- 2074 Asoj · 8 marks
Derivatives at t=0+: 2 H, 100 V, 1 μF
Short answer
At t = 0+, i1 = i2 = 0; di1/dt = 50 A/s, di2/dt = 25 A/s; d²i1/dt² = −125 A/s², d²i2/dt² = −1.25×10⁶ A/s². All results from mesh equations with zero initial inductor current and capacitor voltage.
In the given network of the figure below, both the energy storing elements are initially relaxed i.e. no current is flowing through the inductor and no charge is accumulated across the capacitor before application of voltage. The switch K is closed at t = 0. Find the values of i1, i2, di1/dt, di2/dt, d²i1/dt², d²i2/dt² at t = 0⁺. [Figure: 100 V source; switch K and a 2 H inductor in the top wire of the left mesh (i1); a 10 Ω resistor in the middle vertical branch; a 10 Ω resistor in the top wire of the right mesh (i2); a 1 μF capacitor on the right]
Assumptions: both elements relaxed. Left mesh (current i₁): 100 V, switch K, L = 2 H, common resistor 10 Ω. Right mesh (current i₂): common 10 Ω, another 10 Ω, C = 1 μF.
Mesh equations
Mesh 1: 100 = 2 di₁/dt + 10(i₁ − i₂)
Mesh 2: 10(i₂ − i₁) + 10 i₂ + (1/C)∫i₂ dt = 0 → 20 i₂ − 10 i₁ + v_C = 0
At t = 0⁺ (i_L = 0, v_C = 0)
i₁(0⁺) = 0
20 i₂ − 0 + 0 = 0 → i₂(0⁺) = 0
First derivatives
Mesh 1: 100 = 2 i₁′ + 0 → i₁′(0⁺) = 50 A/s
Mesh 2 differentiated: 20 i₂′ − 10 i₁′ + i₂/C = 0
20 i₂′ = 10 × 50 → i₂′(0⁺) = 25 A/s
Second derivatives
Mesh 1 differentiated: 0 = 2 i₁″ + 10(i₁′ − i₂′)
i₁″ = −10(50 − 25)/2 = −125 A/s²
Mesh 2 differentiated twice: 20 i₂″ − 10 i₁″ + i₂′/C = 0
i₂″ = [10(−125) − 25/10⁻⁶]/20 = (−1250 − 2.5×10⁷)/20
= −1.25006×10⁶ A/s²
| Quantity | Value at 0⁺ |
|---|---|
| i₁ | 0 |
| i₂ | 0 |
| di₁/dt | 50 A/s |
| di₂/dt | 25 A/s |
| d²i₁/dt² | −125 A/s² |
| d²i₂/dt² | −1.25×10⁶ A/s² |
Answer: i₁ = i₂ = 0; di₁/dt = 50, di₂/dt = 25; d²i₁/dt² = −125, d²i₂/dt² = −1.25×10⁶ (SI units).
✓ Answer checked by Claude Opus 5.5 (high effort)
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