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The electric field at (30, 30) cm due to...

The electric field at (30, 30) cm due to a charge of `-8nC` at the origin in `NC^(-1)` is

A

`-400 (bar(i) + bar(j))`

B

`400 (bar(I) + bar(j))`

C

`-200 sqrt2 (bar(i) + bar(j))`

D

`200 sqrt2 (bar(i) + bar(j))`

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The correct Answer is:
To find the electric field at the point (30 cm, 30 cm) due to a charge of -8 nC located at the origin, we can follow these steps: ### Step 1: Convert the coordinates to meters The coordinates given are in centimeters. We need to convert them to meters. - \( x = 30 \, \text{cm} = 0.3 \, \text{m} \) - \( y = 30 \, \text{cm} = 0.3 \, \text{m} \) ### Step 2: Calculate the position vector The position vector \( \vec{r} \) from the origin to the point (0.3 m, 0.3 m) is: \[ \vec{r} = 0.3 \hat{i} + 0.3 \hat{j} \, \text{m} \] ### Step 3: Calculate the magnitude of the position vector The magnitude of \( \vec{r} \) is calculated using the Pythagorean theorem: \[ |\vec{r}| = \sqrt{(0.3)^2 + (0.3)^2} = \sqrt{0.09 + 0.09} = \sqrt{0.18} = 0.3\sqrt{2} \, \text{m} \] ### Step 4: Use the formula for electric field The electric field \( \vec{E} \) due to a point charge \( q \) is given by: \[ \vec{E} = \frac{1}{4 \pi \epsilon_0} \frac{q}{|\vec{r}|^2} \hat{r} \] where \( \hat{r} \) is the unit vector in the direction of \( \vec{r} \). ### Step 5: Calculate the unit vector \( \hat{r} \) The unit vector \( \hat{r} \) is given by: \[ \hat{r} = \frac{\vec{r}}{|\vec{r}|} = \frac{0.3 \hat{i} + 0.3 \hat{j}}{0.3\sqrt{2}} = \frac{1}{\sqrt{2}} \hat{i} + \frac{1}{\sqrt{2}} \hat{j} \] ### Step 6: Substitute values into the electric field equation Given: - \( q = -8 \, \text{nC} = -8 \times 10^{-9} \, \text{C} \) - \( \epsilon_0 = 8.85 \times 10^{-12} \, \text{C}^2/\text{N m}^2 \) Substituting the values into the electric field equation: \[ \vec{E} = \frac{1}{4 \pi (8.85 \times 10^{-12})} \frac{-8 \times 10^{-9}}{(0.3\sqrt{2})^2} \left( \frac{1}{\sqrt{2}} \hat{i} + \frac{1}{\sqrt{2}} \hat{j} \right) \] ### Step 7: Calculate the magnitude of the electric field Calculating the denominator: \[ (0.3\sqrt{2})^2 = 0.18 \, \text{m}^2 \] Now substituting this into the electric field equation: \[ \vec{E} = \frac{1}{4 \pi (8.85 \times 10^{-12})} \frac{-8 \times 10^{-9}}{0.18} \left( \frac{1}{\sqrt{2}} \hat{i} + \frac{1}{\sqrt{2}} \hat{j} \right) \] ### Step 8: Final calculations Calculating the constant: \[ \frac{1}{4 \pi (8.85 \times 10^{-12})} \approx 9 \times 10^9 \, \text{N m}^2/\text{C}^2 \] Thus: \[ \vec{E} = 9 \times 10^9 \cdot \frac{-8 \times 10^{-9}}{0.18} \left( \frac{1}{\sqrt{2}} \hat{i} + \frac{1}{\sqrt{2}} \hat{j} \right) \] Calculating: \[ \vec{E} = \frac{-72 \times 10^0}{0.18} \left( \frac{1}{\sqrt{2}} \hat{i} + \frac{1}{\sqrt{2}} \hat{j} \right) = -400 \sqrt{2} \hat{i} - 400 \sqrt{2} \hat{j} \, \text{N/C} \] ### Final Result The electric field at (30 cm, 30 cm) due to a charge of -8 nC at the origin is: \[ \vec{E} = -200\sqrt{2} \hat{i} - 200\sqrt{2} \hat{j} \, \text{N/C} \]
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AAKASH SERIES-ELECTRIC CHARGES AND FIELDS-Exercise-II
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