18. Newton's 2nd Law
18a. The Third Law
18d. Work against
19.Motion in a Circle
20. Newton's Gravity
21. Kepler's 3rd Law
21a.Applying 3rd Law
21b. Fly to Mars! (1)
21c. Fly to Mars! (2)
21d. Fly to Mars! (3)
A cannon weighing 1 ton (metric ton, 1000 kilograms) fires a 10 kg shell at 1000 meters/second. With what velocity does the cannon recoil?
Let us start the solution process by collecting all the given information. Denoting with subscript 1 quantities related to the shell and with subscript 2 those related to the cannon, we have
Shell: m1 = 10 kg
v1 = 1000 m/s
When a problem involves unspecified quantities, the best strategy usually is to give each of them a name and hope for the best: either their actual values can be found, or they will "drop out," showing they are not essential to the solution.
Such "miracles" may happen if all the information needed for the answer is already given. You will need some experience, though, to judge whether or not all vital pieces of information are already on hand.
What missing quantities are needed by the equations? For starters, the forces (F1, F2) on the shell and cannon, the magnitudes of their accelerations (a1, a2) which we assume to be constant (we know they are in directions opposite to each other), and the length of time t during which they act. We now collect equations:
From the second law
F2 = m2a2
which removes forces from the picture. Also:
Divide left by left and right by right in the last equation, to get
which removes the time t. Going back to equation (1), divide both sides by a1m2. Then
Substitute from (2) to (3), or vice versa, and suddenly the accelerations, too, are gone. All that is left is
where everything is known except for the recoil velocity v2. Its value is isolated by multiplying both sides by v1
Our final equation (4) becomes more symmetric if all fractions are eliminated. Multiplying both sides by the product (m2v1) of the denominators gives
The quantity "mass times velocity" (or "the product of mass and velocity") is called momentum (plural: momenta) and is often denoted by the letter P. One way of interpreting the last equation (5) is to state that the momentum given to the cannon equals the momentum given to the shell.
Conservation of MomentumActually, the momentum P, like the velocity v, is a vector quantity. Suppose we regard velocities in one direction as positive and in the opposite direction as negative. Then
v1= 1000 m/s
P1 = m1v1 = 10 kg x 1000 m/s = 10,000 kg-m/s|
v2= – 10 m/s P2 = m2v2 = 1000 kg x (– 10 m/s) = –10,000 kg
Before the gun was fired, neither mass had any velocity and therefore the total momentum P = P1 + P2 was zero. Afterwards, evidently, the total momentum remained zero. This is a general property (and yet another formulation of Newton's laws) and can be stated as
In a system of objects subject to no forces from the outside, the vector sum of all momenta stays the same ("is conserved").
This also works when three or more objects are involved and each moves along a completely different direction. For instance, "the shells bursting in the air" of the US anthem had the same momentum as the collection of fragments and gases produced imediately after they burst, before air resistance had its say. This is also the principle by which a rocket operates--as it throws mass backwards in a fast jet of gas, it receives an amount of forward momentum equal to the backward momentum given to the jet.
EnergyWhen the cannon recoils, it receives as much momentum as the shell. How is the energy E shared? Since
and for the cannon
Very unequal sharing! The cannon, 100 times massive, receives 100 times less energy. Is that the rule?
Substitute equation (1) in the numerator, then cancel (m2v2) above and below to get
By (4), inverted
The lighter mass always receives the lion's share of the energy!
Next Stop: #18c Work
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Author and Curator: Dr. David P. Stern
Mail to Dr.Stern: stargaze("at" symbol)phy6.org .
Last updated: 9-21-2004
Reformatted 24 March 2006