The Plasma Globe's Dancing Arc · AI Generator #GEN-4D75DF13

Physics · electromagnetism

Problem

In a plasma globe, high-frequency AC voltage creates dancing electric arcs between a central electrode and the glass sphere. Consider a simplified model where a sinusoidal voltage V(t)=V0sin⁡(ωt)V(t) = V_0 \sin(\omega t) with amplitude V0=15.0  kVV_0 = 15.0\;\text{kV} and frequency f=25.0  kHzf = 25.0\;\text{kHz} is applied between two spherical electrodes separated by distance d=8.00  cmd = 8.00\;\text{cm}. The space between electrodes is filled with neon gas at low pressure. When the instantaneous electric field magnitude exceeds the breakdown field Eb=1.20×105  V/mE_b = 1.20 \times 10^5\;\text{V/m}, a conducting plasma channel forms instantaneously, effectively short-circuiting the gap. The plasma channel persists until the current through it drops below the sustaining current Is=2.50  mAI_s = 2.50\;\text{mA}, at which point it extinguishes and the gap becomes insulating again. The circuit can be modeled as the voltage source in series with a resistor R=100  kΩR = 100\;\text{k}\Omega (representing the plasma channel resistance when conducting) and the electrode capacitance C=12.0  pFC = 12.0\;\text{pF}. (a) At what phase angle ϕ1\phi_1 (measured from t=0t = 0) does breakdown first occur in each half-cycle? (b) At what phase angle ϕ2\phi_2 does the plasma extinguish in each half-cycle? (c) What is the average power dissipated in the plasma during one complete cycle?

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