (500^4 - 300^4) \] (Equation 2) ### Step 4: Divide the Equations From Equation 1 and Equation 2, we can eliminate \( \sigma A (500^4 - 300^4) \): \[ \frac{210}{\epsilon_c} = 700 \] Rearranging gives: \[ \epsilon_c = \frac{210}{700} \] ### Step 5: Calculate Emissivity Calculating the above expression: \[ \epsilon_c = \frac{210}{700} = 0.3 \] ### Final Answer The emissivity of the copper sphere is \( \epsilon_c = 0.3 \). ---

To solve the problem of finding the emissivity of the copper sphere, we can follow these steps: ### Step 1: Understand the Problem We have a copper sphere at a constant temperature of 500 K in an evacuated chamber at 300 K. The power required to maintain this temperature when the sphere is in its natural state is 210 W. When the sphere is blackened, the power required increases to 700 W. We need to find the emissivity of the copper sphere. ### Step 2: Use the Stefan-Boltzmann Law According to the Stefan-Boltzmann Law, the power emitted by a body is given by: \[ P = \epsilon \sigma A (T_1^4 - T_0^4) \] ...
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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.

A spherical tungsten pieces of radius 1.0cm is suspended in an evacuated chamber maintained at 300K . The pieces is maintained at 1000K by heating it electrically. Find the rate at which the electrical energy must be supplied. The emissivity of tungsten is 0.30 and the Stefan constant sigma is 6.0xx10^(-s)Wm^(-2)K^(-4) .

Two identical spheres A and B are suspended in an air chamber which is maintained at a temperature of 50^@C . Find the ratio of the heat lost per second from the surface of the spheres if a. A and B are at temperatures 60^@C and 55^@C , respectively. b. A and B are at temperatures 250^@C and 200^@C , respectively.

A blackbody of surface area 1cm^(2) is placed inside an enclosure. The enclosure has a constant temperature 27(@)C and the blackbody is maintained at 327^(@)C by heating it electrically. What electric power is needed to maintain the temperature? sigma=6.0xx10^(-8)Wm^(-2)K^(-2) .

A thin brass rectangular sheet of sides 10 cm and 5 cm is heated in a furnace to 500^(@) C and taken out. How much electric power is needed to maintain the sheet at this temperature ? Its emissivity is 0.25.

A cylindrical block of length 0.4 m and area of cross-section 0.04 m^2 is placed coaxially on a thin metal disc of mass 0.4 kg and of the same cross - section. The upper face of the cylinder is maintained at a constant temperature of 400 K and the initial temperature of the disc is 300K. if the thermal conductivity of the material of the cylinder is 10 "watt"// m-K and the specific heat of the material of the disc is 600J//kg-K , how long will it take for the temperature of the disc to increase to 350 K? Assume for purpose of calculation the thermal conductivity of the disc to be very high and the system to be thermally insulated except for the upper face of the cylinder.

A thin copper rod of uniform cross section A square metres and of length L metres has a spherical metal sphere of radius r metre at tis one end symmetrically attached to the copper rod. The thermal conductivity of copper is K and the emissivity of the spherical surface of the sphere is epsi .The free end of the copper rod is maintained at the temperature T kelving by supplying thermal energy from a P watt source. Steady state conditions are allowed ot be established while the rod is properly insulated aginst heat loss from its lateral surface. Surroundings are at 0^@C Stefan's constant =sigma W//m^(2)K^(4) . If the metal sphere attached at the end of the copper rod is made of brass, whose thermal conductivity is K_b lt K , then which of the following statements is true?

A sphere P (emissivity=1) of radius 2R and and another sphere Q(emissivity=1/2) of radius R are placed in vacuum at some distance threre are no other objects. The temperature of the sphere Q is maintained at 200 K by the means of a heater. A fraction 1/32 of the power emitted by the sphere Q falls on the sphere P. if the equilibrium temperature of the sphere P is 10 T kelvin find the value of T.

A sphere has a surface area of 1.0 m^(2) and a temperature of 400 K and the power radiated from it is 150 W. Assuming the sphere is black body radiator. The power in kilowatt radiated when the area expands to 2.0 m^(2) and the temperature changes to 800 K

A thin copper rod of uniform cross section A square metres and of length L metres has a spherical metal sphere of radius r metre at tis one end symmetrically attached to the copper rod. The thermal conductivity of copper is K and the emissivity of the spherical surface of the sphere is epsi .The free end of the copper rod is maintained at the temperature T kelving by supplying thermal energy from a P watt source. Steady state conditions are allowed ot be established while the rod is properly insulated aginst heat loss from its lateral surface. Surroundings are at 0^@C Stefan's constant =sigmaW//m^(2) K^(4) . The net power that will be radiated out, P_S from the sphere after steady state condition are reached is

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