/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 11 In a chamber, a uniform magnetic... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

In a chamber, a uniform magnetic field of \(6.5 \mathrm{G}\left(1 \mathrm{G}=10^{-4} \mathrm{~T}\right)\) is maintained. An electron is shot into the field with a speed of \(4.8 \times 10^{6} \mathrm{~m} \mathrm{~s}^{-1}\) normal to the field. Explain why the path of the electron is a circle. Determine the radius of the circular orbit. \(\left(e=1.5 \times 10^{-19} \mathrm{C}, m_{e}=9.1 \times 10^{-31} \mathrm{~kg}\right)\)

Short Answer

Expert verified
The path of the electron is a circle due to the magnetic force acting as a centripetal force. The radius of this circular path is 0.216 m.

Step by step solution

01

Analyse the situation

The electron is moving under the influence of a magnetic field in a direction perpendicular to the field. The magnetic force (\( F_m \)) acts as a centripetal force and is given by \( F_m = qvB \) where q is the charge, v is the velocity and B is the magnetic field strength. The centripetal force (\( F_c \)) is given by \( F_c = \frac{m_{e}v^2}{r} \) where \( m_{e} \) is the mass of the electron and r is the radius of the circular path.
02

Equate the forces

Given that the magnetic force and the centripetal force balance each other, we equate them, which gives us \( qvB = \frac{m_{e}v^2}{r} \).
03

Calculate the radius

Rearranging the equation for r, we get \( r = \frac{m_{e}v}{qB} \). Now, we substitute the given values into the equation which are \( m_{e}=9.1 \times 10^{-31} \mathrm{kg} \), \( q=1.6 \times 10^{-19} C \), \( v=4.8 \times 10^{6} ms^{-1} \), \( B = 6.5 G = 6.5 \times 10^{-4} T \). This gives us \( r = \frac{(9.1 \times 10^{-31} kg)(4.8 \times 10^{6} ms^{-1})}{(1.6 \times 10^{-19} C)(6.5 \times 10^{-4} T)} \).
04

Simplify

Simplify the above equation to get the radius r. Solving it yields \( r = 0.216 \) m.

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 91Ó°ÊÓ!

Key Concepts

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

Electron Motion
When an electron enters a magnetic field perpendicularly, it experiences a magnetic force. This force is unique because it acts perpendicular to both the velocity of the electron and the magnetic field itself.
This perpendicular force changes the direction of the electron's motion but not its speed. The outcome is a path that forms a perfect circle.
The magnetic force on the electron can be described by the formula:
  • F_m = qvB
This formula tells us that the force (\(F_m\)) depends on the charge of the electron (\(q\)), its velocity (\(v\)), and the magnetic field strength (\(B\)).
Because this force is always perpendicular to the electron’s path, it constantly changes the electron's direction without altering its speed, thereby making the electron move in a circular path.
Centripetal Force
The concept of centripetal force is essential to understanding the circular motion of electrons in a magnetic field. A centripetal force is any force that keeps a body moving with a uniform speed along a circular path.
For the electron moving in a magnetic field, the magnetic force provides the necessary centripetal force to sustain its circular motion. This is described by:
  • F_c = \frac{m_{e}v^2}{r}
Where:
  • \(F_c\) is the centripetal force.
  • \(m_{e}\) is the mass of the electron.
  • \(v\) is its velocity.
  • \(r\) is the radius of the circular path.
When an electron moves at a constant speed in a circle,
the magnetic force (\(F_m\)) equals the centripetal force (\(F_c\)). These forces balance each other leading to the equation:
  • qvB = \frac{m_{e}v^2}{r}
This equation shows how the magnetic effect causes the electron to follow a curved circular pathway.
Circular Path Radius
The radius of the circular path is a crucial aspect that determines how an electron behaves in a magnetic field.
To find this radius (\(r\)), we rearrange the equation for centripetal force and magnetic force balance:
  • r = \frac{m_{e}v}{qB}
This rearranged formula shows the factors affecting the radius:
  • The mass of the electron (\(m_{e}\))
  • Its velocity (\(v\))
  • The charge of the electron (\(q\))
  • The magnetic field strength (\(B\))
Given the problem's specific values:
  • \(m_{e}=9.1 \times 10^{-31} \text{ kg}\)
  • \(v=4.8 \times 10^{6} \text{ m/s}\)
  • \(q=1.6 \times 10^{-19} \text{ C}\)
  • \(B=6.5 \times 10^{-4} \text{ T}\)
Placing these into the formula gives the radius:\[r = \frac{(9.1 \times 10^{-31} \text{ kg})(4.8 \times 10^{6} \text{ m/s})}{(1.6 \times 10^{-19} \text{ C})(6.5 \times 10^{-4} \text{ T})} = 0.216 \text{ m}\]Understanding these factors helps to comprehend why the electron moves in a circular path with this specific radius.

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 in the horizontal plane carries a current of \(50 \mathrm{~A}\) in north to south direction. Give the magnitude and direction of \(\mathbf{B}\) at a point \(2.5 \mathrm{~m}\) east of the wire.

A galvanometer coil has a resistance of \(15 \Omega\) and the metre shows full scale deflection for a current of \(4 \mathrm{~mA}\). How will you convert the metre into an ammeter of range 0 to \(6 \mathrm{~A} ?\)

What is the magnitude of magnetic force per unit length on a wire carrying a current of 8 A and making an angle of \(30^{\circ}\) with the direction of a uniform magnetic field of \(0.15 \mathrm{~T}\) ?

A straight horizontal conducting rod of length \(0.45 \mathrm{~m}\) and mass \(60 \mathrm{~g}\) is suspended by two vertical wires at its ends. A current of \(5.0 \mathrm{~A}\) is set up in the rod through the wires. (a) What magnetic field should be set up normal to the conductor in order that the tension in the wires is zero? (b) What will be the total tension in the wires if the direction of current is reversed keeping the magnetic field same as before? (Ignore the mass of the wires.) \(g=9.8 \mathrm{~m} \mathrm{~s}^{-2}\).

For a circular coil of radius \(R\) and \(N\) turns carrying current \(I\), the magnitude of the magnetic field at a point on its axis at a distance \(x\) from its centre is given by, \(B=\frac{\mu_{0} I R^{2} N}{2\left(x^{2}+R^{2}\right)^{3 / 2}}\) (a) Show that this reduces to the familiar result for field at the centre of the coil. (b) Consider two parallel co-axial circular coils of equal radius \(R\). and number of turns \(N\), carrying equal currents in the same direction, and separated by a distance \(R\). Show that the field on the axis around the mid- point between the coils is uniform over a distance that is small as compared to \(R\), and is given by, \(B=0.72 \frac{\mu_{0} N I}{R}\), approximately. [Such an arrangement to produce a nearly uniform magnetic field over a small region is known as Helmholtz coils.]

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.