5. Motion in a plane with Constant Acceleration
- Motion in two dimension with constant acceleration we we know is the motion in which velocity changes at a constant rate i.e, acceleration remains constant throughout the motion
- We should set up the kinematic equation of motion for particle moving with constant acceleration in two dimensions.
- Equation's for position and velocity vector can be found generalizing the equation for position and velocity derived earliar while studying motion in one dimension
Thus velocity is given by equation
v=v0+at (8)
where
v is velocity vector
v0 is Intial velocity vector
a is Instantanous acceleration vector
r-r0=v0t+(1/2)at2 (9)
where r0 is Intial position vector
i,e
r0=x0i+y0j
and average velocity is given by the equation
vav=(1/2)(v+v0) (10) - Since we have assumed particle to be moving in x-y plane,the x and y components of equation (8) and (9) are
vx=vx0+axt (11a)
x-x0=v0xt+(1/2)axt2 (11b)
and
vy=vy0+ayt (12a)
y-y0=v0yt+(1/2)ayt2 (12b) - from above equation 11 and 12 ,we can see that for particle moving in (x-y) plane although plane of motion can be treated as two seperate and simultanous 1-D motion with constant acceleration
- Similar result also hold true for motion in a three dimension plane (x-y-z)
Relative velocity in Two Dimension
For two objects A and B moving with the uniform velocities VA and VB.Relative velocity is defined as
VBA=VB-VA
where VBA is relative velocity of B relative to A
Similiary relative velocity of A relative to B
VAB=VA-VB
we will need to add or subtracting components along x & y direction to get the relative velocity
Suppose
vA=vxai + vyaj
vB=vxbi + vybj
Relative velocity of B relative to A
=vxbi + vybj -(vxai + vyaj)
=i(vxb-vxa) + j(vyb-vya)
For three dimensions motion
vA=vxai + vyaj +vzaz
vB=vxbi + vybj + vzbz
Relative velocity of B relative to A
=vxbi + vybj + vzbz -(vxai + vyaj +vzaz)
=i(vxb-vxa) + j(vyb-vya)+z(vyb-vya)
0 comments:
Post a Comment