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Transcript of Chapter-2
Chapter-2
Motion Along a Straight Line
Ch 2-1 Motion Along a Straight Line
Motion of an object along a straight line
Object is point mass Motion along a horizontal or vertical
or inclined (line with finite slope) line Motion: Change in position No change in position, body at rest
Axis are used to define position of an object
Position of an object defined with respect to origin of an axis
Position x of an object is its distance from the origin at any time t
Displacement x, a vector, is change in position.
x = xf-xi
When an object changes its position, it has a velocity
Ch 2-3 Position and Displacement
Ch 2-4 Average Velocity, Average Speed
Average Velocity vavg= x/ t
vavg = (xf-xi) /(tf-ti) Average speed Savg: a scalar
Savg = total distance/ total time Instantaneous Velocity v: v= lim (x/ t) t0 Position-time graph used to
define object position at any time t and to calculate its velocity
v is slope of the line on position-time graph
Ch 2-6 Acceleration
When an object changes its velocity, it undergoes an acceleration
Average acceleration aavg
aavg = v/ t = (vf-vi) /(tf-ti) Instantaneous acceleration
a: a= lim (v/ t) t0 = dv/dt=d2x/dt2
Velocity-time graph used to define object velocity at any time t and calculate its acceleration
a is slope of the line on velocity-time graph
Constant Acceleration: Variable Slope of position-
time graph Constant Slope of velocity
-time graph Zero Slope of acceleration
-time graph For constant acceleration a =aavg= (vf-vi)/(tf-ti)
vavg= (vf+vi)/2
Ch 2-7 Constant Acceleration
Equations for Motion with Constant Acceleration
v=v0+at x-x0=v0t+(at2)/2 v2=v0
2+2a(x-x0) x-x0=t(v+v0)/2 x-x0 =vt-(at2)/2
Ch 2-9 Free Fall Acceleration
Free fall acceleration ‘g’ due to gravity
Directed downward towards Earth’s center along negative y-axis
with a = -g = -9.8 m/s2
equations of motion with constant acceleration are valid for free fall motion
x-x0=vt
x-x0= v dt
v dt= area between velocity curve and time axis from t0 to t
Similarly v-v0= a dt
a dt = area between acceleration curve and time axis from t0 to t
Ch 2-10 Graphical Integration in Motion Analysis