Signal strength of a wave packet

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SUMMARY

The discussion focuses on calculating the signal strength of a wave packet defined by the function g(ω)=C for |ω|<ω0 and g(ω)=0 elsewhere. The signal strength V(t) is derived using the integral V(t) = 1/√(2π) * ∫[g(ω)*exp(iωt)] dω, leading to V(t) = √(2/π)*ω0C * sin(ω0t)/ω0t. Participants also discuss the implications of Δω and Δt in relation to the uncertainty principle, specifically whether the product ΔωΔt satisfies the condition ΔωΔt>1/2.

PREREQUISITES
  • Understanding of wave packets and Fourier transforms
  • Familiarity with complex exponentials and Euler's formula
  • Knowledge of the uncertainty principle in quantum mechanics
  • Basic skills in using mathematical software like Python for plotting
NEXT STEPS
  • Study the properties of Fourier transforms in signal processing
  • Learn about the uncertainty principle and its implications in quantum mechanics
  • Explore the use of Python libraries such as NumPy and Matplotlib for signal visualization
  • Investigate the derivation and applications of the sinc function in wave packet analysis
USEFUL FOR

Students and professionals in physics, particularly those focusing on wave mechanics, signal processing, and quantum mechanics, will benefit from this discussion.

Elvis 123456789
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Homework Statement


Assume a wave packet is has contributions from various frequencies, give by g(ω)=C for |ω|<ω0, and g(ω) =0 for elsewhere.

a)What is the signal strength as a function of time, i.e., V(t)=?

b) Sketch g(ω) and V(t); You can use fooplots.com, for example, or python.

c) Indicate Δω and Δt in the above plots; Does the products of these two satisfy ΔωΔt>1/2?

Homework Equations


V(t) = 1/√(2π) * integral from -∞ to +∞ of [ g(ω)*exp(iωt)] dω

exp(iωt) = cos(ωt) + isin(ωt)

The Attempt at a Solution



a.) V(t) = 1/√(2π) * integral from -ω0 to +ω0 of [ C*exp(iωt)] dω

using eulers formula and the properties of even and odd functions

V(t) = 2/√(2π) * integral from 0 to +ω0 of [ C*cos(ωt)] dω

V(t) = 2C/√(2π) * sin(ω0t)/t = √(2/π)*ω0C * sin(ω0t)/ω0t

b.) the sketches for g(ω) and V(t) are in the attachments

c.) I am not really sure what Δω and Δt in these graphs
 

Attachments

  • phy graph.jpg
    phy graph.jpg
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  • phy graph 2.jpg
    phy graph 2.jpg
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  • signal strength vs time.png
    signal strength vs time.png
    11.1 KB · Views: 605
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Elvis 123456789 said:
V(t) = 2/√(2π) * integral from 0 to +ω0 of [ C*cos(ωt)] dω
Shouldn't the lower integral limit be ##-\omega_0##?
Elvis 123456789 said:
c.) I am not really sure what Δω and Δt in these graphs
Use the definition of standard deviation. For example for V(t), you will use
$$
\Delta t = \sqrt{E[t^2]-(E[t])^2}
$$
where ##E[\,\,]## means taking average over the intensity ##|V(t)|^2##. Similar arguments for ##g(\omega)##.
 
blue_leaf77 said:
Shouldn't the lower integral limit be −ω0−ω0-\omega_0?
I have a factor of 2 in the front to account for that. Is that not right?
 
Elvis 123456789 said:
I have a factor of 2 in the front to account for that. Is that not right?
Ah sorry I missed that, you are right.
 

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