Physics: System of Particles and Center of Mass

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1
position vector of com for system of N particles (for coordinates just replace r with x y or z respectively )
r=(m1r1+m2r2+....+mnrn)/(m1+m2+....+mn)
2
2 point system m1 and m2(com)
xcm=m*0+(m2)r/(m1+m2) r1=(m2)r/(m1+m2) r2=(m1)r/(m1+m2)
3
position of com of continuous mass system
r =integral (dm *r)/integral dm
4
com for various shapes (uniform rod, square lamina, semicircular ring, hemispherical shell ,solid circular cone ,solid hemisphere respectively)
(L/2,0) (L/2,L/2) (0,2R/π) (0,R/2) (0,h/4) (0,3R/8)
5
com of extended body( from one extreme point )
m1r1+m2r2/m1+m2
6
cavity in object
r(remaining)=-m(cavity)*r(cavity/M(remaining) r(remaining)=A1x1-A2x2/(A1-A2)(where x1 is original mass com for question x1 has to be set 0 x2 is removed cavity com)
7
velocity of com vector form
V =(M1V1+M2V2+...)/M1+M2+M3+....
8
acceleration of com vector form
a=(M1a1+M2a2+...)/M1+M2+M3...
9
velocity of com in magnitude
v=√(((m1)^2(v1)^2+(m2)^2(v2)^2+2(m1v1m2v2)cos(theta))/m1+m2)
10
isolated system
M1r1=M2r2
11
moment of inertia
I=mr^2
12
two point mass moment of inertia
I = m1r1^2+m2r2^2 r1=m2r/m1+m2 r2 =m1r/m1+m2 I= m(reduced)r^2 m(red)=m1m2/(m1+m2)
13
moment of inertia about coordinate axes
r(x)=√(y^2+z^2) r(y)=√(x^2+z^2) r(z)=√(x^2+y^2) I(x)=mr(x)^2 etc
14
moment of inertia of continuous mass
I =integral (r^2 dm)
15
moment of inertia and axis passing through centre and perpendicular to planeon various objects (thin rod ,Ring ,disc , hollow cylinder,solid cylinder , hollow sphere, solid sphere)
Thin rod I=ml^2/12 ring=MR^2 disc=MR^2/2 , hollow cylinder=MR^2 ,solid cylinder=MR^2/2 hollow sphere=(2/3)MR^2 solid sphere=(2/5)MR^2
16
theorem of perpendicular axis
Iz=Ix+Iy
17
for 2D symmetric object
2I=Iz
18
ring (parallel to plane) inertia disc(parallel to plane) square sheet (perpendicular to plane , parallel to plane) rectangular sheet (parallel to plane (sides l,b), perpendicular to plane)
Ring=MR^2/2 (parallel to plane)disc=MR^2/4(parallel to plane) square sheet (parallel to plane) =Ml^2/12 (perpendicular to plane )=Ml^2/6 rectangular sheet (parallel to plane )= Ml^2/12,Mb^2/12 (perpendicular to plane )=(M/12)(l^2+b^2)
19
parallel axis theorem
I(parallel)=Icom+Ma^2
20
moment of inertia for various objects (parallel axis) thin rod , ring , disc , hollow cylinder,solid cylinder, hollow sphere, solid sphere
thin rod =ml^2/3, ring (tangent perpendicular to plane) = 2MR^2 (tangent parallel to plane)= 3MR^2/2 disc (tangent perpendicular to plane)=3MR^2/2 (tangent parallel to plane)=5MR^2/4 hollow cylinder=2MR^2 solid cylinder=3MR^2/2 hollow sphere=5MR^2/3 solid sphere=7MR^2/5
21
radius of gyration
I= Mk^2 (k is radius of gyration)
22
annular Disc
I=(M/2)[R1^2+R2^2] here R1 is smaller radius and R2 longer radius
23
torque
F×r =Frsin(theta)
24
principle of moments
F1x1=F2x2
25
angular acceleration
alpha=dw/dt=torque/I =mgsin(theta)l/I
26
rod is released from Horizontal position (angular acceleration,linear acceleration of COM, Linear acceleration of point B at one end opposite from rigid end)
angular acceleration=3g/2L linear acceleration =3g/4 aB=3g/2
27
translatory-rotation combination (angular acceleration, acceleration)
angular acceleration=mgR/(I(disc)+mR^2) acceleration=mg/m+(M/2) =2mg/(2m+M) M is mass of disc
28
equation of rotational motion
w2=w1+alpha(t), theta=w1t+(1/2)alpha(t^2) , (w2)^2=(w1)^2+2aplha.theta, v=rw
29
angular momentum (L)
L=r×p=m(r×v)=mvrsin(theta)
30
spin angular momentum(if axis is at one end )
L=I(at that axis using parallel axis theorem)*w
31
conservation of angular momentum
I1W1=I2W2
32
if mass is constant what is the relation between T and R if density remains constant T and R
mass constant (T proportional to R^2 ) density constant (T proportional to R^5)
33
when two bodies have w in same direction and w in opposite direction wfinial =?
wf(same direction)=I1W1+I2W2/(I1+I2) ,wf(different direction)=I1W1-I2W2/(I1+I2)
34
Work =?
W=torque*theta
35
Energy
K.E=(1/2)IW^2=L^2/2I=Lw/2
36
work energy theorem
(1/2)I((W2)^2-(W1)^2)
37
power(average, instantaneous)
P(average)=Work/time=∆K.E/time P(instantaneous)=torque*W (where W is omega)
38
energy loss when 2 discs are joined (same direction w and different direction w)
same direction (∆K.E=I1I2/2(I1+I2)*(w1-w2)^2 different direction (∆K.E=I1I2/2(I1+I2)*(w1+w2)^2
39
mechanical energy conservation (rod) U is mechanical energy w is omega also what is the equation for omega
Ui=MgL/2 Uf =(1/2)Iw^2 , w=√(3g/l)
40
rolling motion (velocity at points vp)
Vp=v√(2(1+sin(theta))
41
energy in rolling motion (translatory, rotational)
K.E(translatory)=(1/2)mv^2 K.E(rotational)=(1/2)Iw^2 =(1/2)mk^2*(v^2/R^2) K.E(total)=K.E(translatory)+K.E(rotational). K.Etotal/K.Etranslatory=(1+(k^2 /R^2) )
42
motion along an inclined plane(velocity at bottom)
v=√(2gh/(1+(k^2/R^2))) v is proportional to 1/(k^2/R^2)
43
motion along an inclined plane(acceleration)
gsin(theta)/(1+(k^2/R^2)) a is proportional to 1/(k^2/R^2)
44
motion along an inclined plane(time of descend)
t=(1/sin(theta))*√((2h)*(1+(k^2/R^2)) t is proportional to (k^2/R^2)
45
value of velocity (ring/hollow cylinder , disc/solid cylinder, hollow sphere, solid sphere)
ring/hollow cylinder = √gh disc/solid cylinder=√((4/3)gh) hollow sphere=√((6/5)gh). solid sphere= √((10/7)gh)
46
Time to reach bottom
Ring>hollowsphere >Disc>solid sphere
47
velocity comparison
solid sphere > Disc> hollow sphere> Ring
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