Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

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?

Short Answer

Expert verified
Answer: The potential difference induced from the hub of the rotor to the end is approximately 22.3 Volts.

Step by step solution

01

Convert the magnetic field to Tesla

The given magnetic field is in Gauss (G), but we need Tesla (T) to use the formula for the potential difference. To convert Gauss to Tesla, we can use the following relation: 1 Tesla = 10000 Gauss. B = 0.426 G * (1 T / 10000 G) = 0.0000426 T
02

Convert the rotational speed to radians per second

The given rotational speed is in revolutions per minute (rpm). We need to convert it to radians per second (rad/s) to use the formula for the potential difference. To do this, we will first convert rpm to revolutions per second (rps), and then to radians per second: 1 rpm = 1/60 rps, 1 revolution = 2π radians Rotational speed = 10.0 × 10^4 rpm * (1/60 rps/rpm) * (2π rad/revolution) = 1.047 × 10^5 rad/s
03

Calculate the potential difference

Now we can use the formula for the potential difference induced in a rotating conducting rod in a magnetic field: ΔV = B * L²ω/2 ΔV = 0.0000426 T * (10 m)² * (1.047 × 10^5 rad/s) / 2 ΔV ≈ 22.3 Volts Therefore, the potential difference from the hub of the rotor to the end is approximately 22.3 Volts.

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!

Key Concepts

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

Magnetic Field
A magnetic field is an invisible force that exerts magnetic forces on substances which are sensitive to magnetism. A magnetic field is created by moving electric charges and inherent magnetic moments of elementary particles associated with a fundamental quantum property known as the spin. In the context of the given exercise, the helicopter hovers above the north magnetic pole where the magnetic field is quite strong and is oriented perpendicular to the surface of the Earth.

When a conductive material moves within a magnetic field, an electromotive force (EMF) is induced across the material—a phenomenon known as electromagnetic induction. In this scenario, the aluminum rotors of the helicopter, which conduct electricity, are moving due to the rotational motion within the Earth's magnetic field, causing a potential difference, or voltage, to be induced across the length of the rotor blades. This process is governed by Faraday’s law of electromagnetic induction.
Potential Difference
Potential difference, also known as voltage, is the difference in electric potential between two points in an electric field. It provides the push that drives charge through a circuit. In our helicopter example, potential difference is generated due to the rotors cutting through the Earth's magnetic field. This movement creates a flow of electric charges within the rotors, which is manifested as voltage.

To calculate the potential difference, one would typically use the formula \( \Delta V = B \times L^2 \times \omega / 2 \) where \( \Delta V \) is the potential difference, \( B \) is the magnetic field strength in Tesla, \( L \) is the length of the rotor, and \( \omega \) is the angular velocity in radians per second. The factor of \( 1/2 \) comes from a more sophisticated understanding of the electromagnetic effects at play—essentially, the average of the potential across the rotor from one point to another.
Rotational Motion
Rotational motion is the circular movement of an object around a center or axis of rotation. A three-dimensional object always rotates around an imaginary line called a rotation axis. In our example, the helicopter’s rotors are experiencing rotational motion as they spin at high speeds around their hub or axis. This type of motion is often measured in revolutions per minute (rpm) but can also be expressed in radians per second (rad/s) which is needed when applying formulas in physics.

The helicopter’s rotor converting rotational speed from rpm to rad/s involves understanding that a full revolution is equal to \(2\pi\) radians and 1 minute is equal to 60 seconds. This conversion is crucial for calculating the potential difference accurately, which, as highlighted in your exercise improvement advice, ensures students understand the importance of units in physics equations and the need to convert them appropriately for calculations to be correct.

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 rectangular conducting loop with dimensions \(a\) and \(b\) and resistance \(R\), is placed in the \(x y\) -plane. A magnetic field of magnitude \(B\) passes through the loop. The magnetic field is in the positive \(z\) -direction and varies in time according to \(B=B_{0}\left(1+c_{1} t^{3}\right),\) where \(c_{1}\) is a constant with units of \(1 / \mathrm{s}^{3}\) What is the direction of the current induced in the loop, and what is its value at \(t=1 \mathrm{~s}\) (in terms of \(a, b, R, B_{0},\) and \(\left.c_{1}\right) ?\)

A circular loop of area \(A\) is placed perpendicular to a time-varying magnetic field of \(B(t)=B_{0}+a t+b t^{2},\) where \(B_{0}, a,\) and \(b\) are constants. a) What is the magnetic flux through the loop at \(t=0 ?\) b) Derive an equation for the induced potential difference in the loop as a function of time. c) What is the magnitude and the direction of the induced current if the resistance of the loop is \(R ?\)

A circular conducting loop with radius \(a\) and resistance \(R_{2}\) is concentric with a circular conducting loop with radius \(b \gg a(b\) much greater than \(a\) ) and resistance \(R_{1}\). A time-dependent voltage is applied to the larger loop, having a slow sinusoidal variation in time given by \(V(t)=V_{0} \sin \omega t\) where \(V_{0}\) and \(\omega\) are constants with dimensions of voltage and inverse time, respectively. Assuming that the magnetic field throughout the inner loop is uniform (constant in space) and equal to the field at the center of the loop, derive expressions for the potential difference induced in the inner loop and the current \(i\) through that loop.

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.

People with pacemakers or other mechanical devices as implants are often warned to stay away from large machinery or motors. Why?

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