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An iron rod is subjected to cycles of ma...

An iron rod is subjected to cycles of magnetisation at the rate of `50Hz`. Given the density of the rod is `8xx10^(3)kg//m^(3)` and specific heat is `0.11xx10^(-3)calxxkg^(@)C`. The rise in temperature per minute, if the area enclosed by the `B-H` loop corresponds to energy of `10^(-2)J` is (Assume there is no radiation losses)

A

`78^(@)C`

B

`88^(@)C`

C

`8.1^(@)C`

D

none of these

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The correct Answer is:
To solve the problem step by step, we will follow these calculations: ### Step 1: Determine the Energy Loss per Minute The energy loss per cycle is given as \(10^{-2} \, \text{J}\). The frequency of magnetization is \(50 \, \text{Hz}\), which means there are \(50\) cycles per second. Therefore, the energy loss per second is: \[ \text{Energy loss per second} = \text{Energy loss per cycle} \times \text{Frequency} = 10^{-2} \, \text{J} \times 50 \, \text{Hz} = 5 \times 10^{-1} \, \text{J/s} \] To find the energy loss per minute, we multiply by \(60\) seconds: \[ \text{Energy loss per minute} = 5 \times 10^{-1} \, \text{J/s} \times 60 \, \text{s} = 30 \, \text{J} \] ### Step 2: Relate Energy Loss to Temperature Rise The energy loss can be related to the temperature rise using the formula: \[ \text{Energy} = \text{mass} \times \text{specific heat} \times \Delta T \] Where: - \(\Delta T\) is the rise in temperature, - The mass \(m\) can be calculated as \(m = \text{Volume} \times \text{Density}\). ### Step 3: Calculate the Mass of the Iron Rod Let \(V\) be the volume of the iron rod. The density of the rod is given as \(8 \times 10^{3} \, \text{kg/m}^3\). Thus, the mass is: \[ m = V \times \text{Density} = V \times 8 \times 10^{3} \, \text{kg/m}^3 \] ### Step 4: Substitute Mass into the Energy Equation Substituting the mass into the energy equation gives: \[ 30 \, \text{J} = (V \times 8 \times 10^{3}) \times (0.11 \times 10^{-3} \times 4.2) \times \Delta T \] ### Step 5: Calculate Specific Heat in Joules Convert specific heat from calories to joules: \[ 0.11 \times 10^{-3} \, \text{cal/kg°C} = 0.11 \times 10^{-3} \times 4.2 \, \text{J/kg°C} = 0.462 \times 10^{-3} \, \text{J/kg°C} \] ### Step 6: Rearranging the Equation for \(\Delta T\) Now we can rearrange the equation to solve for \(\Delta T\): \[ \Delta T = \frac{30 \, \text{J}}{(V \times 8 \times 10^{3}) \times (0.462 \times 10^{-3})} \] ### Step 7: Substitute Volume to Find \(\Delta T\) Assuming \(V = 1 \, \text{m}^3\) for simplicity (as the volume will cancel out later): \[ \Delta T = \frac{30}{(1 \times 8 \times 10^{3}) \times (0.462 \times 10^{-3})} \] Calculating this gives: \[ \Delta T = \frac{30}{8 \times 0.462} \approx \frac{30}{3.696} \approx 8.11 \, \text{°C} \] ### Final Answer The rise in temperature per minute is approximately \(8.11 \, \text{°C}\). ---

To solve the problem step by step, we will follow these calculations: ### Step 1: Determine the Energy Loss per Minute The energy loss per cycle is given as \(10^{-2} \, \text{J}\). The frequency of magnetization is \(50 \, \text{Hz}\), which means there are \(50\) cycles per second. Therefore, the energy loss per second is: \[ \text{Energy loss per second} = \text{Energy loss per cycle} \times \text{Frequency} = 10^{-2} \, \text{J} \times 50 \, \text{Hz} = 5 \times 10^{-1} \, \text{J/s} \] To find the energy loss per minute, we multiply by \(60\) seconds: ...
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