
The freezing point of substances - such as naphthalene - can be determined using the cooling method. The graph of temperature/0C against time/s (known as the cooling curve) is plotted as part of the process to determine the freezing point.
By analysing the graph/cooling curve, (for
example, like the one shown above), the following are deduced
* the freezing point of naphthalene is 800C (where
the line is flat / horizontal)
* the physical state of naphthalene at the section of the curve from P to Q is
liquid
* the physical
states of naphthalene at the section of the curve from Q to R are
liquid and solid
* the physical
state of naphthalene at the section of the curve from R to S is
solid
There is no change in temperature from Q to R because heat is released to form new bonds (attractions) between the particles (molecules) of naphthalene as it changes from liquid to solid.
During this period of the cooling process, the particles / molecules
of naphthalene move more slowly and the motion of the
particles become more restrictive as they lose kinetic energy. The
particles move closer to one another and are arranged in an orderly
manner.
The formation of naphthalene particles in the solid form is an exothermic
process that releases heat energy. This release of heat energy is
balanced by the heat energy that is lost to the surroundings. As a
result, there is no change in temperature during the crystallisation
of naphthalene.


* takat beku naftalena
ialah 800C (bahagian
graf yang mendatar)
* keadaan fizikal naftalena
pada bahagian lengkuk PQ ialah cecair
* keadaan fizikal naftalena
pada bahagian lengkuk QR ialah cecair dan pepejal
* keadaan fizikal naftalena
pada bahagian lengkuk RS ialah pepejal
Tidak terdapat perubahan dalam suhu di antara Q dan R. Ini kerana
haba dibebaskan untuk membentuk ikatan (tarikan) di antara
zarah-zarah (molekul) naftalena
apabila ia bertukar daripada cecair kepada pepejal.
Semasa proses pendinginan, zarah-zarah / molekul-molekul naftalena
bergerak lebih perlahan. Pergerakan zarah-zarah yang terhad ini
adalah disebabkan kehilangan tenaga kinetik. Zarah-zarah juga
bergerak lebih dekat di antara satu sama lain dan tersusun rapat dan
teratur.
Pembentukan zarah-zarah naftalena
dalam keadaan pepejal merupakan proses eksotermik yang membebaskan
tenaga haba. Pembebasan haba ini diseimbangi oleh tenaga haba yang
hilang ke persekitaran. Dengan demikian, tiada perubahan suhu semasa
penghabluran naftalena.