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Reply to comment on: "Convective flow of granular masses under vertical vibrations"

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HAL Id: jpa-00212401

https://hal.archives-ouvertes.fr/jpa-00212401

Submitted on 1 Jan 1990

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Reply to comment on: ”Convective flow of granular

masses under vertical vibrations”

C. Laroche, S. Douady, S. Fauve

To cite this version:

(2)

700

Reply

to

comment

on:

"Convective flow of

granular

masses

under vertical vibrations"

C.

Laroche,

S.Douady

and S. Fauve

Ecole Normale

Supérieure

de

Lyon,

46 allée

d’Italie,

69364

Lyon,

France

Evesque

claims that the air flow

generated by

the bottom

plate

vibration has no effect in our

experiments.

This is

perfectly

exact and we have not mentioned this

effect,

known as "acoustic

streaming",

in our article. We have written that the effect of the air on the

particles

"results from their motion in the

surrounding

fluid"

(see

our

paper

abstract for

instance).

As said

by

Evesque

in his comment last

remark,

he has not "discussed the effect of

quasistatic surrounding compressible

and viscous fluid on this

pile". Consequently

we don’t understand how he can conclude that the

air effect is

negligible

in our

experiments

without

discussing

the relevant mechanism.

Since the comment of

Evesque

reports

incompletely

our results and can lead to wrong

inter-pretations

about the

physics

of the convective

granular

flow,

let us add a few remarks:

- The main effect of the

surrounding

fluid is to make the thinner

parts

of the

grain layer

collide with the vessel base earlier

(not

to

"carry

grains"

as said

by

Evesque).

- We have

reported

the existence of convective motions when vacuum is

performed

in the

case of narrow cells. This is not

quoted by

Evesque

in his comment, and is

perhaps

the case of his own

experiments.

In the narrow cell

configuration,

we think that the thicker

parts

collide later because of the arch effect.

- The condition that the thinner

parts

collide

earlier,

and the existence of two

regions

of different

packing

structure

during

the

collision,

are necessary to

generate

the convective motion. This is induced in

general by

the

surrounding

fluid,

and in narrow cells

by

the lateral boundaries. Then an

averaged

horizontal flow is created from a vertical excitation. This is the mechanism of the convective flow.

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