Post

Created by @nathanedwards
 at December 9th 2023, 8:11:29 pm.

Question:

A point charge of +4 μC is located at the origin in the xy-plane. A second point charge of -2 μC is located at (3,4) on the xy-plane.

a) Calculate the electric field due to the +4 μC charge at the point (1,2). b) Determine the total electric field at the point (3,4) due to both charges.

Answer:

a) The electric field due to a point charge can be calculated using the formula:

E=kqr2r^ \vec{E} = \frac{k \cdot q}{r^2} \cdot \hat{r}

where k=8.99×109Nm2/C2 k = 8.99 \times 10^9 \, Nm^2/C^2 (Coulomb's constant), q q is the magnitude of the point charge, r r is the distance from the point charge, and r^ \hat{r} is the unit vector pointing from the charge to the point of interest.

Given that q=+4μC=4×106C q = +4 \, \mu C = 4 \times 10^{-6} \, C and the distance r=(10)2+(20)2=5 r = \sqrt{(1-0)^2 + (2-0)^2} = \sqrt{5} .

Plugging these values into the formula, [ \vec{E}_{+4\mu C} = \frac{(8.99 \times 10^9 , Nm^2/C^2) \cdot (4 \times 10^{-6} , C)}{5} \cdot \hat{r} ]

E+4μC=(7.19×106N/C)r^ \vec{E}_{+4\mu C} = (7.19 \times 10^6 \, N/C) \cdot \hat{r}

The unit vector r^ \hat{r} for the point (1,2) is 15i+25j \frac{1}{\sqrt{5}} \vec{i} + \frac{2}{\sqrt{5}} \vec{j} . Therefore, [ \vec{E}_{+4\mu C} = (7.19 \times 10^6 , N/C) \cdot \left( \frac{1}{\sqrt{5}} \vec{i} + \frac{2}{\sqrt{5}} \vec{j} \right) ]

b) The total electric field at the point (3,4) due to both charges can be calculated by summing the electric fields due to each individual charge.

For the +4 μC charge at the origin, the electric field at (3,4) would be: [ \vec{E}_{+4\mu C} = \frac{(8.99 \times 10^9 , Nm^2/C^2) \cdot (4 \times 10^{-6} , C)}{5^2} \cdot \hat{r} = (1.44 \times 10^6 , N/C) \cdot \hat{r} ]

The unit vector r^ \hat{r} for the point (3,4) is 35i+45j \frac{3}{5} \vec{i} + \frac{4}{5} \vec{j} . Therefore, [ \vec{E}_{+4\mu C} = (1.44 \times 10^6 , N/C) \cdot \left( \frac{3}{5} \vec{i} + \frac{4}{5} \vec{j} \right) ]

For the -2 μC charge at (3,4) the electric field magnitude and unit vector are: [ \vec{E}_{-2\mu C} = \frac{(8.99 \times 10^9 , Nm^2/C^2) \cdot (2 \times 10^{-6} , C)}{0^2} \cdot \hat{r} = \infty ]

Since the point is on the charge itself, the electric field due to the -2 μC charge at (3,4) is infinite due to the singularity at the location of the charge.

Adding the electric fields due to both charges gives the total electric field at (3,4): [ \vec{E}{total} = \vec{E}{+4\mu C} + \vec{E}_{-2\mu C} = (1.44 \times 10^6 , N/C) \cdot \left( \frac{3}{5} \vec{i} + \frac{4}{5} \vec{j} \right) + \infty ]

Thus, the total electric field at the point (3,4) is undefined due to the singularity at the location of the -2 μC charge.