Ion moving through electric potential difference and magnetic field

In summary, ions moving through an electric potential difference experience a force that accelerates them in the direction of the electric field, while their motion in a magnetic field results in a force perpendicular to both their velocity and the magnetic field direction. This interaction causes the ions to follow a curved path, with the trajectory determined by the strengths of the electric and magnetic fields. The overall motion is a combination of linear acceleration due to the electric field and circular motion due to the magnetic field, influencing their behavior in various physical and technological applications.
  • #1
zenterix
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Homework Statement
A positively charged ion with charge ##q## and mass ##m##, initially at rest inside the source, is accelerated across a gap by an electric potential difference with magnitude ##\Delta v## . The ion enters a region of uniform magnetic field ##B_1## pointing into the page of the figure below and follows a semi-circular trajectory of radius ##R_1##. The ion is again accelerated across the gap, increasing its speed, by an electric potential difference that has the opposite sign but has the same magnitude ##|\Delta v|##. The ion then enters a region of uniform magnetic field ##B_2## pointing into the page of the figure below and follows a semi-circular trajectory of radius ##R_2##.
Relevant Equations
a) What is the ratio ##B_2/B_1##?

b) What is the ratio ##v_2/v_1##?
My question is about item (b).

1712214908771.png


For item (a) we have uniform circular motion in the regions with uniform magnetic field.

$$\vec{F}_{B_1}=qv\hat{\theta}_1\times B_1(-\hat{k})=-qv_1B_1\hat{r}_1=-mR_1\theta'^2\hat{r}_1\tag{1}$$

$$B_1=\frac{mv_1}{R_1q}\tag{2}$$

A similar calculation for the bottom portion of the trajectory gives

$$B_2=\frac{mv_2}{R_2q}\tag{3}$$

Thus,

$$\frac{B_2}{B_1}=\frac{R_1v_2}{R_2v_1}\tag{4}$$

As for item (b), I don't understand the following.

The problem statement says that the ion is accelerated in both of the gaps. It also says that the electric potential difference in the gap on the left is the negative of the electric potential difference of the gap on the right.

How then can a positively charged ion accelerate across both gaps?

Let's assume that the potential at the "source" is higher than on the top part of the gap above it.

$$q\Delta v=-W=-\Delta K_e=-\frac{mv_1^2}{2}\tag{5}$$

$$v_1=\sqrt{-\frac{2q}\Delta V}{m}}\tag{6}$$

Note that ##\Delta v<0##.

Now consider the gap on the left side.

The speed of the ion is the same ##v_1## when it enters the gap, but now it is traversing from a lower to a higher potential as a positive charge. Shouldn't it slow down (to zero speed)?
 
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  • #2
Note that the problem states that the speed increases during both acceleration stages and the potential difference in the drawing is a magnitude. What does that indicate to you?
 
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  • #3
zenterix said:
$$\frac{B_2}{B_1}=\frac{R_1v_2}{R_2v_1}\tag{4}$$
I don't think the velocities should figure in the answer. Can you see how to get rid of those?
zenterix said:
It also says that the electric potential difference in the gap on the left is the negative of the electric potential difference of the gap on the right.
It must mean the p.d. is in the opposite direction relative to the diagram, so in the same direction relative to the path.
 
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  • #4
zenterix said:
$$v_1=\sqrt{-\frac{2q\Delta V} {m}}\tag{6}$$
Note that ##\Delta v<0##.
Note that the use of ##v## for both speed and voltage is error-prone ! So is the use of ##\Delta v## and ##\Delta V## for one and the same variable

zenterix said:
the speed of the ion is the same v1 when it enters the gap, but now it is traversing from a lower to a higher potential as a positive charge. Shouldn't it slow down (to zero speed)?
That's not the intention:
zenterix said:
The ion is again accelerated across the gap, increasing its speed, by an electric potential difference that has the opposite sign but has the same magnitude ##|\Delta v|##.
but I grant you the wording is confusing. I think they have a ##\Delta V \equiv V_{top}-V_{bot} ## definition.

The cyclotron principle is explained here

##\ ##
 
  • #5
haruspex said:
I don't think the velocities should figure in the answer. Can you see how to get rid of those?
Why don't you think the velocities should be there?

This problem has an automatic grading system. The expression for ##\frac{B_2}{B_1}## checks out.

There is an item (c) to this problem that I did not show. It is to suppose that ##R_2=2R_1## and compute what ##\frac{B_2}{B_1}## is.

Since ##\frac{B_2}{B_1}## has a ##\frac{v_2}{v_1}## term in it, which in item (b) comes out to be ##\sqrt{2}##, we can sub this in to get ##\frac{B_2}{B_1}=\frac{\sqrt{2}}{2}##.
 
  • #6
BvU said:
Note that the use of v for both speed and voltage is error-prone ! So is the use of Δv and ΔV for one and the same variable
I am using ##v## for speed and ##\Delta V## for potential difference. The use of ##\Delta v## in the OP is a typo.
 
  • #7
zenterix said:
Since ##\frac{B_2}{B_1}## has a ##\frac{v_2}{v_1}## term in it, which in item (b) comes out to be ##\sqrt{2}##, we can sub this in to get ##\frac{B_2}{B_1}=\frac{\sqrt{2}}{2}##.
That's why I thought the velocities should not appear in the first answer.
 
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  • #8
The moving charges have intrinsic magnetic loop.
From David J. Griffiths, Introduction to Electrodynamics, Fourth Edition}, page 462, ISBN-13: 978-0-321-85656-2, 2013.

1716318908398.png


The moving charge follows curved trajectory and therefore the intrinsic magnetic loop rotates.
If the intrinsic magnetic loop rotates then the conservation of angular momentum means the plates/device are being torqued in the opposite direction.
Is this correct conclusion?
 
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  • #9
One cannot argue against Newton's third law.
 

FAQ: Ion moving through electric potential difference and magnetic field

1. What happens to an ion when it moves through an electric potential difference?

When an ion moves through an electric potential difference, it experiences a force due to the electric field created by the potential difference. This force accelerates the ion, causing it to gain kinetic energy proportional to the voltage it moves through. The direction of the force depends on the charge of the ion; positive ions are attracted to the negative electrode, while negative ions are attracted to the positive electrode.

2. How does a magnetic field affect the motion of an ion moving through an electric potential difference?

A magnetic field exerts a force on a moving charged particle, such as an ion, known as the Lorentz force. This force is perpendicular to both the velocity of the ion and the direction of the magnetic field. As a result, the ion's path is curved, and its trajectory becomes circular or helical depending on the initial conditions. The combination of the electric and magnetic fields can lead to complex motion, such as the phenomenon known as the Hall effect.

3. What is the relationship between the speed of an ion and the electric potential difference it travels through?

The speed of an ion is directly related to the electric potential difference it travels through. The kinetic energy gained by the ion as it moves through the potential difference is equal to the work done on it by the electric field, which can be expressed as KE = qV, where KE is the kinetic energy, q is the charge of the ion, and V is the potential difference. Therefore, a higher potential difference results in a higher speed of the ion, assuming no other forces act on it.

4. Can an ion be influenced by both electric and magnetic fields simultaneously?

Yes, an ion can be influenced by both electric and magnetic fields simultaneously. When an ion moves through these fields, the electric field accelerates it, while the magnetic field alters its trajectory. The resulting motion is governed by the combined effects of the electric and magnetic forces, leading to complex paths, such as circular or spiral trajectories. This is commonly observed in devices like mass spectrometers and cyclotrons.

5. What applications utilize the principles of ions moving through electric potential differences and magnetic fields?

Several applications utilize the principles of ions moving through electric potential differences and magnetic fields, including mass spectrometry, which separates ions based on their mass-to-charge ratio; ion propulsion systems in spacecraft; and plasma confinement in fusion reactors. Additionally, these principles are applied in various analytical techniques and in the development of particle accelerators for research in particle physics.

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