A charge
q = 1,0 μC is fixed at a point
O in space. A second charge
Q = 25,0.10
−8 C and weight
W = 2,5.10
−2 N is limited in
motion to the vertical passing through
O. The charges are in a vacuum. Determine:
a) Is charge
Q in equilibrium above or below
O?
b) What is the distance between the charges at equilibrium?
c) The type of equilibrium of
Q, stable, unstable, or indifferent?
Problem data:
- Charge q: q = 1.0 μC = 1.0 × 10−6 C;
- Charge Q: Q = 25.0 × 10−8 C;
- Weight of sphere of charge Q: W = 2.5 × 10−2 N;
- Coulomb constant:
\( k_{0}=9\times 10^{9}\;\frac{\text{N.m}^{2}}{\text{C}^{2}} \).
Problem diagram:
We choose a reference frame oriented upwards with the origin at the point where the fixed charge
q is placed, the acceleration due to gravity is equal to g oriented downwards (Figure 1).
The free charge Q is a distance d from the origin. As the two charges are positive, the
electric force
\( {\vec{F}}_{E} \)
between them is a repulsive force and the weight
\( \vec{W} \)
acting on the charge Q points downwards in the same direction as the acceleration due to gravity.
Solution
a) For the system to remain in equilibrium, the resultant of the forces acting on the charge
Q must
be zero.
\[
\begin{gather}
\bbox[#99CCFF,10px]
{\sum \vec{F}=0}
\end{gather}
\]
From Figure 1, we can write
\[
\begin{gather}
F_{E}-W=0 \tag{I}
\end{gather}
\]
according to
Coulomb's Law, the electric force is given by
\[
\begin{gather}
\bbox[#99CCFF,10px]
{F_{E}=k_{0}\frac{|Q|\;|q|}{r^{2}}} \tag{II}
\end{gather}
\]
substituting expression (II) into expression (I)
\[
\begin{gather}
k_{0}\frac{|Q||q|}{r^{2}}-P=0\\[5pt]
9\times 10^{9}\times \frac{|25.0\times 10^{-8}\;||1.0\times 10^{-6}\;|}{d^{2}}-2.5\times 10^{-2}=0\\[5pt]
9\times 10^{9}\times \frac{25.0\times 10^{-8}1.0\times 10^{-6}}{d^{2}}=2.5\times 10^{-2}\\[5pt]
9\times 10^{9}\times 25.0\times 10^{-14}=2.5\times 10^{-2}d^{2}\\[5pt]
d^{2}=\frac{9\times 25,0.10^{-5}}{2.5\times 10^{-2}}\\[5pt]
d^{2}=9\times 10\times 10^{-5}\times 10^{2}\\[5pt]
d^{2}=9\times 10^{-2}\\[5pt]
d=\sqrt{9\times 10^{-2}\;}\\[5pt]
d=\pm 3\times 10^{-1}\;\text{m}
\end{gather}
\]
For the positive root, the charge is above point O, as the charges are positive, the repulsive
force at Q points upwards, and the weight points downwards, these forces cancel each other out,
and the charge is in equilibrium (Figure 2-A). For the negative root, the charge is below point
O, the repulsive force points downwards, and the weight points downwards, there will be a net
force in that direction that will make the charge Q move away from q, the situation is not
one of equilibrium.
Charge Q is in equilibrium
above
point O.
b) At equilibrium, the distance between the charges will be
\[
\begin{gather}
\bbox[#FFCCCC,10px]
{d=3\times 10^{-1}\;\text{m}}
\end{gather}
\]
c) Initially, the charge Q is in an equilibrium position at a distance d from the charge
q, in this point, the electric force and the weight force cancel each other out (Figure 3-A). As
the magnitude of the electric force given by Coulomb's Law is equal to FE if
the charge Q is displaced upwards, increasing the distance d from the charge q, the
denominator of expression (II) increases as a result, and the electric force decreases. As weight is
constant, this gives rise to a net downward force bringing the system back to equilibrium (Figure 3-B).
If the charge Q is shifted downwards, decreasing the distance d from the charge q,
the denominator of expression (II) decreases, and as a result, the electric force increases. As the
weight force is constant, this gives rise to a net upward force which brings the system back to
equilibrium (Figure 3-C).
So the equilibrium is
stable.