Case 1: Air resistance exerts a retarding force on a falling body which is proportional to the velocity.
Case 2: Air resistance exerts a retarding force on a falling body which is proportional to the square of the velocity.
Let the mass of the falling bodies in both Cases be 1 0 kg and the acceleration due to gravity be 1 0 m/s 2 .
If V 1 and V 2 and k 1 and k 2 are the terminal velocities and proportionality constants of case 1 and case 2, respectively, and V 1 V 2 = 1 , find: k 2 k 1 .
This section requires Javascript.
You are seeing this because something didn't load right. We suggest you, (a) try
refreshing the page, (b) enabling javascript if it is disabled on your browser and,
finally, (c)
loading the
non-javascript version of this page
. We're sorry about the hassle.
When body has reached terminal velocity, a = d t d v = 0 So by Newton's Law, m g − k 1 v 1 = m ∗ 0 So k 1 = v 1 m g
In case 2, m g − k 2 v 2 2 = 0 so k 2 = v 2 2 m g
v 1 = v 2 So k 2 k 1 = m g m g = m g = 1 0 0 = 1 0
Thus our answer is 10.
Problem Loading...
Note Loading...
Set Loading...
Case(1):
m d t d v = m g − k 1 v ⟹ d t d v = g − a v , where a = m k 1 ⟹
g − a v d v = d t ⟹ − a 1 ln ( g − a v ) = t + c ⟹
g − a v = C e − a t ⟹ v ( t ) = a 1 ( g − C e − a t )
v ( 0 ) = 0 ⟹ C = g ⟹ v ( t ) = a g ( 1 − e − a t )
The terminal velocity V 1 = l i m t → ∞ v ( t ) = a g = k 1 m g
Case(2):
m d t d v = m g − k 2 v 2 ⟹ d t d v = g − a 2 v , where a 2 = m k 2 ⟹
∫ g − a 2 v 2 d v = ∫ d t + c
Solving ∫ g − a 2 v 2 d v using partial fractions.
( g − a v ) ( g + a v ) 1 = g − a v A + g + a v B ⟹
1 = ( A + B ) g + a ∗ ( A − B ) v ⟹
A + B = g 1 A − B = 0
⟹ A = 2 g 1 = B ⟹ 2 g 1 ∫ g − a v 1 + g + a v 1 d v = 2 g 1 ln ( g − a v g + a v ) = t + c ⟹ g + a v = C e 2 a g t ( g − a v ) ⟹
v ( t ) = a g ( C e 2 a g t + 1 C e 2 a g t − 1 )
v ( 0 ) = 0 ⟹ C = 1 ⟹ v ( t ) = a g ( e 2 a g t + 1 e 2 a g t − 1 )
or v ( t ) = a g ( 1 − e − 2 a g t 1 − e − 2 a g t )
The terminal velocity V 2 = l i m t → ∞ v ( t ) = a g = k 2 m g
V 1 V 2 = 1 ⟹ k 2 k 1 = m g
Using m = 1 0 and g = 1 0 ⟹ k 2 k 1 = 1 0 .