Dirac Delta Function: Scaling and Shifting

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SUMMARY

The discussion focuses on the scaling and shifting of the Dirac delta function in discrete time. It clarifies that scaling the Dirac delta function is represented as \(\delta(ax) = \frac{1}{a}\delta(x)\), meaning that if you scale the argument by a factor of 2, you must divide the function by 2 to maintain its integral property. Therefore, writing \(2 \cdot \delta[n]\) increases the peak value at \(n=0\) to 2, while \(\delta[2n]\) reduces the peak value to \(\frac{1}{2}\) at \(n=0\). This aligns with the fundamental properties of the Dirac delta function.

PREREQUISITES
  • Understanding of the Dirac delta function and its properties
  • Basic knowledge of discrete time signals
  • Familiarity with integral calculus
  • Concepts of scaling and shifting functions
NEXT STEPS
  • Study the properties of the Dirac delta function in continuous time
  • Learn about the implications of scaling and shifting in signal processing
  • Explore applications of the Dirac delta function in systems theory
  • Investigate the relationship between the Dirac delta function and impulse responses
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Students and professionals in signal processing, electrical engineering, and applied mathematics who seek to deepen their understanding of the Dirac delta function and its applications in discrete time systems.

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Just have a question about the dirac delta function. I understand how you would write it if you want to shift it but how would you scale it assuming we are using discrete time. Would you write 2*diracdelta[n] or diracdelta[2n]. Also, would that increase it or reduce it by 2 meaning that instead of it being 1 at n=0, it would be 2 instead or would it be 1/2. Does it work the same way as scaling other functions in other words? Thank you!
 
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Remember the defining property of the Dirac delta:

[tex]\int_{-\infty}^{\infty} \delta(x)dx = 1[/tex]

Thus

[tex]\int_{-\infty}^{\infty} \delta(ax)dx = \frac{1}{a} \int_{-\infty}^{\infty} \delta(y)dy = \frac{1}{a}[/tex]

So we can think of multipling the argument by a as being the same thing as dividing the function by a:

[tex]\delta(ax) = \frac{1}{a}\delta(x)[/tex]
 
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