Calculating Refraction Angles of Light Through a Prism | Snell's Law | n=1.46

  • Thread starter Thread starter cmilho10
  • Start date Start date
  • Tags Tags
    Light Prism
cmilho10
Messages
20
Reaction score
0
Light of wavelength 700 nm is incident on the face of a fused quartz prism at an angle of 80.0° (with respect to the normal to the surface). The apex angle of the prism is 60.0°.

Use the value of n from Figure 35.20, to calculate the following angles.
(a) the angle of refraction at the first surface
(b) the angle of incidence at the second surface
(c) the angle of refraction at the second surface
(d) the angle between the incident and emerging rays

n=1.46

I used snell's law in order to find (a) which is 42 degrees, but when i try to do the geometry for the other parts it says my answers are wrong (i got 18 degrees for part b). It is hard to explain without drawing a picture exactly where i went wrong, but if anybody has any suggestions i would appreciate it.
 
Physics news on Phys.org
cmilho10 said:
Light of wavelength 700 nm is incident on the face of a fused quartz prism at an angle of 80.0° (with respect to the normal to the surface). The apex angle of the prism is 60.0°.
Use the value of n from Figure 35.20, to calculate the following angles.
(a) the angle of refraction at the first surface
(b) the angle of incidence at the second surface
(c) the angle of refraction at the second surface
(d) the angle between the incident and emerging rays
n=1.46
I used snell's law in order to find (a) which is 42 degrees, but when i try to do the geometry for the other parts it says my answers are wrong (i got 18 degrees for part b).

I have to say I don't find any error. Using Snell's law you have indeed 42.4 degrees for (a), and if the apex angle is 60 degrees, this means that you have 17.6 degrees (60 - 42.4) on the other side for (b) wrt to the other normal...
 
##|\Psi|^2=\frac{1}{\sqrt{\pi b^2}}\exp(\frac{-(x-x_0)^2}{b^2}).## ##\braket{x}=\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dx\,x\exp(-\frac{(x-x_0)^2}{b^2}).## ##y=x-x_0 \quad x=y+x_0 \quad dy=dx.## The boundaries remain infinite, I believe. ##\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dy(y+x_0)\exp(\frac{-y^2}{b^2}).## ##\frac{2}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,y\exp(\frac{-y^2}{b^2})+\frac{2x_0}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,\exp(-\frac{y^2}{b^2}).## I then resolved the two...
Hello everyone, I’m considering a point charge q that oscillates harmonically about the origin along the z-axis, e.g. $$z_{q}(t)= A\sin(wt)$$ In a strongly simplified / quasi-instantaneous approximation I ignore retardation and take the electric field at the position ##r=(x,y,z)## simply to be the “Coulomb field at the charge’s instantaneous position”: $$E(r,t)=\frac{q}{4\pi\varepsilon_{0}}\frac{r-r_{q}(t)}{||r-r_{q}(t)||^{3}}$$ with $$r_{q}(t)=(0,0,z_{q}(t))$$ (I’m aware this isn’t...
Hi, I had an exam and I completely messed up a problem. Especially one part which was necessary for the rest of the problem. Basically, I have a wormhole metric: $$(ds)^2 = -(dt)^2 + (dr)^2 + (r^2 + b^2)( (d\theta)^2 + sin^2 \theta (d\phi)^2 )$$ Where ##b=1## with an orbit only in the equatorial plane. We also know from the question that the orbit must satisfy this relationship: $$\varepsilon = \frac{1}{2} (\frac{dr}{d\tau})^2 + V_{eff}(r)$$ Ultimately, I was tasked to find the initial...

Similar threads

Replies
1
Views
2K
Replies
9
Views
2K
Replies
207
Views
12K
Replies
1
Views
1K
Replies
2
Views
2K
Replies
1
Views
2K
Replies
4
Views
3K
Replies
2
Views
2K
Back
Top