\(\eta = 1 - \frac{TC}{TH}\)
\(=\)\(TH - \frac{TC}{TH}\)
\(=\) 26.81%
So,the correct option is (A)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

A body of mass of \(4\;kg\) experiences two forces \(\vec{F_1}=5\hat i+8\hat j+7\hat k \) and \(\vec{F_2}=3\hat i-4\hat j-3\hat k\) then acceleration acting on the body \(R\)
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
The Carnot engine is a theoretical heat engine that operates on the principle of a reversible thermodynamic cycle. It was developed by French engineer Nicolas Léonard Sadi Carnot in the early 19th century and is considered one of the most efficient heat engines that can be constructed.
The Carnot engine consists of four stages: isothermal expansion, adiabatic expansion, isothermal compression, and adiabatic compression. In the first stage, the working fluid in the engine is heated isothermally by a heat source, which provides the energy needed to expand the fluid and do work. In the second stage, the fluid expands adiabatically, meaning that there is no heat transfer between the fluid and its surroundings. In the third stage, the fluid is cooled isothermally by a heat sink, which removes energy from the fluid and allows it to contract and do work. In the fourth stage, the fluid is compressed adiabatically, returning it to its original state and completing the cycle.
Read More: Carnot’s Theorem
The Carnot engine is the most efficient heat engine that can be constructed, as it operates at the maximum possible efficiency for a given temperature difference between the heat source and sink. The efficiency of the Carnot engine is given by the ratio of the temperature difference between the heat source and sink to the absolute temperature of the heat source, or 1 minus the ratio of the absolute temperature of the heat sink to the absolute temperature of the heat source.
Although the Carnot engine is a theoretical construct, it has important practical applications in the design and optimization of real-world heat engines, such as internal combustion engines and steam turbines.