Problem 20
Question
A \(15.0-\Omega\) resistor and a coil are connected in series with a 6.30-V battery with negligible internal resistance and a closed switch. (a) At 200 ms after the switch is opened the current has decayed to 0.210 A. Calculate the inductance of the coil. (b) Calculate the time constant of the circuit. (c) How long after the switch is closed will the current reach 1.00\(\%\) of its original value?
Step-by-Step Solution
Verified Answer
(a) The inductance is 4.32 H. (b) The time constant is 0.288 s. (c) The current reaches 1% in 1.327 s.
1Step 1: Understanding the Circuit and Problem
We have a series circuit with a 15.0 Ω resistor and an inductor. When the switch is open, the current decays exponentially. We need to find the inductance of the coil, time constant, and time for current to reach 1% of its original value.
2Step 2: Using the Formula for Exponential Decay
The current decay when the switch is opened follows the equation: \[ I(t) = I_0 e^{-\frac{t}{\tau}} \]where \( I(t) \) is the current at time \( t \), \( I_0 \) is the initial current, and \( \tau \) is the time constant. We know \( I(t) = 0.210 \text{ A} \) at \( t = 200 \text{ ms} \).
3Step 3: Calculating the Initial Current
The initial current \( I_0 \) when the switch was closed can be determined using Ohm's Law:\[ I_0 = \frac{V}{R} = \frac{6.30 \text{ V}}{15.0 \Omega} = 0.42 \text{ A} \]
4Step 4: Solving for the Time Constant (a)
By rearranging the decay equation, we solve for \( \tau \):\[ 0.210 = 0.42 e^{-\frac{0.2}{\tau}} \]\[ e^{-\frac{0.2}{\tau}} = 0.5 \]Take the natural logarithm of both sides:\[ -\frac{0.2}{\tau} = \ln(0.5) \]\[ \tau = \frac{0.2}{-\ln(0.5)} \approx 0.2 \times 1.443 = 0.288 \text{ s} \]
5Step 5: Calculating the Inductance (b)
Use the relationship between the time constant \( \tau \), inductance \( L \), and resistance \( R \):\[ \tau = \frac{L}{R} \]\[ L = \tau \times R = 0.288 \text{ s} \times 15.0 \Omega = 4.32 \text{ H} \]
6Step 6: Calculating the Time to Reach 1% of Initial Current (c)
To find the time it takes for the current to decay to 1% of its initial value:\[ I(t) = 0.01 \times I_0 = 0.0042 \text{ A} \]\[ 0.0042 = 0.42 e^{-\frac{t}{0.288}} \]\[ e^{-\frac{t}{0.288}} = 0.01 \]Taking the natural logarithm gives:\[ -\frac{t}{0.288} = \ln(0.01) \]\[ t = -0.288 \times \ln(0.01) \approx 0.288 \times 4.605 = 1.327 \text{ s} \]
Key Concepts
Exponential DecayTime ConstantOhm's Law
Exponential Decay
In electrical circuits, exponential decay describes how the current decreases over time when a switch is opened. This behavior is prominent in circuits that include components like resistors and inductors. When the electrical path is broken by the switch, the current doesn't simply stop immediately; instead, it reduces gradually in what we call an exponential decay.
This decay can be captured mathematically by the equation \[ I(t) = I_0 e^{-\frac{t}{\tau}} \]where:
This decay can be captured mathematically by the equation \[ I(t) = I_0 e^{-\frac{t}{\tau}} \]where:
- \( I(t) \) is the current at time \( t \)
- \( I_0 \) is the initial current
- \( \tau \) is known as the time constant
- \( e \) is the base of the natural logarithm
Time Constant
The time constant, denoted as \( \tau \), is a critical factor in understanding the behavior of circuits involving resistors and inductors. It informs us about how fast or slow the exponential decay occurs.
Mathematically, \( \tau \) is described by the equation:\[ \tau = \frac{L}{R} \]where:
A high time constant means the current decays slowly, as energy is released at a slower pace, whereas a low time constant suggests a faster decay.
Mathematically, \( \tau \) is described by the equation:\[ \tau = \frac{L}{R} \]where:
- \( L \) is the inductance of the coil, measured in Henries (H)
- \( R \) is the resistance, measured in Ohms (\( \Omega \))
A high time constant means the current decays slowly, as energy is released at a slower pace, whereas a low time constant suggests a faster decay.
Ohm's Law
Ohm's Law is a fundamental principle in electrical engineering, vital for calculating current flow in circuits. This law states that the current through a conductor between two points is directly proportional to the voltage across the two points and inversely proportional to the resistance of the conductor.
Expressed mathematically, Ohm’s Law is:\[ I = \frac{V}{R} \]where:
Expressed mathematically, Ohm’s Law is:\[ I = \frac{V}{R} \]where:
- \( I \) is the current measured in Amperes (A)
- \( V \) is the voltage measured in Volts (V)
- \( R \) is the resistance measured in Ohms (\( \Omega \))
Other exercises in this chapter
Problem 18
It is proposed to store \(1.00 \mathrm{kW} \cdot \mathrm{h}=3.60 \times 10^{6} \mathrm{J}\) of electrical energy in a uniform magnetic field with magnitude 0.60
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View solution Problem 21
A \(35.0-\mathrm{V}\) battery with negligible internal resistance, a 50.0- \(\Omega\) resistor, and a \(1.25-\mathrm{mH}\) inductor with negligible resistance a
View solution Problem 28
A 20.0 -\muF capacitor is charged by a \(150.0-\mathrm{V}\) power supply, then disconnected from the power and connected in series with a \(0.280-\mathrm{mH}\)
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