How Do You Calculate the Angles of Nodal Lines in a Ripple Tank Experiment?

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Homework Help Overview

The problem involves calculating the angles of nodal lines in a ripple tank experiment, where two point sources create an interference pattern. The given parameters include the distance between the sources, the frequency of the waves, and the wavelength.

Discussion Character

  • Exploratory, Assumption checking

Approaches and Questions Raised

  • Participants discuss the use of the equation dsin(theta) = (n-1/2)lambda to find the angles, with some expressing uncertainty about how to handle the nodal line value 'n'. There is a suggestion to leave 'n' in the equation and express theta as a function of 'n'.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the problem. Some have provided guidance on how to manipulate the equation, while others are questioning the necessity of knowing 'n' to proceed with the calculations.

Contextual Notes

Participants note that certain variables, such as 'x' and 'L', are not provided in the problem, leading to discussions about their relevance in deriving a solution. There is also a recognition that the nodal line number 'n' is not specified, complicating the ability to calculate specific angles.

GoJays32
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Ok, the following problem I've tried several times to solve, although I suspect that somewhere along the line I'm just approaching what appears to be a simple problem in the wrong way:

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A two-point source operates at a frequency of 1.0 Hz to produce an interference patter in a ripple tank. The sources are 2.5 cm apart and the wavelength of the waves is 1.2 cm.

Calculate the angles at which the nodal lines in the pattern are located far from the sources. (Assume the angles are measured from the central line of the pattern.)
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So here's what is given:

d = 2.5 cm
f = 1.0 Hz
lambda = 1.2 cm

Some formulas/expressions to work with:

1. v = f(lambda)

'v' is the speed of the wavelength

2. (d)sin(theta) = (n-1/2)lambda

Where 'theta' is the angle of the nth nodal line, 'lambda' is the wavelength, and 'd' is the distance from the sources. 3. lambda = (d)sin(theta)/(n-1/2)

This is just a variation of (1). 4. theta + alpha = 90 degrees

*EDIT*

5. theta prime + alpha = 90 degrees

theta prime = theta

sin(theta prime) = x/L, sin(theta) = (n-1/2)(lambda/d)

6. Since sin(theta prime) = sin(theta)

x/L = (n-1/2)(lambda/d), so therefore

lambda = (x/L)[d/(n-1/2)]'x' is the perpendicular distance from the right bisector to the point P on the nodal line
'L' is the distance from the midpoint between the two sources to the point P

Although I think it's safe to say that the 'x' and 'L' variables are irrelevant in this case because they aren't given, and are not in the formula used to solve for angles. I suppose that the same goes for the 'n' nodal number, since it's not given, I need to derive an equation which only involves the variables given, as well as sin(theta), so that I can solve for theta, and, in addition, alpha.

If there any helpful suggestions on how to approach this problem, it would be much appreciated.
 
Last edited:
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You have the equation: dsin\theta = (n-\frac{1}{2})\lambda

Just solve for \theta and plug in your values for d and \lambda
 
learningphysics said:
You have the equation: dsin\theta = (n-\frac{1}{2})\lambda

Just solve for \theta and plug in your values for d and \lambda
I would need to have the nodal line value 'n' in order solve for \theta, but I don't. Is there some way to solve for 'n'? That's the part I'm lost at.
 
GoJays32 said:
I would need to have the nodal line value 'n' in order solve for \theta, but I don't. Is there some way to solve for 'n'? That's the part I'm lost at.

Just leave the n in there I think.

so \theta = sin^{-1}(\frac{(n-\frac{1}{2})\lambda}{d})

Just plug in your values for d and \lambda... and that'll be your final answer. It's asking for the angles... so I think they want the angle as a function of n.
 

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