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Cálculo do diâmetro de gotículas de gasolina que levam 1 segundo para cair 10 polegadas, Exercícios de Física

Um problema de física que envolve o cálculo do diâmetro de gotículas de gasolina que levam 1 segundo para cair 10 polegadas, utilizando a segunda lei de newton e dados fornecidos sobre a viscosidade do ar e a densidade da gasolina e da água. O problema é resolvido por meio da integração de duas vezes da equação do movimento e da substituição de m por uma expressão envolvendo o diâmetro d.

Tipologia: Exercícios

2016

Compartilhado em 30/06/2016

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Problem 1.10 [Difficulty: 4]
NOTE : Drag f ormul a is in erro r: It shou ld be:
FD3πVd=
Mg
FD = 3
π
Vd
a = dV/dt
Given: Dat a on sp here and for mula fo r dra g.
Find: Diameter of gasoline droplets that take 1 second to fall 10 in.
Solution: Use given data and data in Appendices; integrate equation of
motion by separating variables.
The data provided, or available in the Appendices, are:
μ4.48 10 7
×lbf s
ft2
= ρw1.94 slug
ft3
= SGgas 0.72=ρgas SGgas ρw
= ρgas 1.40 slug
ft3
=
New ton's 2 nd l aw for the sphere (mass M) is (ignor ing bu oyancy e ffec ts) MdV
dt
Mg3πμVd=
dV
g3πμd
MV
dt=
so
Integrating twice and using limits Vt() Mg
3πμd1e
3πμd
M
t
= xt() Mg
3πμdtM
3πμde
3πμd
M
t
1
+
=
Replacing M with an expression involving diameter d Mρgas
πd3
6
= xt()
ρgas d2
g
18 μt
ρgas d2
18 μe
18μ
ρgas d2
t
1
+
=
This equation must be solved for d so that x1s( ) 10 in= . The answer can be obtained from manual iteration, or by using
Excel's Goal Seek.
d 4.30 10 3
×in=
0 0.025 0.05 0.075 0.1
0.25
0.5
0.75
1
t (s)
x (in)
0 0.25 0.5 0.75 1
2.5
5
7.5
10
t (s)
x (in)
Note That the particle quickly reaches terminal speed, so that a simpler approximate solution would be to solve Mg = 3πµVd for d,
with V = 0.2 5 m/s (a llowing fo r the fact that M is a function of d)!

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Problem 1.10 [Difficulty: 4]

NOTE: Drag formula is in error: It should be:

F

D

= 3 ⋅ π⋅V ⋅d

Mg

FD = 3π Vd

a = dV/dt

Given: Data on sphere and formula for drag.

Find: Diameter of gasoline droplets that take 1 second to fall 10 in.

Solution: Use given data and data in Appendices; integrate equation of

motion by separating variables.

The data provided, or available in the Appendices, are:

μ 4.48 10

− 7

×

lbf s⋅

ft

2

= ⋅ ρ w

slug

ft

3

= ⋅ SG

gas

= 0.72 ρ gas

SG

gas

ρ w

= ⋅ ρ gas

slug

ft

3

Newton's 2nd law for the sphere (mass M) is (ignoring buoyancy effects) (^) M

dV

dt

⋅ =M g⋅ − 3 ⋅ π⋅ μ⋅ V⋅d

dV

g

3 ⋅ π⋅ μ⋅d

M

− ⋅V

= dt

so

Integrating twice and using limits (^) V t( )

M g⋅

3 ⋅ π⋅ μ⋅ d

1 e

− 3 ⋅ π⋅ μ⋅d

M

⋅t

= ⋅ ⎠ x t( )

M g⋅

3 ⋅ π⋅ μ⋅d

t

M

3 ⋅ π ⋅μ ⋅ d

e

− 3 ⋅ π⋅ μ⋅d

M

⋅t

Replacing M with an expression involving diameter d (^) M ρ gas

π d

3

= ⋅ x t( )

ρ gas

d

2

⋅ ⋅g

18 ⋅ μ

t

ρ gas

d

2

18 ⋅ μ

e

− 18 ⋅μ

ρ gas

d

2

⋅ t

This equation must be solved for d so that x 1 s( ⋅) = 10 in⋅. The answer can be obtained from manual iteration, or by using

Excel's Goal Seek.

d 4.30 10

− 3

= × ⋅in

0 0.025 0.05 0.075 0.

1

t (s)

x (in)

0 0.25 0.5 0.75 1

5

10

t (s)

x (in)

Note That the particle quickly reaches terminal speed, so that a simpler approximate solution would be to solve Mg = 3πμ Vd for d ,

with V = 0.25 m/s (allowing for the fact that M is a function of d )!