howto:hambasics:sections:wavemodulationmath
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howto:hambasics:sections:wavemodulationmath [2021/01/03 07:42] – [Mixer] va7fi | howto:hambasics:sections:wavemodulationmath [2021/01/03 08:05] (current) – va7fi | ||
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\begin{align*} | \begin{align*} | ||
\cos(A+B) | \cos(A+B) | ||
- | \cos(A-B) | + | \cos(A-B) |
\end{align*} | \end{align*} | ||
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Use this animation to see what happens when you vary the individual frequencies. | Use this animation to see what happens when you vary the individual frequencies. | ||
- | {{ggb> | + | FIXME: animation in wrong place |
+ | {{ggb>/howto/ | ||
Some things to try: | Some things to try: | ||
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Mathematically, | Mathematically, | ||
- | <WRAP centeralign> | + | \$$2\pi f_c \quad \rightarrow \quad 2\pi f_c + 2\pi k s(t)\$$ |
- | \$$2\pi f_c \quad \rightarrow \quad 2\pi f_c + 2\pi k s(t)\$$. | + | |
- | </ | + | |
* Here, \$f_c\$ is the frequency of the carrier, which is a constant (this is important), | * Here, \$f_c\$ is the frequency of the carrier, which is a constant (this is important), | ||
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Now, it might be tempting to simply substitute this sum in the wave like so: | Now, it might be tempting to simply substitute this sum in the wave like so: | ||
- | <WRAP centeralign> | ||
\$$ \cos(2\pi f_c t) \quad \rightarrow \quad \cos\Big(\big(2\pi f_c + 2\pi k s(t)\big) t\Big) \$$ | \$$ \cos(2\pi f_c t) \quad \rightarrow \quad \cos\Big(\big(2\pi f_c + 2\pi k s(t)\big) t\Big) \$$ | ||
- | </ | + | |
but that's not quite right because the frequency is derived from the change in angle. | but that's not quite right because the frequency is derived from the change in angle. | ||
</ | </ | ||
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To solve this properly, we need some calculus and deduce the angle from our new frequency: | To solve this properly, we need some calculus and deduce the angle from our new frequency: | ||
- | <WRAP centeralign> | ||
\$$ \frac{d}{dt}\theta(t) = 2\pi f_c + 2\pi k s(t) \qquad | \$$ \frac{d}{dt}\theta(t) = 2\pi f_c + 2\pi k s(t) \qquad | ||
- | </ | + | |
The frequency modulated transmission is actually given by: | The frequency modulated transmission is actually given by: | ||
- | <WRAP centeralign> | ||
\$$ \cos\Big(2\pi f_c t + 2\pi k \int_0^{t}s(\tau) d\tau\Big) \$$ | \$$ \cos\Big(2\pi f_c t + 2\pi k \int_0^{t}s(\tau) d\tau\Big) \$$ | ||
- | </ | + | |
In our particular example, with \$s(t) = \cos(2 \pi f_s t)\$, the modulated radio signal becomes: | In our particular example, with \$s(t) = \cos(2 \pi f_s t)\$, the modulated radio signal becomes: | ||
- | <WRAP centeralign> | + | \begin{align*} |
- | \begin{align} | + | |
\cos\Big(2 \pi f_c t + 2\pi k \int_0^{t}s(\tau)d\tau\Big) &= \cos\Big(2 \pi f_c t + 2\pi k \int_0^{t}\cos(2 \pi f_s \tau)d\tau\Big) \\ | \cos\Big(2 \pi f_c t + 2\pi k \int_0^{t}s(\tau)d\tau\Big) &= \cos\Big(2 \pi f_c t + 2\pi k \int_0^{t}\cos(2 \pi f_s \tau)d\tau\Big) \\ | ||
& | & | ||
- | \end{align} | + | \end{align*} |
- | </ | + | |
For more details about FM, see: [[http:// | For more details about FM, see: [[http:// | ||
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Use this animation to see what happens when you vary the individual frequencies. You can use the check boxes to show or hide different waves. | Use this animation to see what happens when you vary the individual frequencies. You can use the check boxes to show or hide different waves. | ||
- | {{ggb> | + | FIXME: animation in wrong place |
+ | {{ggb>/howto/ | ||
Some things to try: | Some things to try: |
howto/hambasics/sections/wavemodulationmath.1609688529.txt.gz · Last modified: 2021/01/03 07:42 by va7fi