Problem 17
Question
A \(150-\) g ball containing \(4.00 \times 10^{8}\) excess electrons is dropped into a \(125-\mathrm{m}\) vertical shaft. At the bottom of the shaft, the ball suddenly enters a uniform horizontal magnetic field that has magnitude 0.250 \(\mathrm{T}\) and direction from east to west. If air resistance is negligibly small, find the magnitude and direction of the force that this magnetic field exerts on the ball just as it enrers the field.
Step-by-Step Solution
Verified Answer
The magnetic force is approximately \(7.94 \times 10^{-10}\) N, directed north.
1Step 1: Calculate Charge of the Electrons
To find the charge of the electrons, we use the charge of a single electron, which is approximately \[ e = 1.602 \times 10^{-19} \, \text{Coulombs}. \]The total excess charge on the ball is then\[ Q = 4.00 \times 10^{8} \times 1.602 \times 10^{-19} \approx 6.408 \times 10^{-11} \, \text{Coulombs}. \]
2Step 2: Apply the Magnetic Force Formula
The magnetic force on a moving charge in a magnetic field is given by the formula \[ F = qvB \sin(\theta), \]where \( q \) is the charge, \( v \) is the velocity of the ball as it enters the magnetic field, \( B \) is the magnetic field, and \( \theta \) is the angle between the velocity and the magnetic field. Here, \( \theta = 90^\circ \) since the magnetic field is horizontal and the motion is vertical.
3Step 3: Calculate the Velocity of the Ball
The ball is dropped from a height of 125 m, so its velocity when it reaches the bottom of the shaft can be found using the equation of motion:\[ v^2 = u^2 + 2gh, \]where \( u = 0 \) (initial velocity), \( g = 9.81 \, \text{m/s}^2 \), and \( h = 125 \, \text{m}. \)Plugging in the values:\[ v^2 = 0 + 2 \times 9.81 \times 125 \v^2 = 2452.5 \v = \sqrt{2452.5} \approx 49.51 \, \text{m/s}. \]
4Step 4: Calculate the Magnetic Force
Now substitute the values into the magnetic force formula:\[ F = QvB \sin(\theta) = 6.408 \times 10^{-11} \, \text{C} \times 49.51 \, \text{m/s} \times 0.250 \, \text{T} \times \sin(90^\circ). \]Calculating the force:\[ F = 6.408 \times 10^{-11} \times 49.51 \times 0.250 \times 1 \approx 7.94 \times 10^{-10} \, \text{N}. \]
5Step 5: Determine the Direction of the Force
Using the Right-hand Rule for the cross product in magnetic fields, with the velocity towards the magnetic field and charge negative, the force direction is towards the north, perpendicular to both the vertical velocity and the horizontal magnetic field.
Key Concepts
Excess ElectronsMagnetic FieldsElectromagnetism Concepts
Excess Electrons
In this exercise, the concept of excess electrons is central to understanding the charge of the ball. An electron carries a negative elementary charge of approximately \( 1.602 \times 10^{-19} \ \text{Coulombs} \). When we say a ball is carrying 'excess electrons', it means there are more electrons than protons in the material, resulting in a net negative charge.
- To find the total charge on the ball, we multiply the number of excess electrons by the charge of one electron.
- For \(4.00 \times 10^{8}\) excess electrons, the total charge \( Q \) can be calculated as:
Magnetic Fields
A magnetic field is a region where a magnetic force can act on moving charges, such as electrons in the ball. This field is characterized by its direction and strength, measured in Teslas (T). In this problem, the magnetic field has a magnitude of 0.250 T, horizontally from east to west.
- Magnetic fields interact with charged particles, exerting a force perpendicular to both the velocity of the particle and the direction of the field.
- In this situation, the magnetic field affects the ball as it gains velocity moving vertically down the shaft and then enters a horizontal magnetic field.
Electromagnetism Concepts
Electromagnetism is the branch of physics that studies the interactions between electric charges and currents with magnetic and electric fields. One of the key relationships in electromagnetism is how magnetic forces are exerted on moving charges. The magnetic force \( F \) on a charged particle moving through a magnetic field is given by the equation \( F = qvB \sin(\theta) \), where:
- \( q \) is the charge.
- \( v \) is the velocity of the particle.
- \( B \) is the magnetic field strength.
- \( \theta \) is the angle between the velocity and the magnetic field direction.
- Since the motion is vertically downwards and the field is horizontal, \( \theta = 90^\circ \) ensuring that \( \sin(\theta) = 1 \).
Other exercises in this chapter
Problem 13
An open plastic soda bottle with an opening diameter of 2.5 \(\mathrm{cm}\) is placed on a table. A uniform \(1.75-\mathrm{T}\) magnetic field directed upward a
View solution Problem 14
A particle with charge \(6.40 \times 10^{-19} \mathrm{C}\) travels in a circular orbit with radius 4.68 \(\mathrm{mm}\) due to the force exerted on it by a magn
View solution Problem 20
(a) An 16 nucleus (charge \(+8 e )\) moving horizontally from west to east with a speed of 500 \(\mathrm{km} / \mathrm{s}\) experiences a magnetic force of 0.00
View solution Problem 21
A deuteron (the nucleus of an isotope of bydrogen) has a mass of \(3.34 \times 10^{-27} \mathrm{kg}\) and a charge of \(+e .\) The deuteron travels in a circula
View solution