00:01
So we need to remember that the heat, delta q, that's transferred or lost by an object that has a mass m and a specific heat c, when it changes temperature by change delta t, is equal to m times c times delta t.
00:23
This is the difference in the heat energy.
00:27
Also, remember that the total energy of a closed system is conserved.
00:35
So the change in energy for a closed system is equal to zero.
00:40
In our case, we have water of mass mh, initially at a temperature, th, that is poured into an aluminum cup that has a mass m -a -l that already contains a mass t -h that already contains a mass t -h that is poured into an aluminum cup that is poured into an aluminum cup that has a mass m -a -l that already contains.
00:59
Of water, mc, initially at a temperature tc, such that th is greater than tc.
01:12
And we can assume that the cup of water also is in thermoacilibrium with the water itself, so the temperature of the aluminum cup is also m -a -l, i'm sorry, is also t -c...