A particle of charge q and mass m is projected from origin with an...

According to the work-energy theorem, the change in kinetic energy of a particle is equal to the total work done by all the forces acting on it.

The forces acting on the particle are the electric force and the magnetic force. The magnetic force is given by $\vec{F}_B = q(\vec{v} \times \vec{B})$. Since the magnetic force is always perpendicular to the velocity vector of the particle, the work done by the magnetic field is zero.

The change in kinetic energy is equal to the work done by the electric field alone. The electric force is $\vec{F}_E = q\vec{E} = qE_0 e^{-\lambda x}\hat{x}$.

The work done by the electric field as the particle moves from $x = 0$ to $x = L$ is given by

$W_E = \int_{0}^{L} \vec{F}_E \cdot d\vec{r} = \int_{0}^{L} qE_0 e^{-\lambda x} dx$

Evaluating the integral, we get

$W_E = qE_0 \left[ \dfrac{e^{-\lambda x}}{-\lambda} \right]_{0}^{L}$

$W_E = -\dfrac{qE_0}{\lambda} (e^{-\lambda L} - e^{0})$

$W_E = \dfrac{qE_0}{\lambda} [1 - e^{-\lambda L}]$

Thus, the change in kinetic energy is $\dfrac{qE_0}{\lambda} [1 - e^{-\lambda L}]$.

Answer: $\dfrac{qE_0}{\lambda}[1 - e^{-\lambda L}]$