
What value (to two decimal places, say) should we assign to the
instantaneous velocity of the melon at time t=1 sec?
f:= t -> 6 + 100*t - 16*t^2;and then calculating average velocities over short intervals which begin or end at t=5:
(f(5.01) - f(5))/ (5.01-5);
(f(5)-f(4.99))/(5-4.99);and so forth. What value would you assign for the instantaneous velocity at t=5?
vav := t -> (f(t+h)-f(t))/h;This will give the average velocity over the time interval [t,t+h] once we have assigned a value to h. Do part (a) again using vav. Then use vav to find the instantaneous velocity at several (at least three) other values of t.
plot({f(t),vav(t)},t=0..6)
Do this several times with decreasing values of h (but only turn in
\it one plot). What do the graphs of all the 'vav' s have in
common? How do they differ? How is the graph of f(t) related
to that of vav(t) . In particular how does f behave
when vav is positive? negative? big? small? -- Is this
behavior precise or only approximate?
plot(f(t),t=0..15,numpoints=250);This statement forces Maple to compute 250 points exactly before trying to ``connect the dots''. (How many points you want to use becomes an accuracy-versus-resources issue, since doing more points takes longer and uses more memory.)
fsolve(diff(f(x),x)=0,x,-5..0)to look only for a solution in the interval [-5,0]. Explain in words what you did and why you did it.
Now think back to last week -- you've previously seen graphs like the ones you just drew. Your graphs should remind you of the graphs of exponential functions. One way to check this out is to see (using Maple) if the derivatives of exponential functions are proportional to themselves:
All right, we have found some (in fact all) solutions to differential equations of the form y'(x)=ay(x), but the relationship between the b in our solutions and the a in the differential equation might seem to be pretty obscure. Mathematicians have come up with a convention which saves us from the trouble of having to figure out the relationship between b and a each time. To do this, they have settled on the name e (in Maple, it's E) for the number with the property that the exponential function y=e^x (and in fact y=Ke^x for any constant K) satisfies our differential equation with proportionality constant a=1. In other words, the derivative of the function y=e^x is precisely y=e^x itself.
F_{net} = mg - bv
where b is the constant of proportionality of air resistance on the skydiver. In general b will depend on the shape of the falling object, so you can reduce b by curling into a ball or increase it by going to the usual spread-eagle position to maximize your time in the air. As the skydiver speeds up, eventually, no matter what value of b is used, the skydiver will hit terminal velocity, the speed at which the drag force equals the gravitational force and no more acceleration occurs. For the spread-eagle position, the terminal velocity is about 130 miles/hour or roughly 60 meters/s. With this information, we can quickly solve for the acceleration at any given time from our previous equation:
a = g - b/m * v
At the terminal velocity, by definition, a = 0, so,
0 = g - b/m * v_t ==> b/m = g/v_t
Thus, we can replace b/m in our original equation of
motion to get
a = g * (1 - v/v_t)
(Warning! this is not as easy as it looks! Make good use of Maple's Help facility and the instructors if you have trouble doing this!).
Make a plot to display your result. How long after starting the jump does it take for the skydiver to reach a speed within 5 m/s of the terminal velocity? Just for fun, can you explain how to find the distance fallen as a function of time? Bonus points will be awarded for those who can produce a correct plot of position vs. time.
The number of pennies always decreases when you
toss them (or at best does not change)
The number of pennies that ``decay'' on any given toss is proportional to the number of pennies you tossed (you cannot lose more pennies than you tossed, but yet the more you toss, the more you tend to lose)
The number of pennies we started with was 100Considering the above, write down the change equation that describes the behavior listed. Your equation should show the number of pennies that will decay for any particular toss. Remember, we assume that the number of decays depends only on the number of pennies we have just before each toss. You'll see later how to make use of the specific number of pennies you started with. Once you have the equation, use Maple to solve it. What functional form do you get? Now try to find the values of the variables which gives the best ``fits'' to your data for the pennies. We can now extrapolate our observations by asking what would happen if we used dice instead of pennies, where a die is said to ``decay'' if it lands, say, with one dot showing up? In this case, we assume a fair die so that the probability of any particular number showing up is about 1/6 for each toss of a die. What do you predict the curve for an experiment of $> 100$\ dice would look like? What would you expect for the theoretical curve which fits the data taken in the experiment? Try it out! Not every group needs to assume that one dot facing up indicates decay. You are allowed to choose which number of dots facing up shows a decayed die.

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