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Two identical beakers A and B contain eq...

Two identical beakers `A` and `B` contain equal volumes of two different liquids at `60^(@)C` each and left to cool down. Liquid in A has density of `8xx10^(2)kg//m^(2)` and specific heat of `2000J kg^(-1)K^(-1)` while liquid in `B` has density of `10^(3)kg m^(-3)` and specific heat of `400J kg^(-1)K^(-1)`. Which of the following best describes their temperature versus time graph schematically? (assume the emissivity of both the beakers to be the same)

A

B

C

D

Text Solution

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The correct Answer is:
To solve the problem, we need to analyze the cooling rates of the two liquids in beakers A and B based on their mass and specific heat capacities. We will use Newton's law of cooling to derive the temperature versus time graph. ### Step-by-Step Solution: 1. **Identify the Given Data:** - Beaker A: - Density, \( \rho_A = 8 \times 10^2 \, \text{kg/m}^3 \) - Specific heat, \( c_A = 2000 \, \text{J/(kg K)} \) - Beaker B: - Density, \( \rho_B = 10^3 \, \text{kg/m}^3 \) - Specific heat, \( c_B = 400 \, \text{J/(kg K)} \) - Both liquids start at \( T_0 = 60^\circ C \). 2. **Calculate the Mass of Liquids:** - Let the volume of each liquid be \( V \). - Mass of liquid in beaker A: \[ m_A = \rho_A \cdot V = (8 \times 10^2) \cdot V = 800V \, \text{kg} \] - Mass of liquid in beaker B: \[ m_B = \rho_B \cdot V = (10^3) \cdot V = 1000V \, \text{kg} \] 3. **Calculate the Heat Capacity (m*c) for Each Liquid:** - Heat capacity for liquid A: \[ m_A \cdot c_A = (800V) \cdot (2000) = 1.6 \times 10^6 V \, \text{J/K} \] - Heat capacity for liquid B: \[ m_B \cdot c_B = (1000V) \cdot (400) = 4.0 \times 10^5 V \, \text{J/K} \] 4. **Determine the Cooling Rate Using Newton's Law of Cooling:** - According to Newton's law of cooling, the rate of change of temperature is proportional to the temperature difference: \[ \frac{dT}{dt} \propto (T - T_{\text{ambient}}) \] - The proportionality constant is inversely related to the heat capacity: \[ \frac{dT}{dt} = -k \cdot \frac{1}{m \cdot c} \cdot (T - T_{\text{ambient}}) \] - Therefore, the cooling rate for each liquid can be expressed as: \[ \frac{dT_A}{dt} = -k_A \cdot (T_A - T_{\text{ambient}}) \quad \text{and} \quad \frac{dT_B}{dt} = -k_B \cdot (T_B - T_{\text{ambient}}) \] - Where \( k_A \) and \( k_B \) are constants depending on the heat capacity. 5. **Compare the Cooling Rates:** - Since \( m_A \cdot c_A = 1.6 \times 10^6 V \) and \( m_B \cdot c_B = 4.0 \times 10^5 V \), we see that: \[ m_A \cdot c_A > m_B \cdot c_B \] - This implies that the cooling rate for liquid A is slower than that for liquid B: \[ \left| \frac{dT_A}{dt} \right| < \left| \frac{dT_B}{dt} \right| \] 6. **Conclusion on Temperature vs. Time Graph:** - Since liquid A cools more slowly than liquid B, the temperature vs. time graph will show that the temperature of liquid A decreases less steeply compared to liquid B. - Thus, the graph for liquid A will be above that of liquid B for the same time interval. ### Final Answer: The best schematic representation of the temperature versus time graph is option **B**, where the slope for liquid A is less than that for liquid B.
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