Concept:
An adiabatic process is a thermodynamic process in which there is no heat exchange between the system and the surroundings.
Therefore,
\[
\boxed{Q=0}
\]
According to the First Law of Thermodynamics,
\[
Q=\Delta U+W,
\]
where
\[
Q=\text{Heat supplied},
\]
\[
\Delta U=\text{Change in internal energy},
\]
\[
W=\text{Work done by the gas}.
\]
Since \(Q=0\),
\[
\boxed{W=-\Delta U.}
\]
For a monoatomic ideal gas,
\[
\boxed{\Delta U=nC_V\Delta T}
\]
where
\[
C_V=\frac{3R}{2}.
\]
Hence,
\[
\boxed{W=-nC_V\Delta T
=-\frac{3}{2}nR\Delta T.}
\]
Step 1: Write the given data.
Given,
\[
n=2\;\text{moles},
\]
\[
T_1=25^{\circ}C,
\]
\[
T_2=35^{\circ}C.
\]
Therefore,
\[
\Delta T
=
T_2-T_1
=
35-25
=
10\,K.
\]
Also,
\[
R=8.314\,J\,mol^{-1}K^{-1}.
\]
Step 2: Calculate the change in internal energy.
For a monoatomic gas,
\[
\Delta U
=
\frac32 nR\Delta T.
\]
Substituting the given values,
\[
\Delta U
=
\frac32\times2\times8.314\times10.
\]
Since,
\[
\frac32\times2=3,
\]
we get
\[
\Delta U
=
3\times8.314\times10.
\]
\[
\Delta U
=
249.42\,J.
\]
Thus,
\[
\boxed{\Delta U=249.4\,J.}
\]
Step 3: Determine the work done.
Since the process is adiabatic,
\[
W=-\Delta U.
\]
Hence,
\[
W
=
-249.4\,J.
\]
Therefore,
\[
\boxed{W=-249.4\,J.}
\]
Thus, the correct answer is
\[
\boxed{\textbf{Option (A)}}.
\]
Important Observation:
Using the standard thermodynamic convention,
\[
\boxed{W=-nC_V\Delta T,}
\]
the work done by the gas is
\[
\boxed{-249.4\,J.}
\]
Therefore, Option (A) is mathematically correct.