Laws of Motion Flashcards
Momentum P =
√2mKE
Impulse J =
change in momentum = Fdt
Area under Ft gives
impulse
Recoil of gun Vr
Vr = -mV/M
Speed Vr =
mV/M
F in recoil of gun
nmV
For a connected system of 2 masses, a =
(m1-m2)g/m1+m2
For a connected system of 2 masses, a =
2m1m2g/m1+m2
Motion along inclined surface V =
√2gLsinθ L = len of inclined surf
= √2gH
Motion along inclined surface, time to reach ground t =
√2L/a = 1/sinθ√2H/g
μk <
μs
Motion in circular path
Vmax = √(μ(s) rg)
W by spring force
Ws = -kx^2/2
W by static fric =
0
W by kinetic fric =
-μmgS
KE =
PV/2
Work energy theorem
W = change in KE
stopping dist
S = mu^2/2F
W against conservative force
ΔPE
W by conservative force
-ΔPE
W by centripetal force
0
1 horsepower =
746W
Wt graph gives
P
Efficiency η =
(O/P) power/(I/P) power
When P = 0, V =
√2Pt/m
When P = 0, a =
√P/2mt
Elastic collision
Linear mom, KE conserved, bodies regain shape, force must be conservative
Inelastic collisoin
L.M conserved, KE not conserved, bodies don’t regain shape, some f may not be conservative
Perfectly inelastic collision
LM conserved, KE not conserved, body is well deformed & don’t regain shape, All F is not conservative
If coeff of restitution = 0,
perfect inelastic
If coeff of restituion = 1
Perfect elastic
If coeff btn 0 & 1
partial inelastic
For perfect elastic,
V1 = [(m1-m2)u1 + 2m2u2]/m1+m2
For perfect inelastic
V = [m1u1 + m2u2]/m1+m2
KE loss =
m1m2(u1-u2)^2/2(m1+m2)
When u1 & u2 are opp, KE loss =
m1m2(u1+u2)^2/2(m1+m2)
r =
(m1r1 + m2r2)/m1+m2
Center of mass for cone
Solid cone - h/4
Hollow cone - h/3
In explosion in parabolic path
m1r1 = m2r2
Shift in trolley in opp dir
x = ml/m+M
Radius of gyration K for ring =
MR^2
K for disc
MR^2/2
K for solid sphere
2/5MR^2
K for hollow sphere =
2/3MR^2
K for rod
ml^2/12
Moment of inertia I =
mr^2
Angular momentum L =
Iω
Angular impulse
ΔL
Rotational power Pr =
τω
KE of pure rolling body
1/2mv^2 β
V for Rolling motion on an inclined plane
V = √2gH/β
a for rolling motion on inclined plane
a = gsinθ/β
t for rolling motion on inclined plane
t = 1/sinθ√2hβ/g