The three charged particles in the figure below are at the vertices of an isosceles -[Free] B56

The three charged particles in the figure below are at the vertices of an isosceles triangle (where d=3.00 cmd = 3.00 \, \text{cm}d=3.00cm). Taking q=8.20 μCq = 8.20 \, \mu\text{C}q=8.20μC, calculate the electric potential at point A, the midpoint of the base.

The three charged particles in the figure below are at the vertices of an isosceles -[Free] B56
Electric Potential at Midpoint of Base — Detailed Calculation

🔷 Electric Potential at the Midpoint of the Base

We calculate the electric potential at point A, the midpoint of the base of an isosceles triangle formed by three charges:

  • One positive charge at the top vertex
  • Two negative charges at the bottom corners
  • Distance between the midpoint and each base corner: d = 3.00 cm = 0.0300 m
  • Charge magnitude: q = 8.20 μC = 8.20 × 10⁻⁶ C

🌟 Step 1 — Concept

The electric potential at a point is the scalar sum of the potentials from all point charges:

V = k · q / r

where:

  • k = 8.99 × 10⁹ Nm²/C² (Coulomb constant)
  • q = charge
  • r = distance from charge to the point

🌟 Step 2 — Contributions from Each Charge

🔷 Left Corner Charge (−q)

Located at a distance d from A:

V₁ = k × (−q) / d

Substitute:

V₁ = 8.99×10⁹ × (−8.20×10⁻⁶) / 0.0300 ≈ −2.4573×10⁶ V

🔷 Right Corner Charge (−q)

Symmetric to the left corner:

V₂ = V₁ ≈ −2.4573×10⁶ V

🔷 Top Vertex Charge (+q)

This charge is at a distance 2d = 0.0600 m from A:

V₃ = k × q / (2d)

Substitute:

V₃ = 8.99×10⁹ × (8.20×10⁻⁶) / 0.0600 ≈ 1.2286×10⁶ V

🌟 Step 3 — Total Electric Potential at A

Sum of all three contributions:

V_A = V₁ + V₂ + V₃

Compute:

V_A = (−2.4573×10⁶) + (−2.4573×10⁶) + (1.2286×10⁶)
V_A ≈ −3.6860×10⁶ V

✨ Final Answer

🔷 The electric potential at point A is approximately: −3.686 × 10⁶ V

This negative result shows that the two negative charges at the base dominate the electric potential at the midpoint.

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