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Prior to \(t=0, \mathrm{a} 100-\mu \mathrm{F}\) capacitance is uncharged. Starting at \(t=0\), the voltage across the capacitor is increased linearly with time to \(100 \mathrm{~V}\) in \(2 \mathrm{~s}\). Then, the voltage remains constant at \(100 \mathrm{~V}\). Sketch the voltage, current, power, and stored energy to scale versus time.

Short Answer

Expert verified
Voltage increases linearly to 100 V in 2 s, current is 5 mA for 2 s then 0. Power increases to 0.5 W then 0, and energy increases to 0.5 J then constant.

Step by step solution

01

Sketch the Voltage vs. Time

The voltage increases linearly from 0 V at \(t=0\) to 100 V at \(t=2\) seconds. After reaching 100 V, it remains constant. Thus, the voltage vs. time graph is a straight line from \((0, 0)\) to \((2, 100)\) followed by a horizontal line until the time ends.
02

Determine the Current vs. Time

The current \(I(t)\) in a capacitor is given by \(I(t) = C \cdot \frac{dV(t)}{dt}\). For \(0 \leq t \leq 2\), \(V(t) = 50t\), so \(I(t) = 100 \times 10^{-6} \cdot 50 = 5 \times 10^{-3}\) A. For \(t > 2\), the derivative of \(V(t)\) is 0, hence the current is 0 A.
03

Sketch the Current vs. Time

The current is 5 mA (from Step 2) from \(t=0\) to \(t=2\). At \(t > 2\), the current drops to 0 A. Thus, the current vs. time graph is a horizontal line at 5 mA from \(t=0\) to \(t=2\) and a horizontal line at 0 A for \(t > 2\).
04

Calculate Power vs. Time

Power \(P(t)\) in a capacitor is given by \(P(t) = V(t) \cdot I(t)\). For \(0 \leq t \leq 2\), since \(V(t) = 50t\) and \(I(t) = 5 \times 10^{-3}\) A, \(P(t) = 50t \times 5 \times 10^{-3} = 0.25t\) W. For \(t > 2\), \(P(t) = 100 \times 0 = 0\) W.
05

Sketch the Power vs. Time

From Step 4, power increases linearly from \(0\) at \(t=0\) to \(0.5 \) W at \(t=2\) s. After \(t=2\), power drops to 0 W and remains there. The power vs. time graph is a sloped line from \(0\) to \(2\) s, then a horizontal line at 0 W.
06

Compute Stored Energy vs. Time

The energy \(E(t)\) stored in the capacitor is \(E(t) = \frac{1}{2}C[V(t)]^2\). For \(0 \leq t \leq 2\), \(E(t) = \frac{1}{2} \times 100 \times 10^{-6} \times (50t)^2 = 0.125t^2\) J. For \(t > 2\), energy remains \(\frac{1}{2} \times 100 \times 10^{-6} \times (100)^2 = 0.5\) J.
07

Sketch the Stored Energy vs. Time

From Step 6, plot the energy as a parabola growing as \(0.125t^2\) from \(t=0\) to \(t=2\), reaching 0.5 J. At \(t > 2\), it stays constant at 0.5 J.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Voltage vs. Time Graph
Understanding a Voltage vs. Time Graph is fundamental when analyzing capacitor behavior, especially during charging. When the voltage across a capacitor is increased linearly, as in this exercise, the graph looks like a straightforward diagonal line starting from the origin. Here, the voltage increases from 0 V at the start (\(t=0\)), reaching 100 V at 2 seconds, and then remains unchanged.

Key points for a linear increase:
  • The graph is a straight line from \(t=0\) to \(t=2\) seconds.
  • After \(t=2\), the graph becomes a horizontal line, indicating a constant voltage.
By visualizing this line on the graph, it becomes clear how the capacitor voltage ramps up steadily until it stabilizes.
Current vs. Time Graph
For a capacitor, the Current vs. Time Graph illustrates how the current changes as the capacitor charges. The relationship between current and voltage in a capacitor is given by \(I(t) = C \cdot \frac{dV(t)}{dt}\). This means that the current is directly related to the rate of change of the voltage.

In this scenario:
  • The current is constant at 5 mA from \(t=0\) to \(t=2\).
  • Once the voltage stops increasing (after \(t=2\)), the current drops to 0 A.
These features result in a graph that has:
  • A horizontal line from \(t=0\) to \(t=2\) at 5 mA.
  • A horizontal line at 0 A for \(t>2\).
This change reflects the fact that when the voltage becomes steady, there is no further current required to charge the capacitor.
Power vs. Time Calculation
Calculating Power vs. Time in a capacitor helps us understand energy consumption during the charging process. The power \(P(t)\) is determined by multiplying voltage \(V(t)\) by current \(I(t)\). During this challenge:

From \(t=0\) to \(t=2\):
  • \(P(t) = V(t) \cdot I(t) = 50t \cdot 5 \times 10^{-3} = 0.25t\) W, showing a steady increase.
  • At \(t=2\), this results in a power of \(0.5\) W.
After \(t=2\):
  • With constant voltage, power becomes zero \(P(t) = 100 \times 0 = 0\) W.
The power graph starts with a slope to reflect the power increase over time and then levels off once the capacitor stops charging.
Stored Energy in a Capacitor
Exploring Stored Energy in a capacitor allows us to see how energy builds up as the capacitor charges. The formula \(E(t) = \frac{1}{2}C[V(t)]^2\) captures this process.

From \(t=0\) to \(t=2\):
  • Here, the stored energy increases as a parabola since the energy depends on \((50t)^2\), or \(E(t) = 0.125t^2\) J.
At \(t=2\) and beyond:
  • The stored energy reaches a maximum of 0.5 J and stays there.
This suggests that before reaching full charge, the energy accumulation is non-linear, while after stabilization, the energy remains constant as the capacitor holds its charge efficiently.

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