Understanding Intensity of Plane SHW in 1D, 2D, and 3D

AI Thread Summary
The discussion centers on the intensity of plane progressive simple harmonic waves and how it relates to waves in different dimensions. Intensity is defined as energy per area, and for 2D and 3D waves, amplitude decreases with distance due to energy conservation, following an inverse square law. The conversation also touches on deriving expressions for amplitude and intensity, emphasizing that the relationship derived for 1D waves may not directly apply to higher dimensions without additional assumptions. The average energy passing through a point in wave motion is discussed, with questions about the consistency of energy distribution in a medium like a string. Overall, the complexities of wave behavior in various dimensions and the assumptions needed for accurate derivations are key points of focus.
sadhu
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I am in eleventh standard , In my book it is given about the plane progressive simple harmonic wave , later somewhere is mentioned about
intensity of wave

what my doubt is
intensity is defined as energy/area
but what about waves in 2d or 1d
plane SHW are 1d as wave progresses in x-axis

how to about for waves in 2d or 3d
surely their amplitude must follow inverse distance or square law?
 
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Well, if I understand your question correctly, then the answer is yes. For 2-D and 3-D waves, as they spread over farther and farther distances, their amplitudes must decrease because of conservation of energy. In fact, this is why a radio signal gets weaker as you move away from the source of the signal.

Is this what you are asking about?
 
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but how to derive expression for the amplitude of such waves (suppose source is point object)
 
This may possibly be a homework question, so I can't give you a full derivation, but maybe I can set you off on the right path and you can derive it yourself.

Start with a spherical wave from a point source, which has an intensity I_o at a distance r_o from the source.

Now, remember that: I=P/A where P is power and A is area of the surface the wave is on. Since energy is conserved, power must also be conserved, so we have:

I_o=P/A_0 and I_1=P/A_1 where I_1 is the intensity at some farther point r_1. Now, can you use these equations and the expressions for the surface areas of the surfaces at r_1 and r_2, to find the ratio of I_1 to I_o? If you can, then how do you relate amplitude to intensity?
 
i =constant * amplitude square
still I don't think one could go that easily
relation between amplitude and intensity is derived in book and other books at my standard using 1 D wave motion , how can we say that that remains true for all dimensions
2,3

i already have thought of something ,but can you tell whether
average energy passing through a point in any wave motion is always half the max. passing through it when its phase=0,2pi etc;
 
sadhu said:
i =constant * amplitude square
still I don't think one could go that easily
relation between amplitude and intensity is derived in book and other books at my standard using 1 D wave motion , how can we say that that remains true for all dimensions
2,3
You can't, you need to make additional assumptions to make the derivation.

For example, the inverse square law assumes a source with spherical wavefronts. You can't apply the inverse square law to laser beams.

Claude.
 
can you please tell the average intensity of a spherical wave with respect to time
i.e when one complete wave pass through that point in time T

one more thing
can,t we suppose spherical wave amplitude as the amplitude of wave passing through the string in which density is directly proportional to distance square.

and
is it that that for a constant power input for a wave at origin in string waves,
energy present in a single particle (infinitely small part of string) is constant through out the string.
 
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