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 particle detector utilizes a solenoid that has 550 turns of wire per centimeter. The wire carries a current of 22 A. A cylindrical detector that lies within the solenoid has an inner radius of \(0.80 \mathrm{~m}\). Electron and positron beams are directed into the solenoid parallel to its axis. What is the minimum momentum perpendicular to the solenoid axis that a particle can have if it is to be able to enter the detector?

Short Answer

Expert verified
Answer: The minimum momentum perpendicular to the solenoid axis that a particle can have if it is to be able to enter the detector is about \(3.04 \times 10^{-24} \, \text{kg m/s}\).

Step by step solution

01

Calculate the magnetic field inside the solenoid

To calculate the magnetic field, we first need to find the number of turns per unit length, n. The number of turns per centimeter is given as 550 turns/cm. Therefore, to find the number of turns per meter, we need to multiply by 100: n = 550 turns/cm * 100 cm/m = 55000 turns/m Now, we can use the formula for the magnetic field inside a solenoid, \(B = \mu_0 nI\): B = (\(4\pi \times 10^{-7} \, \text{T m/A}\) ) * (55000 turns/m) * (22 A) = 0.1519 T The magnetic field inside the solenoid is 0.1519 T (Teslas).
02

Calculate the angular frequency of the particle in the magnetic field

We can now use the formula \(\omega = \frac{qB}{m}\) to find the angular frequency of the particle in the solenoid. Since we are dealing with electrons and positrons, both have the same magnitude of charge (1.6 x 10^{-19} C) and mass (9.109 x 10^{-31} kg): \(\omega = \frac{1.6 \times 10^{-19} C \times 0.1519 T}{9.109 \times 10^{-31} kg} = 2.679 \times 10^{11} \, \text{rad/s}\) The angular frequency of the particle in the magnetic field is about \(2.679 \times 10^{11} \, \text{rad/s}\).
03

Calculate the minimum momentum parallel to the solenoid axis

To find the minimum momentum required to enter the detector, we can use the formulas \(p = mvr\) and \(v = \frac{\omega r}{2\pi}\). Replacing the value of v in the momentum equation: \(p = m\frac{\omega r}{2\pi}\) Now, we will plug in the given values: \(p = (9.109 \times 10^{-31} kg) \frac{(2.679 \times 10^{11} \, \text{rad/s})(0.8 \, \text{m})}{2\pi}\) \(p \approx 3.04 \times 10^{-24} \,\text{kg m/s}\) The minimum momentum perpendicular to the solenoid axis that a particle can have if it is to be able to enter the detector is about \(3.04 \times 10^{-24} \, \text{kg m/s}\).

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 long, straight wire carrying a \(2.00-\mathrm{A}\) current lies along the \(x\) -axis. A particle with charge \(q=-3.00 \mu \mathrm{C}\) moves parallel to the \(y\) -axis through the point \((x, y, z)=(0,2,0)\). Where in the \(x y\) -plane should another long, straight wire be placed so that there is no magnetic force on the particle at the point where it crosses the plane?

A square loop of wire with a side length of \(10.0 \mathrm{~cm}\) carries a current of 0.300 A. What is the magnetic field in the center of the square loop?

The current density in a cylindrical conductor of radius \(R\) varies as \(J(r)=J_{0} e^{-r / R}(\) in the region from zero to \(R\) ). Express the magnitude of the magnetic field in the regions \(rR .\) Produce a sketch of the radial dependence, \(B(r)\).

Suppose that the magnetic field of the Earth were due to a single current moving in a circle of radius \(2.00 \cdot 10^{3} \mathrm{~km}\) through the Earth's molten core. The strength of the Earth's magnetic field on the surface near a magnetic pole is about \(6.00 \cdot 10^{-5} \mathrm{~T}\). About how large a current would be required to produce such a field?

As shown in the figure, a long, hollow, conducting cylinder of inner radius \(a\) and outer radius \(b\) carries a current that is flowing out of the page. Suppose that \(a=5.00 \mathrm{~cm}, b=7.00 \mathrm{~cm},\) and the current \(i=100 . \mathrm{mA}\) uniformly distributed over the cylinder wall (between \(a\) and \(b\) ). Find the magnitude of the magnetic field at each of the following distances \(r\) from the center of the cylinder: a) \(r=4.00 \mathrm{~cm}\) b) \(r=6.50 \mathrm{~cm}\) c) \(r=9.00 \mathrm{~cm}\)

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