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In the movie Back to the Future, time travel is made possible by a flux capacitor, which generates 1.21 GW of power. Assuming that a 1.00 - \(F\) capacitor is charged to its maximum capacity with a \(12.0-\mathrm{V}\) car battery and is discharged through a resistor, what resistance is necessary to produce a peak power output of \(1.21 \mathrm{GW}\) in the resistor? How long would it take for a \(12.0-\mathrm{V}\) car battery to charge the capacitor to \(90.0 \%\) of its maximum capacity through this resistor?

Short Answer

Expert verified
Answer: The necessary resistance to produce a peak power output of 1.21 GW in the resistor is approximately \(1.20 \times 10^{-7}\,\Omega\), and it would take approximately \(3.07 \times 10^{-6}\,\text{s}\) for a 12.0 V car battery to charge the capacitor to 90% of its maximum capacity through this resistor.

Step by step solution

01

Calculate the peak voltage across the capacitor

When the capacitor is fully charged, the maximum voltage across it will be 12.0 V. We can use this value to calculate the peak power output.
02

Apply the power-resistance relationship

The power output (P) in the resistor can be calculated using the equation \( P = \frac{V^2}{R}\), where V is the voltage across the resistor and R is the resistance. Rearranging the equation, we get \( R = \frac{V^2}{P}\).
03

Calculate the necessary resistance

Now, we can plug the values into the equation: \(R = \frac{(12.0\,\text{V})^2}{1.21 \times 10^9\,\text{W}} = 1.20 \times 10^{-7}\,\Omega\) Now, let's find the time required to charge the capacitor to 90% of its maximum capacity through this resistor using a 12.0 V car battery.
04

Calculate the RC time constant

The RC time constant (τ) can be calculated using the equation \( \tau = R \times C\), where R is the resistance and C is the capacitance. Substituting the values, we get \(\tau = (1.20 \times 10^{-7}\,\Omega) \times (1.00\,\text{F}) = 1.20 \times 10^{-7}\,\text{s}\)
05

Use the RC time constant to find the charge time

The voltage across the charging capacitor (V_c) as a function of time (t) is given by the equation \(V_c = V \times (1 - e^{-\frac{t}{\tau}})\), where V is the battery voltage and τ is the RC time constant. We need to find the time t when the capacitor has charged to 90% of its maximum capacity, i.e., the voltage across the capacitor is 90% of the maximum voltage, \(0.90\times12.0\,\text{V} = 10.8\,\text{V}\). We can rearrange the equation to find t: \(t = -\tau \times \ln (1-\frac{V_c}{V})\)
06

Calculate the required charging time

Now, we can plug the values into the equation: \(t = -(1.20 \times 10^{-7}\,\text{s}) \times \ln (1-\frac{10.8\,\text{V}}{12.0\,\text{V}}) = 3.07 \times 10^{-6}\,\text{s}\) So, the required resistance to produce a peak power output of 1.21 GW in the resistor is approximately \(1.20 \times 10^{-7}\,\Omega\), and it would take approximately \(3.07 \times 10^{-6}\,\text{s}\) for a 12.0 V car battery to charge the capacitor to 90% of its maximum capacity through this resistor.

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Most popular questions from this chapter

During a physics demonstration, a fully charged \(90.0-\mu \mathrm{F}\) capacitor is discharged through a \(60.0-\Omega\) resistor. How long will it take for the capacitor to lose \(80.0 \%\) of its initial energy?

The dead battery of your car provides a potential difference of \(9.950 \mathrm{~V}\) and has an internal resistance of \(1.100 \Omega\). You charge it by connecting it with jumper cables to the live battery of another car. The live battery provides a potential difference of \(12.00 \mathrm{~V}\) and has an internal resistance of \(0.01000 \Omega\) and the starter resistance is \(0.07000 \Omega\). a) Draw the circuit diagram for the connected batteries. b) Determine the current in the live battery, in the dead battery, and in the starter immediately after you closed the circuit

In the circuit in the figure, the capacitors are completely uncharged. The switch is then closed for a long time. a) Calculate the current through the \(4.00-\Omega\) resistor. b) Find the potential difference across the \(4.00-\Omega, 6.00-\Omega\), and \(8.00-\Omega\) resistors. c) Find the potential difference across the \(1.00-\mu \mathrm{F}\) capacitor.

Consider a series \(\mathrm{RC}\) circuit with \(R=10.0 \Omega\) \(C=10.0 \mu \mathrm{F}\) and \(V=10.0 \mathrm{~V}\) a) How much time, expressed as a multiple of the time constant, does it take for the capacitor to be charged to half of its maximum value? b) At this instant, what is the ratio of the energy stored in the capacitor to its maximum possible value? c) Now suppose the capacitor is fully charged. At time \(t=0,\) the original circuit is opened and the capacitor is allowed to discharge across another resistor, \(R^{\prime}=1.00 \Omega,\) that is connected across the capacitor. What is the time constant for the discharging of the capacitor? d) How many seconds does it take for the capacitor to discharge half of its maximum stored charge, \(Q ?\)

If the capacitor in an \(\mathrm{RC}\) circuit is replaced with two identical capacitors connected in series, what happens to the time constant for the circuit?

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