Waves and optics pertaining to sinusoidal waves

In summary, the conversation discusses three graphs with the objective of finding the phase constant. One person is having trouble solving the problems and asks for help. The other person gives some hints and asks questions to guide the first person towards the correct solutions. They discuss the derivative of time and its role in determining the phase angle. Ultimately, the first person gains a better understanding of the problem and is able to solve it.
  • #1
jweie29nh
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0

Homework Statement


https://us-mg5.mail.yahoo.com/neo/launch?.rand=768lpb97vo87e#4636076903 The picture displayed shows three graphs and in each problem the objective is to find the phase constant. I'm having an issue attempting any form of strategy to solve these problems. Any help would be greatly appreciated thanks.

Homework Equations


For the first graph D(x=0,t=0)=asin(kx-wt+phase constant)
1=2sin(0-0+phase constant)
phase constant = 30 degrees

For the second graph
1=2sin(0-0+phase constant)
phase constant = 30 degrees

For the third graph
1=2sin((2pi*4)/4 - (2pi)(T/2)/4+phase constant)

Don't have an idea how to solve for the third graph[/B]

The Attempt at a Solution


1. For the first graph I answered 30 degrees
2. For the second graph I answered 30 degrees
 

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  • #2
Your answers would imply that the two pictures both represent ##D = 2 \sin(kx-\omega t + \pi/6)## and are therefore exactly the same.
Clearly, they are not. Perhaps the equation ##\sin\phi = 1/2## has another solution ?
 
  • #3
I agree there are two different solutions however I'm not sure which problem has the solution pi/6 and why it would be considered an answer over the other problem.
 
  • #4
Did you read the 'Note' ? (I have to ask, since in your 1 and 2 answers you do have the same ##\phi_0##)
 
  • #5
From another angle :): In the first picture, is D increasing or decreasing when you take a small step in time ?
 
  • #6
Yes I did read your note, and I just read your second one now. It seems much more clearer and I have a better understanding. So the first graph has a phase constant of pi/6 since d is increasing while in the second graph d is decreasing.
 
  • #7
So in that case the second graph would indicate the answer would be 5pi/6
 
  • #8
:)I didn't mean my note, but the note under the exercise!

Then: if you make a little time step in the first picture, does D really increase ?

Because, if I fill in x = 0, I get ##D = 2 \sin(-\omega t + \pi/6)## and what is the time derivative ##d\;D\over dt## at time zero for that ?
 
  • #9
The derivative of time for that equation would be D=-2wcos(−ωt+π/6) but what does this equation have to do with the problem?

I suppose time doesn't increase or decrease since it is following a pattern.
 
  • #10
I suppose time doesn't increase or decrease since it is following a pattern
Time is running. The picture is a snapshot at t=0. There is even a big fat arrow showing which way the wave is going.
The derivative of time for that equation would be D=-2wcos(−ωt+π/6) but what does this equation have to do with the problem?
So what is this derivative at t=0 ? Is it positive or negative ? This derivative has everything to do with the problem: to determine the phase angle, you have to know if the D is increasing or decreasing.

Look at it this way: If you are sitting on your surfboard at x=0 on t=0 and this huge wave moves as is indicated by the arrow, are you going up or down ?
 
  • #11
-pi/6 is the derivative at t=0, so d is decreasing. It is going down
 
  • #12
And in the second picture, same procedure ?
 
  • #13
I believe the same method is applicable but your guidance is widely accepted
 
  • #14
:) The idea is that you are now in a good position to handle the second picture by yourself ! And yes, the approach is the same.
You see that ##D(0,0) = 2 \sin\phi_0 = 1## which has two solutions (*). Which one is the right one, you decide by looking at the time derivative of D at x=0, t=0.

(*) Actually, it has infinitely many solutions, but only two are in the range ##[0,2\pi]##
 

Related to Waves and optics pertaining to sinusoidal waves

1. What is a sinusoidal wave?

A sinusoidal wave is a type of wave that has a repeating, oscillating pattern with a characteristic shape of a sine curve. It is a type of periodic wave, meaning it repeats at regular intervals, and it is commonly used to describe sound and light waves.

2. How are wavelength and frequency related in sinusoidal waves?

Wavelength and frequency are inversely related in sinusoidal waves. This means that as the wavelength increases, the frequency decreases, and vice versa. This relationship is described by the equation c = λν, where c is the speed of the wave, λ is the wavelength, and ν is the frequency.

3. What is the difference between transverse and longitudinal waves?

Transverse waves are waves in which the particles of the medium vibrate perpendicular to the direction of the wave propagation, while longitudinal waves are waves in which the particles vibrate parallel to the direction of propagation. Sound waves are examples of longitudinal waves, while light waves are examples of transverse waves.

4. How does the amplitude of a sinusoidal wave affect its energy?

The amplitude of a sinusoidal wave is directly proportional to its energy. This means that as the amplitude increases, the energy of the wave also increases. This relationship is described by the equation E ∝ A2, where E is the energy and A is the amplitude.

5. What is the principle of superposition in optics?

The principle of superposition in optics states that when two or more waves meet at a point in space, the resulting displacement at that point is equal to the sum of the individual displacements of each wave. This principle is used to explain the interference of light waves, where the overlapping of waves can result in constructive or destructive interference.

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