1/4
Looks like no tags are added yet.
Name | Mastery | Learn | Test | Matching | Spaced |
---|
No study sessions yet.
impulse
product of avg force acting on body and time fort which it acts on body
Ft = change in p = area under Ft graph
principle conservation of linear momentum
total linear momentum in a system in constant provided no ext force acts on the system
no change in p
types of collision
elastic
KE conserved, relative speed of approach = relative speed of separation
Ua - Ub = Vb - Va
head on collision: bodies move off in a straight line connecting the 2 bodies’ centre of mass after colliding
inelastic collision
KE not conserved, but p is
perfectly inelastic: bodies will coalesce/stick tgt after colliding
special cases of 1D collision
m1=m2
exchange velos
m1 » m2
m1: vlelo approximately unchanged
m2: rebounds with approx 2x the velocity of m1
m1 « m2
m1: velo approx reversed
m2: approx at rest
is collision elastic?
1 direction
RSOA = x
RSOS = y
since x=y, KE conserved, collision elastic
>1 direction
KEi = x
KEf = y
since x=y, KE conserved, collision elastic
can 2 bodies be at rest simultaneously?
find TPi
since p must be conserved given that no net ext force acts on it, Pi=Pf
since TPi is nonzero, TPf shd also be nonzero
hence both bodies cannot be at rest simultaneously