amit25 said:
i think r is suppose to represent distance.
What distance? Can you describe what r represents?
The question gives me the formula in terms of r.
I didn't see any formula given in the question.
I guess my question is if my calculations are correct? Not sure if I am on the right track. I am not sure how many answers to give I wasnt told but I calculated up to 3.
Well, I think you are to find all the values of x between the speakers that correspond to constructive interference. Since one speaker is at x = 0 and the other is at x = L, you need to find all constructive interference locations x that lie between 0 and 1.5 m.
It seems to me that your equation x = (L-nλ)/2 is essentially correct . You can write this as x = L/2 - nλ/2. For n = 0, you get x = L/2. Thus, the midpoint between the speakers is a point of constructive interference. This makes sense because the sound travels the same distance from both speakers to get to this point. (The "path difference" = 0).
You can keep plugging in other integer values of n to get more values of x. As you can see, increasing n by 1 moves the point of interference a half wavelength toward the left speaker. If n gets too large, x becomes negative and therefore does not correspond to a point located between the speakers.
You should also be able to see that you can plug in negative values for n. Or, equivalently, you could write x = L/2 +nλ/2 for positive values of n. Now each successive value of n moves you a half wavelength toward the speaker on the right. When n gets too large, x will be larger than 1.5 m and therefore does not represent a point between the speakers.
[The general idea is that if you are located at a point of constructive interference, then you can get another point of constructive interference by moving a half wavelength to the right (or to the left). That's because you will move a half wavelength closer to one speaker while at the same time moving a half wavelength farther from the other speaker. So, you will have changed the "path difference" of the sound by one full wavelength.]