Let us assume at t = 0 a cart is leaving the origin with zero initial
velocity and constant acceleration of 3 m/s2
in the positive x-direction.
Then a = ∆v/∆t, vf - vi = a(tf - ti), and since vi = ti = 0 we have v(t) = a*t = (3 m/s2)*t.
The velocity (m)/s versus time (s) graph is a straight line with is a straight line passing through the origin with a slope of 3.
The acceleration (m/s2) versus time (s) graph yields a straight line (a = 3) with zero slope.
Let us consider one-dimensional motion in the x-direction.
Let us make this explicit by using the subscript x.
The average acceleration equals the instantaneous acceleration. From
ax = (vxf - vxi)/(tf - ti)
ax(tf - ti) = (vxf - vxi),
vxf = vxi + ax∆t.
The velocity versus time graph is a straight line.
The average velocity in a time interval ∆t therefore is just the sum of the final and the initial velocities divided by 2,
vx(avg) = (vxf + vxi)/2.
The displacement is ∆x = vx(avg)∆t. We can rewrite this expression to obtain xf - xi = ½ (vxf + vxi)∆t, or
xf - xi = vxi∆t + ½ax∆t2.
We can also express the velocity as a function of the displacement.
∆x = ½(vxf + vxi)∆t = ½ (vxf + vxi)(vxf - vxi)/ax = (vxf2 - vxi2)/(2ax) yields
vxf2 = vxi2 + 2ax(xf - xi).
The equations in red are the kinematic equations for motion in the x-direction with constant acceleration.
Link: Kinematic equation solver
Choose your coordinates so that xi = ti = 0. Then x = vit +
This is the equation of a parabola. The position versus time graph is a section of a parabola.
In the limit a = 0 it becomes a straight line.
The speed versus time graph on the right represents the motion of a car. Approximately how far did the car travel during the first 5 seconds?
The speed versus time graph is a straight line.
We have motion with constant acceleration.
The slope of the graph represents the acceleration.
ax = (vxf - vxi)/(tf - ti) = (-40 m/s)/(10 s ) = -4 m/s2.
For motion with constant acceleration we have
∆xi = vxi∆t + ½ax∆t2.
After 5 s we have
∆x = 40m/s * 5 s - ½(4 m/s2)*(5 s)2 = 150 m.
During the first 5 seconds the car traveled 150 m.
A particle is moving with velocity v0 = 60 i (m/s) at t = 0. Between t = 0 and t = 15 s the velocity decreases uniformly to zero. What was the acceleration during this 15 s time interval? What is the significance of the sign in your answer?
Since the velocity decreases uniformly, the acceleration is constant. We therefore have ax = (vxf - vxi)/∆t = (0 - 60 m/s)/15 s = -4m/s2.
The minus sign tells us that the acceleration vector is pointing in the negative x-direction. The velocity and the acceleration vector point in opposite directions. The particle is slowing down.
Blood is accelerated from rest to v = 30.0 cm/s in a distance of 1.80 cm by
the left ventricle of the heart. Assume constant acceleration.
(a) Find the acceleration a.
(b) For how long does the blood accelerate?
(c) Is the answer reasonable when compared with the time for a heartbeat?
(a) Given: vi = 0, vf = 0.3 m/s, ∆v = 0.3 m/s.
xi = 0, xf = 0.018m, ∆x = 0.018 m.
Kinematic equation: vxf2 = vxi2 + 2ax(xf - xi)
Solve for ax = (vxf2 - vxi2)/(2(xf - xi)) = (0.3 m/s)2/(0.036 m) = 2.5 m/s2.
(b) v = at, t = v/a = (0.3 m/s)/(2.5 m/s) = 0.12 s
or vx(avg) = (vxf + vxi)/2 = 0.15 m/s. ∆x = vx(avg)∆t,
∆t = ∆x/vx(avg) = 0.018 m/(0.15 m/s) = 0.12 s.
(c) The figure below shows a typical electrocardiogram waveform. 0.12 s seems a reasonable acceleration time.