Place $+5\times10^{-8}\,\text{C}$ at $x=0$ and $-3\times10^{-8}\,\text{C}$ at $x=0.16\,\text{m}$. For zero potential, $5/r_1=3/r_2$. Between the charges, $r_1=x$ and $r_2=0.16-x$, so $5(0.16-x)=3x$, giving $x=0.10\,\text{m}$. To the right of the negative charge, $r_1=x$ and $r_2=x-0.16$, so $5(x-0.16)=3x$, giving $x=0.40\,\text{m}$. No solution lies to the left of the positive charge.
The potential is zero at a point between the charges, $10\,\text{cm}$ from the $+5\times10^{-8}\,\text{C}$ charge, and at a point outside on the side of the negative charge, $40\,\text{cm}$ from the positive charge.
For a regular hexagon, the distance from the centre to each vertex equals the side, $r=0.10\,\text{m}$. Potential is a scalar, so $V=6(kq/r)=6(9\times10^9)(5\times10^{-6})/0.10=2.7\times10^6\,\text{V}$.
$2.7\times10^6\,\text{V}$.
For any point on the perpendicular bisector plane of AB, the distances from $+2\,\mu\text{C}$ and $-2\,\mu\text{C}$ are equal, so their potentials cancel. Hence the plane is an equipotential surface. Since electric field is normal to an equipotential surface, its direction is along AB, from the positive charge at A to the negative charge at B.
(a) The plane perpendicular to AB through its midpoint is an equipotential surface of zero potential. (b) The electric field is perpendicular to this plane and directed from the positive charge towards the negative charge.
Inside a conductor in electrostatic equilibrium, $E=0$. Outside a charged spherical conductor, the field is as if all charge were at the centre. Just outside, $r=0.12\,\text{m}$, so $E=kq/r^2=9\times10^9(1.6\times10^{-7})/(0.12)^2=1.0\times10^5\,\text{N C}^{-1}$. At $r=0.18\,\text{m}$, $E=9\times10^9(1.6\times10^{-7})/(0.18)^2=4.4\times10^4\,\text{N C}^{-1}$.
(a) $0$; (b) $1.0\times10^5\,\text{N C}^{-1}$, radially outward; (c) $4.4\times10^4\,\text{N C}^{-1}$, radially outward.
For a parallel-plate capacitor, $C\propto K/d$. Initially $K\approx1$ and $C=8\,\text{pF}$. Reducing $d$ to $d/2$ doubles the capacitance, and inserting dielectric $K=6$ multiplies it by 6. Thus $C'=12C=96\,\text{pF}$.
$96\,\text{pF}$.
For three equal capacitors $C$ in series, $C_{\text{eq}}=C/3=9/3=3\,\text{pF}$. The charge on each capacitor in series is the same, and since the capacitances are equal, the voltage divides equally. Therefore each capacitor has $120/3=40\,\text{V}$ across it.
(a) $3\,\text{pF}$; (b) $40\,\text{V}$ across each capacitor.
In parallel, capacitances add: $C_{\text{eq}}=2+3+4=9\,\text{pF}$. Each capacitor has the same potential difference, $100\,\text{V}$. Thus $Q_1=2\,\text{pF}\times100\,\text{V}=200\,\text{pC}$, $Q_2=300\,\text{pC}$ and $Q_3=400\,\text{pC}$.
(a) $9\,\text{pF}$; (b) charges are $200\,\text{pC}$, $300\,\text{pC}$ and $400\,\text{pC}$ respectively.
For air, $C=\epsilon_0A/d=(8.854\times10^{-12})(6\times10^{-3})/(3\times10^{-3})=1.77\times10^{-11}\,\text{F}=17.7\,\text{pF}$. With $V=100\,\text{V}$, $Q=CV=1.77\times10^{-11}\times100=1.77\times10^{-9}\,\text{C}$.
$17.7\,\text{pF}$; charge on each plate has magnitude $1.77\times10^{-9}\,\text{C}$.
The mica fills the full separation, so the capacitance becomes $C'=KC=6C=106\,\text{pF}$. (a) If the battery remains connected, $V$ stays $100\,\text{V}$, so $Q'=C'V=6CV=1.06\times10^{-8}\,\text{C}$; extra charge flows from the battery. (b) If the battery is disconnected before insertion, $Q$ remains $1.77\times10^{-9}\,\text{C}$, while $C$ becomes $6C$. Hence $V'=Q/C'=V/6=16.7\,\text{V}$ and the field and stored energy decrease.
(a) With the supply connected, the voltage remains $100\,\text{V}$ and the capacitance and charge become 6 times larger. (b) With the supply disconnected, charge remains fixed, capacitance becomes 6 times larger, and voltage falls to one-sixth of its original value.
The stored energy is $U=\frac12CV^2$. With $C=12\times10^{-12}\,\text{F}$ and $V=50\,\text{V}$, $U=\frac12(12\times10^{-12})(50)^2=1.5\times10^{-8}\,\text{J}$.
$1.5\times10^{-8}\,\text{J}$.
Initial energy is $U_i=\frac12CV^2=\frac12(600\times10^{-12})(200)^2=1.2\times10^{-5}\,\text{J}$. After connection to an identical uncharged capacitor, charge is shared equally and the final voltage is $100\,\text{V}$. The equivalent capacitance is $1200\,\text{pF}$, so $U_f=\frac12(1200\times10^{-12})(100)^2=6.0\times10^{-6}\,\text{J}$. Energy lost $=U_i-U_f=6.0\times10^{-6}\,\text{J}$.
$6.0\times10^{-6}\,\text{J}$.