I got bored and did something with the dielectric constant

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Eclair_de_XII
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Homework Statement


I want to prove or disprove that the dielectric constant ##K## is the projection of ##\vec E_0## onto ##\vec E## using linear algebra.

Homework Equations


##\vec E = \frac{\vec E_0}{K}##

The Attempt at a Solution


##(\vec E)⋅\vec E = (\vec E)⋅\frac{\vec E_0}{K}##
##K(\vec E)⋅\vec E = (\vec E)⋅\vec E_0##
##K \left\| \vec E \right\|^2=\vec E⋅\vec E_0##
##K=\frac{\vec E⋅\vec E_0}{\left\| \vec E \right\|^2}=proj_\vec E \vec E_0##

Since ##\left\|\vec E_0\right\| > \left\|\vec E\right\|##, ##K>1##. I'm trying to interpret ##K## as the projection of ##\vec E_0## onto ##\vec E## because I was kind of bored one day in physics lecture. I think I remember that ##proj_{\vec u} \vec v ≤ |1|## for some vectors ##\vec u## and ##\vec v##, which contradicts what I'm saying. Should I just go with ##K=\frac{C}{C_0}## since it's much simpler? I think I'm reading too much into this...
 
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Eclair_de_XII said:
I think I'm reading too much into this...
I think so too...
Eclair_de_XII said:
##\vec E = \frac{\vec E_0}{K}##
First, what is ##E_{0}## here? I think what you meant to write is ##\mathbf{D}=K\epsilon_{0}\mathbf{E}##. Either way the projection of ##\mathbf{E}## and ##\mathbf{D}## or ##\mathbf{E_{0}}## is just
$$\text{proj}\frac{\mathbf{D}\cdot\mathbf{E}}{|\mathbf{E}|^{2}}=\frac{K\epsilon_{0} E^{2}}{E^{2}}=K\epsilon_{0}$$
 
NFuller said:
Either way the projection of ##\mathbf{E}## and ##\mathbf{D}## or ##\mathbf{E_{0}}## is just

##\text{proj}\frac{\mathbf{D}\cdot\mathbf{E}}{|\mathbf{E}|^{2}}=\frac{K\epsilon_{0} E^{2}}{E^{2}}=K\epsilon_{0}##

Forgive me if I'm remembering something wrong but aren't projections usually less than or equal to 1 in magnitude? Should it not be: ##\text{proj}\frac{\mathbf{E}\cdot\mathbf{D}}{|\mathbf{E}| |\mathbf{D}|}##? Of course, though, it's meaningless anyway, and does not represent the dielectric constant.
 
Eclair_de_XII said:
aren't projections usually less than or equal to 1 in magnitude?
No, but my notation is messed up. It should be
$$\text{proj}_{\mathbf{E}}\mathbf{D}=\frac{\mathbf{D}\cdot\mathbf{E}}{|\mathbf{E}|^{2}}\mathbf{E}$$