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In an \(R C\) series circuit, emf \(\mathscr{E}=12.0 \mathrm{~V}\), resistance \(R=1.40\) \(M \Omega\), and capacitance \(C=1.80 \mu \mathrm{F}\). (a) Calculate the time constant. (b) Find the maximum charge that will appear on the capacitor during charging. (c) How long does it take for the charge to build up to \(16.0 \mu \mathrm{C} ?\)

Short Answer

Expert verified
(a) 2.52 s; (b) 21.6 µC; (c) 3.52 s.

Step by step solution

01

Calculate the Time Constant

The time constant for an RC circuit is given by the product of the resistance, \( R \), and the capacitance, \( C \). The formula is \( \tau = R \times C \). Substitute \( R = 1.40 \times 10^6 \, \Omega \) and \( C = 1.80 \times 10^{-6} \, F \). Thus, \( \tau = 1.40 \times 10^6 \times 1.80 \times 10^{-6} = 2.52 \, s \).
02

Find the Maximum Charge on the Capacitor

The maximum charge \( Q_{max} \) that can appear on the capacitor is given by \( Q_{max} = C \times \mathscr{E} \). Substituting \( C = 1.80 \times 10^{-6} \, F \) and \( \mathscr{E} = 12.0 \, V \), we have \( Q_{max} = 1.80 \times 10^{-6} \times 12.0 = 21.6 \, \mu C \).
03

Calculate the Time to Reach a Specific Charge

The charge on the capacitor as a function of time \( t \) is given by \( Q(t) = Q_{max} (1 - e^{-t/\tau}) \). To find the time it takes for the charge to reach \( 16.0 \, \mu C \), solve for \( t \) in the equation: \[ 16.0 \times 10^{-6} = 21.6 \times 10^{-6} (1 - e^{-t/2.52}) \]This simplifies to \[ 1 - e^{-t/2.52} = \frac{16.0}{21.6} \]\[ e^{-t/2.52} = 1 - \frac{16.0}{21.6} \approx 0.259 \]Taking the natural logarithm of both sides, \[ -\frac{t}{2.52} = \ln(0.259) \]\[ t = -2.52 \times \ln(0.259) \approx 3.52 \mathrm{~s} \].

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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, denoted as \(\tau\), is a crucial parameter in an RC circuit, representing the time it takes for the system to significantly react to a change in voltage. Specifically, \(\tau\) is the time required for the voltage across the capacitor to reach approximately 63.2% of its maximum value when charging, or decay to about 36.8% during discharging. It's calculated using the formula \(\tau = R \times C\), where \(R\) is the resistance and \(C\) is the capacitance.
  • A larger time constant means the capacitor charges or discharges more slowly.
  • Shorter time constants result in quicker changes in charge.
In this exercise, the resistance \(R\) is \(1.40 \times 10^6 \, \Omega\) and the capacitance \(C\) is \(1.80 \times 10^{-6} \, F\). By multiplying these values, we find \(\tau = 2.52 \, s\). This indicates the time scale over which the capacitor both approaches its maximum charge and loses that charge in an RC circuit.
Capacitance
Capacitance, symbolized by \(C\), refers to the ability of a capacitor to store electric charge. It is directly proportional to the amount of charge that can be held at a particular voltage. The unit of capacitance is the farad (F), but in practical applications, you'll often see microfarads (\(\mu\)F), nanofarads (nF), or picofarads (pF).
  • A large capacitance signifies a high ability to store charge.
  • Capacitance is determined by the size of the plates in the capacitor and the distance between them.
In our problem, the capacitor has a capacitance \(C = 1.80 \mu F\). This tells us how much electric charge it can store per volt of electric potential applied across its plates. The larger the capacitance, the larger the amount of charge at a given voltage.
Maximum Charge
The maximum charge \(Q_{max}\) that a capacitor can hold is defined by the equation \(Q_{max} = C \times \mathscr{E}\), where \(C\) represents the capacitance and \(\mathscr{E}\) is the applied emf or voltage. This expression provides insight into how much charge a capacitor can go up to as it fully charges.
  • An increased emf results in increased maximum charge assuming capacitance stays constant.
  • Understanding this helps design circuits needing specific charge storage.
For this exercise, with a capacitance \(C = 1.80 \times 10^{-6} \, \text{F}\) and voltage \(\mathscr{E} = 12.0 \, \text{V}\), the maximum charge is determined as \(Q_{max} = 21.6 \, \mu C\). This is how much charge the capacitor will hold once it's fully charged under this circuit setup.

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Most popular questions from this chapter

A wire of resistance \(5.0 \Omega\) is connected to a battery whose emf \(\mathscr{E}\) is \(2.0 \mathrm{~V}\) and whose internal resistance is \(1.0 \Omega\). In \(2.0 \mathrm{~min}\), how much energy is (a) transferred from chemical form in the battery, (b) dissipated as thermal energy in the wire, and (c) dissipated as thermal energy in the battery?

Thermal energy is to be generated in a \(0.10 \Omega\) resistor at the rate of \(10 \mathrm{~W}\) by connecting the resistor to a battery whose emf is \(1.5 \mathrm{~V} .\) (a) What potential difference must exist across the resistor? (b) What must be the internal resistance of the battery?

A 10 -km-long underground cable extends east to west and consists of two parallel wires, each of which has resistance 13 \(\Omega / \mathrm{km} .\) An electrical short develops at distance \(x\) from the west end when a conducting path of resistance \(R\) connects the wires (Fig. 27 31). The resistance of the wires and the short is then \(100 \Omega\) when measured from the east end and \(200 \Omega\) when measured from the west end. What are (a) \(x\) and (b) \(R\) ?

A \(15.0 \mathrm{k} \Omega\) resistor and a capacitor are connected in series, and then a \(12.0 \mathrm{~V}\) potential difference is suddenly applied across them. The potential difference across the capacitor rises to \(5.00 \mathrm{~V}\) in \(1.30 \mu \mathrm{s}\). (a) Calculate the time constant of the circuit. (b) Find the capacitance of the capacitor.

A simple ohmmeter is made by connecting a \(1.50 \mathrm{~V}\) flashlight battery in series with a resistance \(R\) and an ammeter that reads from 0 to \(1.00 \mathrm{~mA}\), as shown in Fig. \(27-59 .\) Resistance \(R\) is adjusted so that when the clip leads are shorted together, the meter deflects to its full- scale value of \(1.00 \mathrm{~mA}\). What external resistance across the leads results in a deflection of (a) \(10.0 \%,(\mathrm{~b})\) \(50.0 \%\), and (c) \(90.0 \%\) of full scale? (d) If the ammeter has a resistance of \(20.0 \Omega\) and the internal resistance of the battery is negligible, what is the value of \(R ?\)

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