91Ó°ÊÓ

1. Radius of the circular disc,$\mathrm{r}=2.00\mathrm{cm}$
2. Arrangement of electrons and protons at angles ${\mathrm{θ}}_1=30.0^{∘}$, ${\mathrm{θ}}_2=50.0^{∘}$, ${\mathrm{θ}}_3=30.0^{∘}$, and ${\mathrm{θ}}_4=20.0^{∘}$.

Using the concept of the electric field at a given point, we can get the value of an individual electric field by a charge. Again using the superposition law, we can get the value of the electric field in its direction and this determines the net electric field at that point.

The magnitude of the electric field is given as-

$\left|\stackrel{→}{\mathrm{E}}\right|=\frac{\left|\mathrm{q}\right|}{4{\mathrm{Ï€Î\mu }}_{\mathrm{o}}\mathrm{R}}$ (i)

where, R = The distance of the field point from the charge

q = charge of the particle,

data-custom-editor="chemistry" ${\mathrm{Î\mu }}_{\mathrm{o}}$is the permittivity of vacuum.

The magnitude of the resultant vector,

$\left|\mathrm{V}\right|=\sqrt{{\mathrm{V}}_{\mathrm{x}}^2+{\mathrm{V}}_{\mathrm{y}}^2}$ (ii)

where, V_x is the horizontal component of the vector and V_y is the vertical component of the vector.

The angle or the direction of the electric field made with the x-axis,

data-custom-editor="chemistry" $\mathrm{θ}={\tan }^{-1}\left(\frac{{\mathrm{V}}_{\mathrm{y}}}{{\mathrm{V}}_{\mathrm{x}}}\right)$ (iii)

where, V_x is the horizontal component of the vector and V_y is the vertical component of the vector.

As the magnitude of the charge is the same on all the given particles and all the charges are at the same distance from the center, the magnitude of electric fields at the center will also be the same. The field of each charge can be given using equation (i) and the given values, as:

The directions of the electric fields due to the charge particles are indicated in the phasor diagram below.

Now, the components of electric field in both the x- and y-directions due to the produced fields can be given as: (for clockwise directions)

Thus, the net electric field along x-axis can be given as the sum of all the x-directional electric fields as follows:

$\begin{array}{rcl}{\mathrm{E}}_{\mathrm{x},\mathrm{net}}& =& \left\{\mathrm{Ecos}{0}^{\mathrm{o}}+\mathrm{Ecos}\left(-{150}^{\mathrm{o}}\right)+\mathrm{Ecos}\left(-{100}^{\mathrm{o}}\right)+\mathrm{Ecos}\left({130}^{\mathrm{o}}\right)+\mathrm{Ecos}\left(-{20}^{\mathrm{o}}\right)\right\}\\ & =& \left(3.6×{10}^{-9}\mathrm{N}/\mathrm{C}\right)\left\{\cos 0^{\mathrm{o}}+\cos \left(-{150}^{\mathrm{o}}\right)+\cos \left(-{100}^{\mathrm{o}}\right)+\cos \left({130}^{\mathrm{o}}\right)+\cos \left(-{20}^{\mathrm{o}}\right)\right\}\\ & =& 9.26×{10}^{-7}\mathrm{N}/\mathrm{C}\end{array}$

Now, the net electric field along y--axis can be given as the sum of all the x-directional electric fields as follows:

$\begin{array}{rcl}{\mathrm{E}}_{\mathrm{y},\mathrm{net}}& =& \left\{\mathrm{Esin}{0}^{\mathrm{o}}+\mathrm{Esin}\left(-{150}^{\mathrm{o}}\right)+\mathrm{Esin}\left(-{100}^{\mathrm{o}}\right)+\mathrm{Esin}\left({130}^{\mathrm{o}}\right)+\mathrm{Esin}\left(-{20}^{\mathrm{o}}\right)\right\}\\ & =& \left(3.6×{10}^{-9}\mathrm{N}/\mathrm{C}\right)\left\{\sin 0^{\mathrm{o}}+\sin \left(-{150}^{\mathrm{o}}\right)+\sin \left(-{100}^{\mathrm{o}}\right)+\sin \left({130}^{\mathrm{o}}\right)+\sin \left(-{20}^{\mathrm{o}}\right)\right\}\\ & =& -3.81×{10}^{-6}\mathrm{N}/\mathrm{C}\end{array}$

Thus, the magnitude of the resultant electric field is given using equation as follows:

localid="1662519095157" $\begin{array}{rcl}\left|{\mathrm{E}}_{\mathrm{net}}\right|& =& \sqrt{{\left({\mathrm{E}}_{\mathrm{x},\mathrm{net}}\right)}^2+{\left({\mathrm{E}}_{\mathrm{y},\mathrm{net}}\right)}^2}\\ & =& \sqrt{{\left(9.26×{10}^{-7}\mathrm{N}/\mathrm{C}\right)}^2+{\left(-3.81×{10}^{-6}\mathrm{N}/\mathrm{C}\right)}^2}\\ & =& 3.92×{10}^{-6}\mathrm{N}/\mathrm{C}\end{array}$

Hence, the magnitude of the net electric field is$\begin{array}{rcl}& & 3.92×{10}^{-6}\mathrm{N}/\mathrm{C}\end{array}$

Now, the direction of the net electric field using the data obtained in part (a) calculations can be given using equation (iii) as:

$\begin{array}{rcl}\mathrm{θ}& =& {\tan }^{-1}\left(\frac{-3.81×{10}^{-6}\mathrm{N}/\mathrm{C}}{9.26×{10}^{-7}\mathrm{N}/\mathrm{C}}\right)\\ & =& -76.4^{\mathrm{o}}\end{array}$

Hence, the direction of the field is $-76.4^{\mathrm{o}}$from the positive of x-axis.