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 circular coil with a radius of \(10.0 \mathrm{~cm}\) has 100 turns of wire and carries a current, \(i=100 . \mathrm{mA}\). It is free to rotate in a region with a constant horizontal magnetic field given by \(\vec{B}=(0.0100 \mathrm{~T}) \hat{x}\). If the unit normal vector to the plane of the coil makes an angle of \(30.0^{\circ}\) with the horizontal, what is the magnitude of the net torque acting on the coil?

Short Answer

Expert verified
Question: Determine the net torque acting on a circular coil with a radius of 10.0 cm, 100 turns, a current of 100 mA, and a magnetic field of 0.0100 T. The angle between the unit normal vector and the horizontal is 30.0 degrees. Answer: The net torque acting on the circular coil is 100π N·cm.

Step by step solution

01

Calculating the area of the coil

To calculate the area (A) of the circular coil, we use the formula for the area of a circle: \(A = \pi r^2\), where r is the radius of the coil. In this case, the radius is given as \(10.0 \mathrm{~cm}\), so we have: \(A = \pi (10.0 \mathrm{~cm})^2 = 100\pi\, \mathrm{cm^2}\).
02

Converting the angle from degrees to radians

The angle between the unit normal vector and the horizontal, \(\theta\), is given in degrees (\(30.0^\circ\)). In order to use this angle in our calculation for the torque, we need to convert it to radians. To convert degrees to radians, we use the following formula: \(\mathrm{Radians} = \frac{\mathrm{Degrees}}{180^\circ} \cdot \pi\). Applying this to our given angle, we get: \(\theta = \frac{30.0^\circ}{180^\circ} \cdot \pi = \frac{\pi}{6}\, \mathrm{rad}\).
03

Calculating the net torque acting on the coil

Now, we will use the formula for torque on a current loop, which is \(\tau = N \cdot I \cdot A \cdot B \cdot \sin{\theta}\). We are given the number of turns (N = 100), the current (I = \(100 \mathrm{~mA}\) = \(0.1 \mathrm{~A}\)), the magnetic field (B = \(0.0100 \mathrm{~T}\)), and we have calculated the area (A = \(100\pi\, \mathrm{cm^2}\)) and the angle in radians (\(\theta = \frac{\pi}{6}\)). Plugging these values into the formula, we get: \(\tau = 100 \cdot 0.1 \mathrm{A} \cdot 100\pi\, \mathrm{cm^2} \cdot 0.0100 \mathrm{~T} \cdot \sin{\frac{\pi}{6}} = 100\pi\, \mathrm{N \cdot cm}\).

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

The Earth is showered with particles from space known as muons. They have a charge identical to that of an electron but are many times heavier \(\left(m=1.88 \cdot 10^{-28} \mathrm{~kg}\right)\). Suppose a strong magnetic field is established in a lab \((B=0.500 \mathrm{~T})\) and a muon enters this field with a velocity of \(3.00 \cdot 10^{6} \mathrm{~m} / \mathrm{s}\) at a right angle to the field. What will be the radius of the muon's resulting orbit?

The figure shows a schematic diagram of a simple mass spectrometer, consisting of a velocity selector and a particle detector and being used to separate singly ionized atoms \(\left(q=+e=1.602 \cdot 10^{-19} \mathrm{C}\right)\) of gold \((\mathrm{Au})\) and molybdenum (Mo). The electric field inside the velocity selector has magnitude \(E=1.789 \cdot 10^{4} \mathrm{~V} / \mathrm{m}\) and points toward the top of the page, and the magnetic field has magnitude \(B_{1}=1.000 \mathrm{~T}\) and points out of the page. a) Draw the electric force vector, \(\vec{F}_{E},\) and the magnetic force vector, \(\vec{F}_{B}\), acting on the ions inside the velocity selector. b) Calculate the velocity, \(v_{0},\) of the ions that make it through the velocity selector (those that travel in a straight line). Does \(v_{0}\) depend on the type of ion (gold versus molybdenum), or is it the same for both types of ions? c) Write the equation for the radius of the semicircular path of an ion in the particle detector: \(R=R\left(m, v_{0}, q, B_{2}\right)\) d) The gold ions (represented by the dark gray spheres) exit the particle detector at a distance \(d_{2}=40.00 \mathrm{~cm}\) from the entrance slit, while the molybdenum ions (represented by the light gray spheres) exit the particle detector at a distance \(d_{1}=19.81 \mathrm{~cm}\) from the entrance slit. The mass of a gold ion is \(m_{\text {gold }}=3.271 \cdot 10^{-25} \mathrm{~kg} .\) Calculate the mass of a molybdenum ion.

A proton with an initial velocity given by \((1.00 \hat{x}+2.00 \hat{y}+3.00 \hat{z})\) \(\left(10^{5} \mathrm{~m} / \mathrm{s}\right)\) enters a magnetic field given by \((0.500 \mathrm{~T}) \hat{z}\). Describe the motion of the proton.

A charged particle moves under the influence of an electric field only. Is it possible for the particle to move with a constant speed? What if the electric field is replaced with a magnetic field?

A magnetic field is oriented in a certain direction in a horizontal plane. An electron moves in a certain direction in the horizontal plane. For this situation, there a) is one possible direction for the magnetic force on the electron. b) are two possible directions for the magnetic force on the electron. c) are infinite possible directions for the magnetic force on the electron.

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