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After two time constants, what percentage of the final voltage, emf, is on an initially uncharged capacitor \(C\), charged through a resistance \(R ?\)

Short Answer

Expert verified
Approximately 86.47% of the EMF is on the capacitor after two time constants.

Step by step solution

01

Understand the Charging of a Capacitor

A capacitor charging through a resistor follows an exponential pattern described by the equation: \( V(t) = EMF \cdot (1 - e^{-\frac{t}{RC}}) \), where \( V(t) \) is the voltage across the capacitor at time \( t \), EMF is the electromotive force (final voltage), and \( RC \) is the time constant of the system.
02

Apply the Time Constant

The time constant \( \tau \) is given by the product of the resistance and capacitance: \( \tau = RC \). After two time constants (\( t = 2\tau \)), we can substitute this value into the charging equation to find the percentage of the final voltage:
03

Calculate the Voltage After Two Time Constants

Substitute the time value \( t = 2\tau \) into the charging equation to get: \( V(2\tau) = EMF \cdot (1 - e^{-\frac{2\tau}{RC}}) \). Since \( \tau = RC \), this simplifies to: \( V(2\tau) = EMF \cdot (1 - e^{-2}) \).
04

Find the Percentage of EMF

To find the percentage of the EMF, we calculate: \( \text{Percentage} = \frac{V(2\tau)}{EMF} \times 100\% = (1 - e^{-2}) \times 100\% \approx (1 - 0.1353) \times 100\% \approx 86.47\% \). Therefore, approximately 86.47% of the final voltage (EMF) is on the capacitor after two time constants.

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Key Concepts

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

Time Constant
The time constant, designated by the Greek letter \( \tau \), is a crucial concept for understanding the behavior of circuits that include capacitors and resistors, such as RC circuits. It is defined as the time it takes for the charge on the capacitor to reach approximately 63.2% of its final value, or conversely, for the voltage across the capacitor to reach 63.2% of its maximum value in a charging circuit.

Mathematically, the time constant \( \tau \) is the product of the resistance \( R \) and the capacitance \( C \) in the circuit: \( \tau = RC \). The greater the time constant, the slower the capacitor charges and discharges. Understanding the time constant is crucial since it allows us to calculate how quickly or slowly a capacitor will charge to a certain percentage of the maximum voltage provided by an electromotive force (EMF).
Exponential Decay
Exponential decay is a process where a quantity decreases at a rate proportional to its current value. In the context of capacitors charging in RC circuits, the voltage across the capacitor during discharging, or the remaining charge on the capacitor over time, follows an exponential decay pattern.

An important aspect of exponential decay in capacitors is the formula \( V(t) = EMF \cdot (1 - e^{-\frac{t}{\tau}}) \) where \( V(t) \) represents the voltage across the capacitor at a given time \( t \), EMF is the electromotive force, and \( e \) is the base of the natural logarithm. The exponential term \( e^{-\frac{t}{\tau}} \) quickly falls off as time increases, hence after a few time constants, the voltage across the capacitor is close to the EMF.
Electromotive Force (EMF)
The electromotive force, often abbreviated EMF, refers to the energy that drives electrons around a circuit and is measured in volts. It is essentially the maximum potential difference (voltage) a battery or generator can provide when no current is flowing.

When a capacitor is connected to a source of EMF through a resistor, the EMF acts as the driver of charge buildup on the plates of the capacitor. The voltage across the capacitor rises gradually as it charges up, asymptotically approaching the value of the EMF. This behavior is a manifestation of the EMF as it establishes an electric field within the capacitor leading to the accumulation of charge.
RC Circuits
An RC circuit is a type of electrical circuit that consists of a resistor (R), a capacitor (C), and a power supply which provides the electromotive force. This configuration is commonly used to demonstrate the charging and discharging behavior of capacitors.

In the context of charging a capacitor, when a voltage is applied to an RC circuit, the capacitor starts to charge through the resistor. The charging behavior follows an exponential pattern, dependent on the time constant \( \tau = RC \). This RC time constant dictates how quickly the circuit can respond to changes in voltage, which is essential in filtering applications, timing circuits, and many other electronic devices where control over the rate of charge and discharge is necessary.

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