When a monoatomic ideal gas expands at constant pressure, part of the supplied heat energy is used to do work and the rest increases the internal energy of the gas. For an ideal gas expanding at constant pressure, the heat energy supplied is given by the formula: \[ Q = \Delta U + W \] Where:
\( Q \) is the total heat energy supplied,
\( \Delta U \) is the change in internal energy,
\( W \) is the work done by the gas.
For a monoatomic ideal gas, the change in internal energy is given by:
\[ \Delta U = \frac{3}{2} n R \Delta T \] The work done by the gas during expansion at constant pressure is: \[ W = P \Delta V = n R \Delta T \] The fraction of heat energy converted into work is: \[ \frac{W}{Q} = \frac{n R \Delta T}{\frac{5}{2} n R \Delta T} = \frac{2}{5} \] Thus, the fraction of heat energy converted into work is \(\frac{2}{5}\).
Three conductors of same length having thermal conductivity \(k_1\), \(k_2\), and \(k_3\) are connected as shown in figure. Area of cross sections of 1st and 2nd conductor are same and for 3rd conductor it is double of the 1st conductor. The temperatures are given in the figure. In steady state condition, the value of θ is ________ °C. (Given: \(k_1\) = 60 Js⁻¹m⁻¹K⁻¹,\(k_2\) = 120 Js⁻¹m⁻¹K⁻¹, \(k_3\) = 135 Js⁻¹m⁻¹K⁻¹)
It is defined as the movement of heat across the border of the system due to a difference in temperature between system and its surroundings.
Heat can travel from one place to another in several ways. The different modes of heat transfer include: