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Set 8. Momentum. Today. There is a new (and easy) WebAssign posted. We begin a new chapter (6) in the textbook. MOMENTUM There is a big connection to music that will become clear. We will come back to one of the skipped chapters later.
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Set 8 Momentum
Today • There is a new (and easy) WebAssign posted. • We begin a new chapter (6) in the textbook. • MOMENTUM • There is a big connection to music that will become clear. • We will come back to one of the skipped chapters later. • There will be a WebAssignment on this material as well, so don’t delay with the current assignment. • More on your grades on Monday.
Gas Molecules Collide Brownian Motion
Something to watch .. • Was this accurate? • What really Happens? • Does this make a difference:
Introduction to Momentum • We know that it is harder to get a more massive object moving from rest than a less massive object. • This is the concept of inertia previously introduced. • Building on the concept of inertia, we ask the question, “How hard is it to stop an object?” • We call this property of an object that is related to both its mass and its velocity, the momentum of the object.
Linear Momentum • The linear momentum of an object is defined as the product of its mass and its velocity, and is measured in “kilogram-meters per second.” • The symbol for momentum is p, as in: p = mv The bold-faced symbols above, momentum and velocity, are vectors with identical direction. Look at the equation. Can you guess why the units are defined this way?
Linear Momentum • So an object may have a large momentum due to a large mass, a large velocity, or both. A slow battleship and a rocket-propelled race car (or kayak) have large momenta. • Conceptual Question: Which has the greater momentum, an 18-wheeler parked at the curb, or a Volkswagen rolling down a hill? • 18 wheeler • VW • Both the same • Can’t tell. CLICKER
Linear Momentum • The word momentum is often used in our everyday language in a much looser sense, but it is still roughly consistent with its meaning in the physics world view; that is, something with a lot of momentum is hard to stop. You have probably heard someone say, “We don’t want to lose our momentum!” Coaches are particularly fond of this word. The catcher is protected from the baseball’s momentum by body armor.
What did Newton Really Say?? Definition The impulse to an object = its change Of momentum.
Fast Or Slow, It Doesn’t Matter To The SystemChanging an Object’s Momentum • Because impulse is a product of two things, there are many ways to produce a particular change in momentum. • For example, two ways of changing an object’s momentum by 10 kilogram-meters per second are: • exert a net force of 5 newtons on the object for 2 seconds, or • exert 100 newtons for 0.1 second. • They each produce an impulse of 10 newton-seconds (N·s) and therefore a momentum change of 10 kilogram-meters per second. • The units of impulse (newton-seconds) are equivalent to those of momentum (kilogram-meters per second).
It Matters To UsChanging an Object’s Momentum • Because our bones break when forces are large, the particular combination of force and time interval is important. • Sometimes, as in a gymnasium, a wood floor may be enough of a cushion; in a car, the dashboards are made from foam rubber. Bumpers and air bags further increase the vehicle’s (and the passengers’) Δt. A pole-vaulter lands on thick pads to increase the collision time and thus reduce the force. Otherwise, this could be a nasty fall.
Landing the Hard WayNo Parachute! • Sometimes accidents can fill in for the lack of a parachute: • During World War II, a Royal Air Force airman jumped in just his uniform from a flaming bomber flying at 18,000 ft. His terminal speed (Ch. 3, p. 46) was 120 mph, but tree branches and then 1½ feet of snow cushioned his fall. The result: minor scratches and bruises. • The record for surviving a fall without a parachute is held by Vesna Vulovic. She was serving as a hostess on a Yugoslavian DC-9 that blew up at 33,330 ft in 1972.
So …. • If you are falling, (or just moving along), you have a certain MOMENTUM, just before you come in contact with what is going to stop you. • Assume that your FINAL velocity (and momentum) will be zero. • Your momentum (final momentum=0) will be the impulse necessary to stop your fall.
AND Smaller Dt Bigger Force
Falls for 4 seconds catch
Stuff • Speed=128 ft/sec • Her weight = 100 lbs • W=mg so her mass = 100/32 ~3 English mass units (slugs) • Momentum = mv = 3x128=384 (appropriate units) • F x Dt=384 • F=384/Dt
How Fast is the Stop?? Note: We ignore the acceleration during the “catch”.
Conservation of Linear Momentum • Imagine standing on a giant skateboard, at rest. • The total momentum of you and the skateboard must be zero, because everything is at rest. • Now suppose that you walk on the skateboard. What happens to the skateboard? • When you walk in one direction, the skateboard moves in the other direction, as shown in the figure. • An analogous thing happens when you fire a rifle: the bullet goes in one direction, and the rifle recoils in the opposite direction.
Conservation of Linear Momentum • The force you exert on the skateboard is, by Newton’s third law, equal and opposite to the force the skateboard exerts on you. • Because you and the skateboard each experience the same force for the same time interval, you must each experience the same-size impulse and, therefore, the same-size change in momentum. • Because the impulses are in opposite directions (red arrows, foot/skateboard & you), the changes in the momenta are also in opposite directions. • Thus, your momentum and that of the skateboard still add to zero. Even though you and the skateboard are moving and, individually, have nonzero momenta, the total momentum remains zero.
Conservation • Consider two objects that are moving (or not) in some way. • NO external forces are applied. • Impulse=FDt=Change in momentum • If FDt=0, The total momentum doesn’t change! • This is conservation of momentum.
Need a Volunteer Scateboarder HEAVY!!
No external force! M v v V M Both at Rest: Total Momentun=0 M v + V =0 M
http://www.youtube.com/watch?v=KL8-PbdRYY0 Conservation of Momentum
Conservation of Linear Momentum • Because the changes in the momenta of the two objects are equal in size and opposite in direction, the value of the total momentum does not change. We say that the total momentum is conserved. • We can generalize these findings. Whenever any object is acted on by a force, there must be at least one other object involved. • This other object might be in actual contact with the first, • or it might be interacting at a distance of 150 million km, but it is there. • Consider the objects as a system. Whenever there is no net force acting on the system from the outside (that is, the system is isolated, or closed), the forces that are involved act only between the objects within the system. As a consequence of Newton’s third law, the total momentum of the system remains constant. • This generalization is known as the law of conservation of linear momentum.
Translation into English • Consider a “system” of “interacting” particles. • At one instant of time add up all the momenta of all of the particles in the system. • Vector addition, of course, but let’s not worry much about that. • Wait some amount of time. • After that time, the sum of the momenta is the same as it was when initially measured. • MOMENTUM IS CONSERVED
Conservation of Linear Momentum • The Law of Conservation of Linear Momentum: • The total linear momentum of a system does not change if there is no net external force. A GAS?? Air ???
ExamplesConservation of Linear Momentum • You experience conservation of momentum firsthand when you try to step from a small boat onto a dock. • As you step toward the dock, the boat moves away from the dock, and you may fall into the water. Although the same effect occurs when we disembark from an ocean liner, the large mass of the ocean liner reduces the speed given it by our stepping off. • A large mass requires a small change in velocity to undergo the same change in momentum.
Linear Momentum: Working It OutConservation of Linear Momentum • If a rifle of mass 4.5 kg fires 10-gram bullets at a speed of 900 m/s (2000 mph), what will be the speed of its recoil? • The magnitude of the momentum p of the bullet is: p = mv = (0.01 kg)(900 m/s) = 9 kg·m/s • Because the total momentum of the bullet and rifle was initially zero, conservation of momentum requires that the rifle recoil with an equal momentum in the opposite direction. If the mass of the rifle is M, the speed V of its recoil is given by =2 m/s
Linear Momentum: Working It OutConservation of Linear Momentum • If you do not hold the rifle snugly against your shoulder, the rifle will hit your shoulder at this speed (2 m/s = 4.5 mph) and hurt you. Question: Why does holding the rifle snugly reduce the recoil effects? Answer: Holding the rifle snugly increases the recoiling mass (your mass is now added to that of the rifle) and therefore reduces the recoil speed.
Collisions • Interacting objects don’t need to be initially at rest for conservation of momentum to be valid. Suppose a ball moving to the left with a certain momentum crashes head-on with an identical ball moving to the right with the same-size momentum. • Before the collision, the two momenta are equal in size but opposite in direction, and because they are vectors, they add to zero. • After the collision the balls move apart with equal momenta in opposite directions. • Because the balls are identical and their masses are the same, the speeds after the collision are also the same. These speeds depend on the ball’s physical properties. • In all cases the two momenta are the same size and in opposite directions, and the total momentum remains zero.
Flawed ReasoningCollisions • A question on the final exam asks, “What do we mean when we claim that the total momentum is conserved during a collision?” The following two answers are given: • Answer 1: Total momentum of the system stays the same before and after the collision. • Answer 2: Total momentum of the system is zero before and after the collision. Which answer (if either) do you agree with? • Answer: While we have considered several examples in which the total momentum of the system is zero, this is not the most general case. The momentum of a system can have any magnitude and any direction before the collision. If momentum is conserved, the momentum of the system always has the same magnitude and direction after the collision. Therefore, answer 1 is correct. This is a very powerful principle because of the word always.
So Far • We defined momentum of an object as the product of its mass (a scalar) and its velocity (a vector). We gave it the symbol p. • p=mv • A ball has a mass of 5 kg (a heavy ball) has a velocity of 10 m/s • Its momentum is • 5 kg x 10 m/s = 50 Kg-m/s
Momentum is conserved! • The momentum of a system of interacting particles (usually 2) is the same both before and after the collision. • Example: • A block has a mass of 1 kg and is stationary and resting quietly on a log. Suddenly it is struck by a 0.25 kg piece of sticky putty moving at 5 m/s. It sticks to the first mass. What happens (frictionless log!)? • This is called an “inelastic collision”.
More Collisions • A boxcar traveling at 10 meters per second approaches a string of four identical boxcars sitting stationary on the track. The moving boxcar collides and links with the stationary cars, and the five boxcars move off together along the track. What is the final speed of the five cars immediately after the collision? • Conservation of momentum tells us that the total momentum must be the same before and after the collision. • Before the collision, one car is moving at 10 meters per second. • After the collision, five identical cars are moving with a common final speed. • Because the amount of mass that is moving has increased by a factor of five, the speed must decrease by a factor of five. The cars will have a final speed of 2 meters per second. • Notice that we did not have to know the mass of each boxcar, only that they all had the same mass. Do It !
Collisions • We can use the conservation of momentum to measure the speed of fast-moving objects. For example, consider determining the speed of an arrow shot from a bow. • We first choose a movable, massive target—a wooden block suspended by strings. Before the arrow hits the block (a), the total momentum of the system is equal to that of the arrow (the block is at rest). • After the arrow is embedded in the block (b), the two move with a smaller, more measurable speed. • The final momentum of the block and arrow just after the collision is equal to the initial momentum of the arrow. Knowing the masses, the arrow’s initial speed can be determined.
Investigating Accidents • Accident investigators use conservation of momentum to reconstruct automobile accidents. • Newton’s laws can’t be used to analyze the collision itself because we do not know the detailed forces involved. Conservation of linear momentum, however, tells us that regardless of the details of the crash, the total momentum of the two cars remains the same. • The total momentum immediately before the crash must be equal to that immediately after the crash.
Investigating Accidents • As an example, consider a rear-end collision. Assume that the front car was stopped and the two cars locked bumpers on impact. • From an analysis of the length of the skid marks made after the collision and the type of surface, the total momentum of the two cars just after the collision can be calculated. • Because one car was stationary, the total momentum before the crash must have been due to the moving car. Knowing that the momentum is the product of mass and velocity (mv), we can compute the speed of the car just before the collision. We can thus determine whether the driver was speeding.
Working It OutInvestigating Accidents • Let’s use conservation of momentum to analyze such a collision. • For simplicity assume that each car has a mass of 1000 kg (a metric ton) and that the cars traveled along a straight line. • Further assume that we have determined that the speed of the two cars locked together was 10 m/s (about 22 mph) after the crash. • The total momentum after the crash was equal to the total mass of the two cars multiplied by their combined speed: • But because momentum is conserved, this was also the value before the crash. Before the crash, however, only one car was moving. So if we divide this total momentum by the mass of the moving car, we obtain its speed: • The car was therefore traveling at 20 m/s (~45 mph) at the time of the accident.
What about this?? • Momentum starts at zero; not moving. • Gas is heated explosively and is pushed out the bottom of the rocket. • This gas has a smaller amount of mass but is being shot out at a very high speed. • In any small instant, a “piece” of gas shoots out and by N3, being pushed out by the rocket, it must be pushing back on the rocket. • Momentum must be conserved! • Swoosh ….. Wanna try it???
So now you know all about momentum! Why do we care?
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