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A positive charge 50 muC is located in x...

A positive charge 50 muC is located in xy plane at a position vector `r_0 = 4hati + 4hatj`. the electric field strength E at a point whose position vector is `vecr = 10hati - 4hatj` is (`vecr_0` and `vecr` are expressed in metre)

A

`(-1.6hati - 3.6hatj) kV/m`

B

`(3.6hati + 1.6hatj) kV/m`

C

`(hati - 3hatj) kV/m`

D

`(2.7hati - 3.6hatj)` kV/m

Text Solution

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The correct Answer is:
To find the electric field strength \( \vec{E} \) at a point given a positive charge, we can follow these steps: ### Step 1: Identify the given values - Charge \( Q = 50 \, \mu C = 50 \times 10^{-6} \, C \) - Position vector of the charge \( \vec{r_0} = 4 \hat{i} + 4 \hat{j} \) (in meters) - Position vector where we need to find the electric field \( \vec{r} = 10 \hat{i} - 4 \hat{j} \) (in meters) ### Step 2: Calculate the displacement vector \( \vec{D} \) The displacement vector \( \vec{D} \) from the charge to the point of interest is calculated as: \[ \vec{D} = \vec{r} - \vec{r_0} \] Substituting the values: \[ \vec{D} = (10 \hat{i} - 4 \hat{j}) - (4 \hat{i} + 4 \hat{j}) = (10 - 4) \hat{i} + (-4 - 4) \hat{j} = 6 \hat{i} - 8 \hat{j} \] ### Step 3: Calculate the magnitude of \( \vec{D} \) The magnitude of \( \vec{D} \) is given by: \[ |\vec{D}| = \sqrt{(6)^2 + (-8)^2} = \sqrt{36 + 64} = \sqrt{100} = 10 \, m \] ### Step 4: Calculate the unit vector \( \hat{D} \) The unit vector \( \hat{D} \) in the direction of \( \vec{D} \) is: \[ \hat{D} = \frac{\vec{D}}{|\vec{D}|} = \frac{6 \hat{i} - 8 \hat{j}}{10} = 0.6 \hat{i} - 0.8 \hat{j} \] ### Step 5: Use the formula for electric field \( \vec{E} \) The electric field \( \vec{E} \) due to a point charge is given by: \[ \vec{E} = k \frac{Q}{|\vec{D}|^2} \hat{D} \] Where \( k \) (Coulomb's constant) is \( 9 \times 10^9 \, N m^2/C^2 \). ### Step 6: Substitute the values into the formula Substituting the known values: \[ \vec{E} = 9 \times 10^9 \frac{50 \times 10^{-6}}{10^2} (0.6 \hat{i} - 0.8 \hat{j}) \] Calculating: \[ \vec{E} = 9 \times 10^9 \frac{50 \times 10^{-6}}{100} (0.6 \hat{i} - 0.8 \hat{j}) \] \[ \vec{E} = 9 \times 10^9 \times 0.5 \times 10^{-6} (0.6 \hat{i} - 0.8 \hat{j}) \] \[ \vec{E} = 4.5 \times 10^3 (0.6 \hat{i} - 0.8 \hat{j}) \] \[ \vec{E} = (4.5 \times 0.6 \times 10^3) \hat{i} - (4.5 \times 0.8 \times 10^3) \hat{j} \] \[ \vec{E} = 2700 \hat{i} - 3600 \hat{j} \, V/m \] ### Step 7: Convert to kV/m To convert to kV/m, we divide by 1000: \[ \vec{E} = 2.7 \hat{i} - 3.6 \hat{j} \, kV/m \] ### Final Result The electric field strength at the point is: \[ \vec{E} = 2.7 \hat{i} - 3.6 \hat{j} \, kV/m \]
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Knowledge Check

  • The displacement of a particle from a point having position vector 2hati + 4hatj to another point having position vector 5hatj + 1hatj is

    A
    3 units
    B
    `3sqrt2` units
    C
    5 units
    D
    ` 5sqrt3`units
  • For any vector vecr , ( vecr.hati) hati + ( vecr.hatj) hatj + ( vecr.hatk) hatk =

    A
    `vecr`
    B
    ` 2vecr`
    C
    `3vecr`
    D
    `vec0`
  • Position vectors of a particle moving in xy plane at time t is vecr=a(1-cos ometat)hati+asin omegat hatj . The path of the particle is

    A
    a circle of radius a and center at (a,0)
    B
    a circle of radius a and center at (0,0)
    C
    an ellipse
    D
    neither a circle nor an ellipse
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