Solveeit Logo

Question

Question: Electric field at a point \(\left( {30,30,0} \right)\) due to a point charge of \[8 \times {10^{ - 3...

Electric field at a point (30,30,0)\left( {30,30,0} \right) due to a point charge of 8×103μc8 \times {10^{ - 3}}\mu c placed at origin will be (coordinates are in cm)
(a) 8000N/C\left( a \right){\text{ 8000N/C}}
(b) 4000(i+j)N/C\left( b \right){\text{ 4000}}\left( {\mathop i\limits^ \wedge + \mathop j\limits^ \wedge } \right){\text{N/C}}
(c) 2002(i+j)N/C\left( c \right){\text{ 200}}\sqrt 2 \left( {\mathop i\limits^ \wedge + \mathop j\limits^ \wedge } \right){\text{N/C}}
(d) 4002(i+j)N/C\left( d \right){\text{ 400}}\sqrt 2 \left( {\mathop i\limits^ \wedge + \mathop j\limits^ \wedge } \right){\text{N/C}}

Explanation

Solution

Hint So to solve this problem, first of all, we calculate the distance of the charge from the origin, and then the electric field will be calculated by using the formulaE=14πε0×qd2E = \dfrac{1}{{4\pi {\varepsilon _0}}} \times \dfrac{q}{{{d^2}}}. And then the angle will also be calculated as the electric field we will get is negative. And lastly, the vector form of the electric field will be calculated by using the formulaE=E[cosϕi+sinϕj]\vec E = E\left[ {\cos \phi \mathop i\limits^ \wedge + \sin \phi \mathop j\limits^ \wedge } \right].
Formula used:
Electric field,
E=14πε0×qd2E = \dfrac{1}{{4\pi {\varepsilon _0}}} \times \dfrac{q}{{{d^2}}}
Here,
EE, will be an electric field
qq, will be the charge
dd, will be the separation between them
ε0{\varepsilon _0}, permittivity
The vector form of the electric field is given by-
E=E[cosϕi+sinϕj]\vec E = E\left[ {\cos \phi \mathop i\limits^ \wedge + \sin \phi \mathop j\limits^ \wedge } \right]

Complete Step by Step Solution First of all we will calculate the distance of the charge from the origin
d=0.302+0.302\Rightarrow d = \sqrt {{{0.30}^2} + {{0.30}^2}}
And on solving, we get
0.30×2cm\Rightarrow 0.30 \times \sqrt 2 cm
Now, since we have distance then we will calculate the electric field.
E=14πε0×qd2E = \dfrac{1}{{4\pi {\varepsilon _0}}} \times \dfrac{q}{{{d^2}}}
Substituting the values, we get
9×109×(8×109)×10.302×2NC\Rightarrow 9 \times {10^9} \times \left( { - 8 \times {{10}^{ - 9}}} \right) \times \dfrac{1}{{{{0.30}^2} \times 2}}\dfrac{N}{C}
On solving the above, we get
400NC\Rightarrow - 400\dfrac{N}{C}
Now, we will calculate the electric field strength in the direction of θ\theta
tanθ=30cm30cm\tan \theta = \dfrac{{30cm}}{{30cm}}
And we will get tanθ=1\tan \theta = 1
Since it’s making 450{45^0}with the xaxisx - axis
And from this,
cosθ=12\cos \theta = \dfrac{1}{{\sqrt 2 }} And sinθ=12\sin \theta = \dfrac{1}{{\sqrt 2 }}
Since the EEis negative then the θ\theta will be in the 3rd3rdquadrant
So from this, we can say
θ=1800+450\Rightarrow \theta = {180^0} + {45^0}
In the addition, we get
θ=2250\Rightarrow \theta = {225^0}
Now, the vector form of the electric field will be
E=E[cosϕi+sinϕj]\vec E = E\left[ {\cos \phi \mathop i\limits^ \wedge + \sin \phi \mathop j\limits^ \wedge } \right]
Substituting the values, we get
E=(4002)[i+j]NC\vec E = \left( {\dfrac{{400}}{{\sqrt 2 }}} \right)\left[ {\mathop i\limits^ \wedge + \mathop j\limits^ \wedge } \right]\dfrac{N}{C}
Now we can write it as,
E=(2002)[i+j]NC\vec E = \left( {200\sqrt 2 } \right)\left[ {\mathop i\limits^ \wedge + \mathop j\limits^ \wedge } \right]\dfrac{N}{C}

Therefore, the option (c)\left( c \right) is correct.

Note It is the quality of an electric field at a given point or it can likewise be characterized as the power experienced by a unit positive charge set in the electric field. Electric Field intensity is a property of that point in space, whereas F is a property of the point charge placed at the point - a very subtle difference.