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p

A

=

F

A

100

[N]

100

[N]

p

A

=2 * 10

-5

N

m

2

p

A

=

2

bar

S

A

5

[cm

2

]

5 * 10

-4

[m

2

]

We now calculate the Force

F

E

to be applied on the surface

E

in order to keep it in equilibriumwith the piston

A

.

p

E

=

F

E

F

E

=

p

E

*

S

E

2 * 10

5

[N

m

2

]

* 10

-3

[m

2

] =

200

N F

E

=

200

N

S

E

A

F

F

A

E

F

3

4

Fig. 19

Figure 19

Pos. 3

: the pistons

B

and

C

(with the same section) are now replaced by a single piston

E

whose area is the sum

of the areas

B

and

C

(

S

E

=

S

B

+

S

C

). By applying aForce

F

on only piston

A

, itwill be lowered and consequently

piston

E

rises. Maintaining the Force

F

on piston

A

and exerting the same Force

F

on piston

E

, the larger piston

E

will lower, however it will still have a higher level than

A

. Applying the Force

2F

to piston

E

will bring it into

equilibriumwith

A

.

Pos. 4

: eliminate the piston

E

and plug the tank. Introducing a pressure gauge, we note that in every point of the

metal sheet of the tank the pressure is the same.

Figure 18

Pos. 1

: a tank containing liquid is connected to the pistons

A

and

B

of equal sectionwhich exert the same Force

F

.

Regardless of the section of the tank and of themounting position, the level of the pistons is identical.

By increasing the Force

F

on one of the two pistons, the other will rise.

Pos. 2

: a third piston

C

, of equal section, is added next to

B

. Exerting a Force

F

only on piston

A

, pistons

B

and

C

will rise equally. Applying the same Force

F

on the pistons

A

and

B

, theywill achieve equilibrium, piston

C

will

move upwards. In the case in which the same Force

F

is applied to piston

C

, the three pistons will be positioned

at the same height.

F

F

A

B

F

A

B

C

F

F

1

2

Fig. 18

The explanation of the phenomena described above is illustrated in

Pascal’s principle

, which states that:

pressure

exerted anywhere in a confined incompressible fluid is transmitted equally in all directions throughout the fluid

such that the pressure ratio (initial difference) remains the same

.

Figure 20

Observe the physical effects of this principle:

Assuming that the piston

A

has a section

S

A

=5

cm

2

and the Force

F

A

=100

N

;

calculate the pressure exerted on the fluid

(1

N

/

m

2

=1

bar

= 1 * 10

-5

P

a

)

A

E

F = 100N

S =10 cm

2

E

S =5 cm

2

A

2bar

A

F =?

E

Fig. 20

1

28

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PHYSICS