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PHYSICS

Case A

Figure 14

1

st

phase

: assuming that the pressure remains constant. Using Gay-Lussac’s first law calculate the volume

V

2

of

the gaswhich is heated from a temperature

t

1

=20+273=293

K

to a temperature

t

2

=50+273=323

K

.

V

1

:

V

2

=

t

1

:

t

2

V

1

*

t

2

=

V

2

*

t

1

V

2

=

V

1

* t

2

t

1

V

2

=

0,98

[dm

3

]

* 323

[K]

V

2

=

1,08

dm

3

293

[K]

Due to only the increase of the temperature of the gas, the volume has increased

V

2

=

1,08

dm

3

.

2

nd

phase

: we observe the behaviour of the volume

V

2

with an increase of double the Force applied on the piston.

F

2

= 2 * F

1

F

2

= 2 * 980

N

F

2

=

1960

N

As a result of the increase in the Force

F

2

, applied to the piston, there is a reduction in the volume

V

3

.

V

2

:

V

3

=

F

2

:

F

1

V

3

=

V

2

* F

1

F

2

V

3

=

1,08

[dm

3

]

* 980

[N]

V

3

=

0,54

dm

3

1960

[N]

Under the action of the Force

F

2

and temperature

t

2

the volume is reduceduntil it reaches

V

3

=

0,54

dm

3

.

Case B

The unit of measurement of the pressure is

Kg/cm

2

, it is possible to calculate the value of the pressure using the

value of the load

F

1

,

F

2

and the surface of the piston.

Figure 14

1

st

phase

: calculation of the area of the piston

S

=

r * r *

π

S

=

25

*

25

*

3,14

S

=

1962,5

mm

2

S

=

19,6

cm

2

Calculate the initial pressure

p

1

:

p

1

=

F

1

980

[N]

50

N

cm

2

p

1

5Kg

cm

2

S

19.6

[cm

2

]

Figure 14

2

nd

phase

: calculation of the final pressure

p

2

:

p

2

=

F

2

1960

[N]

100

N

cm

2

p

2

10Kg

cm

2

S

19.6

[cm

2

]

Load and pressure are directly proportional, using Boyle’s law and substituting the known values gives:

V

2

:

V

3

=

p

2

:

p

1

V

2

*

p

1

=

p

2

*

V

3

V

3

=

V

2

* p

1

p

2

V

3

=

1,08

[dm

3

]

* 50

[N / cm

2

]

V

3

=

0,54

dm

3

100

[N / cm

2

]

In both cases the result is

V

3

=

0,54

dm

3

.

1

23

CAMOZZI

>

PHYSICS