• Aucun résultat trouvé

Le meilleur humidificateur

N/A
N/A
Protected

Academic year: 2022

Partager "Le meilleur humidificateur"

Copied!
2
0
0

Texte intégral

(1)

http://people.missouristate.edu/lesreid/ADVarchives.html

Missouri State University’s Advanced Problem May 2011

Vincent Pantaloni (Orléans, France)

Problem : A humidifier has a circular disk of radius r that slowly rotates. It is partially submerged in a tank of water (the disk is perpendicular to the surface of the water). In order to have the greatest humidifying effect, the total area of the wetted part of the disk that is above the water should be maximized. How high above the surface of the water should the center of the disk be to attain this maximum ?

Source : James Stewart Solution :

Here’s a picture of what is happening. We want to find AB=x, such that the blue area is as great as possible. Notice that if we find θ, we findxbeacuse x=rcos

θ 2

. Let’s call Athe blue area. A is the area of the whole ring minus the white circular seg- mentW.

A=π(r2−x2)− W (1) W is the area of the circular sectorADC minus the area of the triangleADC, so withb=DC we have :

W=πr2× θ 2π−1

2b×x= r2 2

θ−b

r ×x r

Ab

Cercle

b

B d

b

C W

A

b

D

θ= 144.7 x

b

E

b

F

b

G

b

H

b

If you consider the right triangle ABC you will see that x

r = cosθ 2 and b

r = 2× b/2

r = 2 sinθ 2. So b

r×x

r = 2 sinθ 2cosθ

2 = sinθ. That gives us a nice formula for W : W=r2

2 (θ−sinθ) (2)

Sincex=rcosθ2 the blue areaAis a function ofθ. Using (1) and (2) we get : A(θ) =π

r2−r2cos2θ 2

−r2

2 (θ−sinθ)

= r2 2

2π+ sinθ−2πcos2θ 2 −θ

= r2

2 (2π+f(θ))

We are now looking for the value ofθ∈[0;π]for whichf(θ) = sinθ−2πcos2θ2−θreaches it’s maximum.

http://prof.pantaloni.free.fr mail me

(2)

http://people.missouristate.edu/lesreid/ADVarchives.html

Let’s differentiatef and have some fun with trigonometry : f(θ) = cosθ−2π×2 cosθ

2 ×

−1 2sinθ

2

−1

= cosθ+π×2 cosθ 2×sinθ

2−1

= cosθ+πsinθ−1

=p π2+ 1

1

√π2+ 1cosθ+ π

√π2+ 1sinθ

−1

=p

π2+ 1×cos

θ−Acos 1

√π2+ 1

−1

Now solving f(θ)>0forθ∈[0;π]gives : f(θ)>0 ⇐⇒ p

π2+ 1×cos

θ−Acos 1

√π2+ 1

−1>0

⇐⇒ cos

θ−Acos 1

√π2+ 1

> 1

√π2+ 1

⇐⇒ θ−Acos 1

√π2+ 1 6Acos 1

√π2+ 1 (BecauseAcosis a decreasing function.)

⇐⇒ θ62Acos 1

√π2+ 1

This shows that f andAare max when

θ= 2Acos 1

√π2+ 1

This angle is approximately equal to 144.7˚as shown on the figure of the previous page. To answer the question we need x=rcos

θ 2

.

x= r

√π2+ 1 ≈0.303×r

http://prof.pantaloni.free.fr mail me

Références

Documents relatifs

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des

Tableau 1 : Liste des différents critères de diagnostic/classification établis sur la MB ...49 Tableau 2 : Critères diagnostiques définis par l’ISG ...50 Tableau 3 :

 The quenching in water allows to burned mortar to recover a portion of its compressive strength (approximately 40%) resulting of a new rehydration of the

(1) The relative centerline displacement of the free surface dependsprimarily upon the momentum flux for values of zo/do great enough that the nozzle acts as a point source

Sensitivity analysis of short-term (24-week) regimen durability and virologic failure among 13,546 antiretroviral na ve HIV-infected patients in the Antiretroviral

10 to 40 Ω.m split into more or less lenses of resistivity: we expect that this corresponds to small sandy aquifers within a clayey background (this.. place the “Beauce”

Tab. 1 presents the physical and mechanical properties of mortar reinforced by Alfa fibers. It’s clearly noticed that the incorporation of Alfa fibers increases the

In previous work (Kaewprasit et al., 1998) a relationship between the specific surface area of International Calibration Cotton Standards (ICCS) fibers, measured by adsorption