MHB Calculating Travel Time for Light in an Optical Fiber

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SUMMARY

The discussion focuses on calculating the travel time of light in an optical fiber with a central plastic core of index of refraction n1 = 1.58 and a surrounding sheath of index n2 = 1.53. The key formulas used include t = n1 * L / c for direct travel along the fiber's axis and t = n1^2 * L / n2 * c for light traveling at critical angles. The difference in travel times between these two paths is calculated as Δt = t zigzag - t direct. The fiber length is specified as 300 m, leading to a clear understanding of how light dispersion affects information transmission.

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Figure 35-57 shows an optical
fiber in which a central plastic
core of index of refraction n1 
1.58 is surrounded by a plastic
sheath of index of refraction n2 
1.53. Light can travel along different
paths within the central
core, leading to different travel times through the fiber.This causes an
initially short pulse of light to spread as it travels along the fiber,
resulting in information loss. Consider light that travels directly along
the central axis of the fiber and light that is repeatedly reflected at the
critical angle along the core–sheath interface, reflecting from side to
side as it travels down the central core. If the fiber length is 300 m,
what is the difference in the travel times along these two routes?

I know that I need to use t=L/v1=n1*L/c which becomes t=L/v1*cos(theta)=n1*L/(c*sqrt(1-(sin(theta)/n1)^2), but now I am stuck trying to figure the time for the question.
 
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chrisliu1234 said:
Figure 35-57 shows an optical
fiber in which a central plastic
core of index of refraction n1 
1.58 is surrounded by a plastic
sheath of index of refraction n2 
1.53. Light can travel along different
paths within the central
core, leading to different travel times through the fiber.This causes an
initially short pulse of light to spread as it travels along the fiber,
resulting in information loss. Consider light that travels directly along
the central axis of the fiber and light that is repeatedly reflected at the
critical angle along the core–sheath interface, reflecting from side to
side as it travels down the central core. If the fiber length is 300 m,
what is the difference in the travel times along these two routes?

I know that I need to use t=L/v1=n1*L/c which becomes t=L/v1*cos(theta)=n1*L/(c*sqrt(1-(sin(theta)/n1)^2), but now I am stuck trying to figure the time for the question.

Hi chrisliu1234! Welcome to MHB! (Smile)

Let's start with $t=\frac{n_1 L}{c}$ for the time to travel along the central axis.
Did you find the corresponding time?

As for the light traveling at critical angles, you're supposed to deduce a formula without theta.
Is that perhaps where your problem is? (Wondering)
 
I like Serena said:
Hi chrisliu1234! Welcome to MHB! (Smile)

Let's start with $t=\frac{n_1 L}{c}$ for the time to travel along the central axis.
Did you find the corresponding time?

As for the light traveling at critical angles, you're supposed to deduce a formula without theta.
Is that perhaps where your problem is? (Wondering)

So does change in time = t zigzag - t direct = n1^2*L/n2*c - n1*L/c?
 
chrisliu1234 said:
So does change in time = t zigzag - t direct = n1^2*L/n2*c - n1*L/c?

That looks right yes. (Nod)
 

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