Question #e4eae

By the law of simple pendulum we know

`"Time period"(T) prop"Effective length"(sqrtL)`

Let the time period of the 1st pendulum having effective length `L_1=90cm` be `" "T_1s`

And the time period of the 2nd pendulum having effective length `L_2=100cm` be `" "T_2s`

So by the law `T_2/T_1=sqrt(L_2/L_1).....(1)`

Let the two pendulum starts oscillation in same phase and after a minimum time t sec they again become in the same phase. During this t sec the 1st pendulum oscillates `N_1`times and the 2ndpendulum oscillates `N_2`times

So `t=N_1xxT_1=N_2xxT_2`

`=>N_1/N_2=T_2/T_1.....(2)`

Comparing (1) and (2)

`=>N_1/N_2=T_2/T_1=sqrt(L_2/L_1)=sqrt(100/90)=sqrt10/3=3.16/3~~1.05=21/20`

So 1st pendulum will oscillate 21 times and 2nd one will oscillate 20 times before they come to same phase again.

But if we take the ratio in inverted way as follows we get different result.

Then `N_2/N_1=sqrt0.9~~0.95=19/20`

Here 1st pendulum will oscillate 20 times and 2nd one will oscillate 19 times before they come to same phase again.

The graph given by respected Gio approximately matches with the second result but does not exactly match with any one.So it may be inferred that the pendulum never exactly comes to the same phase again.

The period of a simple pendulum [small angle of oscillation assumed] is:

`T = 2 pi sqrt(l/g)`

From just plugging the numbers into the period formula [I mirrored this is a spreadsheet so as at least to preserve Excel standard rounding accuracy, shorter numbers are re-produced here]:

`T_(0.9) approx 1.903`s

`T_1 approx 2`s

`delta T = T_1 - T_(0.9) approx 0.103`s

To make it easier, imagine 2 runners racing round a tracking starting on the starting line at `t = 0`.

The faster completes a lap in `T_(0.9)`, the slower in `T_1`. So each time the faster crosses the line, he has gained a further `delta T` on the slower runner.

When `Sigma delta T = T_1`, the faster runner knows he is a full lap ahead because that it how long it takes the slower runner to lap the track.

Turning to the pendulum, if `l_(0.9)` is in phase with `l_1` again after `alpha` complete oscillations of `l_(0.9)`, then `alpha * 0.103 = 2 implies alpha = 19.5`

That happens at time `t = 19.5 * 1.903 = 37.1`

However `alpha notin mathcal Z`, ie this is not a set of complete oscillations for `l_(0.9)`. They are not in phase as such. Using the running analogy, the runners meet short of a complete circuit of the track.

Plotted it on Desmos and they're not matching up as being in phase

Not sure where to go from here. I have asked Wolfram to solve the oscillation as:

`cos sqrt(g/1) t = cos sqrt(g/0.9) t = 1`

...but it's refusing to play along.

I tried plotting the oscillations as cos functions.

Time period of a pendulum is given by the expression
`T=2pisqrt(l/g)`
`:.T_0.9=2pisqrt(0.9/9.81)=1.9`, rounded to one decimal places
`=1900millisec`
and `T_1.0=2pisqrt(1.0/9.81)=2.0`, rounded to one decimal places.
`=2000millisec`

LCM of both time periods will give the time when both will be in unison (phase) again.
LCM of `1900 and 2000` is `38000millisec`
As such the both pendulums will be in phase again after `38 s`

During this time both pendulums will have completed different oscillations, which can be calculated from the data above.

This would be approximate value.