Animated Solution for Physics - Kinematics: A tennis ball is released from a height h and after freely falling on a wooden floor, it rebounds and reaches height h/2. The velocity versus height of the ball during its motion may be represented graphically by (Graphs are drawn schematically and on not to scale)
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Visualized Solution
y=h
Ball is released from rest at height h.
Initial velocity u=0.
v2=u2+2as
Using the third equation of motion:
v2=u2+2g(h−y)
v2=2g(h−y)
Since u=0:
v2=2g(h−y)
Velocity is downward, so v is negative.
Falling Curve
At y=h, v=0
At y=0, v=−2gh
Graph is a parabola in the 4th quadrant.
Rebound
Ball rebounds to height h/2.
Collision is inelastic, kinetic energy is lost.
Rebound Curve
At y=h/2, v=0
Initial rebound velocity v=+gh
Graph is a parabola in the 1st quadrant.
Conclusion
Comparing with options, Option (c) matches our derived graph.
The Way Forward
What if the collision was perfectly elastic?
The ball would rebound to height h.
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The Sigma Insight: Motion in a Straight Line
Solution Diagram
Welcome, future engineers and physicists! Today, we are going to dive into a beautiful problem that perfectly marries physical intuition with graphical representation. We will analyze the motion of a bouncing tennis ball and translate its journey into a velocity-height graph.
Analyzing the Setup
Imagine you are holding a tennis ball at a height h above a solid wooden floor. You release it from rest. The moment you let go, gravity takes over, and the ball begins its free fall.
To translate this physical motion into a mathematical graph, we need our trusty kinematic equations. Since we are interested in the relationship between velocity (v) and height (y), the third equation of motion is our best friend:
v2=u2+2as
The Downward Journey
Let's focus on the fall. The ball starts from rest, so the initial velocity u=0. The acceleration is due to gravity, acting downwards, so a=−g. The displacement from the initial height h to any height y is s=y−h.
Substituting these into our equation, we get:
v2=0+2(−g)(y−h)
v2=2g(h−y)
Notice that v2 is directly proportional to the change in height. Mathematically, this means that if we plot v on the y-axis and h on the x-axis, the relationship y=h−2gv2 represents a parabola.
During the fall, the velocity is directed downwards. By standard convention, we take the downward direction as negative. So, as the height decreases from h to 0, the velocity becomes increasingly negative, starting from 0 and reaching −2gh just before impact. On our graph, this traces a parabolic curve in the fourth quadrant, with an arrow pointing from h towards the negative v-axis.
The Inelastic Rebound
Now comes the exciting part—the collision! The ball hits the floor and rebounds. However, the problem states it only reaches a maximum height of h/2. This tells us that the collision was inelastic; the ball lost some kinetic energy to sound and heat.
For the upward journey, the ball starts at height y=0 with some positive initial velocity v′, and comes to a momentary halt (v=0) at height y=h/2. Using the same kinematic equation:
0=(v′)2−2g(2h)
(v′)2=gh
v′=+gh
Synthesizing the Graph
As the ball rises, its height increases from 0 to h/2, and its positive velocity decreases from +gh to 0. This traces another parabolic curve, this time in the first quadrant. The arrow must point from the positive v-axis towards h/2 on the horizontal axis, indicating the forward flow of time.
When we compare our meticulously constructed graph with the given options, Option (c) is the only one that perfectly captures both the parabolic shapes and the correct directional arrows for the falling and rebounding phases.
Physics is not just about equations; it's about visualizing the story those equations tell. Keep visualizing, and keep conquering!