drive Graphical the equation for position time relation for an object travelling distance S in time T under uniform acceleration
Answers
Answered by
9
There are two kinematic equations connecting velocity and time.
Consider a velocity-time graph of an object which moves with uniform acceleration as shown in Fig below.
Object has initial velocity u at point A, which increases to value v, point B, in time t. The velocity changes at a uniform rate =a.
We draw perpendicular lines BC and BE from point B on time and velocity axes respectively.
Initial velocity is represented by OA, the final velocity is represented by BC and the time interval t is represented by OC.
BD = BC – CD, is the change in velocity during time t.
Draw AD parallel to OC.
In the figure
BC = BD + DC = BD + OA
Now BC = v and OA = u
Therefore we get
v = BD + u
⇒ BD = v−u ........(1)
We know that rate of change of velocity is acceleration a
∴a=change in velocitytime taken
⇒a=BDAD=BDOC
Since OC = t we get
a=BDt
⇒BD=at .............(2)
From (1) and (2) we get
v=u+at .......(3)
From the Fig. the distance traveled s by the object is the area of the trapezium OABC.
Now
Area of OABC= area of the rectangle OADC + area of the Δ ABD
∴s= OA × OC + 12 (AD × BD) .......(4)
Substituting OA = u, OC = AD = tand BD = at, in (4) we get
s=u×t+12(t×at)
⇒s=ut+12at2 .......(5)
=.=.=.=.=.=.=.=.=.=.=.=.=.=.=.=.=.=.=.=.=.=
For sake of completeness
Kinematic Equation for Position-Velocity relation is established as follows.
In the velocity-time graph shown in the Fig. above the distance s travelled by the object in time t while moving under uniform acceleration ais the area of the trapezium OABC. From geometry we know that
Area of the trapezium OABC=OA+BC2× OC
Substituting OA = u, BC = v and OC = t we get
s=u+v2×t .......(5)
The velocity-time relation (3) can be rewritten as
t=v−ua ...........(6)
Substituting value of t from (6) in (5) we get
s=v+u2×v−ua
⇒2as=v2–u2
Consider a velocity-time graph of an object which moves with uniform acceleration as shown in Fig below.
Object has initial velocity u at point A, which increases to value v, point B, in time t. The velocity changes at a uniform rate =a.
We draw perpendicular lines BC and BE from point B on time and velocity axes respectively.
Initial velocity is represented by OA, the final velocity is represented by BC and the time interval t is represented by OC.
BD = BC – CD, is the change in velocity during time t.
Draw AD parallel to OC.
In the figure
BC = BD + DC = BD + OA
Now BC = v and OA = u
Therefore we get
v = BD + u
⇒ BD = v−u ........(1)
We know that rate of change of velocity is acceleration a
∴a=change in velocitytime taken
⇒a=BDAD=BDOC
Since OC = t we get
a=BDt
⇒BD=at .............(2)
From (1) and (2) we get
v=u+at .......(3)
From the Fig. the distance traveled s by the object is the area of the trapezium OABC.
Now
Area of OABC= area of the rectangle OADC + area of the Δ ABD
∴s= OA × OC + 12 (AD × BD) .......(4)
Substituting OA = u, OC = AD = tand BD = at, in (4) we get
s=u×t+12(t×at)
⇒s=ut+12at2 .......(5)
=.=.=.=.=.=.=.=.=.=.=.=.=.=.=.=.=.=.=.=.=.=
For sake of completeness
Kinematic Equation for Position-Velocity relation is established as follows.
In the velocity-time graph shown in the Fig. above the distance s travelled by the object in time t while moving under uniform acceleration ais the area of the trapezium OABC. From geometry we know that
Area of the trapezium OABC=OA+BC2× OC
Substituting OA = u, BC = v and OC = t we get
s=u+v2×t .......(5)
The velocity-time relation (3) can be rewritten as
t=v−ua ...........(6)
Substituting value of t from (6) in (5) we get
s=v+u2×v−ua
⇒2as=v2–u2
Attachments:
Similar questions