Gibbs Free Energy - Equilibrium Constant, Enthalpy & Entropy - Equations & Practice Problems

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00:00:00.000
in this video we're going to focus on
00:00:02.949 00:00:02.959 Delta s entropy enthalpy Delta H and
00:00:07.039 00:00:07.049 Delta G gives free energy so let's start
00:00:10.490 00:00:10.500 with Delta s Delta s is associated with
00:00:14.629 00:00:14.639 entropy and it's basically a measure of
00:00:17.510 00:00:17.520 disorder so the more disorder a system
00:00:21.230 00:00:21.240 has the higher the entropy so we need to
00:00:24.950 00:00:24.960 know is that solids solids have low
00:00:30.740 00:00:30.750 entropy values because the atoms in the
00:00:34.459 00:00:34.469 solid are more organized than the atoms
00:00:37.010 00:00:37.020 in the gas gas molecules they have a
00:00:41.330 00:00:41.340 very high entropy value so let's say if
00:00:48.080 00:00:48.090 you have a reaction let's say carbon
00:00:56.740 00:00:56.750 reacts with oxygen gas to produce two
00:01:06.649 00:01:06.659 carbon dioxide molecules now this
00:01:12.380 00:01:12.390 reaction would you say the change in
00:01:15.170 00:01:15.180 entropy is positive or is it negative
00:01:19.450 00:01:19.460 how would you predict the sign of Delta
00:01:21.859 00:01:21.869 s so notice that we have two gas
00:01:25.219 00:01:25.229 molecules on the right side but only one
00:01:27.560 00:01:27.570 gas model can left and solid so we said
00:01:30.530 00:01:30.540 have a very low entropy value so we
00:01:32.510 00:01:32.520 don't have to worry about it so because
00:01:34.520 00:01:34.530 we have more gas molecules on the right
00:01:36.760 00:01:36.770 the reaction went from a low entropy
00:01:40.249 00:01:40.259 State to a high entropy State so
00:01:42.140 00:01:42.150 therefore we can predict that the sign
00:01:44.120 00:01:44.130 of Delta s will be positive we can say
00:01:46.340 00:01:46.350 that the entropy increases as the
00:01:48.770 00:01:48.780 reaction goes from left to right now
00:01:54.050 00:01:54.060 what about
00:01:57.030 00:01:57.040 the condensation of water as water goes
00:02:00.690 00:02:00.700 from a gas to a liquid predict the sign
00:02:03.810 00:02:03.820 of Delta s for this reaction so as we
00:02:08.070 00:02:08.080 mentioned before gases they have high
00:02:10.050 00:02:10.060 entropy values and liquids relative to a
00:02:13.950 00:02:13.960 gas they have low entropy values so if
00:02:16.620 00:02:16.630 you're going from high to low the change
00:02:18.540 00:02:18.550 in entropy is negative the entropy of
00:02:21.000 00:02:21.010 the system is decreasing now what about
00:02:27.980 00:02:27.990 this example let's say if we have two
00:02:32.250 00:02:32.260 sulfur dioxide molecules and reacts with
00:02:36.450 00:02:36.460 a single oxygen molecule to produce two
00:02:43.020 00:02:43.030 sulphur trioxide molecules is the entry
00:02:48.210 00:02:48.220 change of the system is it positive or
00:02:49.920 00:02:49.930 is it negative what would you say so the
00:02:54.180 00:02:54.190 phases are all the same so let's look at
00:02:55.890 00:02:55.900 the number of gas molecules we have
00:02:57.180 00:02:57.190 three gas molecules on the left two on
00:02:59.160 00:02:59.170 the right so we're going from a system
00:03:01.710 00:03:01.720 of high entropy to a system of low
00:03:04.350 00:03:04.360 entropy so since the change in entropy
00:03:06.930 00:03:06.940 is negative Delta s or the entropy is
00:03:10.979 00:03:10.989 decreasing so Delta s is negative
00:03:16.009 00:03:16.019 consider this example let's say if we
00:03:18.120 00:03:18.130 have magnesium oxide which is a solid
00:03:21.330 00:03:21.340 and it reacts with gaseous carbon
00:03:25.170 00:03:25.180 dioxide to produce solid magnesium
00:03:30.449 00:03:30.459 carbonate predict a sign of Delta s for
00:03:35.340 00:03:35.350 this reaction so we have a solid and a
00:03:39.030 00:03:39.040 gas on the left side so because we have
00:03:41.250 00:03:41.260 the gas we have a system of high entropy
00:03:43.860 00:03:43.870 on the left side we only have a solid on
00:03:46.080 00:03:46.090 the right so the entropy on the right is
00:03:49.500 00:03:49.510 low so as we go from high to low Delta s
00:03:52.320 00:03:52.330 is negative since the entropy is
00:03:54.660 00:03:54.670 decreasing as you go from left to right
00:04:00.050 00:04:00.060 now let's say if you have two gases
00:04:04.470 00:04:04.480 let's say carbon dioxide but one of them
00:04:09.420 00:04:09.430 is at a temperature of 300 Kelvin and
00:04:11.280 00:04:11.290 the other sample is at 400 Kelvin which
00:04:15.800 00:04:15.810 system has a higher entropy value is it
00:04:21.420 00:04:21.430 the one on the left or the one on the
00:04:22.740 00:04:22.750 right now if you have the same substance
00:04:27.120 00:04:27.130 at the same phase it's going to be the
00:04:30.060 00:04:30.070 one with the higher temperature this is
00:04:32.430 00:04:32.440 going to have a higher entropy system
00:04:33.960 00:04:33.970 because at a higher temperature the gas
00:04:36.719 00:04:36.729 molecules move faster in more chaotic
00:04:38.790 00:04:38.800 and so you have less organization and
00:04:42.810 00:04:42.820 keep in mind as you increase the
00:04:43.860 00:04:43.870 temperature of a solid the solid will
00:04:46.469 00:04:46.479 eventually melt into a liquid and if you
00:04:48.570 00:04:48.580 continue to heat it it will become a gas
00:04:50.310 00:04:50.320 so raising the temperature causes the
00:04:52.529 00:04:52.539 system to be to have a higher entropy
00:04:55.050 00:04:55.060 value to be more chaotic and so the one
00:04:59.010 00:04:59.020 with the higher temperature has the
00:05:00.390 00:05:00.400 higher entry value and the one of the
00:05:02.100 00:05:02.110 lower temperature has the lower entropy
00:05:04.170 00:05:04.180 value now let's say if you have three
00:05:09.870 00:05:09.880 compounds calcium carbonate actually
00:05:14.250 00:05:14.260 let's say calcium oxide
00:05:21.170 00:05:21.180 liquid water
00:05:27.620 00:05:27.630 selenium dioxide gas and selenium
00:05:33.590 00:05:33.600 trioxide gas if you have to rank these
00:05:39.260 00:05:39.270 in order of increase in entropy how
00:05:42.590 00:05:42.600 would you do it let's say number one has
00:05:44.000 00:05:44.010 the lowest entropy and number four has
00:05:46.070 00:05:46.080 the highest well we know solids have
00:05:49.640 00:05:49.650 very low entropy so that's going to be
00:05:51.200 00:05:51.210 the lowest then it's the liquid and then
00:05:53.150 00:05:53.160 it's the gas now between these two gas
00:05:55.190 00:05:55.200 molecules which one has more entropy
00:05:58.240 00:05:58.250 when comparing two molecules at the same
00:06:00.560 00:06:00.570 temperature the one that has a higher
00:06:02.870 00:06:02.880 entropy is the one that has more atoms
00:06:04.250 00:06:04.260 two one it's more complicated in
00:06:05.630 00:06:05.640 structure so this is going to be number
00:06:08.030 00:06:08.040 three and because this has four atoms
00:06:09.740 00:06:09.750 instead of three this is number four
00:06:11.840 00:06:11.850 this one has the highest entropy now
00:06:16.490 00:06:16.500 consider this reaction
00:06:32.290 00:06:32.300 let's say if you're given the entropy
00:06:36.400 00:06:36.410 values for each of these gases so let's
00:06:43.540 00:06:43.550 say this reaction occurs at a
00:06:44.830 00:06:44.840 temperature where water is in a gaseous
00:06:47.140 00:06:47.150 state as opposed to liquid state and
00:06:49.540 00:06:49.550 let's say the entry value for hydrogen
00:06:51.850 00:06:51.860 is about 131 402 it's about 205 and for
00:06:57.700 00:06:57.710 water let's say it's about 189 how can
00:07:01.270 00:07:01.280 you use this data to calculate the
00:07:02.740 00:07:02.750 change in entropy for the reaction to
00:07:06.030 00:07:06.040 find the change in entropy for the
00:07:08.080 00:07:08.090 reaction you would you can use the same
00:07:09.850 00:07:09.860 method as you would to find the change
00:07:12.100 00:07:12.110 in enthalpy Delta H for the reaction
00:07:13.890 00:07:13.900 which is basically the sum of the
00:07:16.000 00:07:16.010 products minus the sum of the reactants
00:07:21.480 00:07:21.490 so for the products we have just two
00:07:25.270 00:07:25.280 water molecules and for the reactants
00:07:29.980 00:07:29.990 which is on the Left we have two
00:07:31.960 00:07:31.970 hydrogen molecules one oxygen molecule
00:07:33.820 00:07:33.830 and so we just got to plug in the
00:07:35.500 00:07:35.510 information so it's going to be two
00:07:38.020 00:07:38.030 times 189 minus 2 times 1 31
00:07:46.290 00:07:46.300 Plus 205 for o2
00:07:56.310 00:07:56.320 so two times 189 that's about 378 and
00:08:03.810 00:08:03.820 don't forget to distribute the negative
00:08:05.620 00:08:05.630 sign 2 times 131 that's negative 262
00:08:08.920 00:08:08.930 we're going to have negative 205 so if
00:08:12.610 00:08:12.620 you combine these numbers you should get
00:08:15.510 00:08:15.520 an entropy value of negative 89 now if
00:08:20.470 00:08:20.480 you're using a standard thermodynamic
00:08:21.580 00:08:21.590 table it's going to have the unit's
00:08:23.860 00:08:23.870 joules per mole per Kelvin and so that's
00:08:27.430 00:08:27.440 how you can calculate the entropy of a
00:08:29.380 00:08:29.390 reaction now there are some other
00:08:33.339 00:08:33.349 equations that you need to know
00:08:34.719 00:08:34.729 regarding entropy Delta s can be
00:08:38.320 00:08:38.330 calculated by taking Q the amount of
00:08:41.350 00:08:41.360 heat that's absorbed or released in the
00:08:43.330 00:08:43.340 system divided by the temperature and
00:08:46.740 00:08:46.750 this must be a reversible process by the
00:08:49.420 00:08:49.430 way so keep in mind Delta s has unit
00:08:54.370 00:08:54.380 joules per mole per Kelvin which means Q
00:08:58.810 00:08:58.820 has to have the unit's joules per mole
00:09:01.060 00:09:01.070 and the temperature of course is going
00:09:03.430 00:09:03.440 to be in Kelvin now there are some other
00:09:06.550 00:09:06.560 things need to know about entropy
00:09:09.870 00:09:09.880 especially as it relates to the second
00:09:12.280 00:09:12.290 law of thermodynamics for a spontaneous
00:09:17.830 00:09:17.840 reaction the entropy of the universe
00:09:21.000 00:09:21.010 which is the sum of the change in
00:09:23.890 00:09:23.900 entropy of the system plus the change in
00:09:28.840 00:09:28.850 entropy of the surroundings is always
00:09:33.430 00:09:33.440 greater than zero for process that is
00:09:36.130 00:09:36.140 spontaneous would basically the second
00:09:38.440 00:09:38.450 law of thermodynamics states that the
00:09:40.000 00:09:40.010 entropy of the universe increases for a
00:09:42.520 00:09:42.530 spontaneous process now for a process
00:09:47.470 00:09:47.480 that is reversible where the system is
00:09:51.340 00:09:51.350 at equilibrium than the entropy of the
00:09:53.860 00:09:53.870 universe which is the sum of the entropy
00:09:59.980 00:09:59.990 of the system plus the change in entropy
00:10:02.800 00:10:02.810 of the surroundings that's going to be
00:10:07.180 00:10:07.190 equal to zero
00:10:09.180 00:10:09.190 if it's a reversible process at
00:10:13.090 00:10:13.100 equilibrium
00:10:21.079 00:10:21.089 now if it's spontaneous then it's going
00:10:25.699 00:10:25.709 to be greater than zero the entropy of
00:10:27.139 00:10:27.149 the universe increases for a spontaneous
00:10:29.059 00:10:29.069 process but if it's reversible then the
00:10:33.499 00:10:33.509 entropy of the universe can equal zero
00:10:35.479 00:10:35.489 if it's at a system of equilibrium
00:10:39.189 00:10:39.199 now another equation that you need to
00:10:41.419 00:10:41.429 know is this one Delta G which
00:10:44.809 00:10:44.819 represents the change in free energy
00:10:47.349 00:10:47.359 also known as Gibbs free energy is equal
00:10:49.849 00:10:49.859 to Delta H to change the enthalpy change
00:10:52.359 00:10:52.369 minus T times Delta s now Delta G
00:10:57.879 00:10:57.889 represents the amount of free energy
00:11:01.129 00:11:01.139 that's available to do useful work and
00:11:04.779 00:11:04.789 it usually has the unit's it could be in
00:11:07.669 00:11:07.679 joules per mole or kilojoules per mole
00:11:11.619 00:11:11.629 Delta H is usually provided in
00:11:13.849 00:11:13.859 kilojoules per mole the temperature is
00:11:17.419 00:11:17.429 in Kelvin now Delta s is usually
00:11:20.119 00:11:20.129 provided in joules per mole but you need
00:11:21.709 00:11:21.719 to convert it to kilojoules per mole to
00:11:25.129 00:11:25.139 make this equation work now Delta H is
00:11:30.169 00:11:30.179 usually the amount of heat energy that's
00:11:32.389 00:11:32.399 absorbed or release in a system at a
00:11:34.639 00:11:34.649 constant pressure Delta G is the amount
00:11:37.669 00:11:37.679 of free energy that's available to do
00:11:39.259 00:11:39.269 useful work Delta S which is entropy we
00:11:43.729 00:11:43.739 described it as a measure of disorder of
00:11:45.559 00:11:45.569 a system but it can also be described as
00:11:47.869 00:11:47.879 the energy that's unavailable to do
00:11:51.589 00:11:51.599 useful work so typically when you
00:11:54.439 00:11:54.449 whenever you have a process let's say
00:11:55.759 00:11:55.769 like a combustible heat engine and if
00:12:00.279 00:12:00.289 you can generate heat let's say if you
00:12:04.099 00:12:04.109 have a system at high temperature and
00:12:07.729 00:12:07.739 let's say the surroundings is at low
00:12:09.259 00:12:09.269 temperature heat flows from hot to cold
00:12:14.109 00:12:14.119 now some of that heat energy can be used
00:12:16.579 00:12:16.589 to do useful work however some of the
00:12:20.869 00:12:20.879 heat energy will also radiate out into
00:12:23.749 00:12:23.759 the surroundings and that energy will be
00:12:25.579 00:12:25.589 lost and so you can think of entropy as
00:12:30.379 00:12:30.389 the dispersal of energy in a way
00:12:33.620 00:12:33.630 as that heat energy leaves into the
00:12:35.449 00:12:35.459 surrounding to the temperature of the
00:12:36.740 00:12:36.750 surrounding to go up and whenever the
00:12:38.300 00:12:38.310 temperature goes up the entropy of that
00:12:40.460 00:12:40.470 of the surroundings will go up as well
00:12:42.620 00:12:42.630 and so that heat energy loss it's hard
00:12:46.970 00:12:46.980 to get it back it's hard to use it to do
00:12:48.860 00:12:48.870 what useful work because it's gone so
00:12:53.300 00:12:53.310 another way to describe entropy is the
00:12:55.730 00:12:55.740 dispersal of energy or the energy that's
00:12:58.069 00:12:58.079 unavailable to do useful work now there
00:13:02.269 00:13:02.279 are some other things you need to know
00:13:03.610 00:13:03.620 when Delta G is negative the reaction is
00:13:09.379 00:13:09.389 spontaneous in the forward direction so
00:13:13.100 00:13:13.110 if it's spontaneous in the forward
00:13:14.300 00:13:14.310 direction that means it's a non
00:13:16.430 00:13:16.440 spontaneous in the reverse direction
00:13:18.970 00:13:18.980 when Delta G is zero the system is at
00:13:23.150 00:13:23.160 equilibrium and so the rate of the
00:13:27.019 00:13:27.029 forward reaction equals the rate of the
00:13:28.759 00:13:28.769 reverse reaction so at that point the
00:13:31.730 00:13:31.740 reaction is reversible and when Delta G
00:13:34.939 00:13:34.949 is positive the reaction is non
00:13:38.689 00:13:38.699 spontaneous in the four direction which
00:13:42.439 00:13:42.449 means that it's spontaneous in the
00:13:44.300 00:13:44.310 reverse direction so those are some
00:13:47.360 00:13:47.370 things that you need to know regarding
00:13:48.679 00:13:48.689 the sign of Delta G now when Delta H is
00:13:55.639 00:13:55.649 negative that means that the reaction is
00:13:58.249 00:13:58.259 exothermic that means that heat energy
00:14:01.120 00:14:01.130 is being released from the system into
00:14:04.519 00:14:04.529 the ceramics and when Delta H is
00:14:07.160 00:14:07.170 positive the reaction is endothermic
00:14:09.740 00:14:09.750 that means heat energy is being absorbed
00:14:12.530 00:14:12.540 by the system from the surroundings now
00:14:20.929 00:14:20.939 here's the question for you let's say if
00:14:22.629 00:14:22.639 you have the enthalpy change of the
00:14:25.460 00:14:25.470 reaction let's say it's negative 100
00:14:31.600 00:14:31.610 kilojoules per mole and you also have
00:14:35.629 00:14:35.639 the entropy change of the reaction let's
00:14:38.960 00:14:38.970 say this is positive 200 joules per mole
00:14:45.049 00:14:45.059 per Kelvin
00:14:48.850 00:14:48.860 S is always positive but the change in s
00:14:52.189 00:14:52.199 can be positive or negative by the way
00:14:55.689 00:14:55.699 now let's say the temperature is 300
00:14:58.429 00:14:58.439 Kelvin using this information how can
00:15:01.189 00:15:01.199 you calculate Delta G of this reaction
00:15:04.119 00:15:04.129 how can you find the amount of free
00:15:07.340 00:15:07.350 energy that is available to do useful
00:15:09.470 00:15:09.480 work so let's use the equation Delta G
00:15:15.049 00:15:15.059 is equal to Delta H minus T Delta s so
00:15:19.309 00:15:19.319 Delta H is in kilojoules per mole minus
00:15:24.980 00:15:24.990 the temperature now Delta s is in joules
00:15:27.559 00:15:27.569 per mole per Kelvin so if you plug in
00:15:29.960 00:15:29.970 200 you will not get the answer right
00:15:31.460 00:15:31.470 you need to make sure the unit's match
00:15:32.989 00:15:32.999 so we need to divide 200 by a thousand
00:15:35.989 00:15:35.999 to convert joules in to kilojoules so
00:15:39.170 00:15:39.180 200 joules is the same as point to
00:15:41.420 00:15:41.430 kilojoules and now it can work so this
00:15:44.480 00:15:44.490 is going to be negative 100 and 300
00:15:47.360 00:15:47.370 times 0.2 well 3 times 300 times 2 is
00:15:52.249 00:15:52.259 600 so 300 times 0.2 must be 60 so this
00:15:56.150 00:15:56.160 is going to be negative 60 and so Delta
00:16:01.429 00:16:01.439 G is equal to negative 116 kilojoules
00:16:04.730 00:16:04.740 per mole for this particular example so
00:16:07.519 00:16:07.529 whenever you use the equation make sure
00:16:10.009 00:16:10.019 that these two units match if you want
00:16:12.889 00:16:12.899 to get the right answer now let's say if
00:16:17.389 00:16:17.399 you have Delta H for a certain process
00:16:21.740 00:16:21.750 let's say it's 300 kilojoules per mole
00:16:25.610 00:16:25.620 and you also have Delta S which is
00:16:35.560 00:16:35.570 150 joules per mole per Kelvin now let's
00:16:41.960 00:16:41.970 say these values correspond to the
00:16:46.190 00:16:46.200 vaporization of a substance how can you
00:16:48.920 00:16:48.930 calculate the boiling point of that
00:16:52.070 00:16:52.080 substance used in Delta H and Delta s so
00:16:55.250 00:16:55.260 let's say the substance is B we'll call
00:16:57.800 00:16:57.810 it um some substance B at the boiling
00:17:03.500 00:17:03.510 point the liquid and the gas phase they
00:17:07.760 00:17:07.770 coexist so at that temperature these two
00:17:11.090 00:17:11.100 they're reversible they can the liquid
00:17:13.340 00:17:13.350 can go into the gas phase and the gas
00:17:14.990 00:17:15.000 molecules can go back into the liquid
00:17:16.460 00:17:16.470 phase so we have a reversible system so
00:17:19.640 00:17:19.650 how can we estimate the temperature of
00:17:21.610 00:17:21.620 the boiling point of the substance so we
00:17:27.980 00:17:27.990 can use this equation Delta G is equal
00:17:29.930 00:17:29.940 to Delta H minus T Delta s so at the
00:17:35.000 00:17:35.010 boiling point or at the phase change of
00:17:38.000 00:17:38.010 a substance in this case the liquid and
00:17:42.200 00:17:42.210 gas coexist because we have a reversible
00:17:44.210 00:17:44.220 reaction the system is at equilibrium
00:17:46.270 00:17:46.280 whenever the system is at equilibrium
00:17:48.080 00:17:48.090 Delta G is zero and so since we have the
00:17:51.830 00:17:51.840 values of Delta H and Delta s we can
00:17:54.260 00:17:54.270 solve for T let's add T Delta s to both
00:17:59.000 00:17:59.010 sides
00:18:04.300 00:18:04.310 you
00:18:10.970 00:18:10.980 so this is what we now have now to solve
00:18:14.000 00:18:14.010 for the temperature and when you set
00:18:15.230 00:18:15.240 divide both sides by Delta s and so the
00:18:20.150 00:18:20.160 temperature or the boiling point
00:18:23.090 00:18:23.100 temperature is equal to the change in
00:18:25.580 00:18:25.590 enthalpy divided by the change in
00:18:27.230 00:18:27.240 entropy so that's how you can find the
00:18:29.480 00:18:29.490 boiling point of a substance if you know
00:18:32.780 00:18:32.790 Delta H Delta F so you could just divide
00:18:34.520 00:18:34.530 the two so Delta H is 300 kilojoules
00:18:41.500 00:18:41.510 well actually let's convert kilojoules
00:18:44.000 00:18:44.010 inch into joules because these units
00:18:45.740 00:18:45.750 they have to match so 300 kilojoules is
00:18:51.230 00:18:51.240 the same as 300 thousand joules to
00:18:54.920 00:18:54.930 convert kilojoules to joules you need to
00:18:57.830 00:18:57.840 multiply by a thousand and to convert
00:19:00.320 00:19:00.330 Joules to kilojoules he needs to divide
00:19:03.200 00:19:03.210 by a thousand so since we're going from
00:19:05.900 00:19:05.910 kilojoules to joules we'll multiply
00:19:07.160 00:19:07.170 three hundred by thousand so we have
00:19:09.230 00:19:09.240 three hundred thousand joules per mole
00:19:10.610 00:19:10.620 and Delta s we can leave it as 150
00:19:13.250 00:19:13.260 joules per mole per Kelvin
00:19:19.960 00:19:19.970 so the units joules per mole will cancel
00:19:23.110 00:19:23.120 given us the Kelvin temperature so
00:19:26.259 00:19:26.269 what's three hundred thousand divided by
00:19:28.360 00:19:28.370 150 well we know we can at least cancel
00:19:33.009 00:19:33.019 a zero and so what we now have is 30,000
00:19:38.850 00:19:38.860 divided by 15 30,000 is basically 30
00:19:43.029 00:19:43.039 times a thousand and 30 is 15 times two
00:19:49.769 00:19:49.779 so we can cancel the 15s so what we have
00:19:53.919 00:19:53.929 left over is two times a thousand which
00:19:56.379 00:19:56.389 is two thousand so for this particular
00:19:58.990 00:19:59.000 substance based on the information that
00:20:00.669 00:20:00.679 we have the boiling point is two
00:20:03.129 00:20:03.139 thousand Kelvin now if we want to we can
00:20:09.730 00:20:09.740 convert Kelvin into Celsius by
00:20:12.820 00:20:12.830 subtracting it by 273 so 17 this is
00:20:18.820 00:20:18.830 going to be 17 27 degrees Celsius make
00:20:24.220 00:20:24.230 sure my math is correct yeah that's
00:20:27.580 00:20:27.590 right so keep in mind the Kelvin
00:20:29.350 00:20:29.360 temperature is the Celsius temperature
00:20:31.450 00:20:31.460 plus 273 so if you need to find a
00:20:33.850 00:20:33.860 Celsius temperature and subtract the
00:20:35.289 00:20:35.299 Kelvin temperature by 273 now the next
00:20:42.789 00:20:42.799 thing we need to talk about is how to
00:20:44.740 00:20:44.750 tell if a reaction is going to be
00:20:47.259 00:20:47.269 spontaneous at low temperature high
00:20:50.320 00:20:50.330 temperature or if it's always
00:20:54.850 00:20:54.860 spontaneous or never spontaneous so you
00:20:58.509 00:20:58.519 can find this out based on the equation
00:21:00.460 00:21:00.470 Delta G is equal to Delta H minus T
00:21:02.470 00:21:02.480 Delta s but first let me give you the
00:21:04.450 00:21:04.460 table they need to know
00:21:43.880 00:21:43.890 l stands for low temperature H stands
00:21:46.669 00:21:46.679 for high temperature
00:21:55.070 00:21:55.080 so let's say if Delta H is positive and
00:21:59.049 00:21:59.059 if Delta s is positive is it going to be
00:22:03.169 00:22:03.179 spontaneous at low temperature or at
00:22:04.970 00:22:04.980 high temperature now if both were
00:22:09.680 00:22:09.690 positive it's going to be spontaneous at
00:22:13.029 00:22:13.039 high temperature so that means that it's
00:22:18.139 00:22:18.149 going to be spawned non spontaneous at
00:22:20.060 00:22:20.070 low temperature so at little temperature
00:22:24.350 00:22:24.360 the sine is positive which means that
00:22:26.299 00:22:26.309 it's non spontaneous and at high
00:22:28.940 00:22:28.950 temperature it's negative which means
00:22:32.299 00:22:32.309 that it's spontaneous so I want you to
00:22:34.460 00:22:34.470 understand the way I wrote it
00:22:36.220 00:22:36.230 so I'm going to highlight at high
00:22:39.440 00:22:39.450 temperature it's spontaneous so those
00:22:44.239 00:22:44.249 two correspond to each other now what
00:22:45.889 00:22:45.899 about if Delta H is positive and if
00:22:48.799 00:22:48.809 Delta s is negative is the spontaneous
00:22:52.310 00:22:52.320 non spontaneous how would you describe
00:22:55.190 00:22:55.200 it now Delta H is positive for this term
00:22:58.549 00:22:58.559 is positive and if Delta s is negative
00:23:00.879 00:23:00.889 and while T Reddy has a negative sign
00:23:03.320 00:23:03.330 plus this is negative which means it's
00:23:05.060 00:23:05.070 positive so everything is positive so it
00:23:08.090 00:23:08.100 doesn't matter what the temperature is
00:23:09.169 00:23:09.179 it's always going to be positive so
00:23:12.979 00:23:12.989 regardless if the system is at low
00:23:15.200 00:23:15.210 temperature or at high temperature Delta
00:23:17.450 00:23:17.460 G is always positive which means that
00:23:19.039 00:23:19.049 it's non spontaneous for all temperature
00:23:21.499 00:23:21.509 whenever Delta H is positive and Delta s
00:23:23.840 00:23:23.850 is negative now what about the next one
00:23:26.570 00:23:26.580 when Delta H is negative but Delta s is
00:23:28.700 00:23:28.710 positive so if Delta s is positive what
00:23:34.460 00:23:34.470 that means is that the first term is
00:23:36.560 00:23:36.570 going to be negative and the second term
00:23:38.629 00:23:38.639 negative and a positive is negative
00:23:39.919 00:23:39.929 whenever you add two negative numbers is
00:23:42.019 00:23:42.029 always going to be negative so at any
00:23:44.599 00:23:44.609 temperature under these conditions is
00:23:47.060 00:23:47.070 always Delta G will always be negative
00:23:48.560 00:23:48.570 so it's always going to be spontaneous
00:23:50.529 00:23:50.539 so I'm just going to put a negative sign
00:23:52.549 00:23:52.559 which means that it's always spontaneous
00:23:54.289 00:23:54.299 regardless of the temperature if it's a
00:23:56.599 00:23:56.609 low or high now when Delta H and Delta s
00:24:00.440 00:24:00.450 are both negative it's going to be
00:24:03.320 00:24:03.330 spontaneous at low temperature which
00:24:06.590 00:24:06.600 means that high temperature is not
00:24:08.029 00:24:08.039 enos so I'm going to put a box for
00:24:10.430 00:24:10.440 also-- at low temperature and
00:24:11.659 00:24:11.669 spontaneous because sometimes you might
00:24:15.019 00:24:15.029 have a question saying okay under what
00:24:18.440 00:24:18.450 conditions of enthalpy and entropy is it
00:24:20.419 00:24:20.429 always spontaneous that's the only time
00:24:24.049 00:24:24.059 it's always spontaneous if you have an
00:24:26.419 00:24:26.429 exothermic reaction and if Delta s for
00:24:28.879 00:24:28.889 the reaction is positive then it's
00:24:30.560 00:24:30.570 always spontaneous so they might ask you
00:24:34.190 00:24:34.200 okay if Delta H is positive and if Delta
00:24:37.070 00:24:37.080 s is positive is the reaction
00:24:39.489 00:24:39.499 spontaneous that low temperature or at
00:24:42.320 00:24:42.330 high temperature you'd have to say it's
00:24:44.299 00:24:44.309 spontaneous at high temperature so you
00:24:47.690 00:24:47.700 need to be familiar with this table
00:24:49.039 00:24:49.049 because it's going to help you to answer
00:24:50.299 00:24:50.309 certain questions so let's say if you
00:24:59.029 00:24:59.039 have the following reaction sulfur plus
00:25:03.859 00:25:03.869 oxygen reacts to form actually think of
00:25:10.519 00:25:10.529 a different reaction so hydrogen gas
00:25:15.649 00:25:15.659 reacts with nitrogen gas to produce
00:25:18.049 00:25:18.059 ammonia and if we balance it it's going
00:25:20.719 00:25:20.729 to be to a 1 and a 3 now all of these
00:25:24.259 00:25:24.269 are gases and let's say that this
00:25:26.539 00:25:26.549 reaction is an exothermic reaction so
00:25:31.810 00:25:31.820 here's a question for you will this
00:25:34.700 00:25:34.710 reaction be spontaneous at low
00:25:36.739 00:25:36.749 temperature at high temperature or is it
00:25:39.169 00:25:39.179 always spontaneous or never spontaneous
00:25:41.180 00:25:41.190 based on the way it's written in the
00:25:43.249 00:25:43.259 forward direction so we know that Delta
00:25:47.060 00:25:47.070 H is negative because it's an exothermic
00:25:49.279 00:25:49.289 reaction and we can predict the sign of
00:25:52.399 00:25:52.409 Delta s by looking at the coefficients
00:25:54.440 00:25:54.450 we have for gas molecules on the left
00:25:57.499 00:25:57.509 side two on the right side so going from
00:26:00.259 00:26:00.269 a system of high entropy to a system of
00:26:02.659 00:26:02.669 low entropy which means that Delta s is
00:26:04.879 00:26:04.889 negative now when Delta H and Delta s
00:26:07.519 00:26:07.529 are both negative is it spontaneous at
00:26:10.519 00:26:10.529 high temperatures low temperatures or
00:26:12.919 00:26:12.929 all temperatures or at no temperatures
00:26:15.549 00:26:15.559 so that's when you need to use a table
00:26:17.930 00:26:17.940 if you go back to the table you can see
00:26:20.749 00:26:20.759 that it's pond
00:26:21.890 00:26:21.900 only at low temperatures but now let's
00:26:26.090 00:26:26.100 say if you don't have the table with you
00:26:27.200 00:26:27.210 what can you do now the first thing I
00:26:31.580 00:26:31.590 will do is start with equation Delta G
00:26:34.250 00:26:34.260 is equal to Delta H minus T Delta s let
00:26:39.020 00:26:39.030 me just clear away the page first
00:26:45.940 00:26:45.950 now choose a value for Delta H and Delta
00:26:48.860 00:26:48.870 s just to keep things simple let's make
00:26:51.650 00:26:51.660 sure that they're the same what I would
00:26:53.780 00:26:53.790 do is choose 100 now Delta H is negative
00:26:56.510 00:26:56.520 so I'm going to pick a negative 100 and
00:26:59.440 00:26:59.450 Delta s is also negative so I'm going to
00:27:03.200 00:27:03.210 choose 100 let's not worry about the
00:27:05.270 00:27:05.280 unit's here what we need to focus on is
00:27:07.900 00:27:07.910 plugging in a low temperature value and
00:27:10.250 00:27:10.260 a high temperature value and see what
00:27:11.750 00:27:11.760 happens to the sign of Delta G so you
00:27:15.200 00:27:15.210 want to plug in the number that's less
00:27:17.210 00:27:17.220 than 140 and the number that's greater
00:27:18.950 00:27:18.960 than 140 if Delta H Delta s are both the
00:27:22.040 00:27:22.050 same so make sure you just plug in 100
00:27:23.810 00:27:23.820 for H and 100 for s so let's plug in a
00:27:27.200 00:27:27.210 low value for T let's say 0.1 so this is
00:27:31.490 00:27:31.500 going to be negative 100 point one times
00:27:34.160 00:27:34.170 100 is 10 so this is new positive 10 so
00:27:37.040 00:27:37.050 this is going to be negative 90 so we
00:27:38.930 00:27:38.940 can see that it's spontaneous when we
00:27:41.120 00:27:41.130 plug in a low temperature a temperature
00:27:42.890 00:27:42.900 less than one now what's going to happen
00:27:45.380 00:27:45.390 if we plug in a high temperature so
00:27:49.880 00:27:49.890 Delta H is going to be the same and
00:27:51.580 00:27:51.590 Delta s is still going to be negative
00:27:53.600 00:27:53.610 100 but instead of plugging point 1
00:27:55.910 00:27:55.920 let's plug in a number that's greater
00:27:56.870 00:27:56.880 than 1 like 10 so this is going to be
00:28:00.590 00:28:00.600 negative 110 times 1 hundreds of
00:28:02.330 00:28:02.340 thousand but it's going to be positive
00:28:03.680 00:28:03.690 thousand so now negative 100 plus a
00:28:06.770 00:28:06.780 thousand is positive 900 so as we can
00:28:10.160 00:28:10.170 see when we plug in a relatively higher
00:28:12.080 00:28:12.090 temperature the Delta H became more
00:28:15.770 00:28:15.780 positive so it's not spontaneous at high
00:28:21.770 00:28:21.780 temperatures but at low temperatures its
00:28:26.750 00:28:26.760 spontaneous
00:28:32.480 00:28:32.490 so as you can see under low temperature
00:28:36.269 00:28:36.279 conditions when Delta H is negative and
00:28:38.340 00:28:38.350 Delta s is negative the reaction will be
00:28:40.980 00:28:40.990 spontaneous in the forward direction if
00:28:42.659 00:28:42.669 you increase the temperature is going to
00:28:44.250 00:28:44.260 be non spontaneous so that's how you can
00:28:46.320 00:28:46.330 tell if you ever forget the table just
00:28:48.899 00:28:48.909 make sure you plug in two values for H
00:28:50.730 00:28:50.740 and s then plug in a high temperature
00:28:52.919 00:28:52.929 value and the low temperature value and
00:28:54.630 00:28:54.640 see what happens to the sign of Delta G
00:29:00.470 00:29:00.480 now let's say if we have this reaction
00:29:24.539 00:29:24.549 and let's say we're given the values for
00:29:27.959 00:29:27.969 the standard change in Delta G for so2
00:29:32.339 00:29:32.349 let's say it's about negative 304 h2s
00:29:36.979 00:29:36.989 negative 33 and for h2o the gaseous form
00:29:41.430 00:29:41.440 let's say negative 229 how can you use
00:29:45.389 00:29:45.399 these values to calculate the Delta G of
00:29:50.549 00:29:50.559 the reaction to calculate Delta G we can
00:29:54.619 00:29:54.629 simply use the sum of the products minus
00:29:58.379 00:29:58.389 the sum of the reactants if you're given
00:30:01.859 00:30:01.869 the Delta G for each reactant and
00:30:03.779 00:30:03.789 product of course so on a product side
00:30:07.259 00:30:07.269 we have H 2 s plus 2 H 2 O and on the
00:30:11.430 00:30:11.440 reactant side we have simply 3 h2 plus
00:30:15.569 00:30:15.579 so2 now the value for H 2 s is negative
00:30:24.119 00:30:24.129 33 and for H 2 O it's going to be 2
00:30:28.259 00:30:28.269 times negative 2 29 now H 2 is the pure
00:30:35.129 00:30:35.139 element so that's going to be 0 and for
00:30:38.659 00:30:38.669 so2 it's a negative 300 so this is going
00:30:45.930 00:30:45.940 to be negative 33 and 2 times 2 29
00:30:50.930 00:30:50.940 that's 458 but it's going to be negative
00:30:53.639 00:30:53.649 458 and we got to distribute this
00:30:56.099 00:30:56.109 negative sign to this one so it's going
00:30:58.499 00:30:58.509 to plus 300 so if we add these numbers
00:31:01.919 00:31:01.929 negative 33 minus 458 plus 300 that is
00:31:06.690 00:31:06.700 equal to negative 191 kilojoules per
00:31:10.199 00:31:10.209 mole
00:31:16.700 00:31:16.710 so now that we have the Delta G of the
00:31:20.430 00:31:20.440 reaction which is so negative 91 91
00:31:24.840 00:31:24.850 kilojoules per mole how can we calculate
00:31:27.960 00:31:27.970 the equilibrium constant for the
00:31:30.990 00:31:31.000 reaction how can we calculate K using
00:31:34.980 00:31:34.990 this value now keep in mind Delta G is
00:31:37.770 00:31:37.780 equal to negative RT natural log of K
00:31:41.790 00:31:41.800 and this is of course the standard Delta
00:31:44.460 00:31:44.470 G value so we got to isolate K the first
00:31:49.140 00:31:49.150 thing I will do is divide both sides by
00:31:51.000 00:31:51.010 negative RT so then Ln K is equal to
00:31:57.000 00:31:57.010 Delta G divided by negative RT now the
00:32:01.500 00:32:01.510 base of natural log is e and a property
00:32:06.030 00:32:06.040 of logs allows you to convert it to its
00:32:08.910 00:32:08.920 exponential form let's say if you have
00:32:10.200 00:32:10.210 log base a of B is equal to C a raised
00:32:14.190 00:32:14.200 to the C power is equal to B so you can
00:32:16.590 00:32:16.600 convert it to this form if you want
00:32:19.669 00:32:19.679 that's what we need to do in this
00:32:22.110 00:32:22.120 particular example so e raised to
00:32:28.049 00:32:28.059 everything on the right is equal to
00:32:30.299 00:32:30.309 what's inside of Ln which is K so
00:32:34.560 00:32:34.570 therefore we're going to have this
00:32:37.020 00:32:37.030 equation K is equal to e raised to the
00:32:44.669 00:32:44.679 negative Delta G divided by RT now you
00:32:48.450 00:32:48.460 need to pay attention to the units of
00:32:49.980 00:32:49.990 our our it's nine point zero eight 206
00:32:53.970 00:32:53.980 in this particular equation its 8.3145
00:32:57.060 00:32:57.070 and it has units joules per mole per
00:33:00.390 00:33:00.400 Kelvin now because R is in joules Delta
00:33:03.360 00:33:03.370 G has to be in joules so you can't plug
00:33:05.730 00:33:05.740 in negative 191 because that's in
00:33:07.290 00:33:07.300 kilojoules it's not going to work you
00:33:09.060 00:33:09.070 won't get the right answer you have to
00:33:10.680 00:33:10.690 convert kilojoules into joules so to
00:33:14.220 00:33:14.230 convert kilojoules into tools we need to
00:33:16.049 00:33:16.059 multiply by a thousand if you want to
00:33:18.419 00:33:18.429 write out the conversion it's going to
00:33:20.220 00:33:20.230 look something like this so we know that
00:33:23.250 00:33:23.260 one kilojoule is equal to a thousand
00:33:25.980 00:33:25.990 joules and so as we can see the unit's
00:33:28.919 00:33:28.929 can
00:33:29.280 00:33:29.290 so it's going to be 191 times a thousand
00:33:31.770 00:33:31.780 which is 191,000 so that's what we need
00:33:37.710 00:33:37.720 to plug in for Delta G so k is equal to
00:33:43.680 00:33:43.690 e raised to the negative 191,000 divided
00:33:51.360 00:33:51.370 by 8.3145 now let's say the temperature
00:33:55.110 00:33:55.120 is at 300 Kelvin so let's multiply that
00:33:58.290 00:33:58.300 by 300 so negative one hundred ninety
00:34:04.020 00:34:04.030 one thousand divided by 8.3145 that's
00:34:08.850 00:34:08.860 like negative twenty three thousand four
00:34:10.620 00:34:10.630 hundred fifty and if you divide that by
00:34:12.419 00:34:12.429 three hundred you're going to get
00:34:15.470 00:34:15.480 negative 78 point one seven now I almost
00:34:23.070 00:34:23.080 made a mistake because there's a
00:34:25.980 00:34:25.990 negative sign here and Delta G itself is
00:34:29.130 00:34:29.140 negative so this should have been like
00:34:30.710 00:34:30.720 negative negative so that's two
00:34:34.230 00:34:34.240 negatives which is going to be positive
00:34:36.120 00:34:36.130 so this is really II to the positive 78
00:34:40.980 00:34:40.990 point if I'm one my answer to be more
00:34:44.010 00:34:44.020 accurate it's like one six six it's a
00:34:51.900 00:34:51.910 lot of sixes
00:34:54.270 00:34:54.280 so it's that number so it's e raise to
00:35:00.550 00:35:00.560 the seventy eight point one six six
00:35:02.610 00:35:02.620 which is about eight point eight five
00:35:07.300 00:35:07.310 times ten to the thirty three so that's
00:35:11.260 00:35:11.270 the equilibrium constant K for this
00:35:13.150 00:35:13.160 reaction notice that K is very large
00:35:16.840 00:35:16.850 when Delta G is negative so let's talk
00:35:19.990 00:35:20.000 about that when Delta G is a very large
00:35:26.050 00:35:26.060 negative value K is going to be
00:35:29.200 00:35:29.210 significantly then one in the last
00:35:31.930 00:35:31.940 example Delta G was negative 191
00:35:33.910 00:35:33.920 kilojoules per mole and K was like 8
00:35:36.160 00:35:36.170 times 10 to the 33 that's a very huge
00:35:38.320 00:35:38.330 number when K significantly large the
00:35:41.140 00:35:41.150 reaction is product favored and so
00:35:44.620 00:35:44.630 whenever it's a product favored the
00:35:47.050 00:35:47.060 reaction is also spontaneous now when
00:35:53.680 00:35:53.690 Delta G is zero this is the standard
00:35:58.510 00:35:58.520 Delta G of the reaction K is going to be
00:36:01.270 00:36:01.280 approximately close to 1 and so the
00:36:06.400 00:36:06.410 system is for the most part at
00:36:08.260 00:36:08.270 equilibrium now keep in mind Delta G is
00:36:14.590 00:36:14.600 negative RT Ln K so if K is 1 the
00:36:20.860 00:36:20.870 natural log of one is equal to zero so
00:36:22.930 00:36:22.940 therefore Delta G is zero now the last
00:36:25.990 00:36:26.000 one when Delta G is positive K is going
00:36:28.930 00:36:28.940 to be significantly less than one but K
00:36:31.150 00:36:31.160 is never negative so K is going to be
00:36:32.770 00:36:32.780 between zero and one so K is going to be
00:36:38.410 00:36:38.420 a very small number like 5 times 10 to
00:36:40.870 00:36:40.880 the negative 21 K significally small
00:36:44.200 00:36:44.210 it's going to be reactant favored so the
00:36:51.280 00:36:51.290 reaction is going to be non spontaneous
00:36:52.960 00:36:52.970 in the forward direction which means
00:36:55.990 00:36:56.000 it's spontaneous in the reverse
00:36:57.610 00:36:57.620 direction or towards the reactant side
00:37:00.190 00:37:00.200 cents into the active favored so if it's
00:37:02.920 00:37:02.930 to go into the left it's going to be
00:37:04.150 00:37:04.160 spontaneous to the right not spontaneous
00:37:07.099 00:37:07.109 now for this one is spontaneous in the
00:37:09.319 00:37:09.329 forward direction towards the product
00:37:10.849 00:37:10.859 side because it's product favored so
00:37:15.380 00:37:15.390 here's another problem for you let's say
00:37:16.579 00:37:16.589 if K is equal to 2 times 10 to the 12
00:37:21.819 00:37:21.829 calculate Delta G of the reaction to
00:37:25.460 00:37:25.470 standard Delta G so let's use the
00:37:29.180 00:37:29.190 equation Delta G is equal to negative RT
00:37:31.339 00:37:31.349 Ln K so R that's going to be negative
00:37:37.630 00:37:37.640 8.3145 and I keep again in the
00:37:43.430 00:37:43.440 temperature let's say the temperature is
00:37:46.630 00:37:46.640 300 Kelvin or 298 Kelvin let's go with
00:37:53.569 00:37:53.579 that
00:37:58.289 00:37:58.299 and then it's going to be Ln two times
00:38:01.140 00:38:01.150 10 to the 12 so if you have K it's
00:38:04.439 00:38:04.449 fairly easy to find Delta G you just got
00:38:06.150 00:38:06.160 a plug name 298 of 8.3145 times 273 and
00:38:22.079 00:38:22.089 79 but the units is in joules per mole
00:38:25.169 00:38:25.179 because that sentence of art it has the
00:38:27.929 00:38:27.939 units of ira joules per mole per Kelvin
00:38:29.309 00:38:29.319 and it's going to cancel with the Kelvin
00:38:32.729 00:38:32.739 temperature so R has unit joules per
00:38:35.549 00:38:35.559 mole per Kelvin and the temperature is
00:38:38.489 00:38:38.499 in Kelvin and usually K typically would
00:38:42.359 00:38:42.369 have to worry about the units of K so
00:38:44.669 00:38:44.679 Delta G is going to have the unit's
00:38:46.410 00:38:46.420 joules per mole now sometimes in a
00:38:49.229 00:38:49.239 multiple-choice exam they may want you
00:38:51.419 00:38:51.429 to report the answer in kilojoules per
00:38:52.949 00:38:52.959 mole so to convert jewels into
00:38:55.439 00:38:55.449 kilojoules you need to divide it by a
00:38:57.029 00:38:57.039 thousand so this is going to be negative
00:38:59.130 00:38:59.140 70 point two kilojoules per mole and so
00:39:03.959 00:39:03.969 now you know how to calculate Delta G of
00:39:05.910 00:39:05.920 the reaction if you're given the
00:39:08.069 00:39:08.079 equilibrium constant K now let's go back
00:39:14.130 00:39:14.140 to the reaction that we had earlier and
00:39:18.410 00:39:18.420 what we're going to do this time we're
00:39:21.059 00:39:21.069 going to calculate Delta G under
00:39:23.599 00:39:23.609 non-standard conditions so all of these
00:39:31.890 00:39:31.900 are in the gas phase now let's say that
00:39:38.130 00:39:38.140 the partial pressure for h2s let's say
00:39:42.689 00:39:42.699 it's 0.1 and for h2o it's a point two
00:39:47.999 00:39:48.009 and for h2 let's say the partial
00:39:51.839 00:39:51.849 pressure is three and for so2 its to how
00:39:56.819 00:39:56.829 can you calculate the standard I mean
00:39:59.640 00:39:59.650 the non-standard
00:40:00.390 00:40:00.400 Delta G for this reaction now we have
00:40:03.959 00:40:03.969 the standard value the standard value is
00:40:07.709 00:40:07.719 negative 191 kilojoules per mole what's
00:40:10.410 00:40:10.420 the non-standard value
00:40:13.579 00:40:13.589 here's the equation that you need to
00:40:15.690 00:40:15.700 find the non-standard value Delta G is
00:40:19.259 00:40:19.269 equal to Delta G naught plus RT Ln Q so
00:40:26.339 00:40:26.349 the standard value you have this
00:40:29.789 00:40:29.799 whenever the partial pressures of all
00:40:31.920 00:40:31.930 reactants and products is equal to one
00:40:34.470 00:40:34.480 ATM or if you're dealing with
00:40:37.829 00:40:37.839 concentration has to be one that's the
00:40:40.170 00:40:40.180 standard value if it's not one then
00:40:43.349 00:40:43.359 Delta G is going to change so you got to
00:40:45.779 00:40:45.789 calculate the non-standard Delta G value
00:40:49.789 00:40:49.799 now because we have our R is in the
00:40:53.670 00:40:53.680 units of joules per mole per Kelvin that
00:40:55.650 00:40:55.660 means Delta G naught has to be in joules
00:40:59.039 00:40:59.049 per mole so we got to convert it right
00:41:01.559 00:41:01.569 now the only thing that's different here
00:41:03.180 00:41:03.190 is Q we need to understand how to
00:41:05.910 00:41:05.920 calculate the reaction quotient Q so I
00:41:09.210 00:41:09.220 think we should do that first and then
00:41:10.380 00:41:10.390 we'll get back to the equation Q is the
00:41:15.720 00:41:15.730 reaction quotient and like K you can
00:41:18.210 00:41:18.220 find it by dividing the products by the
00:41:21.089 00:41:21.099 reactants so the products are h2s and
00:41:25.730 00:41:25.740 h2o but there's a two in front of h2o so
00:41:30.349 00:41:30.359 we're going to put a two on the exponent
00:41:33.509 00:41:33.519 of h2 them and then divided by h2 x SL
00:41:39.120 00:41:39.130 two so the coefficient for h2 is 3 so
00:41:42.990 00:41:43.000 let's put a 3 here so the value for h2s
00:41:47.400 00:41:47.410 is 0.1 and for h2o its point two squared
00:41:52.789 00:41:52.799 divided by the value for H 2 which is 3
00:41:55.970 00:41:55.980 cubed times that for so2 which is 2 so
00:42:01.970 00:42:01.980 0.1 times 0.2 squared that's about point
00:42:06.690 00:42:06.700 zero zero four three to the third power
00:42:10.410 00:42:10.420 is 27 times 2 that's 54 so if you take
00:42:16.289 00:42:16.299 point zero zero four divided by 54 you
00:42:19.650 00:42:19.660 should get seven point four zero seven
00:42:22.829 00:42:22.839 times 10 to negative 5
00:42:24.910 00:42:24.920 so that's the value of the reaction
00:42:26.960 00:42:26.970 quotient Q so with that we can now find
00:42:32.060 00:42:32.070 00:42:33.800 00:42:33.810 Delta G value
00:42:43.530 00:42:43.540 so let's plug in negative 191,000 joules
00:42:48.840 00:42:48.850 for Delta G naught it has to be in
00:42:50.310 00:42:50.320 joules per mole so R is going to be
00:42:53.540 00:42:53.550 8.3145
00:42:54.810 00:42:54.820 and let's say the temperature is 298
00:42:57.180 00:42:57.190 Kelvin times the natural log of Q which
00:43:03.330 00:43:03.340 was seven point four zero seven times 10
00:43:07.560 00:43:07.570 to negative five the natural log of
00:43:11.250 00:43:11.260 seven point four zero seven times ten to
00:43:14.160 00:43:14.170 95 that's negative nine point five one
00:43:18.030 00:43:18.040 if you multiply that by 298 and 8.3145
00:43:22.790 00:43:22.800 you should get negative twenty three
00:43:30.150 00:43:30.160 thousand five hundred sixty-four so
00:43:34.320 00:43:34.330 notice that the contribution of RT Ln Q
00:43:39.240 00:43:39.250 is negative that means that the reaction
00:43:41.190 00:43:41.200 is becoming more spontaneous notice that
00:43:46.680 00:43:46.690 we have a large amount of reactants and
00:43:49.170 00:43:49.180 a small amount of products if you
00:43:52.080 00:43:52.090 increase the reactants according to
00:43:55.740 00:43:55.750 Lateisha Talia's principle the reaction
00:43:58.830 00:43:58.840 is going to shift to the right and as it
00:44:03.450 00:44:03.460 shifts to the right it becomes more
00:44:05.040 00:44:05.050 spontaneous and so that's why the Delta
00:44:07.590 00:44:07.600 G is going to be more negative so if we
00:44:10.110 00:44:10.120 add negative one ninety one thousand and
00:44:13.440 00:44:13.450 twenty three thousand five sixty four
00:44:16.580 00:44:16.590 the Delta G the non standard Delta G is
00:44:19.830 00:44:19.840 going to be negative two hundred
00:44:20.850 00:44:20.860 fourteen thousand five hundred sixty
00:44:23.250 00:44:23.260 four joules per mole and if you want to
00:44:26.280 00:44:26.290 convert it to kilojoules per mole
00:44:27.450 00:44:27.460 divided by thousand so it's going to be
00:44:29.190 00:44:29.200 negative two fourteen point six
00:44:31.160 00:44:31.170 kilojoules per mole so anytime you
00:44:33.960 00:44:33.970 increase the reactants the reaction is
00:44:35.700 00:44:35.710 going to shift to the right and Delta G
00:44:38.640 00:44:38.650 will be more negative it's going to be
00:44:39.960 00:44:39.970 more spontaneous whenever it shifts to
00:44:43.110 00:44:43.120 the right
00:44:47.089 00:44:47.099 now consider the following reversible
00:44:51.019 00:44:51.029 reaction let's say we have a which is a
00:44:53.959 00:44:53.969 solid plus B which is a gas and let's
00:44:57.380 00:44:57.390 say we have two of B and this turns into
00:45:00.410 00:45:00.420 C which is a liquid and D which is a gas
00:45:08.109 00:45:08.119 so what's going to happen if we increase
00:45:11.019 00:45:11.029 the concentration of B will the reaction
00:45:13.640 00:45:13.650 shift to the right or to the left
00:45:15.140 00:45:15.150 well according to Lateisha Talia's
00:45:17.329 00:45:17.339 principle whenever you impose a change
00:45:19.789 00:45:19.799 on a system the system is going to try
00:45:21.799 00:45:21.809 to undo that change so if you increase
00:45:24.259 00:45:24.269 the reactants the system is going to try
00:45:26.420 00:45:26.430 to decrease the value of the reactants
00:45:28.069 00:45:28.079 so it's going to shift to the right
00:45:31.099 00:45:31.109 because when it shifts to the right the
00:45:33.170 00:45:33.180 value of the products go up but the
00:45:35.539 00:45:35.549 value of the reactants go down and
00:45:36.890 00:45:36.900 that's how it bring this back down the
00:45:39.410 00:45:39.420 value of the reactants so whenever you
00:45:42.229 00:45:42.239 increase the concentration of reactants
00:45:44.390 00:45:44.400 is going to shift to the right and any
00:45:45.769 00:45:45.779 time the reaction shifts to the right
00:45:47.229 00:45:47.239 Delta G will become more negative
00:45:50.150 00:45:50.160 meaning that Delta G will decrease and
00:45:52.609 00:45:52.619 so the Spontini of the reaction will
00:45:57.289 00:45:57.299 increase the reaction will become more
00:45:58.939 00:45:58.949 spontaneous now what about D if we
00:46:02.930 00:46:02.940 increase the value of D if you increase
00:46:05.509 00:46:05.519 the concentration or the partial
00:46:07.670 00:46:07.680 pressure of a product the reaction is
00:46:09.890 00:46:09.900 going to shift to left it does that to
00:46:13.549 00:46:13.559 decrease the value of the products since
00:46:16.249 00:46:16.259 you increased it it's going to try to
00:46:17.569 00:46:17.579 undo the change that you impose to them
00:46:19.309 00:46:19.319 anytime the reaction goes to the left
00:46:21.259 00:46:21.269 the value of the products go down and
00:46:23.420 00:46:23.430 the value of the reactants go up so as
00:46:27.289 00:46:27.299 it shifts to the left
00:46:28.189 00:46:28.199 Delta G that will increase in value it's
00:46:30.769 00:46:30.779 going to become more more positive
00:46:32.380 00:46:32.390 meaning that the reaction is going to be
00:46:36.019 00:46:36.029 it's going to become more and not
00:46:37.849 00:46:37.859 spontaneous in the four direction but
00:46:40.459 00:46:40.469 00:46:41.660 00:46:41.670 because it's going to the left so in a
00:46:44.599 00:46:44.609 forward direction it's going to be non
00:46:46.640 00:46:46.650 00:46:51.769 00:46:51.779 now what happens if we increase the
00:46:54.509 00:46:54.519 amount of reactant a now I need to keep
00:46:58.230 00:46:58.240 in mind that solids and liquids have no
00:47:00.029 00:47:00.039 effect on the position of equilibrium so
00:47:02.430 00:47:02.440 if you increase the amount of a the
00:47:04.620 00:47:04.630 reaction will not shift to the right or
00:47:06.150 00:47:06.160 to the left so therefore there's going
00:47:08.910 00:47:08.920 to be no change and if it doesn't shift
00:47:12.569 00:47:12.579 to the right or to the left
00:47:13.819 00:47:13.829 Delta G will remain constant now let's
00:47:20.970 00:47:20.980 say if we increase the volume of the
00:47:23.400 00:47:23.410 container that holds the reaction what's
00:47:25.019 00:47:25.029 going to happen well whenever you
00:47:27.089 00:47:27.099 increase the volume since we have gases
00:47:29.870 00:47:29.880 the pressure will be reduced and so
00:47:34.950 00:47:34.960 therefore whenever the pressure is
00:47:37.049 00:47:37.059 reduced the system is going to try to
00:47:39.259 00:47:39.269 undo the change that you impose to it
00:47:41.549 00:47:41.559 it's going to try to increase the
00:47:42.539 00:47:42.549 pressure in order for it to increase the
00:47:44.370 00:47:44.380 pressure it has to shift to the side
00:47:46.470 00:47:46.480 with more moles of gas now we have two
00:47:50.039 00:47:50.049 gas molecules on the left only one on
00:47:52.319 00:47:52.329 the right so it's going to shift to the
00:47:54.059 00:47:54.069 left to increase the pressure to bring
00:47:56.789 00:47:56.799 it back to where it was and so as it
00:47:59.730 00:47:59.740 shifts to the left
00:48:00.420 00:48:00.430 we know that its reactant favored so
00:48:04.200 00:48:04.210 it's going to be non spontaneous in the
00:48:06.109 00:48:06.119 four direction so Delta G is going to
00:48:09.960 00:48:09.970 increase in value it's going to become
00:48:12.210 00:48:12.220 more positive if whenever the reaction
00:48:14.370 00:48:14.380 shifts to the left now let's say if we
00:48:17.640 00:48:17.650 have an endothermic reaction where Delta
00:48:22.890 00:48:22.900 H is positive what's going to happen if
00:48:26.130 00:48:26.140 we increase the temperature if you raise
00:48:29.279 00:48:29.289 the temperature then energy is going to
00:48:35.339 00:48:35.349 go into the system whenever you raise
00:48:37.109 00:48:37.119 the temperature particularly the
00:48:38.430 00:48:38.440 surroundings so if you raise the
00:48:40.109 00:48:40.119 temperature for an endothermic reaction
00:48:41.779 00:48:41.789 the reaction is going to shift to the
00:48:44.009 00:48:44.019 right a simple way that you can find out
00:48:46.589 00:48:46.599 the direction if it's an O thermic put
00:48:48.539 00:48:48.549 Delta H on the left side if its X with
00:48:50.849 00:48:50.859 let me put it on the right side so
00:48:52.589 00:48:52.599 whenever you raise the value of the
00:48:53.849 00:48:53.859 reactants the reaction is going to shift
00:48:55.799 00:48:55.809 to the right likewise if you increase
00:48:58.049 00:48:58.059 the temperature for an endothermic
00:48:59.069 00:48:59.079 reaction it's going to shift to the
00:49:00.720 00:49:00.730 right so Delta G will decrease in value
00:49:03.180 00:49:03.190 which means that
00:49:04.800 00:49:04.810 cause delta g is becoming more negative
00:49:06.120 00:49:06.130 it's going to be more spontaneous and
00:49:11.690 00:49:11.700 also the equally makan stink a will be
00:49:14.520 00:49:14.530 affected if you increase the
00:49:17.010 00:49:17.020 concentration of let's say reaction b d
00:49:19.440 00:49:19.450 or if you change the pressure or volume
00:49:21.120 00:49:21.130 the equilibrium constant is going to
00:49:23.310 00:49:23.320 stay the same it's not going to change
00:49:24.690 00:49:24.700 however the equilibrium constant will
00:49:27.420 00:49:27.430 change due to changes in temperature so
00:49:29.910 00:49:29.920 if you raise the temperature and if the
00:49:31.950 00:49:31.960 reaction shifts to the right the value
00:49:34.230 00:49:34.240 of the products will go up and the value
00:49:36.090 00:49:36.100 of the reactants will go down and k is
00:49:39.830 00:49:39.840 equal to the ratio of the products
00:49:42.600 00:49:42.610 divided by the reactants whenever you
00:49:44.910 00:49:44.920 increase the numerator of a fraction in
00:49:46.830 00:49:46.840 this case the products the value of the
00:49:48.780 00:49:48.790 whole fraction goes up and if you
00:49:51.990 00:49:52.000 increase the denominator the value goes
00:49:54.240 00:49:54.250 down but if you decrease the denominator
00:49:56.610 00:49:56.620 or decrease the value of the reactants
00:49:58.620 00:49:58.630 the value of the whole fraction goes up
00:50:00.620 00:50:00.630 so as the reaction shifts to the right
00:50:03.120 00:50:03.130 due to a temperature change okay the
00:50:06.120 00:50:06.130 equilibrium constant is going to
00:50:07.380 00:50:07.390 increase and the reaction will be more
00:50:09.540 00:50:09.550 00:50:12.920 00:50:12.930 so now let's understand how the reaction
00:50:18.000 00:50:18.010 is going to shift to the right if it's
00:50:20.040 00:50:20.050 endothermic so Delta H let's say it's
00:50:24.750 00:50:24.760 positive 50 now I'm going to draw a box
00:50:29.070 00:50:29.080 inside the box represents a system now
00:50:34.170 00:50:34.180 keep in mind you need to know the
00:50:35.340 00:50:35.350 difference between an open system a
00:50:37.800 00:50:37.810 closed system and the isolated system an
00:50:39.720 00:50:39.730 open system is a system where mass and
00:50:42.960 00:50:42.970 energy can be exchanged with the
00:50:44.550 00:50:44.560 surroundings in a closed system the mass
00:50:49.140 00:50:49.150 cannot be exchanged
00:50:50.610 00:50:50.620 however energy like heat energy can flow
00:50:53.250 00:50:53.260 into or out of a closed system
00:50:55.710 00:50:55.720 but gas molecules can't enter a closed
00:50:58.440 00:50:58.450 system now if you have an isolated
00:51:00.750 00:51:00.760 system heat cannot flow into or out of
00:51:03.390 00:51:03.400 an isolated system nor can a gas
00:51:05.610 00:51:05.620 molecule enter or leave an isolated
00:51:08.280 00:51:08.290 system nothing
00:51:09.690 00:51:09.700 enters or leaves an isolated system but
00:51:12.720 00:51:12.730 now the example that we are going to
00:51:14.070 00:51:14.080 have is a closed system where heat can
00:51:16.110 00:51:16.120 flow into or out of it so
00:51:18.510 00:51:18.520 let's say we have the surroundings on
00:51:20.610 00:51:20.620 the outside and the system on the inside
00:51:23.480 00:51:23.490 so let's say the temperature the system
00:51:25.470 00:51:25.480 is 50 but let's say that of let's say if
00:51:28.380 00:51:28.390 we raise the temperature of the
00:51:29.970 00:51:29.980 surroundings to about 200 degrees
00:51:31.920 00:51:31.930 Celsius heat is going to flow from hot
00:51:35.160 00:51:35.170 to cold so 200 is hot 50 is relatively
00:51:39.360 00:51:39.370 cold compared to 200 so heat is going to
00:51:42.540 00:51:42.550 flow into the system as heat flows into
00:51:46.890 00:51:46.900 the system it's going to be ml thermic
00:51:51.710 00:51:51.720 because the system is absorbing heat and
00:51:54.530 00:51:54.540 so as it absorbs heat the reaction is
00:51:58.980 00:51:58.990 going to shift to the right because one
00:52:02.100 00:52:02.110 of the action shifts to the right it's
00:52:05.190 00:52:05.200 going to be endothermic if you reverse
00:52:07.680 00:52:07.690 the reaction is going to be exothermic
00:52:11.270 00:52:11.280 so the only way to reverse the reaction
00:52:14.010 00:52:14.020 is to decrease the temperature of the
00:52:15.720 00:52:15.730 surroundings so let's say if we decrease
00:52:18.540 00:52:18.550 it to about zero degrees Celsius heat is
00:52:21.180 00:52:21.190 going to flow out of the system and the
00:52:23.820 00:52:23.830 only way to extract heat from the system
00:52:25.740 00:52:25.750 is if the reaction reverses direction so
00:52:29.700 00:52:29.710 it's going to shift to the left if we
00:52:31.770 00:52:31.780 reverse the reaction and then the
00:52:35.520 00:52:35.530 enthalpy has to be reversed it's going
00:52:38.160 00:52:38.170 to be instead of being positive 50 it's
00:52:41.100 00:52:41.110 going to be negative 50 and so it's
00:52:44.310 00:52:44.320 going to be an exothermic reaction so by
00:52:47.250 00:52:47.260 cooling the surroundings we can cause
00:52:48.840 00:52:48.850 the reaction to reverse in direction we
00:52:51.390 00:52:51.400 can cause it to go to the left and if we
00:52:54.300 00:52:54.310 increase the temperature of the
00:52:55.500 00:52:55.510 surroundings we can cause the reaction
00:52:57.510 00:52:57.520 become endothermic and it's going to
00:52:59.400 00:52:59.410 shift to the right so we can control the
00:53:02.070 00:53:02.080 direction of the reaction by controlling
00:53:04.200 00:53:04.210 the temperature of the surroundings so
00:53:06.600 00:53:06.610 if we increase the temperature of the
00:53:09.240 00:53:09.250 surroundings we can see that the
00:53:11.670 00:53:11.680 reaction is going to shift to the right
00:53:13.320 00:53:13.330 because it's going to be endothermic
00:53:14.760 00:53:14.770 heat is going to flow into the system
00:53:17.390 00:53:17.400 and when it shifts to the right Delta G
00:53:20.640 00:53:20.650 will decrease and the reaction will
00:53:22.980 00:53:22.990 become more spontaneous in the four
00:53:25.170 00:53:25.180 direction now if we decrease the
00:53:27.990 00:53:28.000 temperature the reaction is going to
00:53:30.030 00:53:30.040 shift to the left and Delta G will
00:53:31.980 00:53:31.990 this can be more positive which means
00:53:34.050 00:53:34.060 that it's more non-spontaneous in the
00:53:36.030 00:53:36.040 four direction but because it's going to
00:53:38.250 00:53:38.260 the left its spontaneous in the reverse
00:53:40.170 00:53:40.180 direction and so you can adjust the
00:53:44.130 00:53:44.140 value of Delta G by controlling the
00:53:46.200 00:53:46.210 temperature of the surroundings but that
00:53:48.480 00:53:48.490 is it for this video that's all I got
00:53:50.670 00:53:50.680 hopefully you found it to be educational
00:53:52.650 00:53:52.660 thanks for watching and have a great day
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