We are given a thermodynamic process involving temperature changes. Let’s break down the problem step by step:
We start with the following temperature relationships:
We are given the temperature changes over a time interval and can use the following relationship between the initial and final temperatures:
\(T_0 = T\)
The first equation is based on the temperature change from \( 3T \) to \( 2T \) over 10 minutes:
\(\left(\frac{3T - 2T}{10}\right) = c_1 \left(\frac{3T + 2T}{2} - T\right) \) ....(\)
This equation is based on the fact that heat exchange rate is proportional to the temperature difference.
The second equation is based on the temperature change from \( 2T \) to \( T_f \) over 10 minutes:
\(\left(\frac{2T - T_f}{10}\right) = c_1 \left(\frac{2T + T_f}{2} - T\right) \) ....(i\)
Next, we need to take the ratio of the two equations (i) and (ii) to solve for the final temperature \( T_f \):
\(\frac{E(i)}{E(ii)} \Rightarrow \frac{\frac{T}{10}}{\frac{2T - T_f}{10}} = \frac{\frac{5T - 2T}{2}}{\frac{T_f}{2}}\)
After simplifying the equation, we get:
\(\frac{T}{2T - T_f} = \frac{3T}{T_f}\)
Rearranging this equation to solve for \( T_f \), we get:
\(T_f = 6T - 3T_f\)
Now, simplify further:
\(4T_f = 6T\)
Finally, we find the value of \( T_f \):
\(T_f = \frac{3}{2} T\)
The final temperature \( T_f \) is:
\(T_f = \frac{3}{2} T\)
What is the cause of “Green house effect”
Consider two rods of the same length and different specific heats (S1, S2), conductivities (K1, K2), and area of cross-sections (A1, A2) and both having temperature T1 and T2 at their ends. If the rate of loss of heat due to conduction is equal, then