We describe some solvable models which illustrate the Jarzynski theorem and related fluctuation theorems. We consider a charged particle in the presence of magnetic field in a two dimensional harmonic well. In the first case the centre of the harmonic potential is translated with a uniform velocity, while in the other case the particle is subjected to an ac force. We show that Jarzynski identity complements Bohr-van Leeuwen theorem on the absence of diamagnetism in equilibrium classical system. PACS numbers: 05.70. Ln, 05.40. a, 05.40.Jc Most processes that occur in nature are far from equilibrium and hence cannot be treated within the framework of classical thermodynamics. The traditional nonequilibrium statistical mechanics deals with systems near equilibrium in the linear response regime. Its success has lead to the formulation of fluctuation-dissipation relation, Onsagar's reciprocity relations and the KuboGreen formulae, etc. However, very recent developments in nonequilibrium statistical mechanics have resulted in the discovery of some exact theoretical results for systems driven far away from equilibrium and are collectively called fluctuation theorems [1]. These results include entropy production theorems The concept of free energy is of central importance in statistical mechanics and thermodynamics. With the help of free energy one can calculate all the phases of a system and their physical properties. However, the free energy of the system relative to an arbitrary reference state is often difficult to determine. Jarzynski equality(JE) relates non-equilibrium quantities with equilibrium free energies [3]. In this prescription, initially the system is assumed to be in equilibrium state determined by a thermodynamic parameter A defined by a control parameter λ A and is kept in contact with a heat bath at temperature T. The nonequilibrium process is obtained by changing the thermodynamic control parameter λ in a finite time τ according to a prescribed protocol λ(t), from λ A = λ(t=0) to some final value λ B = λ(t = τ ). The final state of the system at time τ (at the end of the protocol) will in general not be at equilibrium. It will equilibrate to a final state B(≡ λ B ) if it is further allowed to evolve by keeping parameter λ B fixed. JE states thatWhere ∆F is the free energy difference between equilibrium states A and B. Angular bracket ... denotes the average taken over different realizations for fixed protocol λ(t). W is work expended during each repetation of the protocol and is a realization dependent random variable. Jarzynski's theorem has been derived using various methods with different system dynamics [3][4][5]8]. This remarkable identity provides a practical tool to determine equilibrium thermodynamic potentials from processes carried out arbitrarily far away from equilibrium. This identity has been used to extract equilibrium free energy differences in experiments. Work distributions have been calculated analytically for several model systems and tested against various fluctuati...