How to calculate this inverse Fourier Transform?

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The discussion revolves around calculating the inverse Fourier Transform of a given expression involving Dirac delta functions. Participants highlight the use of the Dirac delta sampling property, which simplifies the integral by allowing the evaluation of the function at specific frequencies, ±100 Hz in this case. The conversation includes attempts to convert complex numbers to polar form and discussions about simplifying the resulting expressions into cosine form. There is some confusion regarding the correct application of properties and simplifications, but the consensus is that the approach is fundamentally correct. The final goal is to express the result in a clear cosine format, which is acknowledged as a common outcome for such transforms.
Nat3
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Homework Statement



Take the inverse Fourier Transform of

5[\delta(f+100)+\delta(f-100)]\bigg(\frac{180+j2\pi f*0.0135}{1680+j2\pi f*0.0135}\bigg)

Homework Equations



g(t)=\int_{-\infty}^{\infty} G(f)e^{j2\pi ft}dt

The Attempt at a Solution



g(t)=\int_{-\infty}^{\infty} 5[\delta(f+100)+\delta(f-100)]\bigg(\frac{180+j2\pi f*0.0135}{1680+j2\pi f*0.0135}\bigg) e^{j2\pi ft}dt

My professor gave the hint that the dirac delta sampling property can be used, but I don't see how since I'm taking the inverse Fourier Transform and not just a regular integral.

I've been reading about the different properties of the FT and dirac delta function, but simply can't figure out how to proceed. Any suggestions?
 
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?? The inverse Fourier Transform is a "regular integral"! And the "Dirac delta sampling property" is that \int_{-\infty}^\infty \delta(x- a)f(x)dx= f(a). That should make this problem easy.
 
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Ah.. I'm not sure what I was thinking, lol :-)

OK, so having this equation:

g(t)=\int_{-\infty}^{\infty} 5[\delta(f+100)+\delta(f-100)]\bigg(\frac{180+j2\pi f*0.0135}{1680+j2\pi f*0.0135}\bigg) e^{j2\pi ft}dt

When using the sifting/sampling property of the Dirac Delta function:

\int_{-\infty}^\infty \phi (t) \delta(t - T)dt = \phi (T)

Should I replace f or t in the above equation with \pm 100? It seems like I should replace the f:

g(t)=5\bigg (\frac{180+j2\pi f*0.0135}{1680+j2\pi f*0.0135}\bigg) e^{j2\pi ft} \bigg |_{f=100}+5\bigg (\frac{180+j2\pi f*0.0135}{1680+j2\pi f*0.0135}\bigg) e^{j2\pi ft} \bigg |_{f=-100}

g(t)=5\bigg (\frac{180+j2\pi *1.35}{1680+j2\pi *1.35}\bigg) e^{j200\pi t}+5\bigg (\frac{180-j2\pi *1.35}{1680-j2\pi *1.35}\bigg) e^{-j200\pi t}

But I'm not sure if that's correct?
 
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Does anyone know if what I did is correct? Operating under that assumption, I tried converting the rectangular coordinate complex numbers to polar form:

g(t)=5\bigg (\frac{180.2\angle 2.70^\circ}{1680.02\angle 0.29^\circ}\bigg) e^{j200\pi t}+5\bigg (\frac{180.2\angle -2.70^\circ}{1680.02\angle -0.29^\circ}\bigg) e^{-j200\pi t}

g(t)=5\bigg (\frac{180.2\angle 2.70^\circ}{1680.02\angle 0.29^\circ}\bigg) e^{j200\pi t}+5\bigg (\frac{180.2\angle -2.70^\circ}{1680.02\angle -0.29^\circ}\bigg) e^{-j200\pi t}

g(t)=5(0.11\angle 2.41^\circ) e^{j200\pi t}+5(0.11\angle -2.41^\circ) e^{-j200\pi t}

I think I might be doing something wrong though, because I think the answer is supposed to work out to be:

1.1\cos(2\pi (100)t+2.41^\circ)
 
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Nat3 said:
Ah.. I'm not sure what I was thinking, lol :-)

OK, so having this equation:

g(t)=\int_{-\infty}^{\infty} 5[\delta(f+100)+\delta(f-100)]\bigg(\frac{180+j2\pi f*0.0135}{1680+j2\pi f*0.0135}\bigg) e^{j2\pi ft}dt
The integral should be with respect to ##f##, not ##t##.

When using the sifting/sampling property of the Dirac Delta function:

\int_{-\infty}^\infty \phi (t) \delta(t - T)dt = \phi (T)

Should I replace f or t in the above equation with \pm 100? It seems like I should replace the f:

g(t)=5\bigg (\frac{180+j2\pi f*0.0135}{1680+j2\pi f*0.0135}\bigg) e^{j2\pi ft} \bigg |_{f=100}+5\bigg (\frac{180+j2\pi f*0.0135}{1680+j2\pi f*0.0135}\bigg) e^{j2\pi ft} \bigg |_{f=-100}

g(t)=5\bigg (\frac{180+j2\pi *1.35}{1680+j2\pi *1.35}\bigg) e^{j200\pi t}+5\bigg (\frac{180-j2\pi *1.35}{1680-j2\pi *1.35}\bigg) e^{-j200\pi t}

But I'm not sure if that's correct?
That's right.
 
Nat3 said:
Does anyone know if what I did is correct? Operating under that assumption, I tried converting the rectangular coordinate complex numbers to polar form:

g(t)=5\bigg (\frac{180.2\angle 2.70^\circ}{1680.02\angle 0.29^\circ}\bigg) e^{j200\pi t}+5\bigg (\frac{180.2\angle -2.70^\circ}{1680.02\angle -0.29^\circ}\bigg) e^{-j200\pi t}

g(t)=5\bigg (\frac{180.2\angle 2.70^\circ}{1680.02\angle 0.29^\circ}\bigg) e^{j200\pi t}+5\bigg (\frac{180.2\angle -2.70^\circ}{1680.02\angle -0.29^\circ}\bigg) e^{-j200\pi t}

g(t)=5(0.11\angle 2.41^\circ) e^{j200\pi t}+5(0.11\angle -2.41^\circ) e^{-j200\pi t}

I think I might be doing something wrong though, because I think the answer is supposed to work out to be:

1.1\cos(2\pi (100)t+2.41^\circ)
You're right so far. You just have to keep going with the simplification.

It might be simpler if you note at the start that the two terms are conjugates and use the fact that ##z+\bar{z} = 2\text{Re}(z)##.
 
Hmm... I've been trying to simplify it and am not sure how to proceed. I tried changing the polar portion to ##\cos## and using Euler's identity to change the exponentials to ##\cos## and ##\sin##, which gives:

##g(t) = 5[0.11\cos(\omega t + 2.41^\circ)[\cos(200\pi t) + j\sin(200\pi t)] + 0.11\cos(\omega t - 2.41^\circ)[\cos(200\pi t) - j\sin(200\pi t)]]##

But I feel like I'm on the wrong track here. If I multiply that out then it becomes a mess. Did I go in the wrong direction with this?

Really appreciate your help :)
 
Hint: ##0.11\angle 2.41^\circ = 0.11 e^{j 2.41^\circ}##
 
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vela said:
Hint: ##0.11\angle 2.41^\circ = 0.11 e^{j 2.41^\circ}##

Did you by any chance mean:

##0.11\angle 2.41^\circ = Re(0.11 e^{j 2.41^\circ})##? Otherwise, I'm really confused :smile:

Because:

##0.11\angle 2.41^\circ = 0.11\cos(\omega t + 2.41^\circ)##

And:

##0.11 e^{j 2.41^\circ} = 0.11\cos(\omega t + 2.41^\circ) + j0.11\sin(\omega t + 2.41^\circ)##
 
  • #10
Nat3 said:
$$g(t)=5 \left( \frac{180.2\angle 2.70^\circ}{1680.02\angle 0.29^\circ}\right) e^{j200\pi t} + 5 \left( \frac{180.2\angle {-2.70}^\circ}{1680.02\angle {-0.29}^\circ}\right) e^{-j200\pi t}$$
What I mean is express the fractions in polar form, i.e. ##re^{j\theta}##.
 
  • #11
vela said:
What I mean is express the fractions in polar form, i.e. ##re^{j\theta}##.

Like this?

g(t)=5\bigg (\frac{180.2\angle 2.70^\circ}{1680.02\angle 0.29^\circ}\bigg) e^{j200\pi t}+5\bigg (\frac{180.2\angle -2.70^\circ}{1680.02\angle -0.29^\circ}\bigg) e^{-j200\pi t}

g(t)=5(0.11\angle 2.41^\circ) e^{j200\pi t}+5(0.11\angle -2.41^\circ) e^{-j200\pi t}

g(t)=5Re(0.11e^{j2.41^\circ})e^{j200\pi t} + 5Re(0.11e^{-j2.41^\circ})e^{-j200\pi t}

I can't combine the exponentials being multiplied together (because one is only the real part), can I?
 
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  • #12
Nat3 said:
$$g(t)=5 \left( \frac{180+j2\pi *1.35}{1680+j2\pi *1.35} \right) e^{j200\pi t} + 5 \left(\frac{180-j2\pi *1.35}{1680-j2\pi *1.35}\right) e^{-j200\pi t}$$
OK, let's back up one more step. Convert the complex numbers from rectangular to polar form then simplify.
 
  • #13
Nat3, I admire that you write all these equations in LaTeX. But one hint: if you want your formula to have its own line, then you should use tex, and not itex. I have changed this for you in your posts. The result really is a lot easier on the eyes. Check the difference between post 4 and the quoted part in post 5, for example.
 

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