Q.The electrostatic force on a small sphere of charge 0.4μC due to another small sphere of charge −0.8μC in air is 0.2N.
Concept understanding — Coulomb Force Superposition
Coulomb Force Superposition – From Intuition to Precision
Imagine you're in a room with three friends. Each friend can push or pull you. If two friends push you from the same side, you feel a stronger push — the combined effect. If one pushes from the left and another from the right, you feel the net effect, which might be smaller or even zero if they push equally hard.
This is exactly how electric forces work. When multiple charged particles are present, each one exerts its own force on a given charge. The total force that charge feels is simply the vector sum of all the individual forces — as if each other charge were acting alone, completely ignoring the presence of the rest.
That's the core idea: forces add like arrows, not like numbers.
The Precise Statement
Fnet on q0=∑i=1nFi→0=4πε01∑i=1nri02q0qir^i0
Where:
- q0 is the charge you're calculating the force on
- qi are all other charges (excluding q0 itself)
- ri0 is the distance between qi and q0
- r^i0 is a unit vector pointing from qi to q0 (or away, depending on sign convention — be consistent)
The key point: Each pair of charges interacts independently. The presence of a third charge does not alter the force between the first two. This is what "superposition" means — the forces simply layer on top of each other.
Why This Matters (and a Common Trap)
Never add the magnitudes of forces directly unless all forces are along the same line and in the same direction. Force is a vector — direction matters.
If two forces point in opposite directions, they partially cancel. If they're at right angles, the net force is found using the Pythagorean theorem, not simple addition.
Example: Three charges on a line:
- q1=+2μC at x=0
- q2=−1μC at x=3cm
- q0=+1μC at x=1cm
Step 1: Force from q1 on q0 — both positive, so repulsive. q0 is pushed to the right.
Step 2: Force from q2 on q0 — opposite signs, so attractive. q0 is pulled to the right (toward q2).
Step 3: Both forces point right. Now you add magnitudes: Fnet=F1→0+F2→0.
If q2 were also positive, the force from q2 would push q0 left, and you'd subtract.
The Deeper Reason
Coulomb's law is a linear law — the force is proportional to each charge individually. If you double q1, the force from q1 doubles, but the force from q2 stays the same. This linearity is what makes superposition possible. It's not a coincidence — it's a fundamental property of electromagnetic interactions at the classical level.
Superposition works because electric forces obey a linear inverse-square law. If the force depended on products of three charges (like q0q1q2), superposition would fail. It doesn't — and that's why we can break down any multi-charge problem into a series of two-charge calculations.
How to Use It in Exams
- Draw all charges and label distances.
- For each other charge, sketch the direction of the force on your target charge (like charges repel, opposites attract).
- Write the magnitude of each force using Coulomb's law.
- Resolve into components if forces aren't along the same line.
- Add components separately: Fnet,x=∑Fi,x, same for y, z.
- Combine components to get the net force vector.
In symmetric arrangements (e.g., an equilateral triangle with equal charges), many components cancel. Always check for symmetry before diving into heavy algebra — it can save you minutes.
One Last Check
If you place a test charge q0 at a point and there are 10 other charges around it, you calculate 10 separate Coulomb forces and add them as vectors. That's it. No extra physics, no hidden interactions. The universe, at this level, is beautifully simple: each pair talks only to each other, and you just listen to all the conversations at once.
"Coulomb's law superposition principle examples" and "electrostatics class 12 physics important questions" are frequently searched, both grounded in the Electrostatics chapter of the NCERT/CBSE Class 12 Physics curriculum. Multi-charge force problems using superposition are a near-guaranteed topic in JEE Main and NEET.
Why this formula?
Coulomb Force Superposition — Why the Formula Holds
The principle of superposition for Coulomb forces states that the net electrostatic force on a given charge due to a collection of other charges is the vector sum of the individual forces from each charge, as if the others were absent.
The Key Formula
If we have a charge q0 at position r0, and N other point charges q1,q2,…,qN at positions r1,r2,…,rN, the net force on q0 is:
Fnet=4πε01∑i=1N∣r0−ri∣2q0qir^0i
where r^0i is the unit vector pointing from qi to q0.
Why This Works — The Physical Reasoning
1. Coulomb's Law is a Two-Body Interaction
Coulomb's law describes the force between exactly two point charges. It depends only on:
- The product of their charges (q0qi)
- The inverse square of the distance between them
- The direction along the line joining them
Crucially, the force between q0 and qi does not depend on the presence of any other charges qj.
2. Forces Add as Vectors (Newton's Third Law + Linearity)
Electrostatic forces are real physical forces — they obey Newton's laws. If multiple forces act on the same charge, the net effect is the vector sum of each individual force. This is a fundamental property of forces in classical mechanics.
3. The Electric Field is Linear
A deeper reason: the electric field E obeys superposition. Since F=q0E, and E from multiple sources adds linearly, the force automatically adds linearly.
The electric field at r0 due to qi is:
Ei(r0)=4πε01∣r0−ri∣2qir^0i
Then:
Fnet=q0∑iEi=∑iFi
The Crucial Assumption (Why It's Not Trivial)
Superposition holds because Maxwell's equations are linear in the electric field. If the equations were nonlinear (e.g., if the field depended on E2), then the force from two charges together would not be the sum of the individual forces.
In electrostatics, the electric field satisfies:
∇⋅E=ε0ρ,∇×E=0
Both equations are linear — if E1 and E2 are solutions, then E1+E2 is also a solution. This linearity is the mathematical reason superposition works.
Exam-Relevant Takeaway
| Concept | Why It Holds |
|---|---|
| Superposition of forces | Coulomb force is a two-body interaction; forces add as vectors |
| Superposition of fields | Maxwell's equations are linear in E |
| Net force formula | Fnet=∑Fi — vector sum of individual Coulomb forces |
Never forget: The unit vector r^0i points from the source charge to the test charge — this determines the correct direction of each term.
Quick Example (To Cement the "Why")
Suppose q0=+1μC at the origin, q1=+2μC at (1,0), q2=−2μC at (0,1).
- Force from q1: repulsive, along +x direction
- Force from q2: attractive, along +y direction
The net force is not just the sum of magnitudes — it's the vector sum:
Fnet=F1x^+F2y^
This works because the two forces are independent — q1 doesn't "know" about q2, and vice versa. The superposition principle is simply the statement that this independence holds.
Concept: Inverse Square Law Comparison — Coulomb’s law gives the force between two point charges as F=kr2∣q1q2∣, where k=9×109 N m2/C2 in air.
(a)
F=0.2 N, q1=0.4×10−6 C, q2=−0.8×10−6 C.
Using r2=kF∣q1q2∣:
r2=9×109×0.2(0.4×10−6)(0.8×10−6)=9×109×0.23.2×10−13=9×109×1.6×10−12=1.44×10−2.
So r=1.44×10−2=0.12 m.
(b)
By Newton’s third law, the force on the second sphere due to the first is equal in magnitude and opposite in direction: 0.2 N, attractive.
The distance is 0.12 m and the force on the second sphere is 0.2 N (attractive).
Using Coulomb’s law, the distance is found from F=kr2∣q1q2∣, and by Newton’s third law the force on the second sphere is equal in magnitude and opposite in direction to the force on the first. The distance is 0.12m and the force on the second sphere is 0.2N (attractive).
The problem is a direct application of Coulomb’s law for the electrostatic force between two point charges. The key idea is that the force magnitude depends only on the product of the charges and the square of the distance between them — the sign of the charges tells us the direction (attractive or repulsive), but the magnitude is given by the absolute values.
Because the two charges are opposite in sign, the force is attractive. The problem gives the force on the first sphere, and part (b) simply asks for the force on the second sphere — which, by Newton’s third law, must be equal in magnitude and opposite in direction.
Let’s work through it step by step.
- Write down Coulomb’s law in magnitude form The electrostatic force between two point charges q1 and q2 separated by a distance r in vacuum (or air, which has nearly the same permittivity) is:
F=kr2∣q1q2∣
where k=4πε01=9×109N m2/C2.
-
Identify the given quantities
- q1=0.4μC=0.4×10−6C=4×10−7C
- q2=−0.8μC=−0.8×10−6C=−8×10−7C
- F=0.2N (magnitude of force on q1 due to q2)
The product ∣q1q2∣=(4×10−7)(8×10−7)=32×10−14=3.2×10−13C2.
-
Solve for the distance r
Rearranging Coulomb’s law:
r2=kF∣q1q2∣
Substitute the values:
r2=(9×109)×0.23.2×10−13
First compute the fraction:
0.23.2×10−13=1.6×10−12
Then:
r2=9×109×1.6×10−12=14.4×10−3=1.44×10−2
Taking the square root:
r=1.44×10−2=1.44×10−1=1.2×10−1=0.12m
So the distance between the spheres is 0.12 metres (or 12 cm).
Notice that we used the magnitude of the charges. The negative sign on q2 only tells us the force is attractive — it doesn’t affect the distance calculation.
- Answer part (b) using Newton’s third law The force on the second sphere due to the first is equal in magnitude and opposite in direction to the force on the first sphere due to the second. Magnitude: 0.2N Direction: Since the charges are opposite, the force is attractive — so the second sphere is pulled toward the first. Thus the force on the second sphere is 0.2N (attractive).
A common mistake is to think the force on the second sphere is different because the charges have different magnitudes. But Coulomb’s law gives the force on each charge as the same magnitude — the product ∣q1q2∣ is symmetric. Newton’s third law guarantees equality.
The distance between the spheres is 0.12m and the force on the second sphere due to the first is 0.2N (attractive).
Method: Coulomb’s Law (Inverse Square Law)
We use Coulomb’s Law for electrostatic force between two point charges:
F=kr2∣q1q2∣
where:
- F = magnitude of electrostatic force (N)
- k=9×109 N m2/C2 (Coulomb’s constant for air)
- q1,q2 = charges (C)
- r = distance between charges (m)
Step 1: Identify given values
- q1=0.4 μC=0.4×10−6 C
- q2=−0.8 μC=−0.8×10−6 C
- F=0.2 N
Note: Force magnitude uses absolute values of charges. The negative sign on q2 only tells us the force is attractive.
Step 2: Solve for distance r (part a)
From Coulomb’s Law:
r2=kF∣q1q2∣
Substitute values:
r2=(9×109)×0.2(0.4×10−6)×(0.8×10−6)
Simplify numerator:
0.4×0.8=0.32
10−6×10−6=10−12
So ∣q1q2∣=0.32×10−12 C2
Now:
r2=9×109×0.20.32×10−12
r2=9×109×1.6×10−12
r2=14.4×10−3=0.0144
Take square root:
r=0.0144=0.12 m
Answer (a): 0.12 m (or 12 cm)
Step 3: Force on second sphere (part b)
By Newton’s Third Law, the force on the second sphere due to the first is equal in magnitude and opposite in direction to the force on the first sphere due to the second.
- Magnitude: 0.2 N
- Direction: attractive (toward the first sphere)
Answer (b): 0.2 N (attractive, toward the first sphere)
Key Concept Check
- The inverse square law means: if distance doubles, force becomes 41.
- Force magnitude depends only on product of charges and distance — not on which charge we consider.
- The negative sign on q2 indicates opposite charges → attraction.
Common Mistakes & How to Avoid Them
Mistake 1: Forgetting to convert microcoulombs (μC) to coulombs (C)
The error: Students plug 0.4 and 0.8 directly into Coulomb's law, forgetting the μ (micro) means 10−6.
Why it happens: The problem gives charges in μC, but Coulomb's law requires SI units (C). The conversion factor is easy to overlook under time pressure.
How to avoid: Always write the conversion explicitly before substituting:
q1=0.4μC=0.4×10−6C=4×10−7C
q2=−0.8μC=−0.8×10−6C=−8×10−7C
Pro tip: Circle or underline the unit in the question. If it's not in base SI, convert first — every time.
Mistake 2: Using the wrong value of k or forgetting it entirely
The error: Some students use k=9×109 but forget the units, or mistakenly use k=1 (thinking "in air" means vacuum permittivity is irrelevant).
Why it happens: The constant k=4πε01=9×109N m2/C2 is often memorised without understanding its role.
How to avoid: Write Coulomb's law fully:
F=kr2∣q1q2∣
Then substitute k=9×109 with its units. This helps you check that your final distance comes out in metres.
Mistake 3: Ignoring the sign of the charges when calculating force magnitude
The error: Students include the negative sign of q2=−0.8μC in the product q1q2, getting a negative value, then panic or get confused.
Why it happens: Coulomb's law for magnitude uses absolute values. The sign only tells you attraction (opposite signs) or repulsion (same sign).
How to avoid: For part (a), use only magnitudes:
F=kr2∣q1∣⋅∣q2∣
So ∣q1∣=4×10−7C and ∣q2∣=8×10−7C. The force 0.2N is already positive — it's the magnitude.
Key insight: The sign of the force (attractive/repulsive) is a direction concept, not a magnitude concept. Part (a) only asks for distance, so signs are irrelevant.
Mistake 4: Solving for r incorrectly (algebra errors)
The error: After substituting, students make mistakes like:
- Forgetting to take the square root
- Inverting the fraction
- Misplacing powers of 10
How to avoid: Solve step-by-step:
- Write: r2=kF∣q1q2∣
- Substitute carefully:
r2=(9×109)×0.2(4×10−7)(8×10−7)
- Simplify powers of 10 separately:
=9×109×0.232×10−14
=9×109×160×10−14
=1440×10−5=1.44×10−2
- Take square root: r=1.44×10−2=1.2×10−1=0.12m
Check: 0.12m=12cm — a reasonable distance for these charges and force.
Mistake 5: Answering part (b) with a different value than 0.2N
The error: Students recalculate the force using the distance found in (a), but make an arithmetic slip, or think the force on the second sphere is somehow different.
Why it happens: They forget Newton's Third Law — electrostatic forces are action-reaction pairs.
How to avoid: Remember: The force on sphere 2 due to sphere 1 is equal in magnitude and opposite in direction to the force on sphere 1 due to sphere 2.
So part (b) answer is simply:
0.2N
Direction: Attractive (since charges are opposite), but the question only asks for force magnitude.
Mistake 6: Giving the distance in wrong units
The error: After calculating r=0.12m, students write the answer as 0.12 without units, or convert unnecessarily to cm without being asked.
How to avoid: Always state the unit. The standard SI unit for distance is metres. Write:
0.12m
If you prefer, you can add (12cm) in brackets, but the primary answer should be in metres unless the question specifies otherwise.
Quick Summary Checklist
| Mistake | How to Avoid |
|---|---|
| Forgetting μ conversion | Convert to C before plugging in |
| Wrong k value | Write k=9×109 with units |
| Including sign in magnitude | Use $ |
| Algebra errors in r | Solve stepwise, check powers of 10 |
| Wrong force in (b) | Newton's Third Law: same magnitude |
| Missing units | Always write the unit with the number |
- GUJCET 2026Set x1 markMCQQ.Two infinitely long thin straight parallel wires are kept a perpendicular distance 2R having uniform linear charge densities +λ and −λ respectively. The magnitude of electric field at a mid point between two wires will be ______. (A) πε0Rλ (B) 2πε0Rλ (C) πε0R2λ (D) 4πε0Rλ
›Reveal solutionSolution
Fields of the +λ and −λ wires add at the midpoint: E=λ/πε0R.
Field of an infinite line at distance r: E=2πε0rλ. The midpoint is at r=R from each wire.
At the midpoint the field of the positive wire points away from it, and the field of the negative wire points toward it — both in the same direction, so they add:
E=2×2πε0Rλ=πε0Rλ.
✓Final answerOption (A) πε0Rλ
ANSWER: (A)
- GSEB Higher Secondary Certificate (HSC) Examination 2025Set ANNUAL1 markMCQQ.The electrostatic force on a small sphere of charge 0.4μC due to another small sphere of charge -0.8μC in air is 0.2 N. What is the distance between the two spheres?(a) 12 m(b) 0.12 m(c) 1.2 m(d) 0.012 m
›Reveal solutionSolution
Coulomb's law relates the electrostatic force between two point charges to their separation: F = kq1q2/r².
Given q1 = 0.4 μC = 4 × 10⁻⁷ C, q2 = 0.8 μC = 8 × 10⁻⁷ C (magnitudes), F = 0.2 N, k = 9 × 10⁹ N m²/C².
r² = kq1q2/F = (9 × 10⁹)(4 × 10⁻⁷)(8 × 10⁻⁷)/0.2 = (9 × 10⁹)(3.2 × 10⁻¹³)/0.2 = 2.88 × 10⁻³/0.2 = 1.44 × 10⁻².
r = √(1.44 × 10⁻²) = 0.12 m.
✓Final answer(b) 0.12 m.
- GSEB Higher Secondary Certificate (HSC) Examination 2024Set ANNUAL1 markMCQQ.Two identical conducting spheres A and B having charges +q and -q are kept at 'd' distance apart experience coulombian force F between them. If 50% of charge is transferred from sphere B to A then the new coulombian force between them is ___.(a) F(b) F/2(c) F/4(d) 2F/3
›Reveal solutionSolution
Coulomb's force is proportional to the product of the two charges; recompute the new charges after the transfer and rescale F accordingly.
Original force: F = k q (q)/d² (magnitude, using |+q| and |−q| = q each).
50% of sphere B's charge (−q) is transferred to A: transferred charge = −q/2.
New charge on B: −q − (−q/2) = −q/2.
New charge on A: q + (−q/2) = q/2.
New force F' = k |q/2| |q/2| / d² = k q²/(4d²) = F/4.
✓Final answer(c) F/4.
- GSEB Higher Secondary Certificate (HSC) Examination 2024Set ANNUAL1 markMCQQ.As shown in figure charges +q each are placed at the four vertices of a square. Then the coulombian force acting on charge placed at vertex D is ___.(a) (√2 + 1/2) kq^2/a^2(b) (√2 - 1/2) kq^2/a^2(c) √2 kq^2/a^2(d) kq^2/2a^2
›Reveal solutionSolution
The net force on a corner charge in a square of equal charges is the vector sum of two equal edge forces (perpendicular to each other) and one diagonal force.
Charge at D experiences:
- Force from A (distance a, along DA): magnitude kq²/a²
- Force from C (distance a, along DC): magnitude kq²/a², perpendicular to the A-force
- Force from B (diagonal, distance a√2): magnitude kq²/(a√2)² = kq²/(2a²), directed along the diagonal DB
The two equal perpendicular edge forces combine (Pythagoras) to give a resultant of magnitude √2 × kq²/a², directed exactly along the diagonal — the same direction as the diagonal force from B.
Total force = √2 kq²/a² + kq²/(2a²) = (√2 + 1/2) kq²/a².
✓Final answer(a) (√2 + 1/2) kq²/a².
- GSEB Higher Secondary Certificate (HSC) Examination 2023Set ANNUAL1 markMCQQ.The Coulombian repulsive force between two alpha particles kept at a distance of 3 cm in air is ___ N.(a) 1.024 x 10^-27(b) 1.024 x 10^-25(c) 1.024 x 10^-24(d) 1.024 x 10^-23
›Reveal solutionSolution
Alpha charge = 2e = 3.2x10^-19 C; Coulomb's law with r = 0.03 m gives F = 1.024 x 10^-24 N.
Each alpha particle has charge q = 2e = 3.2 x 10^-19 C. Separation r = 3 cm = 0.03 m.
Coulomb force: F = k q^2 / r^2 = (9 x 10^9)(3.2 x 10^-19)^2/(0.03)^2.
(3.2 x 10^-19)^2 = 1.024 x 10^-37; (0.03)^2 = 9 x 10^-4.
F = (9 x 10^9)(1.024 x 10^-37)/(9 x 10^-4) = (1.024 x 10^-37)(10^13) = 1.024 x 10^-24 N.
✓Final answer(c) 1.024 x 10^-24 N.
- GUJCET 2021Set 151 markMCQQ.Two large, thin metal plates are parallel and close to each other. On their inner faces, the plates have surface charge densities of same signs and of magnitude 17.7×10−22 C/m2. What is E in the outer region of the second plate? (A) 4×10−10 NC−1 (B) 2×10−10 NC−1 (C) 1×10−10 NC−1 (D) Zero
›Reveal solutionSolution
Same-sign charged plates give E=σ/ε0 in the outer region (fields add).
Concept: Each sheet produces 2ε0σ. In the region outside the second plate both fields point the same way and add:
E=2ε0σ+2ε0σ=ε0σ=8.85×10−1217.7×10−22≈2×10−10 N C−1.
✓Final answer(B) 2×10−10 NC−1
ANSWER: (B)
- GUJCET 2020Set 071 markMCQQ.Two point electric charges +10−8 C and −10−8 C are placed 0.1 m apart. Find the magnitude of Total Electric Field at the center of the line joining the two charges. (A) Zero (B) 3.6×104NC−1 (C) 7.2×104NC−1 (D) 12.96×104NC−1
›Reveal solutionSolution
At the centre of a dipole-like pair, both fields point the same way and add.
Concept — superposition of fields. At the midpoint, the field of +q points away from it and the field of −q points toward it — both in the same direction, so they add.
Steps.
- Distance from each charge: r=0.05 m.
- Eone=r2kq=(0.05)29×109×10−8=0.002590=3.6×104 NC−1.
- Total: E=2Eone=7.2×104 NC−1.
✓Final answerOption (C) 7.2×104NC−1
ANSWER: (C)
- GUJCET 2019Set 131 markMCQQ.When two sppheres having 4Q and −2Q charge are placed at a certain distance, the force acting between them is F. Now they are connected by a conducting wire and again separated from each other. Now they are kept at a distance half of the previous one. The force acting between them is .......... (A) 8F (B) 2F (C) 4F (D) F
›Reveal solutionSolution
Charges redistribute to Q each, and at half the separation the force is F/2.
Concept: When two conductors are joined by a wire the total charge shares equally. Coulomb force F=r2kq1q2.
Steps:
- Initial magnitude: F=d2k(4Q)(2Q)=d28kQ2.
- After connection each sphere has 24Q+(−2Q)=Q.
- New separation d/2: F′=(d/2)2kQ⋅Q=d24kQ2.
- Ratio: FF′=84=21, so F′=2F.
✓Final answerOption (B) — F/2
ANSWER: (B)
- GUJCET 2019Set 131 markMCQQ.Charge of 1μC each is placed on the five corners of a ragular hexagon of side 1m. The electric field at its centre is ...........N/C. (A) 10−6K (B) 56×10−6K (C) 5×10−6K (D) 65×10−6K
›Reveal solutionSolution
Missing one of six symmetric charges leaves a net field equal to a single charge's field, 10−6K.
Concept: By symmetry, six equal charges at the vertices of a regular hexagon produce zero field at the centre (each field cancels its diametric opposite). Removing one charge is equivalent to superposing the full symmetric set (field 0) with a single negative-of-that charge at that vertex, leaving the field of one charge.
Steps:
- For a regular hexagon, centre-to-vertex distance = side = 1 m.
- Field of one charge: E=r2kQ=12K(10−6)=10−6K N/C.
✓Final answerOption (A) — 10−6K
ANSWER: (A)
- GUJCET 2015Set C1 markMCQQ.A point charge q is situated at a distance r on axis from one end of a thin conducting rod of length L having a charge Q [Uniformly distributed along its length]. The magnitude of electric force between the two is _____. (A) r2KQq (B) r(r+L)2KQ (C) r(r−L)KQq (D) r(r+L)KQq
›Reveal solutionSolution
[!TLDR] Integrating the point-charge force over the uniformly charged rod gives F=r(r+L)KQq.
Concept
A charge distributed along a line is handled by integration: split it into elements dq, write the Coulomb force dF=x2Kqdq from each element at distance x, and integrate. Here all forces are collinear (rod on the axis), so they add as scalars.
Solution
Linear charge density λ=LQ, so dq=LQdx. The near end of the rod is at distance r, the far end at r+L.
F=∫rr+Lx2Kq⋅LQdx=LKqQ[−x1]rr+L=LKqQ(r1−r+L1).
=LKqQ⋅r(r+L)(r+L)−r=LKqQ⋅r(r+L)L=r(r+L)KqQ.
[!ANSWER] (D) r(r+L)KQq
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