When I started preparation for jee, I thought Irodov is very difficult. A close reading of the book reveals that it is not so provided, i repeat, one reads HCV .
Let us take 1 example.
Q. 1.1
A motorboat going downstream overcame a raft at a point A ; t= 60 mins later it turned back and after some time passed the raft at a distance L= 6.0 km from the point A. Find the flow velocity assuming the duty of the engine to be constant.
solution :
How to solve the problem ??
Basically this requires the concept of relative motion---more specifically, relative motion in one dimension.
Let us assume that the flow of water is from left to right ( +ve dirn of x axis ).
This is downstream. The motorboat is going downstream.
At t = 0 , ( beginning ) , the raft and motorboat are at point A. The velocity of the raft ( no engine ) is = velocity of the river.
At t = 60 mins, motorboat ( with engine ) goes far away from raft , say , at point P ( in the +ve dirn of x axis ) , ahead of raft which proceeds only up to point B ( in the +ve dirn of x axis ) .
Clearly, time taken by the boat to reach P from A = time taken by the raft to reach B from A.
Then the boat turns back from the point P , but raft proceeds from B to C.
Then the 2 meet at point C. The boat going upstream and raft going downstream.
Let the 2 meet at time = t + t 1 at point C.
So, time taken by raft to reach from B to C = time taken by boat to reach C from P in the reverse motion ( upstream motion )
For our visualization, we can consider a line along X axis with origin at A , then B. then C and then point P.
Now V a = actual velocity of boat ( with engine )
V b = actual velocity of raft = velocity of river.
so, during downstream ( going along +ve X axis ) ,
if V c = relative velocity of motor wrt stream, then
V c = V a -- V b
V a = V b + V c
so time t = AP / V a = AP / ( V b + V c )
But AB = distance travelled by raft in time t = t ( V b )
now let us focuss abt upstream when the motorboat turns back. ( going from right to left or towards -ve X axis ).
During upstream V c = V a + V b
( the boat turns back but raft goes forward )
so, V a = V c -- V b
So, PC = distance travelled by motorboat in upstream in time t c
= ( V c -- V b ) t c
BC = distance travelled by raft in time t c = ( V b ) t c
now
AP - PC = AC = L [ note again A, B then C and then P ]
( V b + V c ) t -- ( V c -- V b ) t c = L
V c t + V b t -- V c t c + V b t c = L ..................(1)
again
AB + BC = L
or, V b t + V b t c = L
V b = L / ( t + t c ) ..........................................(2)
manipulating 2 and 1 , we get
V b = L / 2t
Q.1.2
A point traversed half the distance with a velocity V 0 . The remaining part of the velocity was covered with velocity V 1 for half the time and with velocity V 2 for other half of the time. Find the mean velocity of the point averaged over the whole time of motion
soln :
Basically this requires the concept of average velocity in one dimension.
V av = total displacement / total time
Let us again visualize points A, B and C serially along X axis from left to right.
Let the particle starts from A at t = 0 . It goes to B at t = t 1 and then to C
at t = t 2 .
now, AB = BC = L ( say )
t1 = L / V 0 ......................................( 1)
The time taken by the particle to reach C from B is t 0 = t 2 - t1
BC = L = V 1 ( t 2 - t 1 ) / 2 + V 2 ( t 2 - t 1 ) / 2 ............(2)
V av = total displacement / total time = AC / t 2 = 2L / t2
from 1 and 2, L = V 1 ( t 2 - t 1 ) / 2 + V 2 ( t 2 - t 1 ) / 2
V 0 t 1 = V 1 ( t 2 - t 1 ) / 2 + V 2 ( t 2 - t 1 ) / 2
doing manipulation,
V av = 2 V 0 ( V 1 + V 2 ) / 2 V 0 + V 1 + V 2
This result can be memorized for short -cut.