Pattern of Power Radiated | Santa Fe College - Edubirdie

University:
Santa Fe College
Course:
ETS 2527C | Electromechanical Components and Mechanisms
Academic year:

2024
Views:

371

Pages:

5
Author:

Jabin F.

# Pattern of power radiated: Donut Shape If a charge particle S.H.M in Z-axis: Maximum power along X-Y plane. (because θ = 90°) No power along z-axis. (θ = 0°) Equations: Ē² - c²𝐵² = 0 Ē = Ē₀ * exp(i(ωt - 𝑘 ∙ 𝑟)) 𝐵 = (1/c) * (𝑘̂ × Ē) 𝐸(𝑟,𝑡) + 𝐵(𝑟,𝑡) = 0 𝑆 → 0, so 𝐸₀ = 0 𝜆₀ = λ / γ 𝜆 = λ₀γ 𝐸₂ = (q₂ / 4πr²ε₀) * (1 - (v²/c²)) * sinθ * (î - (v/c)cosθ ĵ) 𝐵₂ = (1/c) * (𝑣 × 𝐸₂) Equations: 𝐸₂ = (q₂ / 4πε₀r²) * (1 - (v²/c²)) * sinθ * (î - (v/c)cosθ ĵ) 𝐵₂ = (μ₀q₂v / 4πr²) * sinθ * k̂ 𝐹_net = q₂(Ē₂ + (v × 𝐵₂)) 𝐹_net = (q₂² / 4πε₀r²) * (1 - (v²/c²)) * sinθ * k̂

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