Chapter 3 Acceleration and free fall - Light and Matter
Chapter 3 Acceleration and free fall - Light and Matter
Chapter 3 Acceleration and free fall - Light and Matter
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it must be zero.<br />
128 <strong>Chapter</strong> 4 Force <strong>and</strong> motion<br />
In a future physics course or in another textbook, you may encounter<br />
the term “net force,” which is simply a synonym for total<br />
force.<br />
What happens if the total force on an object is not zero? It<br />
accelerates. Numerical prediction of the resulting acceleration is the<br />
topic of Newton’s second law, which we’ll discuss in the following<br />
section.<br />
This is the first of Newton’s three laws of motion. It is not<br />
important to memorize which of Newton’s three laws are numbers<br />
one, two, <strong>and</strong> three. If a future physics teacher asks you something<br />
like, “Which of Newton’s laws are you thinking of?,” a perfectly<br />
acceptable answer is “The one about constant velocity when there’s<br />
zero total force.” The concepts are more important than any specific<br />
formulation of them. Newton wrote in Latin, <strong>and</strong> I am not<br />
aware of any modern textbook that uses a verbatim translation of<br />
his statement of the laws of motion. Clear writing was not in vogue<br />
in Newton’s day, <strong>and</strong> he formulated his three laws in terms of a concept<br />
now called momentum, only later relating it to the concept of<br />
force. Nearly all modern texts, including this one, start with force<br />
<strong>and</strong> do momentum later.<br />
An elevator example 1<br />
⊲ An elevator has a weight of 5000 N. Compare the forces that the<br />
cable must exert to raise it at constant velocity, lower it at constant<br />
velocity, <strong>and</strong> just keep it hanging.<br />
⊲ In all three cases the cable must pull up with a force of exactly<br />
5000 N. Most people think you’d need at least a little more than<br />
5000 N to make it go up, <strong>and</strong> a little less than 5000 N to let it down,<br />
but that’s incorrect. Extra force from the cable is only necessary<br />
for speeding the car up when it starts going up or slowing it down<br />
when it finishes going down. Decreased force is needed to speed<br />
the car up when it gets going down <strong>and</strong> to slow it down when it<br />
finishes going up. But when the elevator is cruising at constant<br />
velocity, Newton’s first law says that you just need to cancel the<br />
force of the earth’s gravity.<br />
To many students, the statement in the example that the cable’s<br />
upward force “cancels” the earth’s downward gravitational force implies<br />
that there has been a contest, <strong>and</strong> the cable’s force has won,<br />
vanquishing the earth’s gravitational force <strong>and</strong> making it disappear.<br />
That is incorrect. Both forces continue to exist, but because they<br />
add up numerically to zero, the elevator has no center-of-mass acceleration.<br />
We know that both forces continue to exist because they<br />
both have side-effects other than their effects on the car’s center-ofmass<br />
motion. The force acting between the cable <strong>and</strong> the car continues<br />
to produce tension in the cable <strong>and</strong> keep the cable taut. The