689. Four charges $q_1 = 1 \, \mu C$, $q_2 = -1 \, \mu C$, $q_3 = 2 \, \mu C$, and $q_4 = -2 \, \mu C$ are placed at the corners of a square of side $1 \, m$. What is the direction of the net force on $q_1$?
Key Concept: Superposition principle, vector form
c) At $77.2^\circ$ below the $-x$ axis
[Solution Description]
Let the square have vertices at $(0,0)$, $(1,0)$, $(1,1)$, and $(0,1)$, with $q_1$ at $(0,0)$.
Force due to $q_2$ (at $(1,0)$):
$\vec{F}_{12} = k \frac{q_1 q_2}{r^2} \, \hat{i} = 9 \times 10^9 \frac{(1 \times 10^{-6})(-1 \times 10^{-6})}{1^2} \, \hat{i} = -9 \times 10^{-3} \, \hat{i} \, N$
Force due to $q_3$ (at $(1,1)$):
The distance is $\sqrt{1^2 + 1^2} = \sqrt{2} \, m$.
The force components are:
$F_{13x} = F_{13y} = 9 \times 10^9 \frac{(1 \times 10^{-6})(2 \times 10^{-6})}{(\sqrt{2})^2} \cdot \frac{1}{\sqrt{2}} = \frac{18 \times 10^{-3}}{2} \cdot \frac{1}{\sqrt{2}} = 6.36 \times 10^{-3} \, N$
Thus, $\vec{F}_{13} = 6.36 \times 10^{-3} \, \hat{i} + 6.36 \times 10^{-3} \, \hat{j} \, N$
Force due to $q_4$ (at $(0,1)$):
$\vec{F}_{14} = k \frac{q_1 q_4}{r^2} \, \hat{j} = 9 \times 10^9 \frac{(1 \times 10^{-6})(-2 \times 10^{-6})}{1^2} \, \hat{j} = -18 \times 10^{-3} \, \hat{j} \, N$
Net force:
$\vec{F}_{\text{net}} = \vec{F}_{12} + \vec{F}_{13} + \vec{F}_{14}$
$\vec{F}_{\text{net}} = (-9 + 6.36) \times 10^{-3} \, \hat{i} + (6.36 - 18) \times 10^{-3} \, \hat{j}$
$\vec{F}_{\text{net}} = -2.64 \times 10^{-3} \, \hat{i} - 11.64 \times 10^{-3} \, \hat{j} \, N$
The direction is given by:
$\theta = \tan^{-1}\left(\frac{-11.64}{-2.64}\right) \approx 77.2^\circ$
This is in the third quadrant, towards $-x$ and $-y$.
Your Answer is correct.
c) At $77.2^\circ$ below the $-x$ axis
[Solution Description]
Let the square have vertices at $(0,0)$, $(1,0)$, $(1,1)$, and $(0,1)$, with $q_1$ at $(0,0)$.
Force due to $q_2$ (at $(1,0)$):
$\vec{F}_{12} = k \frac{q_1 q_2}{r^2} \, \hat{i} = 9 \times 10^9 \frac{(1 \times 10^{-6})(-1 \times 10^{-6})}{1^2} \, \hat{i} = -9 \times 10^{-3} \, \hat{i} \, N$
Force due to $q_3$ (at $(1,1)$):
The distance is $\sqrt{1^2 + 1^2} = \sqrt{2} \, m$.
The force components are:
$F_{13x} = F_{13y} = 9 \times 10^9 \frac{(1 \times 10^{-6})(2 \times 10^{-6})}{(\sqrt{2})^2} \cdot \frac{1}{\sqrt{2}} = \frac{18 \times 10^{-3}}{2} \cdot \frac{1}{\sqrt{2}} = 6.36 \times 10^{-3} \, N$
Thus, $\vec{F}_{13} = 6.36 \times 10^{-3} \, \hat{i} + 6.36 \times 10^{-3} \, \hat{j} \, N$
Force due to $q_4$ (at $(0,1)$):
$\vec{F}_{14} = k \frac{q_1 q_4}{r^2} \, \hat{j} = 9 \times 10^9 \frac{(1 \times 10^{-6})(-2 \times 10^{-6})}{1^2} \, \hat{j} = -18 \times 10^{-3} \, \hat{j} \, N$
Net force:
$\vec{F}_{\text{net}} = \vec{F}_{12} + \vec{F}_{13} + \vec{F}_{14}$
$\vec{F}_{\text{net}} = (-9 + 6.36) \times 10^{-3} \, \hat{i} + (6.36 - 18) \times 10^{-3} \, \hat{j}$
$\vec{F}_{\text{net}} = -2.64 \times 10^{-3} \, \hat{i} - 11.64 \times 10^{-3} \, \hat{j} \, N$
The direction is given by:
$\theta = \tan^{-1}\left(\frac{-11.64}{-2.64}\right) \approx 77.2^\circ$
This is in the third quadrant, towards $-x$ and $-y$.