Concept:
The total electrostatic potential energy of a system of charges placed in an external electric field consists of two separate contributions:
• Potential energy of each charge due to the external electric field.
• Mutual interaction energy between the charges themselves.
Thus, for two charges $q_1$ and $q_2$,
\[
U_{\text{total}}
=
q_1V(r_1)+q_2V(r_2)
+
\frac{1}{4\pi\varepsilon_0}
\frac{q_1q_2}{r_{12}},
\]
where
\[
V(r)=\text{electric potential due to the external field},
\]
and
\[
r_{12}=\text{distance between the two charges}.
\]
Therefore, our first task is to determine the electric potential corresponding to the given electric field.
Step 1: Determine the electric potential associated with the given electric field.
The electric field is given as
\[
E(r)=1.8\times10^5r^{-2}.
\]
The relationship between electric field and electric potential is
\[
E=-\frac{dV}{dr}.
\]
Hence,
\[
V=-\int E\,dr.
\]
Substituting the given field,
\[
V
=
-\int 1.8\times10^5r^{-2}\,dr.
\]
Since
\[
\int r^{-2}dr=-r^{-1},
\]
we obtain
\[
V
=
-\left[
1.8\times10^5(-r^{-1})
\right].
\]
Therefore,
\[
V(r)
=
\frac{1.8\times10^5}{r}.
\]
Thus, the electric potential at a distance $r$ from the origin is
\[
V(r)=\frac{1.8\times10^5}{r}.
\]
Step 2: Calculate the electric potential at the locations of both charges.
The coordinates of the charges are
\[
(-2.7\text{ cm},0)
\]
and
\[
(2.7\text{ cm},0).
\]
Both charges are at the same distance from the origin:
\[
r_1=r_2=2.7\text{ cm}.
\]
Converting into SI units,
\[
r_1=r_2=0.027\text{ m}.
\]
Therefore,
\[
V(r_1)=V(r_2)
=
\frac{1.8\times10^5}{0.027}.
\]
Writing
\[
0.027=27\times10^{-3},
\]
we get
\[
V
=
\frac{1.8\times10^5}{27\times10^{-3}}
=
\frac{1.8}{27}\times10^8.
\]
Since
\[
\frac{1.8}{27}
=
\frac{1}{15},
\]
therefore
\[
V
=
\frac{10^8}{15}
=
6.67\times10^6\text{ V}.
\]
Equivalently,
\[
V
=
\frac{2}{3}\times10^7\text{ V}.
\]
Step 3: Calculate the potential energy of the first charge in the external field.
For
\[
q_1=+6\mu\text{C}
=
6\times10^{-6}\text{ C},
\]
the potential energy is
\[
U_1=q_1V.
\]
Thus,
\[
U_1
=
(6\times10^{-6})
\left(
\frac{2}{3}\times10^7
\right).
\]
Simplifying,
\[
U_1
=
4\times10^1.
\]
Hence,
\[
U_1=40\text{ J}.
\]
Step 4: Calculate the potential energy of the second charge in the external field.
For
\[
q_2=-3\mu\text{C}
=
-3\times10^{-6}\text{ C},
\]
the potential energy is
\[
U_2=q_2V.
\]
Substituting,
\[
U_2
=
(-3\times10^{-6})
\left(
\frac{2}{3}\times10^7
\right).
\]
Therefore,
\[
U_2=-20\text{ J}.
\]
Step 5: Calculate the mutual interaction energy between the two charges.
The separation between the charges is
\[
r_{12}
=
2.7-(-2.7).
\]
Thus,
\[
r_{12}=5.4\text{ cm}.
\]
Converting into SI units,
\[
r_{12}=0.054\text{ m}.
\]
The interaction energy is
\[
U_{12}
=
\frac{1}{4\pi\varepsilon_0}
\frac{q_1q_2}{r_{12}}.
\]
Substituting the values,
\[
U_{12}
=
\frac{9\times10^9
(6\times10^{-6})
(-3\times10^{-6})}
{0.054}.
\]
Simplifying,
\[
U_{12}
=
\frac{-162\times10^{-3}}
{54\times10^{-3}}.
\]
Therefore,
\[
U_{12}=-3\text{ J}.
\]
The negative sign indicates attraction between opposite charges.
Step 6: Calculate the total electrostatic energy of the system.
The total energy is
\[
U_{\text{total}}
=
U_1+U_2+U_{12}.
\]
Substituting the calculated values,
\[
U_{\text{total}}
=
40+(-20)+(-3).
\]
Hence,
\[
U_{\text{total}}
=
17\text{ J}.
\]
Final Conclusion:
The net electrostatic energy of the two-charge system is
\[
\boxed{17\text{ J}}.
\]
Therefore, the correct answer is
\[
\boxed{\text{(B) }17\text{ J}}.
\]