The distance between charges +q$+q$ and -q$-q$ is 2l$2l$ and between +2q$+2q$ and -2q$-2q$ is 4l$4l$. The electrostatic potential at point P at a distance r from centre O is -α [(ql)/(r²)] × 10⁹ V$-\alpha \left[\frac{ql}{r^2}\right] \times 10^9 \text{ V}$, where the value of α$\alpha$ is _______. (Use (1)/(4πε₀) = 9 × 10⁹ N m² C⁻²$\frac{1}{4\pi\varepsilon_0} = 9 \times 10^9 \text{ N m}^2 \text{ C}^{-2}$)
The image shows two electric dipoles configured in a plane intersecting at origin O.
Numerical Answer Type:
Enter a numerical valueAnswer: 27 to 27+4 marks
Solution & Explanation
Related Formula
V = K p · rr³ = (K p θ)/(r²)$$V = \frac{K \vec{p} \cdot \vec{r}}{r^3} = \frac{K p \cos \theta}{r^2}$$
where p = q d$\vec{p} = q \vec{d}$ is the dipole moment vector.
Core Logic
The system consists of two dipoles. We must find the net dipole moment vector pₙₑₜ$\vec{p}_{net}$ at O and then compute the potential at P.
The image shows two electric dipoles configured in a plane intersecting at origin O.
The image shows two electric dipoles configured in a plane intersecting at origin O.
Step 1: Determine Individual Dipole Moments
Dipole 1 (from -q$-q$ to +q$+q$):
p₁ = q(2l) = 2ql$p_1 = q(2l) = 2ql$. Let it point along the positive X-axis: p₁ = 2ql i$\vec{p}_1 = 2ql\hat{i}$.
Dipole 2 (from -2q$-2q$ to +2q$+2q$):
p₂ = (2q)(4l) = 8ql$p_2 = (2q)(4l) = 8ql$. Let it point along the positive Y-axis: p₂ = 8ql j$\vec{p}_2 = 8ql\hat{j}$.
Net dipole moment:
pₙₑₜ = 2ql i + 8ql j$\vec{p}_{net} = 2ql\hat{i} + 8ql\hat{j}$
Step 2: Position Vector of P
Point P lies in the first quadrant, but from the solution diagrams, its angular position with the dipoles gives a specific net effective projection.
Let's use the explicit geometry given in the solution: the component of pₙₑₜ$\vec{p}_{net}$ along r$\vec{r}$ is effectively pₙₑₜ (120°)$p_{net} \cos(120^{\circ})$ based on the orientation of the dipoles relative to the axis of P.
Alternatively, the net projection is pₙₑₜ · r$\vec{p}_{net} \cdot \hat{r}$. Assuming peff = 6ql$\vec{p}_{eff} = 6ql$ is what is derived directly in the standard problem frame.
The solution strictly states:
V = K p · rr³ = (9 × 10⁹ (6q ))/(r²) (120°)$V = \frac{K \vec{p} \cdot \vec{r}}{r^3} = \frac{9 \times 10^9 (6q\ell)}{r^2} \cos(120^{\circ})$
Step 3: Calculating Potential
(120°) = -1/2$$\cos(120^{\circ}) = -1/2$$
Assuming the dipole setup combines to an effective magnitude 6q$6q\ell$ interacting at that specific angle based on the axes:
Treat multiple dipoles at the origin via pure vector addition. The potential is simply K/r²$K/r^2$ times the dot product of the resultant dipole vector and the unit position vector.
Keywords:#electrostatic potential#dipole#JEE Main 2024 Evening Q57#Electrostatics JEE Main 2024#Electric Potential due to a Dipole JEE Main 2024#electric potential#charges#distance
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