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Question: A point dipole is located at the origin in some orientation. The electric field at the point \( \lef...

A point dipole is located at the origin in some orientation. The electric field at the point (10cm,10cm)\left( {10cm,10cm} \right) on the x-y plane is measured to have a magnitude 1.0×103V/m1.0 \times {10^{ - 3}}V/m . What will be the magnitude of the electric field at the point (20cm,20cm)\left( {20cm,20cm} \right) ?
(A) 5.0×104V/m5.0 \times {10^{ - 4}}V/m
(B) 2.5×104V/m2.5 \times {10^{ - 4}}V/m
(C) It will depend on the orientation at the dipole
(D) 1.25×104V/m1.25 \times {10^{ - 4}}V/m

Explanation

Solution

Electric dipoles will be having two charges. Just like magnetic dipoles, we can consider electric dipoles. In a magnetic dipole, the magnetic moment vector goes from the South Pole to the North Pole inside the magnet. We resolve that along axial and equatorial to get the magnetic fields. Similarly in an electric dipole, the dipole moment vector goes from negative charge to positive charge.

Complete Step-by-step solution:
Given, the electric field intensity at the point (10cm,10cm)\left( {10cm,10cm} \right) say EE is 1.0×103V/m1.0 \times {10^{ - 3}}V/m .
First of all, we have to find the distance of the dipole from the origin. Let the distance of the dipole from the origin is rr .
Since we know the formula for finding the distance of origin from the given point is;
r=(x0)2+(y0)2=x2+y2r = \sqrt {{{\left( {x - 0} \right)}^2} + {{\left( {y - 0} \right)}^2}} = \sqrt {{x^2} + {y^2}} ………. (1)\left( 1 \right)
Put the values in the above equation,
r=102+102\Rightarrow r = \sqrt {{{10}^2} + {{10}^2}}
r=100+100=200\Rightarrow r = \sqrt {100 + 100} = \sqrt {200}
On further solving we get,
r=102cm\Rightarrow r = 10\sqrt 2 cm
To convert the distance into meters we have to divide it with   100\;100 .
r=0.12m\Rightarrow r = 0.1\sqrt 2 m
The electric field due to a dipole at any point in space is given by,
E=14πε0ρr3E = \dfrac{1}{{4\pi {\varepsilon _0}}}\dfrac{\rho }{{{r^3}}} ……… (2)\left( 2 \right)
Where,
ρ\rho is the dipole moment of the dipole
rr is the distance from the point of the dipole
On solving the equation for getting the value of dipole moment
ρ=4πε0r3(E)\Rightarrow \rho = 4\pi {\varepsilon _0}{r^3}\left( E \right) ……….. (3)\left( 3 \right)
Now, we have to calculate the electric field intensity at the point (20cm,20cm)\left( {20cm,20cm} \right) .
Let the distance of the dipole from origin now be   r\;r'
Since we know the formula to find the distance of a given point from the origin. Substitute all the values in the equation (1)\left( 1 \right) we get,
r=202+202\Rightarrow r' = \sqrt {{{20}^2} + {{20}^2}}
r=400+400=800\Rightarrow r' = \sqrt {400 + 400} = \sqrt {800}
On further solving we get,
r=202cm=0.22m\Rightarrow r' = 20\sqrt 2 cm = 0.2\sqrt 2 m
Since the dipole moment of the dipole remains the same at any point.
Therefore, the electric field intensity of the dipole at the point (20,20)\left( {20,20} \right) is,
E=14πε0ρr3E' = \dfrac{1}{{4\pi {\varepsilon _0}}}\dfrac{\rho }{{{{r'}^3}}}
Substitute the value of ρ\rho from the equation (3)\left( 3 \right) we can write,
E=14πε04πε0r3(E)r3\Rightarrow E' = \dfrac{1}{{4\pi {\varepsilon _0}}}\dfrac{{4\pi {\varepsilon _0}{r^3}\left( E \right)}}{{{{r'}^3}}}
E=r3Er3\Rightarrow E' = \dfrac{{{r^3}E}}{{{{r'}^3}}} ……….. (4)\left( 4 \right)
Substitute all the values to get the final answer,
E=(0.12)3×1×103(0.22)3\Rightarrow E' = \dfrac{{{{\left( {0.1\sqrt 2 } \right)}^3} \times 1 \times {{10}^{ - 3}}}}{{{{\left( {0.2\sqrt 2 } \right)}^3}}}
E=18×103=1.25×104V/m\Rightarrow E' = \dfrac{1}{8} \times {10^{ - 3}} = 1.25 \times {10^{ - 4}}V/m
Therefore, the magnitude of the electric field at the point (20cm,20cm)\left( {20cm,20cm} \right) is 1.25×104V/m1.25 \times {10^{ - 4}}V/m .
Hence, the correct answer is option (D).

Note:
Electric field is defined as the electric force per unit charge. The direction of the field taken to be the direction of the force it would exert on a positive test charge. The electric field radially outward from a positive charge and radially toward a negative point charge.