\(ΔQ_{rej} = 50 × 540 + 50 × 1 × (100 – 20)\)
\(ΔQ_{rej} = 50 × [540 + 80]\)
\(ΔQ_{rej} = 50 × 620\)
\(ΔQ_{rej}= 31000\ cal\)
\(ΔQ_{rej} = 31 × 10^3\ cal\)
So, the answer is \(31\).
In the given cycle ABCDA, the heat required for an ideal monoatomic gas will be:
Three identical rods are joined as shown in the figure. The left and right ends are kept at \( 0^\circ C \) and \( 90^\circ C \) as shown in the figure. The temperature \( \theta \) at the junction of the rods is:
List-I | List-II | ||
P | The value of \(I1\) in Ampere is | I | \(0\) |
Q | The value of I2 in Ampere is | II | \(2\) |
R | The value of \(\omega_0\) in kilo-radians/s is | III | \(4\) |
S | The value of \(V_0\) in Volt is | IV | \(20\) |
200 |
In thermodynamics, work is a way of energy transfer from a system to surroundings, under the influence of external factors such gravity, electromagnetic forces, pressure/volume etc.
Energy (ΔU) can cross the boundary of a system in two forms -> Work (W) and Heat (q). Both work and heat refer to processes by which energy is transferred to or from a substance.
ΔU=W+q
Work done by a system is defined as the quantity of energy exchanged between a system and its surroundings. It is governed by external factors such as an external force, pressure or volume or change in temperature etc.
Work (W) in mechanics is displacement (d) against a resisting force (F).
Work has units of energy (Joule, J)