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One end of a metal rod is kept in a furnace. In steady state, the temperature of the rod

a)increases ,b)decreases c)remains constant d)is non uniform

2)One end of a metal rod is dipped in a boiling water and the other is dipped in melting ice

a)all parts of the rod are in thermal equilibrium with each other

b)we can assign a temperature to the rod

c)we can assign a temp. to it after steady state is reached

d)the state of the rod does not change after steady state is reached

3)the heat current is written as ,why don't we write

plz give reasons

Kevin Nash , 12 Years ago
Grade upto college level
anser 1 Answers
Askiitians Tutor Team

Let's break down your questions step by step, focusing on the principles of heat transfer and thermal equilibrium. These concepts are fundamental in understanding how temperature changes in materials, especially in metal rods subjected to different thermal environments.

Temperature Changes in a Metal Rod in a Furnace

When one end of a metal rod is placed in a furnace, the temperature at that end will increase due to the heat being transferred from the furnace to the rod. However, the temperature along the length of the rod will not be uniform immediately. Over time, as heat continues to flow through the rod, a steady state will be reached where the temperature gradient stabilizes.

  • Increases: Initially, the temperature at the heated end rises.
  • Decreases: This is not applicable here since the heated end is gaining heat.
  • Remains Constant: This is only true once a steady state is reached, but not initially.
  • Is Non-Uniform: Yes, at any given moment before reaching steady state, the temperature will vary along the rod.

Thus, the correct answer is that the temperature of the rod is non-uniform (d) until it reaches a steady state.

Behavior of a Metal Rod in Boiling Water and Ice

Now, consider a scenario where one end of a metal rod is dipped in boiling water and the other in melting ice. Initially, there will be a significant temperature difference between the two ends. As heat flows from the boiling water to the ice, the rod will start to reach thermal equilibrium.

  • All parts of the rod are in thermal equilibrium with each other: This is not true initially, as there is a temperature gradient.
  • We can assign a temperature to the rod: This is also not accurate until steady state is achieved.
  • We can assign a temperature to it after steady state is reached: Correct! Once thermal equilibrium is achieved, the entire rod will have a uniform temperature.
  • The state of the rod does not change after steady state is reached: This is true, as long as the conditions remain constant.

Therefore, the most accurate statement is that we can assign a temperature to it after steady state is reached (c).

Understanding Heat Current and Its Representation

Heat current, or heat transfer rate, is often represented mathematically in terms of temperature difference and material properties. The equation typically used is Fourier's law of heat conduction, which states that the heat current (Q) is proportional to the temperature gradient (dT/dx) and the cross-sectional area (A) of the rod, as well as the material's thermal conductivity (k):

Q = -k * A * (dT/dx)

Now, regarding your question about why we don't write "heat current" in a different way, it’s important to note that the negative sign indicates the direction of heat flow—from higher to lower temperature. This convention is crucial for understanding the flow of heat in physical systems.

  • Directionality: The negative sign in the equation signifies that heat flows from hot to cold.
  • Proportionality: The equation shows that heat current is directly proportional to the temperature difference, which is a fundamental principle in thermodynamics.
  • Material Properties: The thermal conductivity (k) varies for different materials, affecting how heat is transferred.

In summary, the representation of heat current is designed to convey essential information about the direction and rate of heat transfer, making it a critical concept in thermal physics.

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