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Question: Two electric dipoles of moment \(P\) and \(64P\) are placed in opposite directions on a line at a di...

Two electric dipoles of moment PP and 64P64P are placed in opposite directions on a line at a distance of 25cm25cm. The electric field will be zero at point between the dipoles whose distance from the dipole of moment PP is
A.5cm5cm
B.259cm\dfrac{25}{9}cm
C.10cm10cm
D.413cm\dfrac{4}{13}cm

Explanation

Solution

We are given two dipoles of different magnitudes which are inclined along the axial position with respect to each other. The electric field due to these two dipoles must be equal to zero at some point between the two dipoles on the line joining them. Thus, we shall apply the formula of electric field on the dipoles given and then find the distance x from dipole PPat which the electric field is zero.

Complete answer:
The electric field (E)\left( {\vec{E}} \right) due to an electric dipole at axial position is given as:
E=2kpr3\vec{E}=\dfrac{2kp}{{{r}^{3}}}
Where,
k=14πε0=9×109Nm2C2k=\dfrac{1}{4\pi {{\varepsilon }_{0}}}=9\times {{10}^{9}}N{{m}^{2}}{{C}^{-2}} and ε0=8.85×1012Fm1{{\varepsilon }_{0}}=8.85\times {{10}^{-12}}F{{m}^{-1}} is the permittivity of free space
p=p= magnitude of dipole moment
r=r= distance between dipole and point of observation
Let the electric field be zero at a distance xx from dipole PP.

For dipole 1, we have p=Pp=P and r=xr=x,
Substituting these values, we get
E=2kPx3\vec{E}=\dfrac{2kP}{{{x}^{3}}} ……………….. equation (1)
For dipole 2, we have p=64Pp=64P and r=25xr=25-x,
Substituting these values, we get
E=2k(64P)(25x)3\vec{E}=\dfrac{2k\left( 64P \right)}{{{\left( 25-x \right)}^{3}}} ……………….. equation (2)
Since the electric field at distance xx is zero, thus we shall take the net electric fields due to both dipoles at this point and equate it to zero.
From equation (1) and (2), we have
2kPx32k(64P)(25x)3=0\dfrac{2kP}{{{x}^{3}}}-\dfrac{2k\left( 64P \right)}{{{\left( 25-x \right)}^{3}}}=0
Taking 2,k,P2,k,P common in both terms and cancelling them with zero, we get
1x364(25x)3=0\dfrac{1}{{{x}^{3}}}-\dfrac{64}{{{\left( 25-x \right)}^{3}}}=0
We shall now transpose one term to the right-hand side and simplify further.
1x3=64(25x)3\Rightarrow \dfrac{1}{{{x}^{3}}}=\dfrac{64}{{{\left( 25-x \right)}^{3}}}
(25x)3=64x3\Rightarrow {{\left( 25-x \right)}^{3}}=64{{x}^{3}}
We know that 64=4×4×464=4\times 4\times 4, it can also be written as 64=4364={{4}^{3}}. Thus, substituting this value of 64, we get
(25x)3=43.x3 (25x)3=(4x)3 \begin{aligned} & \Rightarrow {{\left( 25-x \right)}^{3}}={{4}^{3}}.{{x}^{3}} \\\ & \Rightarrow {{\left( 25-x \right)}^{3}}={{\left( 4x \right)}^{3}} \\\ \end{aligned}
Now, king cube roots on both sides, we get
(25x)33=(4x)33 25x=4x \begin{aligned} & \Rightarrow \sqrt[3]{{{\left( 25-x \right)}^{3}}}=\sqrt[3]{{{\left( 4x \right)}^{3}}} \\\ & \Rightarrow 25-x=4x \\\ \end{aligned}
Here, we have a linear equation in variable-x. Thus, transposing -x to the right-hand side, we get
25=4x+x\Rightarrow 25=4x+x
25=5x\Rightarrow 25=5x
Dividing both sides by 5, we get
5x5=255 x=5 \begin{aligned} & \Rightarrow \dfrac{5x}{5}=\dfrac{25}{5} \\\ & \Rightarrow x=5 \\\ \end{aligned}
Therefore, the electric field will be zero at a point between the dipoles whose distance from the dipole of moment PP is 5cm5cm.

Therefore, the correct option is (B) 5cm5cm.

Note:
One possible mistake we could have done was expanding the expression raised to the power of 3 using the mathematical properties. If we would have expanded the expression, (25x)3{{\left( 25-x \right)}^{3}}, then the equation would have become very complex consisting of 2-degree and 3-degree variables also which would have become very difficult to solve.