2) From assumption (c), the velocity (v) at time (t) of the water droplet is 3 v' + v = g. t+ro If the water drops from stationary, solve for v(t).

Advanced Engineering Mathematics
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Chapter2: Second-order Linear Odes
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Differential equation: Solving a (general) linear first order equations

(2) From assumption (c), the velocity (v) at time (t) of the water droplet is
3 ()
v' +
v = g.
t + ro
If the water drops from stationary, solve for v(t).
Transcribed Image Text:(2) From assumption (c), the velocity (v) at time (t) of the water droplet is 3 () v' + v = g. t + ro If the water drops from stationary, solve for v(t).
A water droplet evaporates before they reach the ground.
Figure 1: Water droplets (source]
In this situation, a few assumptions are made:
a) At initial point, a typical water droplet is in sphere shape with radius r and remain spherical
while evaporating.
b) The rate of evaporation (when it loses mass (m)) is proportional to the surface area, S.
c) There is no air-resistance and downward direction is the positive direction.
To describe this problem, given that p is the mass density of water, r,is the radius of water before it
drops, m is the water mass, V is the water volume and k is the constant of proportionality.
Transcribed Image Text:A water droplet evaporates before they reach the ground. Figure 1: Water droplets (source] In this situation, a few assumptions are made: a) At initial point, a typical water droplet is in sphere shape with radius r and remain spherical while evaporating. b) The rate of evaporation (when it loses mass (m)) is proportional to the surface area, S. c) There is no air-resistance and downward direction is the positive direction. To describe this problem, given that p is the mass density of water, r,is the radius of water before it drops, m is the water mass, V is the water volume and k is the constant of proportionality.
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