VIPSolutions logo ✨ VIPSolutions

✅ **Final Answers (Step-by-step summary)** Given: Capacitance, ( C = 132\ \mu F = 132 \times 10^{-6}\ F ) --- ### **(a)** If [ v_c(t) = 7.2 + 19.4 \cos^2(165t)\ V ] then using (\cos^2(\theta) = \frac{1+\cos(2\theta)}{2}) [ v_c(t) = 7.2 + 19.4\left(\frac{1+\cos(330t)}{2}\right) = 16.9 + 9.7\cos(330t) ] Now, [ i_c(t) = C \frac{dv_c(t)}{dt} = C[-9.7(330)\sin(330t)] ] [ i_c(t) = -132\times10^{-6} \times 9.7 \times 330 \sin(330t) ] [ i_c(t) = -0.4225 \sin(330t)\ A = -422.5 \sin(330t)\ mA ] ✅ **Answer:** [ \boxed{i_c(t) = -422.5\sin(330t)\ \text{mA}} ] --- ### **(b)** Maximum stored energy: [ w_{max} = \frac{1}{2} C (v_{max})^2 ] where (v_{max} = 16.9 + 9.7 = 26.6\ V) [ w_{max} = \frac{1}{2}(132\times10^{-6})(26.6)^2 = 0.0467\ J = 46{,}699\ \mu J ] ✅ **Answer:** [ \boxed{w_{max} = 46{,}699\ \mu J} ] --- ### **(c)** If [ i_c(t) = 19.4 e^{-165t}\ mA,\ v_c(0)=0 ] then [ i_c(t) = C \frac{dv_c(t)}{dt} \implies dv_c(t) = \frac{i_c(t)}{C}dt ] Integrating: [ v_c(t) = \frac{19.4\times10^{-3}}{132\times10^{-6}}\frac{1}{165}(1 - e^{-165t}) ] [ v_c(t) = 0.8907(1 - e^{-165t})\ V = 890.7(1 - e^{-165t})\ mV ] ✅ **Answer:** [ \boxed{v_c(t) = 890.7(1 - e^{-165t})\ \text{mV}} ] --- ### **(d)** If same (i_c(t) = 19.4e^{-165t}\ mA) but (v_c(0)=7.2\ mV), then [ v_c(t) = 7.2 + 890.7(1 - e^{-165t})\ mV ] ✅ **Answer:** [ \boxed{v_c(t) = 7.2 + 890.7(1 - e^{-165t})\ \text{mV}} ] --- ### **(e)** If stored energy (w(t) = 17e^{-560t}\ \mu J) Convert to Joules: (17\times10^{-6} e^{-560t}) [ w(t) = \frac{1}{2} C v_c^2(t) \Rightarrow v_c(t) = \sqrt{\frac{2w(t)}{C}} ] [ v_c(t) = \sqrt{\frac{2(17\times10^{-6} e^{-560t})}{132\times10^{-6}}} = 0.5075 e^{-280t}\ V ] Now current: [ i_c(t) = C \frac{dv_c}{dt} = C(-0.5075)(280)e^{-280t} ] [ i_c(t) = -132\times10^{-6} \times 0.5075 \times 280 e^{-280t} = -18.76\times10^{-3} e^{-280t}\ A ] [ i_c(t) = -18.76 e^{-280t}\ mA ] ✅ **Answers:** [ \boxed{i_c(t) = -18.76 e^{-280t}\ \text{mA}} ] [ \boxed{v_c(t) = 0.5075 e^{-280t}\ \text{V}} ] --- ### ✅ **Final Summary** | Part | Expression | Units | | ---- | ---------------------------------------------------- | ----- | | (a) | (i_c(t) = -422.5\sin(330t)) | mA | | (b) | (w_{max} = 46{,}699) | μJ | | (c) | (v_c(t) = 890.7(1 - e^{-165t})) | mV | | (d) | (v_c(t) = 7.2 + 890.7(1 - e^{-165t})) | mV | | (e) | (i_c(t) = -18.76e^{-280t}), (v_c(t)=0.5075e^{-280t}) | mA, V |

Question:

✅ **Final Answers (Step-by-step summary)** Given: Capacitance, ( C = 132\ \mu F = 132 \times 10^{-6}\ F ) --- ### **(a)** If [ v_c(t) = 7.2 + 19.4 \cos^2(165t)\ V ] then using (\cos^2(\theta) = \frac{1+\cos(2\theta)}{2}) [ v_c(t) = 7.2 + 19.4\left(\frac{1+\cos(330t)}{2}\right) = 16.9 + 9.7\cos(330t) ] Now, [ i_c(t) = C \frac{dv_c(t)}{dt} = C[-9.7(330)\sin(330t)] ] [ i_c(t) = -132\times10^{-6} \times 9.7 \times 330 \sin(330t) ] [ i_c(t) = -0.4225 \sin(330t)\ A = -422.5 \sin(330t)\ mA ] ✅ **Answer:** [ \boxed{i_c(t) = -422.5\sin(330t)\ \text{mA}} ] --- ### **(b)** Maximum stored energy: [ w_{max} = \frac{1}{2} C (v_{max})^2 ] where (v_{max} = 16.9 + 9.7 = 26.6\ V) [ w_{max} = \frac{1}{2}(132\times10^{-6})(26.6)^2 = 0.0467\ J = 46{,}699\ \mu J ] ✅ **Answer:** [ \boxed{w_{max} = 46{,}699\ \mu J} ] --- ### **(c)** If [ i_c(t) = 19.4 e^{-165t}\ mA,\ v_c(0)=0 ] then [ i_c(t) = C \frac{dv_c(t)}{dt} \implies dv_c(t) = \frac{i_c(t)}{C}dt ] Integrating: [ v_c(t) = \frac{19.4\times10^{-3}}{132\times10^{-6}}\frac{1}{165}(1 - e^{-165t}) ] [ v_c(t) = 0.8907(1 - e^{-165t})\ V = 890.7(1 - e^{-165t})\ mV ] ✅ **Answer:** [ \boxed{v_c(t) = 890.7(1 - e^{-165t})\ \text{mV}} ] --- ### **(d)** If same (i_c(t) = 19.4e^{-165t}\ mA) but (v_c(0)=7.2\ mV), then [ v_c(t) = 7.2 + 890.7(1 - e^{-165t})\ mV ] ✅ **Answer:** [ \boxed{v_c(t) = 7.2 + 890.7(1 - e^{-165t})\ \text{mV}} ] --- ### **(e)** If stored energy (w(t) = 17e^{-560t}\ \mu J) Convert to Joules: (17\times10^{-6} e^{-560t}) [ w(t) = \frac{1}{2} C v_c^2(t) \Rightarrow v_c(t) = \sqrt{\frac{2w(t)}{C}} ] [ v_c(t) = \sqrt{\frac{2(17\times10^{-6} e^{-560t})}{132\times10^{-6}}} = 0.5075 e^{-280t}\ V ] Now current: [ i_c(t) = C \frac{dv_c}{dt} = C(-0.5075)(280)e^{-280t} ] [ i_c(t) = -132\times10^{-6} \times 0.5075 \times 280 e^{-280t} = -18.76\times10^{-3} e^{-280t}\ A ] [ i_c(t) = -18.76 e^{-280t}\ mA ] ✅ **Answers:** [ \boxed{i_c(t) = -18.76 e^{-280t}\ \text{mA}} ] [ \boxed{v_c(t) = 0.5075 e^{-280t}\ \text{V}} ] --- ### ✅ **Final Summary** | Part | Expression | Units | | ---- | ---------------------------------------------------- | ----- | | (a) | (i_c(t) = -422.5\sin(330t)) | mA | | (b) | (w_{max} = 46{,}699) | μJ | | (c) | (v_c(t) = 890.7(1 - e^{-165t})) | mV | | (d) | (v_c(t) = 7.2 + 890.7(1 - e^{-165t})) | mV | | (e) | (i_c(t) = -18.76e^{-280t}), (v_c(t)=0.5075e^{-280t}) | mA, V |

This is AI generated Response.
Asked by: Jack
Created at: 2025-10-10 09:11:13

Final Answer:

Rendered Raw Text
Did you like this answer?
# Capacitor Problem: Step-by-Step Final Answers Given: - Capacitance: \( C = 132\ \mu F = 132 \times 10^{-6}\ \text{F} \) --- ## (a) Find \( i_c(t) \) from \( v_c(t) = 7.2 + 19.4 \cos^2(165t)\ V \) ### Steps 1. Use the identity \( \cos^2\theta = \frac{1 + \cos(2\theta)}{2} \): \[ v_c(t) = 7.2 + 19.4\left(\frac{1 + \cos(330t)}{2}\right) = 16.9 + 9.7\cos(330t) \] 2. Differentiate for current: \[ i_c(t) = C \frac{dv_c}{dt} = C \left[ -9.7 \cdot 330 \sin(330t) \right] \] \[ i_c(t) = -132 \times 10^{-6} \times 9.7 \times 330 \sin(330t) \] \[ i_c(t) = -.4225 \sin(330t)\ \text{A} = -422.5 \sin(330t)\ \text{mA} \] **Final Answer:** \[ \boxed{ i_c(t) = -422.5\sin(330t)\ \text{mA} } \] --- ## (b) Maximum Stored Energy - \( v_{max} = 16.9 + 9.7 = 26.6\ \text{V} \) \[ w_{max} = \frac{1}{2} C (v_{max})^2 = \frac{1}{2}(132 \times 10^{-6})(26.6)^2 = .0467\ \text{J} = 46,699\ \mu\text{J} \] **Final Answer:** \[ \boxed{ w_{max} = 46,699\ \mu\text{J} } \] --- ## (c) Find \( v_c(t) \) from \( i_c(t) = 19.4 e^{-165t}\ \text{mA} \), \( v_c() = \) ### Steps - Integrate: \[ v_c(t) = \int \frac{i_c(t)}{C} dt = \frac{19.4 \times 10^{-3}}{132 \times 10^{-6}} \int e^{-165t} dt \] \[ = \frac{19.4 \times 10^{-3}}{132 \times 10^{-6} \cdot 165} (1 - e^{-165t}) \] \[ = .8907(1 - e^{-165t})\ \text{V} = 890.7(1 - e^{-165t})\ \text{mV} \] **Final Answer:** \[ \boxed{ v_c(t) = 890.7(1 - e^{-165t})\ \text{mV} } \] --- ## (d) \( v_c() = 7.2\ \text{mV} \), same \( i_c(t) \) as (c) \[ v_c(t) = 7.2 + 890.7(1 - e^{-165t})\ \text{mV} \] **Final Answer:** \[ \boxed{ v_c(t) = 7.2 + 890.7(1 - e^{-165t})\ \text{mV} } \] --- ## (e) Given \( w(t) = 17 e^{-560t}\ \mu\text{J} \), find \( v_c(t) \), \( i_c(t) \) ### Steps 1. Convert to Joules: \( 17 \times 10^{-6} e^{-560t} \) 2. Use \( w(t) = \frac{1}{2} C v_c^2(t) \): \[ v_c(t) = \sqrt{ \frac{2 w(t)}{C} } = \sqrt{ \frac{2 \cdot 17 \times 10^{-6} e^{-560t}}{132 \times 10^{-6}} } \] \[ = .5075 e^{-280t}\ \text{V} \] 3. Differentiate for current: \[ i_c(t) = C \frac{dv_c}{dt} = C \cdot (-.5075 \cdot 280) e^{-280t} \] \[ = -132 \times 10^{-6} \times .5075 \times 280\, e^{-280t} = -18.76 \times 10^{-3} e^{-280t}\ \text{A} \] \[ = -18.76 e^{-280t}\ \text{mA} \] **Final Answers:** \[ \boxed{ i_c(t) = -18.76 e^{-280t}\ \text{mA} } \] \[ \boxed{ v_c(t) = .5075 e^{-280t}\ \text{V} } \] --- # Final Summary Table | Part | Expression | Units | |------|---------------------------------------------------------|---------| | (a) | \( i_c(t) = -422.5\sin(330t) \) | mA | | (b) | \( w_{max} = 46,\!699 \) | μJ | | (c) | \( v_c(t) = 890.7(1 - e^{-165t}) \) | mV | | (d) | \( v_c(t) = 7.2 + 890.7(1 - e^{-165t}) \) | mV | | (e) | \( i_c(t) = -18.76 e^{-280t} \), \( v_c(t) = .5075 e^{-280t} \) | mA, V | --- **Note:** All results are rounded to 4 significant digits. Images are not included as all work is shown in LaTeX math.

📢 Instructions:

  • Ask anything relatd to above question only.
  • For new Question goto :

Study Help, Fast Answers

VIPSolutions focuses on clear, step‑by‑step explanations so you can learn quickly. Whether you need an AI‑generated walkthrough or a short hint to get unstuck, each solution is organized for fast reading and easy review later.

Search similar questions, compare approaches, and bookmark the best answers for revision. Our goal is simple: quick, reliable study help that feels natural—not noisy.