So now using the scalar u instead of the vector notation from 1.179 we have,
Saturday, June 7, 2008
Irodov Problem 1.180
This problem is a straightforward variation of 1.179 where v=wt and we have to determine at what rate the mass changes. One thing to note here is that the escape velocity of the gas u in this problem is not bold and is a scaler. This may be a bit confusing especially since in 1.178 and 1.179, he uses the bold vector notation. The essential idea in the notation is simply that when he uses vector notation, if the direction of ejection is in the opposite direction to that of the rocket, the corresponding scalar will only be negative in other words,

So now using the scalar u instead of the vector notation from 1.179 we have,
So now using the scalar u instead of the vector notation from 1.179 we have,
Irodov Problem 1.178
Suppose that at some instant of time the mass of the rocket was . Suppose that over the next infinitesimally small interval of time dt, fuel of mass
The change in momentum dP of the entire (rocket + fuel) system is given by,
Irodov Problem 1.177
As with the last few problems, momentum will be conserved before and after collision of the molecules and so we have,
In case the collision is elastic no energy will be lost and so we have,
Here
Now (7) can only be true if
In case of an inelastic collision we will have,
Clearly then
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