Find the range of ##k## for which ##\omega## is imaginary

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Homework Help Overview

The discussion revolves around finding the range of the wave number ##k## for which the oscillation frequency ##\omega## is imaginary, based on a given relation involving the function ##\epsilon(k, \omega)##. Participants explore the implications of certain mathematical inequalities and assumptions regarding the parameters involved.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants examine the relationship between ##\omega## and the parameters, questioning the conditions under which ##\omega## becomes imaginary. They discuss inequalities derived from assumptions about the parameters and the implications of these inequalities on the values of ##k##.

Discussion Status

There is an ongoing exploration of the mathematical relationships and assumptions. Some participants have identified potential ranges for ##k##, while others are questioning the validity of their assumptions and the implications of their findings. The discussion remains open with various interpretations being considered.

Contextual Notes

Participants assume that parameters such as ##\omega_p, k, v_0## are real, and they are navigating through the implications of this assumption on the derived inequalities. There is also a focus on the behavior of the function as it relates to the imaginary nature of ##\omega##.

JD_PM
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Homework Statement
Given the relation (treat ##k, \omega## as variables and ##v_0, \omega_p## as constants).


$$y^2=1+2\alpha^2 \pm(1+8\alpha^2)^{1/2}, \ \text{where} \ \alpha:= kv_0/\omega_p, \ y:= \sqrt{2}\omega/\omega_p$$



a) Find the range of wave numbers ##k## for which the oscillation frequency ##\omega## is imaginary



b) Find ##k_{max}## and ##\text{Im}(\omega_{max})##. Hint: sketch the solution for ##\text{Im}(\omega)##
Relevant Equations
N/A
Out of the given information I see no way of solving neither of the two sections.

So I did some reading and it turns out that the given relation is a solution of the following function (I won't prove it here)

$$\epsilon (k, \omega) = 1 - \frac 1 2 \left[ \frac{\omega_p^2}{(\omega-kv_0)^2} + \frac{\omega_p^2}{(\omega+kv_0)^2}\right] = 0$$

So I think that finding the range of wave numbers ##k## for which the oscillation frequency ##\omega## is imaginary on the ##\epsilon## function should be equivalent. I did some manipulations

$$\frac{\omega_p^2}{(\omega-kv_0)^2} + \frac{\omega_p^2}{(\omega+kv_0)^2} = 2 \Rightarrow \omega_p^2\left( \frac{\omega^2+2kv_0+k^2v_0^2+\omega^2-2kv_0+k^2v_0^2}{(\omega^2-k^2v_0^2)^2} \right) = 2$$

$$\frac{(\omega^2+k^2v_0^2)}{(\omega^2-k^2v_0^2)^2} = \frac{1}{\omega_p^2}$$

But got stuck in the above step...

I strongly think we better avoid using the function and focus on the given relation to answer the questions.

Might you please guide me through?

Thanks.
 
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If ##y^2 < 0##, then y will be imaginary, and since ## y = \sqrt 2 \frac \omega {\omega_p}##, its seems likely that ##\omega## will also be imaginary, but without knowing whether ##\omega_p## is real, I can't say for sure.

Assuming for the moment that y being imaginary implies that ##\omega## will be imaginary, I'll continue on. Assuming that ##\alpha## is real, ##y^2 < 0## when ##1 + 2\alpha^2 - \sqrt{1 + 8\alpha^2} < 0##; i.e., when ##1 + 2\alpha^2 < \sqrt{1 + 8\alpha^2}## . Solving this inequality gives you a range of values for ##\alpha##, and presumably you can find a range of values for k.
 
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Let's assume ##\omega_p, k, v_0## to be real.

$$(1 + 2\alpha^2)^2 < 1 + 8\alpha^2 \Rightarrow \alpha^2 + \alpha^4 < 2\alpha^2 \Rightarrow \alpha^2(\alpha^2 - 1) < 0$$

Hence ##\alpha^2 < 0## or ##\alpha^2 < 1##. We assumed ##\omega_p, k, v_0## to be real so, by definition, ##\alpha## is real. Then, we stick to ##\alpha^2 < 0##.

Assuming ##v_0 \neq 0, \omega_p \neq 0##

$$k^4 < 0$$

Mmm but I expected to get a shorter range, I think I made a mistake somewhere.
 
JD_PM said:
Hence ##\alpha^2 < 0## or ##\alpha^2 < 1##. We assumed ##\omega_p, k, v_0## to be real so, by definition, ##\alpha## is real. Then, we stick to ##\alpha^2 < 0##.
If ##\alpha## is real, then its square can never be negative. On the other hand, ##\alpha^2 < 1 \Rightarrow -1 < \alpha < 1##.
 
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Mark44 said:
If ##\alpha## is real, then its square can never be negative.
That was my naïve mistake indeed! Thanks.

Hence the ##k## range is given by

$$-\left| \frac{\omega_p}{v_0}\right| < k < \left| \frac{\omega_p}{v_0}\right|$$

If you agree, let's tackle the next section

JD_PM said:
b) Find ##k_{max}## and ##\text{Im}(\omega_{max})##. Hint: sketch the solution for ##\text{Im}(\omega)##
About the hint: do they want us to sketch the imaginary solution for the relation

$$y^2=1+2\alpha^2 \pm(1+8\alpha^2)^{1/2}, \ \text{where} \ \alpha:= kv_0/\omega_p, \ y:= \sqrt{2}\omega/\omega_p$$

?

That is

$$0 > y^2=1+2\alpha^2 - (1+8\alpha^2)^{1/2}$$

With ##\omega## in the vertical axis and ##k## in the horizontal axis.
 
JD_PM said:
Hence the k range is given by $$-\left| \frac{\omega_p}{v_0}\right| < k < \left| \frac{\omega_p}{v_0}\right|$$
Looks fine. Let me think about your other question...
 
Given that ##y = \frac{\sqrt 2}{\omega_p}\omega##, then
##\left(\frac{\sqrt 2}{\omega_p}\omega \right)^2 = 1 + 2\alpha^2 - \sqrt{1 + 8\alpha^2}##
Solve for ##\omega## and then plug in some well-chosen values for ##\alpha##. That's what I would do. Note that due to the range of values for k, the graph should lie between the left- and right bounds for k shown above.
 
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Mark44 said:
Given that ##y = \frac{\sqrt 2}{\omega_p}\omega##, then
##\left(\frac{\sqrt 2}{\omega_p}\omega \right)^2 = 1 + 2\alpha^2 - \sqrt{1 + 8\alpha^2}##
Solve for ##\omega## and then plug in some well-chosen values for ##\alpha##.
We have

$$\omega = \pm \sqrt{\frac{\omega_p^2}{2} + \omega_p^2 \alpha^2 - \frac{\omega_p^2}{2} \sqrt{1 + 8\alpha^2} }$$

We know that ##-1 < \alpha < 1##, so I plotted the ##\omega## solution (y axis ##\omega##, x-axis ##\alpha##; I set ##\omega_p:= 1## for simplicity)

aiii.png
Mark44 said:
Note that due to the range of values for k, the graph should lie between the left- and right bounds for k shown above.

Mmm I am doing something wrong, because within the left- and right bounds for ##k## I get nothing...

I thought of plugging special values for ##\alpha##, such as ##\alpha = 1##, but I get the trivial solution ##\omega = 0## ofc...
 
Mark44 said:
##\left(\frac{\sqrt 2}{\omega_p}\omega \right)^2 = 1 + 2\alpha^2 - \sqrt{1 + 8\alpha^2}##
It's probably better to solve for ##\omega^2##, and plot ##\omega^2## (vertical axis) vs. ##alpha## (horizontal axis). Remember my assumption that ##\omega## would be imaginary.

Here are some values I got in Excel, with ##\alpha## in the first column, and ##\omega^2## in the second column. I don't know the value for ##\omega_p##, so I just used 1, which seems to be what you did, as well.


-0.9​
-0.05748​
-0.8​
-0.09693​
-0.7​
-0.11905​
-0.6​
-0.12489​
-0.5​
-0.11603​
-0.4​
-0.09498​
-0.3​
-0.06574​
-0.2​
-0.03446​
-0.1​
-0.00962​
-1.4E-16​
0​
0.1​
-0.00962​
0.2​
-0.03446​
0.3​
-0.06574​
 
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  • #10
Mark44 said:
It's probably better to solve for ##\omega^2##, and plot ##\omega^2## (vertical axis) vs. ##alpha## (horizontal axis). Remember my assumption that ##\omega## would be imaginary.

.This is what I get for the ##\omega^2## (vertical axis) vs. ##alpha## (horizontal axis) plot (with ##\omega_p:= 1##)

aiii.png


However, the hyperbolic behavior of the plot does not match your excel data...

Given that we are interested in plotting ##\text{Im}(\omega)## to eventually find ##k_{max}## and ##\text{Im}(\omega_{max})##, wouldn't be best to plot ##\omega## instead of ##\omega^2##? I would say that if we were to plot the former then ##\text{Im}(\omega)## would simply correspond to the ##-1 < \alpha < 1## range. Then, to find ##\text{Im}(\omega_{max})## we would just have to look at the maximum value of ##\omega## in that range and ##k_{max}## would be equivalent to find ##\alpha_{max}## (by definition of ##\alpha##).
 
  • #11
JD_PM said:
Hence ##\alpha^2 < 0## or ##\alpha^2 < 1##.
Which I explained by saying that the first inequality couldn't occur for any real ##\alpha##, and the second one meant that ##-1 < \alpha < 1##.

JD_PM said:
However, the hyperbolic behavior of the plot does not match your excel data..
Sure it does. In the spreadsheet I was interested only in values of ##\alpha## in the interval (-1, 1). For these values, the corresponding values of ##\omega^2## are negative, hence the values of ##\omega## are imaginary. Think back to the title you chose for this thread.
 
  • #12
Do you see the following plot OK? (with the axis as mentioned)
JD_PM said:
.This is what I get for the ##\omega^2## (vertical axis) vs. ##alpha## (horizontal axis) plot (with ##\omega_p:= 1##)

View attachment 295082

Mark44 said:
Sure it does. In the spreadsheet I was interested only in values of ##\alpha## in the interval (-1, 1). For these values, the corresponding values of ##\omega^2## are negative, hence the values of ##\omega## are imaginary. Think back to the title you chose for this thread.

I am thinking about this.
 
  • #13
JD_PM said:
Do you see the following plot OK? (with the axis as mentioned)
Yes, I saw the plot in that post. The part between the two parts of the hyperbola is precisely the part where ##\omega## is imaginary, which is what you asked about at the start of this thread.
 
  • #14
JD_PM said:
Do you see the following plot OK? (with the axis as mentioned)

I am thinking about this.
The spreadsheet values that @Mark44 posted are for ##\omega^2## versus ##\alpha##, whereas it appears that your graphing package takes the square root of the values it calculates for ##\omega^2## and plots that versus ##\alpha##.
 
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  • #15
Hey guys, sorry for the late reply. After some thoughts and discussion with a smart colleague we got an answer! :biggrin:

The plots are not required to solve the exercise, are just suggested. Let's try to avoid them for now.

JD_PM said:
b) Find ##k_{max}## and ##\text{Im}(\omega_{max})##. Hint: sketch the solution for ##\text{Im}(\omega)##

To find ##k_{max}## we can simply take ##\frac{d y}{d \alpha} = 0##. This leads to ##\alpha_{max} \pm \frac{2 \alpha_{max}}{\sqrt{1 + 8 \alpha_{max}^2}} = 0 \Rightarrow \alpha_{max} = \frac{\sqrt{6}}{4}##. We have defined ##\alpha:= kv_0/\omega_p##, so it follows that ##k_{max} = \frac{\sqrt{6}}{4} \frac{\omega_p}{v_0}##

Let's find ##\text{Im}(\omega_{max})##. We already know that ##\alpha_{max} = \frac{\sqrt{6}}{4}##. We have defined ##y:= \sqrt{2}\omega/\omega_p##. Hence plugging ##\alpha_{max}## into ##y##

$$\begin{align*}
\text{Im}(\omega_{max}) &= \pm \frac{\omega_p}{\sqrt{2}}\sqrt{1 + 2\alpha_{max}^2 \pm \sqrt{1 + 8\alpha_{max}^2}} \\
&= \pm \frac{\omega_p}{\sqrt{2}} \sqrt{1 + \frac 3 4 \pm 2} \\
&= \pm \frac{\omega_p}{2} \sqrt{\frac{15}{2}}
\end{align*}$$

Where I have used the fact that the imaginary part of a complex number is real.

Let me know your thoughts on the solution if you wish :smile:
 
  • #16
JD_PM said:
Hey guys, sorry for the late reply. After some thoughts and discussion with a smart colleague we got an answer! :biggrin:

The plots are not required to solve the exercise, are just suggested. Let's try to avoid them for now.
To find ##k_{max}## we can simply take ##\frac{d y}{d \alpha} = 0##. This leads to ##\alpha_{max} \pm \frac{2 \alpha_{max}}{\sqrt{1 + 8 \alpha_{max}^2}} = 0 \Rightarrow \alpha_{max} = \frac{\sqrt{6}}{4}##. We have defined ##\alpha:= kv_0/\omega_p##, so it follows that ##k_{max} = \frac{\sqrt{6}}{4} \frac{\omega_p}{v_0}##

Let's find ##\text{Im}(\omega_{max})##. We already know that ##\alpha_{max} = \frac{\sqrt{6}}{4}##. We have defined ##y:= \sqrt{2}\omega/\omega_p##. Hence plugging ##\alpha_{max}## into ##y##

$$\begin{align*}
\text{Im}(\omega_{max}) &= \pm \frac{\omega_p}{\sqrt{2}}\sqrt{1 + 2\alpha_{max}^2 \pm \sqrt{1 + 8\alpha_{max}^2}} \\
&= \pm \frac{\omega_p}{\sqrt{2}} \sqrt{1 + \frac 3 4 \pm 2} \\
&= \pm \frac{\omega_p}{2} \sqrt{\frac{15}{2}}
\end{align*}$$

Where I have used the fact that the imaginary part of a complex number is real.

Let me know your thoughts on the solution if you wish :smile:
Not quite right.

Remember, ##y##, and thus ##\omega##, is imaginary only when

##1 + 2\alpha_{max}^2 \pm \sqrt{1 + 8\alpha_{max}^2} < 0 ##

That happens only for the minus, not the plus, of the "##\pm##" and if ##0<\alpha^2<1##.

Added in Edit 40 minutes later:

I think you will also find that ##\dfrac{d y}{d \alpha} = 0## only for minus, not for the plus.
... except, of course, at ##\alpha =0##.
 
Last edited:
  • #17
In particular, notice that ##\sqrt{1 + \dfrac 3 4 + 2} = \sqrt{\dfrac{15}{2}}## is a real number,

whereas ##\sqrt{1 + \dfrac 3 4 - 2} = \sqrt{\dfrac{-1}{4}} = \dfrac{1}{2} i \ ## is imaginary.
 
Last edited:
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