Kinetic Energy in B field (is it really conserved)

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Discussion Overview

The discussion centers around the conservation of kinetic energy in the context of a charged particle moving in a magnetic field. Participants explore the implications of magnetic forces on the velocity and kinetic energy of an electron, questioning whether the magnetic force can change the kinetic energy despite being perpendicular to the velocity vector.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • Some participants reference MIT notes stating that magnetic force does not change the speed of a charged particle, leading to questions about how this aligns with the concept of acceleration and changes in velocity.
  • One participant argues that while the magnetic force changes the direction of the velocity, it does not change its magnitude, thus suggesting that kinetic energy remains constant.
  • Another participant presents a mathematical argument showing that the initial and final speeds of the particle, considering the z-component of velocity, appear to contradict the conservation of kinetic energy.
  • Some participants clarify that as the z-component of velocity increases, the x and/or y components must decrease to keep the overall speed constant, using the analogy of a ball on a string to illustrate this point.
  • There is a discussion about the representation of variables used in the mathematical explanations, with participants seeking clarification on notation.

Areas of Agreement / Disagreement

Participants express differing views on whether the magnetic force can change the kinetic energy of a charged particle. Some assert that kinetic energy is conserved, while others challenge this notion, leading to an unresolved debate.

Contextual Notes

The discussion involves assumptions about the definitions of speed and kinetic energy, and the implications of magnetic forces on motion. There are unresolved mathematical steps regarding the integration of acceleration and its effects on velocity components.

Who May Find This Useful

Readers interested in the dynamics of charged particles in magnetic fields, as well as those exploring the concepts of kinetic energy and force interactions in physics.

hms.tech
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Here is a quote from one of the MIT notes on magnetism :

"Note that F(magnetic force) is perpendicular to v and B , and cannot change the particle’s speed v (and thus the kinetic energy). In other words, magnetic force cannot speed up or slow down a charged particle. "

How is this possible, it kind of conflicts with the idea of acceleration and "change" in velocity.

lets say the velocity of an electron is v in the direction of increasing x axis, while the direction of the B field is along the positive y axis. A force will act on the electron directed towards the negative z axis.

The initial velocity was in the x-y plane only but after the force acts on the charge, the "z" component of its velocity changes.

Would this not change the total Kinetic Energy possessed by the electron?
Clearly the velocity is not the same as before !
Thus the magnetic force HAS changed the velocity.

Can anyone help clarify this ?
 
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hms.tech said:
Here is a quote from one of the MIT notes on magnetism :

"Note that F(magnetic force) is perpendicular to v and B , and cannot change the particle’s speed v (and thus the kinetic energy). In other words, magnetic force cannot speed up or slow down a charged particle. "

How is this possible, it kind of conflicts with the idea of acceleration and "change" in velocity.

lets say the velocity of an electron is v in the direction of increasing x axis, while the direction of the B field is along the positive y axis. A force will act on the electron directed towards the negative z axis.

The initial velocity was in the x-y plane only but after the force acts on the charge, the "z" component of its velocity changes.

Would this not change the total Kinetic Energy possessed by the electron?
Clearly the velocity is not the same as before !
Thus the magnetic force HAS changed the velocity.

Can anyone help clarify this ?

Kinetic energy (K=\frac{1}{2}mv^2 non-relativistically) depends on the speed of the particle. the direction of the velocity can change, but its magnitude, the speed of the particle cannot.
 
gabbagabbahey said:
Kinetic energy (K=\frac{1}{2}mv^2 non-relativistically) depends on the speed of the particle. the direction of the velocity can change, but its magnitude, the speed of the particle cannot.

Speed, v , initially = √(x^2+y^2)

speed , v , final (after magnetic force acts on the electron) = √(x^2+y^2+z^2)

Note that the x and y components of velocity remain constant thus the only difference between the final speed and the initial speed is the "z" component of velocity.

As you said the the kinetic energy is same then :

x^2+y^2 = x^2 + y^2 + z^2

thus z=0

Which is clearly another contradiction with the statement that the kinetic energy is conserved.
 
hms.tech said:
Note that the x and y components of velocity remain constant thus the only difference between the final speed and the initial speed is the "z" component of velocity.

No. As the z component increases, the x and/or y components decrease in a way that exactly compensates to keep the magnitude of the velocity constant.

It may help to thing about a simpler example. Consider say, a ball on a string being whirled round in a circle at constant speed. Here the string's force always points perpendicular to the ball's current velocity, with the result that the ball's speed is constant.
 
hms.tech said:
Speed, v , initially = √(x^2+y^2)

speed , v , final (after magnetic force acts on the electron) = √(x^2+y^2+z^2)

Note that the x and y components of velocity remain constant thus the only difference between the final speed and the initial speed is the "z" component of velocity.

No, initially \mathbf{v}(t=0)=v_0\mathbf{e}_x and the force is \mathbf{F}(t=0)=v_0|\mathbf{B}|\mathbf{e}_z.

An infinitesmal time later, the velocity is \mathbf{v}(t=0+dt) = v_0\mathbf{e}_x +\frac{v_0|\mathbf{B}|}{m}dt\mathbf{e}_z and the force is \mathbf{F}(t=0 +dt)=v_0|\mathbf{B}|\mathbf{e}_z - \frac{v_0|\mathbf{B}|^2}{m}dt\mathbf{e}_y (Notice the force has a negative y-component).

But we don't measure at infinitesimal time intervals, only at finite time intervals. To do that, we integrate the acceleration:

\mathbf{v}(t) = \int_0^{t} \frac{\mathbf{F}(t')}{m} dt' = \int_0^{t} \frac{q}{m}(\mathbf{v}(t') \times \mathbf{B}(t'))dt'

The easiest way to see that the speed is constant is to look at v^2 = \mathbf{v} \cdot \mathbf{v} (if the square of the speed is constant, then so is the speed):

\frac{d}{dt}v^2= \frac{d}{dt}\left[ \mathbf{v} \cdot \mathbf{v}\right] = 2\mathbf{v} \cdot \frac{d\mathbf{v}}{dt} = 2\mathbf{v} \cdot \left(\frac{q}{m} \mathbf{v} \times \mathbf{B} \right) = \frac{2q}{m}\mathbf{B} \cdot (\mathbf{v} \times \mathbf{v}) = 0

where the second last step comes from the triple product identity \mathbf{A} \cdot ( \mathbf{B} \times \mathbf{C}) = \mathbf{B} \cdot ( \mathbf{C} \times \mathbf{A}) = \mathbf{C} \cdot ( \mathbf{A} \times \mathbf{B}).

Evidently, v^2, and hence v and K, is constant.
 
I understood the method of Kinetic energy but i didn't really catch the first part of your post no.5

Would you please explain/define what the variables represent .
 
I used v_0 to represent the initial speed of the particle, \mathbf{v}(t) to represent the velocity vector of the particle at time t, \mathbf{B} to represent the external magnetic field, and \mathbf{F} to represent the force on the particle.
 
Alright, but u missed one which is troubling me

e (subscript x or y or z)
 
gabbagabbahey said:
No, initially \mathbf{v}(t=0)=v_0\mathbf{e}_x

what does e(x) represent
 
  • #10
hms.tech said:
what does e(x) represent

\mathbf{e}_x is just one of many common ways to write the unit vector in the positive x-direction. Other common ways to write it include \mathbf{i}, \mathbf{\hat{x}}, \mathbf{\hat{e}}_1, and \hat{i} .
 

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