Skip to content Skip to navigation

OpenStax_CNX

You are here: Home » Content » Collisions of Extended Bodies in Two Dimensions

Navigation

Recently Viewed

This feature requires Javascript to be enabled.

Tags

(What is a tag?)

These tags come from the endorsement, affiliation, and other lenses that include this content.
 

Collisions of Extended Bodies in Two Dimensions

Module by: OpenStax College. E-mail the author

Summary:

  • Observe collisions of extended bodies in two dimensions.
  • Examine collision at the point of percussion.

Note: You are viewing an old version of this document. The latest version is available here.

Bowling pins are sent flying and spinning when hit by a bowling ball—angular momentum as well as linear momentum and energy have been imparted to the pins. (See Figure 1). Many collisions involve angular momentum. Cars, for example, may spin and collide on ice or a wet surface. Baseball pitchers throw curves by putting spin on the baseball. A tennis player can put a lot of top spin on the tennis ball which causes it to dive down onto the court once it crosses the net. We now take a brief look at what happens when objects that can rotate collide.

Consider the relatively simple collision shown in Figure 2, in which a disk strikes and adheres to an initially motionless stick nailed at one end to a frictionless surface. After the collision, the two rotate about the nail. There is an unbalanced external force on the system at the nail. This force exerts no torque because its lever arm rr size 12{r} {} is zero. Angular momentum is therefore conserved in the collision. Kinetic energy is not conserved, because the collision is inelastic. It is possible that momentum is not conserved either because the force at the nail may have a component in the direction of the disk’s initial velocity. Let us examine a case of rotation in a collision in Example 1.

Figure 1: The bowling ball causes the pins to fly, some of them spinning violently. (credit: Tinou Bao, Flickr)
A bowling ball, just as it is striking the pins.
Figure 2: (a) A disk slides toward a motionless stick on a frictionless surface. (b) The disk hits the stick at one end and adheres to it, and they rotate together, pivoting around the nail. Angular momentum is conserved for this inelastic collision because the surface is frictionless and the unbalanced external force at the nail exerts no torque.
Figure a shows a disc m sliding toward a motionless stick M of length r pivoted about a nail, on a frictionless surface. In figure b, a disk hits the stick at one end and adheres to it, and the stick rotates, pivoting around the nail in a direction shown by the arrow in the clockwise direction and angular velocity omega.

Example 1: Rotation in a Collision

Suppose the disk in Figure 2 has a mass of 50.0 g and an initial velocity of 30.0 m/s when it strikes the stick that is 1.20 m long and 2.00 kg.

(a) What is the angular velocity of the two after the collision?

(b) What is the kinetic energy before and after the collision?

(c) What is the total linear momentum before and after the collision?

Strategy for (a)

We can answer the first question using conservation of angular momentum as noted. Because angular momentum is size 12{Iω} {}, we can solve for angular velocity.

Solution for (a)

Conservation of angular momentum states

L=L,L=L, size 12{L=L'} {}
(1)

where primed quantities stand for conditions after the collision and both momenta are calculated relative to the pivot point. The initial angular momentum of the system of stick-disk is that of the disk just before it strikes the stick. That is,

L=,L=, size 12{L=Iω} {}
(2)

where II size 12{I} {} is the moment of inertia of the disk and ωω size 12{ω} {} is its angular velocity around the pivot point. Now, I=mr2I=mr2 size 12{I= ital "mr" rSup { size 8{2} } } {} (taking the disk to be approximately a point mass) and ω=v/rω=v/r size 12{ω=v/r} {}, so that

L=mr2vr=mvr.L=mr2vr=mvr. size 12{L= ital "mr" rSup { size 8{2} } { {v} over {r} } = ital "mvr"} {}
(3)

After the collision,

L=Iω.L=Iω. size 12{L'=I'ω'} {}
(4)

It is ω ω size 12{ω rSup { size 8{'} } } {} that we wish to find. Conservation of angular momentum gives

Iω=mvr.Iω=mvr. size 12{I'ω'= ital "mvr"} {}
(5)

Rearranging the equation yields

ω=mvrI,ω=mvrI, size 12{ω'= { { ital "mvr"} over {I'} } } {}
(6)

where II size 12{I'} {} is the moment of inertia of the stick and disk stuck together, which is the sum of their individual moments of inertia about the nail. (Reference) gives the formula for a rod rotating around one end to be I=Mr2/3I=Mr2/3 size 12{I= ital "Mr" rSup { size 8{2} } /3} {}. Thus,

I=mr2+Mr23=m+M3r2.I=mr2+Mr23=m+M3r2. size 12{I'= ital "mr" rSup { size 8{2} } + { { ital "Mr" rSup { size 8{2} } } over {3} } = left (m+ { {M} over {3} } right )r rSup { size 8{2} } } {}
(7)

Entering known values in this equation yields,

I=0.0500 kg+0.667 kg1.20 m2=1.032 kgm2.I=0.0500 kg+0.667 kg1.20 m2=1.032 kgm2. size 12{I'= left (0 "." "0500"" kg"+0 "." "667 kg" right ) left (1 "." "20"" m" right ) rSup { size 8{2} } =1 "." "032"" kg" cdot m rSup { size 8{2} } } {}
(8)

The value of II is now entered into the expression for ωω, which yields

ω=mvrI=0.0500 kg30.0 m/s1.20 m1.032 kgm2=1.744 rad/s1.74 rad/s.ω=mvrI=0.0500 kg30.0 m/s1.20 m1.032 kgm2=1.744 rad/s1.74 rad/s.
(9)

Strategy for (b)

The kinetic energy before the collision is the incoming disk’s translational kinetic energy, and after the collision, it is the rotational kinetic energy of the two stuck together.

Solution for (b)

First, we calculate the translational kinetic energy by entering given values for the mass and speed of the incoming disk.

KE = 1 2 mv 2 = ( 0 . 500 ) 0 . 0500 kg 30 . 0 m/s 2 = 22.5 J KE = 1 2 mv 2 = ( 0 . 500 ) 0 . 0500 kg 30 . 0 m/s 2 = 22.5 J size 12{"KE"= { {1} over {2} } ital "mv" rSup { size 8{2} } =0 "." "500" left (0 "." "0500"" kg" right ) left ("30" "." 0" m/s" right ) rSup { size 8{2} } ="22" "." 5" J"} {}
(10)

After the collision, the rotational kinetic energy can be found because we now know the final angular velocity and the final moment of inertia. Thus, entering the values into the rotational kinetic energy equation gives

KE′=12Iω2= ( 0.5 ) 1.032 kgm21.744rads2=1.57 J.KE′=12Iω2= ( 0.5 ) 1.032 kgm21.744rads2=1.57 J.
(11)

Strategy for (c)

The linear momentum before the collision is that of the disk. After the collision, it is the sum of the disk’s momentum and that of the center of mass of the stick.

Solution of (c)

Before the collision, then, linear momentum is

p=mv=0.0500 kg30.0 m/s=1.50 kgm/s.p=mv=0.0500 kg30.0 m/s=1.50 kgm/s. size 12{p= ital "mv"= left (0 "." "0500"" kg" right ) left ("30" "." 0" m/s" right )=1 "." "50"" kg" cdot "m/s"} {}
(12)

After the collision, the disk and the stick’s center of mass move in the same direction. The total linear momentum is that of the disk moving at a new velocity v=v= size 12{v'=rω'} {} plus that of the stick’s center of mass,

which moves at half this speed because vCM=r2ω=v2vCM=r2ω=v2 size 12{v rSub { size 8{"CM"} } = left ( { {r} over {2} } right )ω'= { {v'} over {2} } } {}. Thus,

p=mv+MvCM=mv+Mv2.p=mv+MvCM=mv+Mv2. size 12{p'= ital "mv"'+ ital "Mv" rSub { size 8{"CM"} } '= ital "mv"'+ { { ital "Mv"'} over {2} } } {}
(13)

Gathering similar terms in the equation yields,

p = m + M 2 v p = m + M 2 v size 12{p'= left (m+ { {M} over {2} } right )v'} {}
(14)

so that

p=m+M2.p=m+M2. size 12{p'= left (m+ { {M} over {2} } right )rω'} {}
(15)

Substituting known values into the equation,

p=1.050 kg1.20 m1.744 rad/s=2.20 kgm/s.p=1.050 kg1.20 m1.744 rad/s=2.20 kgm/s.
(16)

Discussion

First note that the kinetic energy is less after the collision, as predicted, because the collision is inelastic. More surprising is that the momentum after the collision is actually greater than before the collision. This result can be understood if you consider how the nail affects the stick and vice versa. Apparently, the stick pushes backward on the nail when first struck by the disk. The nail’s reaction (consistent with Newton’s third law) is to push forward on the stick, imparting momentum to it in the same direction in which the disk was initially moving, thereby increasing the momentum of the system.

The above example has other implications. For example, what would happen if the disk hit very close to the nail? Obviously, a force would be exerted on the nail in the forward direction. So, when the stick is struck at the end farthest from the nail, a backward force is exerted on the nail, and when it is hit at the end nearest the nail, a forward force is exerted on the nail. Thus, striking it at a certain point in between produces no force on the nail. This intermediate point is known as the percussion point.

An analogous situation occurs in tennis as seen in Figure 3. If you hit a ball with the end of your racquet, the handle is pulled away from your hand. If you hit a ball much farther down, for example, on the shaft of the racquet, the handle is pushed into your palm. And if you hit the ball at the racquet’s percussion point (what some people call the “sweet spot”), then little or no force is exerted on your hand, and there is less vibration, reducing chances of a tennis elbow. The same effect occurs for a baseball bat.

Figure 3: A disk hitting a stick is compared to a tennis ball being hit by a racquet. (a) When the ball strikes the racquet near the end, a backward force is exerted on the hand. (b) When the racquet is struck much farther down, a forward force is exerted on the hand. (c) When the racquet is struck at the percussion point, no force is delivered to the hand.
In figure a, a disk hitting a stick is compared to a tennis ball being hit by a racquet. When the ball strikes the racquet near the end with a force denoted by f ball as shown by the direction of the arrow, a backward force, f hand is exerted on the hand, In figure b, when the racquet is struck much farther down by a force F ball, a forward force, f hand is exerted on the hand as shown by the arrows. In figure (c), when the racquet is struck by the ball with a force f ball at the percussion point, no force is delivered to the hand. This implies that f hand is equal to zero.

Check Your Understanding

Is rotational kinetic energy a vector? Justify your answer.

Solution

No, energy is always scalar whether motion is involved or not. No form of energy has a direction in space and you can see that rotational kinetic energy does not depend on the direction of motion just as linear kinetic energy is independent of the direction of motion.

Section Summary

  • Angular momentum LL is analogous to linear momentum and is given by L=L= size 12{L=Iω} {}.
  • Angular momentum is changed by torque, following the relationship net τ = Δ L Δ t . net τ = Δ L Δ t .
  • Angular momentum is conserved if the net torque is zero L = constant net τ = 0 L = constant net τ = 0 or L = L net τ = 0 L = L net τ = 0 . This equation is known as the law of conservation of angular momentum, which may be conserved in collisions.

Conceptual Questions

Exercise 1

Describe two different collisions—one in which angular momentum is conserved, and the other in which it is not. Which condition determines whether or not angular momentum is conserved in a collision?

Exercise 2

Suppose an ice hockey puck strikes a hockey stick that lies flat on the ice and is free to move in any direction. Which quantities are likely to be conserved: angular momentum, linear momentum, or kinetic energy (assuming the puck and stick are very resilient)?

Exercise 3

While driving his motorcycle at highway speed, a physics student notices that pulling back lightly on the right handlebar tips the cycle to the left and produces a left turn. Explain why this happens.

Problems & Exercises

Exercise 1

Repeat Example 1 in which the disk strikes and adheres to the stick 0.100 m from the nail.

Solution

(a) 0.156 rad/s0.156 rad/s

(b) 1.17×102 J1.17×102 J size 12{1 "." "17" times "10" rSup { size 8{ - 2} } " J"} {}

(c) 0.188 kgm/s0.188 kgm/s size 12{0 "." "188 kg" cdot "m/s"} {}

Exercise 2

Repeat Example 1 in which the disk originally spins clockwise at 1000 rpm and has a radius of 1.50 cm.

Exercise 3

Twin skaters approach one another as shown in Figure 4 and lock hands. (a) Calculate their final angular velocity, given each had an initial speed of 2.50 m/s relative to the ice. Each has a mass of 70.0 kg, and each has a center of mass located 0.800 m from their locked hands. You may approximate their moments of inertia to be that of point masses at this radius. (b) Compare the initial kinetic energy and final kinetic energy.

Figure 4: Twin skaters approach each other with identical speeds. Then, the skaters lock hands and spin.
Figure a shows two skaters from the top view approaching each other from opposite directions with velocity v. In figure b two skaters then lock their right hands and start to spin in the clockwise direction with angular velocity omega.

Solution

(a) 3.13 rad/s

(b) Initial KE = 438 J, final KE = 438 J

Exercise 1

Suppose a 0.250-kg ball is thrown at 15.0 m/s to a motionless person standing on ice who catches it with an outstretched arm as shown in Figure 5.

(a) Calculate the final linear velocity of the person, given his mass is 70.0 kg.

(b) What is his angular velocity if each arm is 5.00 kg? You may treat his arms as uniform rods (each has a length of 0.900 m) and the rest of his body as a uniform cylinder of radius 0.180 m. Neglect the effect of the ball on his center of mass so that his center of mass remains in his geometrical center.

(c) Compare the initial and final total kinetic energies.

Figure 5: The figure shows the overhead view of a person standing motionless on ice about to catch a ball. Both arms are outstretched. After catching the ball, the skater recoils and rotates.
Figure a shows a skater through an overhead view with both his hands outstretched. A ball is seen approaching toward him in air with velocity v. Figure b shows that skater catching two balls in his left hand, and then, recoiling toward the left, in clockwise direction, with angular velocity omega and finally, the balls have velocity v prime.

Exercise 4

Repeat Example 1 in which the stick is free to have translational motion as well as rotational motion.

Solution

(a) 1.70 rad/s

(b) Initial KE = 22.5 J, final KE = 2.04 J

(c) 1.50 kgm/s1.50 kgm/s size 12{1 "." "50 kg" cdot "m/s"} {}

Content actions

Download module as:

Add module to:

My Favorites (?)

'My Favorites' is a special kind of lens which you can use to bookmark modules and collections. 'My Favorites' can only be seen by you, and collections saved in 'My Favorites' can remember the last module you were on. You need an account to use 'My Favorites'.

| A lens I own (?)

Definition of a lens

Lenses

A lens is a custom view of the content in the repository. You can think of it as a fancy kind of list that will let you see content through the eyes of organizations and people you trust.

What is in a lens?

Lens makers point to materials (modules and collections), creating a guide that includes their own comments and descriptive tags about the content.

Who can create a lens?

Any individual member, a community, or a respected organization.

What are tags? tag icon

Tags are descriptors added by lens makers to help label content, attaching a vocabulary that is meaningful in the context of the lens.

| External bookmarks