In the coupled pendulums of Figure 1 let us write the modulation
frequency as ωm =(ω0 − ω0)/2 and the average frequency as ωp = (ω0
+ ω0)/2 and suppose that the spring is so weak that it stores a
negligible amount of energy.
a) Let the modulated amplitude.
be constant over one cycle at the
average frequency ωp to show that the energies of the masses can be
written as
b) Show that the total energy E remains constant and that
the difference in energies at any instant of time is
c) prove that
to thus show that the constant total
energy is completely exchanged between the two pendulums at the
beat frequency (ω0 − ω0).
Ao cos(wmt) ó Ao sen(wmt)
1 ΕΙ II 5mAĞw cos? (wmt) , 5mAwsen"(wmt). 2 1 E2
. [t( ولما - أنا)]E1 - E2 = E cos
Ei E12R2 号 [1+cos(u' - un) [1-cos(L. - up)]. E2
Qo0000000000000 elle 20000000000 444 Г. III
In the coupled pendulums of Figure 1 let us write the modulation frequency as ωm =(ω0 − ω0)/2 and the average frequency
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In the coupled pendulums of Figure 1 let us write the modulation frequency as ωm =(ω0 − ω0)/2 and the average frequency
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