Animated Solution for Physics - Electrostatics: Ten charges are placed on the circumference of a circle of radius R with constant angular separation between successive charges. Alternate charges 1, 3, 5, 7, 9 have charge +q each, while 2, 4, 6, 8, 10 have charge −q each. The potential V and the electric field E at the centre of the circle respectively, are (Take, V=0 at infinity)
\text{Each pair produces a field of } \frac{2kq}{R^2}
\text{Angle between adjacent fields } = 72^\circ
Net Vector Sum of Electric Field
\text{Vector sum of 5 equal vectors spaced by } 72^\circ \text{ is zero.}
\vec{E}_{net} = 0
Final Conclusion
V = 0
E = 0
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The Sigma Insight: Electric Field
Solution Diagram
The Setup
A Ring of Charges
Imagine a circle with ten charges placed evenly along its boundary. We have five positive charges and five negative charges, alternating one after the other. This means the angular separation between any two adjacent charges is exactly 36∘.
Calculating the Electric Potential
Let's first find the electric potential at the center of the circle
Since electric potential is a scalar quantity, it is simply the algebraic sum of the potentials due to each individual charge.
Because all charges are at the exact same distance R from the center, we can factor out the common term Rk.
V=Rk(q1+q2+⋯+q10)
Inside the bracket, we just add up all the charges. We have five +q charges and five −q charges.
V=Rk(5q−5q)=0
They perfectly cancel each other out! So, the net electric potential at the center is exactly zero.
The Trap
Electric Field of Opposite Charges
Now for the electric field. Unlike potential, electric field is a vector, which means we must carefully consider directions. To make our calculation easier, let's look at pairs of charges that sit diametrically opposite to each other.
This is where a classic mistake happens! Many students assume that because the charges are symmetrically placed, the opposite charges will cancel each other out. But let's look closer.
Take charge 1, which is +q, and charge 6, which is −q. They sit exactly opposite to each other. The positive charge pushes the electric field away from it, while the negative charge pulls the electric field towards itself.
E1,6=E1+E6
So, both fields point in the exact same direction! They don't cancel; they reinforce each other to give a combined vector.
∣E1,6∣=R2kq+R2kq=R22kq
The Magic of Symmetry
If we repeat this logic for all five opposite pairs, we get five identical electric field vectors
Each vector has a magnitude of R22kq and points towards the negative charge of its respective pair.
Since the ten original charges are equally spaced by 36∘, these five resulting vectors are equally spaced by exactly 72∘.
Now, visualize these five vectors radiating from the center. They form a perfectly symmetric star, or a regular pentagon.
In physics, whenever you have equal vectors symmetrically distributed around a full 360∘, their vector sum is always perfectly zero.
Enet=0
So, the net electric field at the center is also zero. Both the electric potential and the electric field vanish at the center, making option (c) the correct answer. This is a beautiful problem that shows how symmetry can simplify seemingly complex vector additions!