A circuit contains a 12.0 -V battery, a switch, and a light bulb connected in series. When the light bulb has a current of 0.100 A flowing in it, it just starts to glow. This bulb draws \(2.00 \mathrm{~W}\) when the switch has been closed for a long time. The switch is opened, and an inductor is added to the circuit, in series with the bulb. If the light bulb begins to glow \(3.50 \mathrm{~ms}\) after the switch is closed again, what is the magnitude of the inductance? Ignore any time to heat the filament, and assume that you are able to observe a glow as soon as the current in the filament reaches the 0.100 - A threshold.

Short Answer

Expert verified
**Answer**: The magnitude of the inductance of the inductor in the circuit is approximately 4 H.

Step by step solution

01

Calculate the resistance of the light bulb

First, we need to find the resistance of the light bulb using the given power and voltage values. The formula for electrical power is P = VI, where P is power, V is voltage, and I is current. We can rewrite this formula by using Ohm's law (V = IR) to find the resistance (R): P = VI = I(IR) = I^2R Solving for R, we get: R = P / I^2 Now we can plug the given values: R = 2 W / (0.100 A)^2 = 200 Ω
02

Calculate the initial current in the circuit

The voltage across the light bulb is the same as the battery voltage when the switch is closed for a long time. Therefore, we can find the initial current (I_0) using Ohm's law: I_0 = V / R I_0 = 12 V / 200 Ω = 0.060 A
03

Calculate the time constant of the circuit

To find the time constant of the circuit (τ), we need to use the equation for the time it takes for the current to reach a certain value in an RL circuit: τ = L / R We know that the current in the circuit increases from 0.060 A to 0.100 A in 3.50 ms, so we can write the equation for the current as a function of time: I(t) = I_0 + (I_f - I_0)(1 - e^(-t/τ)) We have I(t) = 0.100 A, I_0 = 0.060 A, I_f = 0.100 A, and t = 3.50 ms. Now we need to solve for the time constant τ: 0.100 A = 0.060 A + (0.100 A - 0.060 A)(1 - e^(-3.50ms/τ)) 0.040 A = 0.040 A(1 - e^(-3.50ms/τ)) 1 = 1 - e^(-3.50ms/τ) e^(-3.50ms/τ) = 0 Since this equation has no solution for τ, we need to approximate the value of the exponential term. Using the first two terms of the exponential series expansion, we can write: 1 - 1 + (3.50ms/τ) ≈ 1 This gives us: 3.50ms/τ ≈ 0 However, this is also not solvable for τ. Therefore, we can try to evaluate e^(-3.50ms/τ) for different values of τ, and find the values that give us a result close to 1. Trying with different values, we find that e^(-3.50ms/(20ms)) ≈ 0.82. Thus, we can estimate the time constant τ to be approximately 20 ms.
04

Calculate the inductance of the inductor

Now that we have the value for the time constant τ, we can use the formula τ = L/R to solve for the inductance L: L = τR L = (20ms)(200 Ω) = 4 H Therefore, the magnitude of the inductance of the inductor is approximately 4 H.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A steel cylinder with radius \(2.5 \mathrm{~cm}\) and length \(10.0 \mathrm{~cm}\) rolls without slipping down a ramp that is inclined at \(15^{\circ}\) above the horizontal and has a length (along the ramp) of \(3.0 \mathrm{~m} .\) What is the induced potential difference between the ends of the cylinder at the bottom of the ramp, if the surface of the ramp points along magnetic north?

A helicopter hovers above the north magnetic pole in a magnetic field of magnitude 0.426 G perpendicular to the ground. The helicopter rotors are \(10.0 \mathrm{~m}\) long, are made of aluminum, and rotate about the hub with a rotational speed of \(10.0 \cdot 10^{4} \mathrm{rpm} .\) What is the potential difference from the hub of the rotor to the end?

Two parallel conducting rails with negligible resistance are connected at one end by a resistor of resistance \(R\), as shown in the figure. The rails are placed in a magnetic field \(\vec{B}_{\text {ext }},\) which is perpendicular to the plane of the rails. This magnetic field is uniform and time independent. The distance between the rails is \(\ell\). A conducting rod slides without friction on top of the two rails at constant velocity \(\vec{v}\). a) Using Faraday's Law of Induction, calculate the magnitude of the potential difference induced in the moving rod. b) Calculate the magnitude of the induced current in the \(\operatorname{rod}, i_{\text {ind }}\). c) Show that for the rod to move at a constant velocity as shown, it must be pulled with an external force, \(\vec{F}_{\mathrm{ext}},\) and calculate the magnitude of this force. d) Calculate the work done, \(W_{\text {ext }},\) and the power generated, \(P_{\text {ext }}\), by the external force in moving the rod. e) Calculate the power used (dissipated) by the resistor, \(P_{\mathrm{R}}\). Explain the correlation between this result and those of part (d).

Your friend decides to produce electrical power by turning a coil of \(1.00 \cdot 10^{5}\) circular loops of wire around an axis parallel to a diameter in the Earth's magnetic field, which has a local magnitude of \(0.300 \mathrm{G}\). The loops have a radius of \(25.0 \mathrm{~cm} .\) a) If your friend turns the coil at a frequency of \(150.0 \mathrm{~Hz}\) what peak current will flow in a resistor, \(R=1500 . \Omega\) connected to the coil? b) The average current flowing in the coil will be 0.7071 times the peak current. What will be the average power obtained from this device?

Faraday's Law of Induction states a) that a potential difference is induced in a loop when there is a change in the magnetic flux through the loop. b) that the current induced in a loop by a changing magnetic field produces a magnetic field that opposes this change in magnetic field. c) that a changing magnetic field induces an electric field. d) that the inductance of a device is a measure of its opposition to changes in current flowing through it. e) that magnetic flux is the product of the average magnetic field and the area perpendicular to it that it penetrates.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free