a. The point of collision above the top of the cliff. Let the particle meet after time t.
For the first particle,s = s1, v0=v1, a = -g.
Then, s1=v1t−(1/2)gt2 (i)
For the second particle,s = s2, v0=v2, a = -g.
Then, s2=v2t−(1/2)gt2 (ii)
Referring to Fig.
s2−s1=h
Substituting s1 from (i), s2 from (ii) in (iii), we have
t=h(v2−v1
b. The point of collision of the particle in between the top and bottom of the cliff.
For the first particle,s = −s1, v0=v1, a = -g.
Position-time relation for the first particle,
−s1=v1t−(1/2)gt2
This gives s1=(1/2)gt2−v1t (i)
Similarly, for the second particle,s = s2, v0=v2, a = -g.
Then s2=v2t−(1/2)gt2 (ii)
Referring to the Fig., s1+s2=h (iii)
Substituting s1 from (i), s2 from (ii) in (iii), we have
t=h(v2−v1)
c. The point of collision of the particles below the bottom of the cliff (let us
assume a ditch at the base of the cliff).
For article 1, s=−s1,v0=v1 and a = -g.
Position-time relation for the first particle
−s1=v1t−(1/2)gt2
This gives s1=(1/2)gt2−v1t (i)
Similarly, for particle 2, s=−s1,v0=v1 and a = -g.
We have s2=(1/2)gt2−v2t (ii)
From Fig. s1−s2=h (iii)
Substituting s1 from (i), s2 from (ii) in (iii), we have
t=h(v2−v1)