Concept:
When an electric dipole is placed in a uniform electric field,
• the net force on the dipole is zero,
• a torque acts on the dipole if its dipole moment is not parallel to the field.
The force on a charge in an electric field is
\[
\vec F=q\vec E.
\]
The torque on a dipole is
\[
\vec\tau=\vec p\times\vec E.
\]
Step 1: Determine the dipole moment.
The charges are situated along the \(x\)-axis.
Therefore the dipole axis lies along the \(x\)-direction.
Hence
\[
\vec p
=
p\,\hat{i}.
\]
where
\[
p=q|a-b|.
\]
Step 2: Calculate the net force on the dipole.
Force on charge \(+q\) is
\[
\vec F_1
=
q\vec E.
\]
Since
\[
\vec E=2\hat{i},
\]
\[
\vec F_1
=
2q\hat{i}.
\]
Force on charge \(-q\) is
\[
\vec F_2
=
(-q)\vec E.
\]
Therefore,
\[
\vec F_2
=
-2q\hat{i}.
\]
Hence total force is
\[
\vec F
=
\vec F_1+\vec F_2.
\]
\[
\vec F
=
2q\hat{i}-2q\hat{i}.
\]
\[
\boxed{
\vec F=0
}
\]
Thus a uniform electric field exerts no net translational force on the dipole.
Step 3: Calculate the torque on the dipole.
The torque is
\[
\vec\tau
=
\vec p\times\vec E.
\]
Since both \(\vec p\) and \(\vec E\) are along the \(x\)-axis,
\[
\vec p
=
p\hat{i},
\qquad
\vec E
=
2\hat{i}.
\]
Therefore,
\[
\vec\tau
=
(p\hat{i})\times(2\hat{i}).
\]
Since
\[
\hat{i}\times\hat{i}=0,
\]
we get
\[
\boxed{
\vec\tau=0
}
\]
Final Answer:
\[
\boxed{\vec F=0}
\]
and
\[
\boxed{\vec\tau=0}
\]