Materials :
•
Four dierent texts about a pratialexample of funtion.•
Slideshow with the fourformulas and graphs.1 – Team work on one document 25 mins
Workinginteamsoffourorvepeople,studentsworkonatextaboutapratialexample
of funtion. Eah teamhas toprepare apresentation showing
•
in whateld the funtionappears;•
what itused for;•
the formulaof the funtion;•
the graph of the funtion, with preise informationonthe axes.2 – Oral presentations 30 mins
Eah team goesto the board to present their funtion tothe lass.
Anysoundisavibration,aseriesofvariationsofpressure,emittedbyasoure,transmitted
in the air and reeived by our ear. Musial sounds are periodi vibrations,whereas noise
is made of randomvibrations.
A pure sound is a simple, sinusoidal vibration. The number of atual vibrations during
one seond is alled the frequeny. The greater the frequeny, the higher the sound. For
example, the A (la)above middle C(do) on apiano itsusually set toa frequeny of 440
Hz, whihmeans
440
vibrations inone seond.Ofallmusialinstruments,onlysynthesisersanproduepuresounds.Otherinstruments,
suhastheguitarortheviolin,produeamixofdierentpuresounds:aomplexsound.
Let's look more losely at the example of the ute. When playingthe note A with a220
Hz frequeny, a ute emits in fat three simultaneous pure sound : the main one with a
frequeny of 220 Hz,aseond one,more diulttohear, withafrequeny of 440 Hzand
the thirdone,easier tohearthanthe seondbutstillbehindthe mainsound,afrequeny
of 660Hz. The resulting sound an be expressed as a funtion
s
, where the variations ofpressure
s(t)
are given asa funtion of the timet
in seonds :s(t) = 1 sin(220t) + 0.1 sin(440t) + 0.4 sin(660t).
The graph of this funtion is shown below :
0.5 1.0
− 0.5
− 1.0
0.01 0.02 0.03 0.04
− 0.01
− 0.02
− 0.03
− 0.04
− 0.05
Aninome tax isataxleviedbythegovernmentovertheinomeofindividuals,organisa-
tions orompanies. InFrane, theinome taxpaid by eahfamilydepends onthe family
quotient, whih is equal tothe net inome of the family(the total inomeminor various
dedutions) dividedby the number ofpeople inthe family(hildren being ounted as0.5
most of the time).
For a single person, the family quotient is therefore equal to the net inome. The rule
to ompute the inome tax
T
in this ase is given by the government as the followingformula, wherethe net inomeis
I
:T (I) =
0
ifI 6 5687
I × 0.055 − 312.79
if5688 6 I 6 11344 I × 0.14 − 1277.03
if11345 6 I 6 25195 I × 0.30 − 5308.23
if25196 6 I 6 67546 I × 0.40 − 12062.83
ifI > 67546
This funtion an begraphed asshown below:
5 6 8 8 1 1 3 4 4 2 5 1 9 5 6 7 5 4 6
+ + + + + + + + + + +
2000
4000
6000
8000
10000
12000
14000
16000
18000
20000
22000
A volleyballisthrown intothe airby aplayer. During itstrajetory,beforeitreahes the
ground oranother player, the positionof avolleyballan desribed by threeoordinates,
the absissa
x
, the ordinatey
and the altitudez
They all depend on the timet
elapsedsine the momentthe ballwasthrown.
Tosimplifytheproblem,wenegletairfrition,and wealsosupposethat theballdoesn't
move sideways, so that the oordinate
y
isonstant, always equalto0
.In these onditions, the trajetory depends only on three parameters : the initial speed
of the ball, whih is related to the strength and tehnique of the player throwing it, the
initialheight of the ball, and the angle between the ground and the diretion of the ball
when itisthrown. Suppose that theinitialspeed is
v 0 = 12
metersperseond, the initialheightis
2
metersand the angle isα = 30 ◦
.Then, the altitudez
of the ballasa funtionof the absissa
x
, is given by the formulaz(x) = −0.04x 2 + 0.58x + 2.
Thegraphofthisfuntion,shownbelow,givesagraphialrepresentationofthetrajetory,
the groundbeing the
x
-axis.1 2 3 4
2 4 6 8 10 12 14 16 18
z
Radioative deay is the proess in whih an unstable atomi nuleus loses energy by
emittingionisingpartilesand radiation.Thisdeay,orlossof energy,resultsin anatom
of one type,alled the parent nulide,transforming toan atomof adierent type, alled
the daughter nulide. For example : a lead-214 atom (the parent) emits radiation and
transforms to a bismuth-214 atom (the daughter). This is a random proess on the
atomilevel,inthat itisimpossible topreditwhena given atom willdeay, butgiven a
large numberof similar atoms,the deay rate, on average,is preditable.
Thehalf-life ofaradioativenulideisthetimeittakesforhalfthe quantitytotransform.
For the lead-214 atom, it's approximately
27
minutes, or1620
seonds. This means thatif atone moment we have
1
kg of lead-214,then27
minutes later there will onlybe500
gleft, the other
500
g having deayed. Another27
minutes later, only25
g willbe left.Thenumber
N
ofatomsoflead-214thereforedependsonthetimet
sineitrstappeared(forexamplewhenit'sgeneratedbyanotherradioativesubstane,suhasthepolonium-
218). If the initialweight of lead-214 is
1
kg, then the weight aftert
seonds is preiselygiven by the formula
N (t) = 2 − 1620 t .
The graph of this funtion is given below.