The transporter experiences three forces:
- The electrostatic force due to the charges $Q$ and $-Q$.
- The friction force opposing its motion.
- The net force causing the acceleration.
The net force $F_{net}$ is given by Newton's second law:
\(F_{net} = ma\)
where $m$ is the mass of the transporter and $a$ is the acceleration.
Given $m = 1.0 \, g = 1.0 \times 10^{-3} \, kg$ and $a = 1.0 \, m/s^2$, we have:
\(F_{net} = (1.0 \times 10^{-3} \, kg)(1.0 \, m/s^2) = 1.0 \times 10^{-3} \, N\)
The net force is the difference between the electrostatic force $F_e$ and the friction force $F_f$:
\(F_{net} = F_e - F_f\)
Given $F_f = 7.0 \times 10^{-3} \, N$, we can find the electrostatic force:
\(F_e = F_{net} + F_f = 1.0 \times 10^{-3} \, N + 7.0 \times 10^{-3} \, N = 8.0 \times 10^{-3} \, N\)
The electrostatic force on the transporter is given by:
\(F_e = qE\)
where $q$ is the charge of the transporter and $E$ is the net electric field at its position.
We can find the electric field:
\(E = \frac{F_e}{q} = \frac{8.0 \times 10^{-3} \, N}{6.0 \times 10^{-10} \, C} = \frac{4}{3} \times 10^7 \, N/C\)
The net electric field due to the two charges $Q$ and $-Q$ at the location of the transporter (charge $q$) can be approximated as the field due to two point charges:
\(E = \frac{kQ}{r_1^2} - \frac{k(-Q)}{r_2^2}\),
where $r_1$ and $r_2$ are the distances from the charges $+Q$ and $-Q$ to the charge $q$ respectively, and $k = 8.99 \times 10^9 \, N m^2/C^2$ is Coulomb's constant.
Here $r_1 = 6.0 \, mm = 6.0 \times 10^{-3} \, m$ and $r_2 = 36.0 \, mm + 6.0 \, mm = 42.0 \, mm = 42.0 \times 10^{-3} \, m$.
So, \(E = kQ (\frac{1}{r_1^2} + \frac{1}{r_2^2}) \).
Therefore, \(Q = \frac{E}{k (\frac{1}{r_1^2} + \frac{1}{r_2^2})} = \frac{\frac{4}{3} \times 10^7}{8.99 \times 10^9 (\frac{1}{(6 \times 10^{-3})^2} + \frac{1}{(42 \times 10^{-3})^2})} \approx 1.667 \times 10^{-6} C\)
\\(\boxed{Q = 1.7 \times 10^{-6} C}\\)