MadSci Network: Physics |
Start with the answer to 873909296.Ph
If v is not vertical but at some angle q
r then what we called "w" in the previous answer has a larger x
component. This addition to the x component is v sin(q
r). So the components of w are then
wx = vx + s
where vx = v sin(q
r) and
wy = vy
where vy = v cos(q
r)
The angle that w makes with the vertical is then tan-1(w
x / wy) = qw
Using the areas of the person's body as in the previous answer we now
get, for the total rain collected,
RC = w cos(qw) D T t + w sin(qw) D 5 T t
where, as before, t = x / s
It can be shown that cos(qw) = v
cos(qr) / w
and
sin(qw) = (v sin(qr) + s ) / w
It can also be shown, although it's not necessary for the answer to this
exercise, that
w = (v2 + 2vs sin(qr)
+ s2) 0.5
So the rain collected is now
RC = D x [ (v T cos(qr) / s ) +
(5 v T sin(qr) / s ) + 5 T ]
As before, if s = 0 we obtain an infinite amount of rain collected by the body, so don't stand in the rain even if the rain is not falling straight down. This makes sense.
If s approaches infinity then the first two terms in the brackets become zero and we are left, as before, with the term 5 T so that the total rain collected is D x 5 T, which is the same as before where the rain was falling straight down. If you think about going infinitely fast and sweeping up all the rain drops that are in a body-shaped row that is x units long, then this answer makes sense, as before.
John Link, MadSci Physicist
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