Online HVAC Training

WEBVTT
Kind: captions
Language: en

00:00:06.450
all right
00:00:15.870 00:00:15.880 all right we're going to go through some
00:00:17.130 00:00:17.140 definitions first and go through the gas
00:00:19.890 00:00:19.900 laws and then we will get into the basic
00:00:23.339 00:00:23.349 refrigeration cycle and we'll see how
00:00:26.909 00:00:26.919 that all relates I know modules 1 & 2
00:00:29.190 00:00:29.200 are tough a lot of formulas a lot of
00:00:31.560 00:00:31.570 talk about how many BTUs does it take to
00:00:35.430 00:00:35.440 take a 10 pound block of ice at -10
00:00:37.950 00:00:37.960 degrees and make it into 250 degrees
00:00:40.560 00:00:40.570 steam but that's all for purpose we'll
00:00:43.079 00:00:43.089 kind of get into that in just a bit
00:00:44.509 00:00:44.519 okay the first definition heat now when
00:00:48.840 00:00:48.850 you think of heat as a human being that
00:00:52.170 00:00:52.180 is like your stove and it's hot and you
00:00:53.850 00:00:53.860 get burnt but truly heat is just a form
00:00:56.549 00:00:56.559 of energy and it's molecules in motion
00:00:58.260 00:00:58.270 so even with an ice cube that's at 32
00:01:01.080 00:01:01.090 degrees there are molecules in that ice
00:01:03.479 00:01:03.489 that are moving and they're still heat
00:01:05.340 00:01:05.350 there isn't until you get down to minus
00:01:09.120 00:01:09.130 460 degrees and all molecular motion
00:01:11.760 00:01:11.770 stops and that's never been reached yet
00:01:14.100 00:01:14.110 that you can get down pretty close to
00:01:15.749 00:01:15.759 that but so I want you to start thinking
00:01:18.480 00:01:18.490 of heat as molecules in motion not so
00:01:22.020 00:01:22.030 much as something that is hot to your
00:01:25.020 00:01:25.030 touch and heat always flows from a
00:01:27.690 00:01:27.700 substance that has more heat or more
00:01:29.789 00:01:29.799 molecules and motions to one with less
00:01:31.980 00:01:31.990 heat
00:01:34.640 00:01:34.650 this will give you a quick example right
00:01:37.320 00:01:37.330 here
00:01:41.219 00:01:41.229 for example this block of ice at 32°
00:01:43.620 00:01:43.630 does have molecules in motion but
00:01:45.780 00:01:45.790 they're pretty much bonded together and
00:01:47.429 00:01:47.439 they're not moving very much they're
00:01:49.080 00:01:49.090 just sitting here pretty while they are
00:01:51.990 00:01:52.000 moving they are not bouncing into each
00:01:54.660 00:01:54.670 other too much are more or less bound
00:01:56.370 00:01:56.380 together and that's why we that gives
00:01:58.590 00:01:58.600 ice it's solid form and as we start to
00:02:01.889 00:02:01.899 add heat to the the ice and it begins to
00:02:05.190 00:02:05.200 melt those molecules begin to move a
00:02:07.620 00:02:07.630 little bit faster so not only are they
00:02:09.270 00:02:09.280 bound together they they start to cut
00:02:12.300 00:02:12.310 loose their binds with each other and
00:02:15.020 00:02:15.030 turn into a liquid and they start to
00:02:17.400 00:02:17.410 exert some force in the downwards and
00:02:20.789 00:02:20.799 outwards direction like in this
00:02:22.350 00:02:22.360 container then as we add more and heat
00:02:25.110 00:02:25.120 and we turn this water and liquid into
00:02:29.130 00:02:29.140 vapour those molecules are bouncing
00:02:32.039 00:02:32.049 around really fast and it exerts
00:02:34.800 00:02:34.810 pressure in all directions and
00:02:38.320 00:02:38.330 and that's the one thing you need to
00:02:39.910 00:02:39.920 remember when we're talking about
00:02:41.410 00:02:41.420 pressure that's where you get pressure
00:02:43.240 00:02:43.250 that this example here that shows that
00:02:45.760 00:02:45.770 blows the cork off the bottom you get so
00:02:47.620 00:02:47.630 much energy and pressure in here that in
00:02:51.120 00:02:51.130 the form of heat
00:02:59.400 00:02:59.410 you
00:03:02.530 00:03:02.540 okay heat flow
00:03:05.680 00:03:05.690 when I talked about Heat earliest
00:03:08.350 00:03:08.360 molecules in motion so this makes sense
00:03:11.340 00:03:11.350 to us if we have a hundred degree
00:03:14.050 00:03:14.060 fahrenheit block of lead here and set it
00:03:17.290 00:03:17.300 next to a 75 degree Fahrenheit block of
00:03:20.620 00:03:20.630 lead of course we we recognize that the
00:03:23.560 00:03:23.570 heat will flow from the substance with
00:03:25.900 00:03:25.910 more heat or molecules of motion to one
00:03:27.880 00:03:27.890 with less but now we we don't usually
00:03:30.310 00:03:30.320 think of minus 200 degree Fahrenheit and
00:03:33.280 00:03:33.290 minus 350 degree Fahrenheit as having
00:03:36.010 00:03:36.020 heat but it still does it has molecules
00:03:38.410 00:03:38.420 in motion although not as much as these
00:03:40.810 00:03:40.820 blocks up here they're armed there is
00:03:43.810 00:03:43.820 heat energy contained in this block of
00:03:47.470 00:03:47.480 lead and the molecular motion or heat
00:03:50.590 00:03:50.600 energy will in fact flow from a
00:03:53.430 00:03:53.440 substance that is minus 200 degrees to
00:03:56.410 00:03:56.420 minus 350 degrees Fahrenheit and that's
00:03:59.080 00:03:59.090 why I want you to think about heat again
00:04:00.820 00:04:00.830 as molecules of motion not something
00:04:03.220 00:04:03.230 that is hot or cold to the to our touch
00:04:12.089 00:04:12.099 alright there's in air conditioning we
00:04:16.199 00:04:16.209 have two forms of the types of heat that
00:04:18.659 00:04:18.669 we like to talk about one is sensible
00:04:21.090 00:04:21.100 00:04:23.210 00:04:23.220 and that is where if you add heat or
00:04:28.010 00:04:28.020 molecules or heat energy in molecules in
00:04:31.160 00:04:31.170 motion as to a substance it changes the
00:04:35.030 00:04:35.040 temperature that you can measure with a
00:04:36.650 00:04:36.660 thermometer and then we have latent heat
00:04:39.470 00:04:39.480 and that latent means hidden and that's
00:04:42.230 00:04:42.240 heat that cannot be measured by a
00:04:46.370 00:04:46.380 thermometer and what it does is at a
00:04:49.460 00:04:49.470 certain point and if we use water in the
00:04:51.770 00:04:51.780 example in the textbook when you start
00:04:55.430 00:04:55.440 with a 75 degree pan of water and put it
00:04:59.150 00:04:59.160 on the 500 degrees stove it starts to
00:05:01.910 00:05:01.920 increase the temperature and if you have
00:05:03.410 00:05:03.420 a thermometer in there it's going to
00:05:05.510 00:05:05.520 show that temperature increase that's
00:05:07.520 00:05:07.530 the sensible heat at a certain point at
00:05:11.210 00:05:11.220 if you're at sea level it's 212 degrees
00:05:13.520 00:05:13.530 the water begins to boil and and that's
00:05:18.260 00:05:18.270 changing of state from a liquid to vapor
00:05:20.840 00:05:20.850 and it remains steady at 212 degrees and
00:05:25.280 00:05:25.290 will not that water does not increase
00:05:27.680 00:05:27.690 temperature because all of that heat
00:05:30.080 00:05:30.090 energy that's being absorbed is changing
00:05:33.170 00:05:33.180 the state of the water from liquid to
00:05:34.850 00:05:34.860 vapor
00:05:35.330 00:05:35.340 that's called latent heat because even
00:05:38.150 00:05:38.160 though you're adding heat you can't
00:05:39.469 00:05:39.479 measure with your thermometer
00:05:47.760 00:05:47.770 okay saturation
00:05:51.500 00:05:51.510 we'll talk about water first then we're
00:05:54.350 00:05:54.360 going to talk about refrigerants because
00:05:55.730 00:05:55.740 it's some they're very similar in their
00:05:57.500 00:05:57.510 properties the saturation is when a
00:06:00.950 00:06:00.960 substance is in the form of both liquid
00:06:03.710 00:06:03.720 and vapor
00:06:07.900 00:06:07.910 and if heat is added
00:06:11.770 00:06:11.780 you'll begin to change state into vapor
00:06:14.500 00:06:14.510 and if heat is removed
00:06:18.800 00:06:18.810 it will change state back into liquid so
00:06:21.680 00:06:21.690 the definition of saturation is when a
00:06:24.410 00:06:24.420 00:06:26.630 00:06:26.640 and vapor when we add Heat
00:06:28.760 00:06:28.770 it changes state begins to change state
00:06:31.400 00:06:31.410 into vapor and when we remove heat it
00:06:34.340 00:06:34.350 will begin to change state back into
00:06:36.140 00:06:36.150 liquid
00:06:43.600 00:06:43.610 and I just want to let everyone know if
00:06:45.399 00:06:45.409 you do have audio problems please call
00:06:47.080 00:06:47.090 in on the number up at top I just got a
00:06:49.360 00:06:49.370 message
00:06:52.810 00:06:52.820 from one of our viewers here
00:06:59.909 00:06:59.919 okay changing state and this is very
00:07:03.119 00:07:03.129 important when when we are changing
00:07:06.149 00:07:06.159 state of a liquid to a vapor it takes a
00:07:10.019 00:07:10.029 tremendous amount of heat energy and
00:07:12.839 00:07:12.849 which is molecule which are molecules in
00:07:15.360 00:07:15.370 motion to change that state from liquid
00:07:17.939 00:07:17.949 to vapor and when that condenses back
00:07:19.920 00:07:19.930 down from vapor to liquid all the energy
00:07:23.219 00:07:23.229 the heat energy that's been absorbed is
00:07:25.730 00:07:25.740 released so when you boil your water it
00:07:30.749 00:07:30.759 all that heat energy when it hits your
00:07:32.760 00:07:32.770 cool window and turns back into water
00:07:34.649 00:07:34.659 releases all of that heat back into the
00:07:36.990 00:07:37.000 atmosphere
00:07:41.220 00:07:41.230 okay and from now on I want us to think
00:07:43.620 00:07:43.630 about not to think about boiling anymore
00:07:46.170 00:07:46.180 because that's just like heat for us
00:07:48.210 00:07:48.220 boiling we equate to water and it's hot
00:07:50.250 00:07:50.260 we want to think about changing state
00:07:54.690 00:07:54.700 rather than boiling because it gets
00:07:57.690 00:07:57.700 confusing with refrigerant again it
00:07:59.190 00:07:59.200 makes sense when you have a beaker of
00:08:01.950 00:08:01.960 water here and you're adding heat to it
00:08:03.810 00:08:03.820 and it's boiling and you put your finger
00:08:05.460 00:08:05.470 in there and you get burned but when we
00:08:09.930 00:08:09.940 talk about refrigerate refrigerants they
00:08:12.000 00:08:12.010 boil at much lower temperatures so we're
00:08:14.310 00:08:14.320 going to we're going to erase boiling
00:08:16.080 00:08:16.090 from our vocabulary and changing state
00:08:19.140 00:08:19.150 is what we're going to talk about from
00:08:21.570 00:08:21.580 here on out
00:08:30.640 00:08:30.650 all right so here is the diagram from
00:08:33.320 00:08:33.330 our textbook and it starts out at the
00:08:37.370 00:08:37.380 bottom of the graph at with the zero
00:08:41.420 00:08:41.430 Degree ice we're not going to worry
00:08:43.850 00:08:43.860 about much about this zero Degree ice
00:08:46.550 00:08:46.560 until we hit 32 degree water at this
00:08:50.510 00:08:50.520 point right here let's talk about this
00:08:53.150 00:08:53.160 water we have that water on the stove
00:08:55.010 00:08:55.020 like we talked about earlier and as it
00:08:58.730 00:08:58.740 is
00:09:00.609 00:09:00.619 heated up on the stove the temperature
00:09:03.309 00:09:03.319 begins to rise at this point we're at
00:09:05.519 00:09:05.529 100 degrees over here now the as that
00:09:12.129 00:09:12.139 heat that is being added raises the
00:09:13.929 00:09:13.939 temperature that is the sensible heat
00:09:15.909 00:09:15.919 remember sensible heat is heat they can
00:09:18.729 00:09:18.739 be measured with a thermometer at 212
00:09:23.829 00:09:23.839 degrees
00:09:26.540 00:09:26.550 our water is that saturation is that a
00:09:29.630 00:09:29.640 saturation point it is absorbed as much
00:09:32.230 00:09:32.240 sensible heat as it can absorb and any
00:09:35.510 00:09:35.520 heat that is added
00:09:40.390 00:09:40.400 went on
00:09:42.510 00:09:42.520 changes the state of the water from
00:09:45.950 00:09:45.960 liquid to vapor and it doesn't matter
00:09:48.810 00:09:48.820 how many how much heat we put on there
00:09:51.180 00:09:51.190 as long as
00:09:53.840 00:09:53.850 we have liquid in both liquid and vapor
00:09:56.090 00:09:56.100 together it will absorb a tremendous
00:09:59.450 00:09:59.460 amount of heat to change the state from
00:10:03.070 00:10:03.080 liquid to vapor at a certain point when
00:10:06.740 00:10:06.750 all of the liquid has been changed to
00:10:08.870 00:10:08.880 vapor it will again start to pick up
00:10:10.960 00:10:10.970 sensible heat here and it raises the
00:10:14.720 00:10:14.730 temperature of the steam
00:10:17.160 00:10:17.170 now once you take a look at this if we
00:10:19.679 00:10:19.689 take
00:10:21.860 00:10:21.870 32-degree water and we go back down here
00:10:24.290 00:10:24.300 it is it is a hundred and sixty BTUs to
00:10:29.030 00:10:29.040 get it to that point and then we raise
00:10:31.910 00:10:31.920 the temperature to 212 degrees it only
00:10:36.620 00:10:36.630 takes one hundred and eighty BTUs of
00:10:38.510 00:10:38.520 heat to do that that's not a lot of
00:10:41.360 00:10:41.370 energy in the form of molecules in
00:10:43.519 00:10:43.529 motion so raising the temperature of
00:10:46.850 00:10:46.860 something really doesn't absorb or
00:10:49.820 00:10:49.830 release a lot of heat but when we hit
00:10:52.370 00:10:52.380 this point right here where it's at its
00:10:54.079 00:10:54.089 saturation point and we take that pan of
00:10:57.829 00:10:57.839 water and we turn it from liquid into
00:11:00.320 00:11:00.330 00:11:00.800 00:11:00.810 it takes 970 BTUs of latent heat to do
00:11:06.920 00:11:06.930 that and this is with one pound of water
00:11:09.070 00:11:09.080 so this is where the refrigeration
00:11:12.590 00:11:12.600 process happens not with water but with
00:11:15.860 00:11:15.870 refrigerant so I want you to remember
00:11:17.150 00:11:17.160 that changing of state is requires a
00:11:21.440 00:11:21.450 tremendous amount of heat in the form of
00:11:25.760 00:11:25.770 molecules of motion and if we go
00:11:27.470 00:11:27.480 backwards down this down this chart and
00:11:32.060 00:11:32.070 we hit the saturation point where it is
00:11:35.110 00:11:35.120 almost all steam and just starting to
00:11:38.090 00:11:38.100 turn into liquid from vapor to liquid
00:11:40.040 00:11:40.050 all of the heat that we gained as we
00:11:43.220 00:11:43.230 travel back down from vapor to liquid
00:11:45.820 00:11:45.830 that all that 970 BTUs is released from
00:11:50.660 00:11:50.670 the water until it hits 211 degrees and
00:11:55.610 00:11:55.620 then it's going to start losing its
00:11:57.650 00:11:57.660 sensible heat again this is where the
00:11:59.930 00:11:59.940 refrigeration process takes takes place
00:12:10.900 00:12:10.910 all right superheat once that liquid and
00:12:16.270 00:12:16.280 in this case water but refrigerant as
00:12:18.640 00:12:18.650 well once that liquid has changed state
00:12:22.900 00:12:22.910 completely in the vapor adding any more
00:12:25.030 00:12:25.040 heat will increase the temperature now
00:12:31.020 00:12:31.030 that's where we talked about right here
00:12:36.730 00:12:36.740 we've changed we have changed the
00:12:42.850 00:12:42.860 liquid-vapor combination into 100% vapor
00:12:46.600 00:12:46.610 any heat that is added this is our super
00:12:49.690 00:12:49.700 heat heat that is added is called super
00:12:52.690 00:12:52.700 heat and this is where this happens so
00:12:55.480 00:12:55.490 that is this part of the chart right
00:12:58.960 00:12:58.970 here so when you think about super heat
00:13:02.560 00:13:02.570 is heat that is added above the
00:13:06.370 00:13:06.380 saturation point after it turns into
00:13:08.949 00:13:08.959 100% vapor whether it be water or
00:13:13.139 00:13:13.149 refrigerant
00:13:16.720 00:13:16.730 so if you measure the temperature
00:13:20.750 00:13:20.760 if you measure the temperature of your
00:13:22.420 00:13:22.430 refrigerant or water
00:13:25.970 00:13:25.980 and you subtract the saturation
00:13:28.060 00:13:28.070 temperature from it what is remaining is
00:13:30.860 00:13:30.870 the superheat and this is it this is
00:13:33.560 00:13:33.570 when it's in the vapor form
00:13:40.430 00:13:40.440 now this has a lot to do with
00:13:41.630 00:13:41.640 refrigeration troubleshooting which
00:13:43.100 00:13:43.110 we'll get into in another webinar but
00:13:46.400 00:13:46.410 superheat and
00:13:49.610 00:13:49.620 subcooling
00:13:53.960 00:13:53.970 Orton so subcooling okay so once our
00:13:57.410 00:13:57.420 vapors changed completely back into
00:14:00.319 00:14:00.329 liquid or 100 percent liquid removing
00:14:03.769 00:14:03.779 heat will decrease the temperature so
00:14:06.879 00:14:06.889 we're removing sensible heat so if you
00:14:09.650 00:14:09.660 take your saturation temperature and
00:14:11.329 00:14:11.339 then you measure measure
00:14:15.440 00:14:15.450 the temperature of the liquid the
00:14:18.170 00:14:18.180 difference is sub cooling now on our
00:14:21.380 00:14:21.390 chart
00:14:25.670 00:14:25.680 that's what happens right down here so
00:14:28.450 00:14:28.460 here we're at saturation point we're
00:14:30.950 00:14:30.960 dumping all of the latent heat latent
00:14:33.170 00:14:33.180 heat latent heat latent heat at this
00:14:35.300 00:14:35.310 point from here
00:14:38.260 00:14:38.270 from here downwards
00:14:42.230 00:14:42.240 is our is our subcooling so
00:14:46.890 00:14:46.900 we'll get into this again in more detail
00:14:48.750 00:14:48.760 but they're actually the entire
00:14:51.300 00:14:51.310 refrigeration cycle happens between sub
00:14:54.870 00:14:54.880 cooled liquid through the saturation
00:14:57.390 00:14:57.400 point up to superheated vapor and then
00:15:00.780 00:15:00.790 back down again
00:15:01.920 00:15:01.930 down to this chart and we'll get into
00:15:03.960 00:15:03.970 the refrigeration cycle we will
00:15:07.520 00:15:07.530 we will explore this chart a little bit
00:15:09.740 00:15:09.750 further
00:15:14.260 00:15:14.270 okay gas laws I know they had Boyle's
00:15:16.960 00:15:16.970 law dalton's law the law of combined gas
00:15:19.949 00:15:19.959 what you really need to know is if you
00:15:22.510 00:15:22.520 compress a gas and reduce its volume
00:15:25.500 00:15:25.510 both the temperature
00:15:29.020 00:15:29.030 and pressure will increase so if you if
00:15:31.120 00:15:31.130 you have a piston then you put air in
00:15:33.550 00:15:33.560 that piston and you compress that piston
00:15:35.640 00:15:35.650 you think about it heat is more heat and
00:15:38.440 00:15:38.450 pressure are molecules in motions so if
00:15:40.690 00:15:40.700 you reduce the amount of space those
00:15:42.190 00:15:42.200 molecules have to bounce around that
00:15:45.010 00:15:45.020 heat is increased and so is the
00:15:46.540 00:15:46.550 temperature and conversely if you expand
00:15:48.910 00:15:48.920 that gas and put and pull that piston
00:15:51.700 00:15:51.710 back down both the temperature and the
00:15:54.580 00:15:54.590 pressure will decrease because those
00:15:56.170 00:15:56.180 molecules that are in motion aren't
00:15:58.830 00:15:58.840 don't bounce as fast and and against
00:16:03.550 00:16:03.560 each other to create that heat and
00:16:05.140 00:16:05.150 pressure so that's the one thing you
00:16:06.880 00:16:06.890 need to remember with with the gas law
00:16:10.210 00:16:10.220 if you increase pressure you increase
00:16:13.420 00:16:13.430 temperature if you increase temperature
00:16:14.980 00:16:14.990 you increase pressure as well and the
00:16:18.580 00:16:18.590 same thing if you decrease the pressure
00:16:21.700 00:16:21.710 you decrease the temperature that they
00:16:24.580 00:16:24.590 happen together
00:16:31.970 00:16:31.980 00:16:33.870 00:16:33.880 okay and here's an example of that so
00:16:37.350 00:16:37.360 here's our piston and we fill this
00:16:39.710 00:16:39.720 piston with air and it's at atmospheric
00:16:43.559 00:16:43.569 pressure which is 14 point 7 psi and we
00:16:47.819 00:16:47.829 reduce this piston by half the size we
00:16:51.749 00:16:51.759 compress this gas and we reduce the
00:16:54.449 00:16:54.459 volume in half it doubles the pressure
00:16:56.939 00:16:56.949 it's also going to increase the heat
00:17:00.960 00:17:00.970 because these molecules are bouncing
00:17:02.790 00:17:02.800 around in here at whatever rate they are
00:17:07.079 00:17:07.089 but if we decrease the area and the
00:17:10.439 00:17:10.449 volume of where these molecules bounce
00:17:12.840 00:17:12.850 around they bounce around faster and
00:17:14.970 00:17:14.980 when they bounce around faster that
00:17:16.740 00:17:16.750 remember heat is our molecules in motion
00:17:18.779 00:17:18.789 the more motion the more heat that's
00:17:20.760 00:17:20.770 generated
00:17:27.250 00:17:27.260 okay and this is just an illustration
00:17:29.289 00:17:29.299 here of
00:17:32.530 00:17:32.540 a bottle of liquid that's at its
00:17:35.440 00:17:35.450 saturation point as refrigerant at 75
00:17:39.220 00:17:39.230 degrees it's 132 psi and if we reduce
00:17:43.240 00:17:43.250 the temperature
00:17:46.150 00:17:46.160 it reduces the pressure as well and if
00:17:49.690 00:17:49.700 we have this jug over here and we read
00:17:52.420 00:17:52.430 we vent off some of this pressure it's
00:17:55.690 00:17:55.700 and decrease the pressure is also going
00:17:58.450 00:17:58.460 to decrease the temperature
00:18:01.600 00:18:01.610 so remember pressure increase
00:18:03.430 00:18:03.440 temperature increase
00:18:05.810 00:18:05.820 pressure decrease temperature decrease
00:18:09.560 00:18:09.570 make sense all right
00:18:16.460 00:18:16.470 now we're still again talking about
00:18:19.100 00:18:19.110 water the changing of state of water at
00:18:24.110 00:18:24.120 atmospheric pressure happens at 212
00:18:27.980 00:18:27.990 degrees Fahrenheit
00:18:34.770 00:18:34.780 and we can see that right here this is a
00:18:38.040 00:18:38.050 pressure temperature chart for water
00:18:42.770 00:18:42.780 and the way
00:18:47.890 00:18:47.900 when we're looking at any type of
00:18:49.090 00:18:49.100 pressure
00:18:49.629 00:18:49.639 temperature chart this is talking about
00:18:53.039 00:18:53.049 saturation
00:18:56.970 00:18:56.980 temperatures and pressures that's when
00:18:59.100 00:18:59.110 we are both liquid and vapor
00:19:01.990 00:19:02.000 and if we add any heat it's going to
00:19:04.540 00:19:04.550 change state from liquid to vapor and if
00:19:07.270 00:19:07.280 we remove heat is going to change state
00:19:09.040 00:19:09.050 from vapor to liquid once we're 100%
00:19:11.440 00:19:11.450 liquid or 100% vapor this chart right
00:19:14.320 00:19:14.330 here has no bearing whatsoever on what's
00:19:17.920 00:19:17.930 going on so there are this is a pressure
00:19:20.940 00:19:20.950 temperature chart or Pt chart for water
00:19:23.620 00:19:23.630 and we we have these charts for
00:19:27.370 00:19:27.380 refrigerant as well but let's look at
00:19:29.710 00:19:29.720 this this is atmospheric pressure down
00:19:31.900 00:19:31.910 here at the bottom 14.7 PSI and
00:19:40.730 00:19:40.740 at four at atmospheric pressure water
00:19:43.850 00:19:43.860 will change state at 212 degrees now
00:19:47.210 00:19:47.220 let's say we reduce that atmospheric
00:19:50.810 00:19:50.820 pressure and we put the water into
00:19:55.129 00:19:55.139 somewhat of a vacuum we can change the
00:19:57.590 00:19:57.600 state of that water at 70 degrees
00:20:00.129 00:20:00.139 Fahrenheit
00:20:03.049 00:20:03.059 and the same thing happens if you
00:20:04.909 00:20:04.919 increase the pressure and it increases
00:20:08.989 00:20:08.999 the temperature that the water changes
00:20:10.669 00:20:10.679 State and we'll get into this again when
00:20:12.710 00:20:12.720 we get in the refrigeration cycle this
00:20:14.210 00:20:14.220 will start to make some more sense
00:20:19.510 00:20:19.520 so at 5115 psi and a pressure cooker
00:20:23.980 00:20:23.990 water doesn't change state until you
00:20:26.470 00:20:26.480 till it hits the 250 degree fahrenheit
00:20:30.420 00:20:30.430 range and that's when I hit saturation
00:20:33.490 00:20:33.500 where it's both liquid and vapor present
00:20:35.680 00:20:35.690 and if we add Heat it's going to change
00:20:39.370 00:20:39.380 state from liquid to vapor and if we
00:20:42.220 00:20:42.230 remove heat it's going to change state
00:20:44.080 00:20:44.090 from vapor to liquid
00:20:52.500 00:20:52.510 00:20:55.090 00:20:55.100 okay and this is just an example if we
00:20:57.399 00:20:57.409 have a bell jar and week and we have a
00:21:00.279 00:21:00.289 vacuum pumping and back it out we can
00:21:03.430 00:21:03.440 make water change state at 70 degrees
00:21:06.820 00:21:06.830 00:21:09.409 00:21:09.419 all right so let's get into the basic
00:21:10.849 00:21:10.859 refrigeration cycle step by step we're
00:21:12.649 00:21:12.659 going to go we'll talk about saturation
00:21:14.949 00:21:14.959 superheat sub cooling changing of state
00:21:17.839 00:21:17.849 and energy that's required to do this
00:21:20.829 00:21:20.839 the refrigeration process as we go along
00:21:25.129 00:21:25.139 00:21:27.780 00:21:27.790 all right so let me clarify some things
00:21:29.700 00:21:29.710 here to make a little bit more sense
00:21:31.400 00:21:31.410 this
00:21:34.940 00:21:34.950 signifies the wall in your home
00:21:39.760 00:21:39.770 the wall is the indoor unit this is the
00:21:42.010 00:21:42.020 blower where you change your filter
00:21:43.420 00:21:43.430 here's our fan
00:21:45.990 00:21:46.000 here's our cooling coil or evaporator
00:21:49.259 00:21:49.269 coil right here
00:21:53.220 00:21:53.230 these are the lines that connect the
00:21:55.350 00:21:55.360 copper lines that connect the indoor
00:21:57.810 00:21:57.820 unit now yours may be in a closet in an
00:22:00.299 00:22:00.309 attic or garage crawlspace wherever it
00:22:02.399 00:22:02.409 may be this this part is the indoor unit
00:22:10.230 00:22:10.240 our copper lines they pass through the
00:22:12.600 00:22:12.610 wall they go out to the outdoor unit
00:22:14.370 00:22:14.380 which is the condenser and this is what
00:22:17.190 00:22:17.200 sets outside your home here's the
00:22:19.230 00:22:19.240 condenser fan
00:22:21.220 00:22:21.230 here's the condenser coil everything
00:22:23.800 00:22:23.810 else has been removed from this diagram
00:22:25.510 00:22:25.520 to help us get a better idea of the
00:22:28.930 00:22:28.940 refrigeration cycle
00:22:33.039 00:22:33.049 our textbook starts the refrigeration
00:22:35.229 00:22:35.239 cycle at the compressor I like to start
00:22:39.249 00:22:39.259 it here at the metering device and right
00:22:42.220 00:22:42.230 at the beginning of the metering device
00:22:43.950 00:22:43.960 we're going to start so we will start
00:22:49.180 00:22:49.190 and we'll get back to this point and
00:22:50.919 00:22:50.929 we'll end up right here we are going to
00:22:52.989 00:22:52.999 start with 100% liquid refrigerant
00:22:56.759 00:22:56.769 entering the metering device and for the
00:22:59.979 00:22:59.989 sake of this webinar we are going to
00:23:05.099 00:23:05.109 just take a look think about our our
00:23:08.229 00:23:08.239 metering device
00:23:10.820 00:23:10.830 as
00:23:15.000 00:23:15.010 a restriction in the in our line right
00:23:18.480 00:23:18.490 here and what it does is it will
00:23:21.440 00:23:21.450 whatever type of muting device it may be
00:23:24.590 00:23:24.600 it will reduce the pressure
00:23:29.480 00:23:29.490 as a refrigerant moves through the
00:23:32.510 00:23:32.520 00:23:33.440 00:23:33.450 now the
00:23:37.320 00:23:37.330 our gas laws tell us when we reduce
00:23:39.749 00:23:39.759 pressure we also reduce temperature so
00:23:43.499 00:23:43.509 at this point in the refrigeration
00:23:47.580 00:23:47.590 process after the liquid refrigerant has
00:23:50.220 00:23:50.230 passed through the metering device the
00:23:54.269 00:23:54.279 refrigerant itself is 25 percent vapor
00:23:57.779 00:23:57.789 and 75 percent liquid and remember that
00:24:02.940 00:24:02.950 puts it right from liquid directly into
00:24:05.700 00:24:05.710 the saturation point because saturation
00:24:07.979 00:24:07.989 is when we have both liquid and vapor
00:24:10.399 00:24:10.409 present so we now have saturated
00:24:13.489 00:24:13.499 refrigerant at our indoor coil
00:24:19.060 00:24:19.070 and
00:24:21.230 00:24:21.240 we are we have our indoor fan that is
00:24:23.990 00:24:24.000 blowing 75 degree room air
00:24:28.480 00:24:28.490 across our evaporator coil with our
00:24:32.620 00:24:32.630 saturated refrigerant in there and
00:24:34.660 00:24:34.670 remember when refrigerant or anything
00:24:37.630 00:24:37.640 else is at its saturation point if you
00:24:39.370 00:24:39.380 add
00:24:41.810 00:24:41.820 kind of heat it's going to change the
00:24:43.760 00:24:43.770 state of the refrigerant so it's going
00:24:46.250 00:24:46.260 to start it's already 75 percent liquid
00:24:48.350 00:24:48.360 and 25 percent vapor and it is going to
00:24:51.640 00:24:51.650 continue to change state as it passes
00:24:54.590 00:24:54.600 through the evaporator coil and it's
00:24:58.340 00:24:58.350 changing state from liquid to vapor and
00:25:00.620 00:25:00.630 remember that when we are changing state
00:25:03.890 00:25:03.900 that requires a tremendous amount of
00:25:06.320 00:25:06.330 heat energy so all of the indoor 75
00:25:10.640 00:25:10.650 degree air that's passing across this
00:25:13.310 00:25:13.320 coil the heat energy in the form of
00:25:16.760 00:25:16.770 molecules of motion are being removed
00:25:19.810 00:25:19.820 from the air so as we remove the heat
00:25:23.600 00:25:23.610 we're able to now blow out
00:25:26.240 00:25:26.250 55 degree fahrenheit room air and and
00:25:31.220 00:25:31.230 begin to cool the home so we really
00:25:33.740 00:25:33.750 don't cool the house we remove the heat
00:25:36.890 00:25:36.900 from the air which makes it feel cooler
00:25:39.880 00:25:39.890 now let's take a look at something here
00:25:42.050 00:25:42.060 so we're at 75 percent liquid 25 percent
00:25:45.650 00:25:45.660 vapor as we exit the metering device and
00:25:52.320 00:25:52.330 we are at sixteen
00:25:53.940 00:25:53.950 PSIG
00:25:57.470 00:25:57.480 which equates to 40 degrees Fahrenheit
00:26:07.210 00:26:07.220 now this is the PT chart that we have in
00:26:09.980 00:26:09.990 our book
00:26:11.610 00:26:11.620 and let's just verify that now remember
00:26:13.710 00:26:13.720 we talked about the PT chart this only
00:26:15.870 00:26:15.880 has the it it only relates to our
00:26:22.440 00:26:22.450 refrigerant when is that the saturation
00:26:24.450 00:26:24.460 point so that's when we were at that
00:26:27.060 00:26:27.070 saturation point right now at the coil
00:26:28.920 00:26:28.930 now in this example we're using our
00:26:31.830 00:26:31.840 twenty two refrigerant which happens to
00:26:34.200 00:26:34.210 be this column right here and if we go
00:26:36.570 00:26:36.580 back
00:26:42.800 00:26:42.810 we're at 69 PSIG
00:26:47.050 00:26:47.060 so let's take a look let's go down this
00:26:48.970 00:26:48.980 let's go down this chart
00:26:53.779 00:26:53.789 and this is our pressure column for our
00:26:58.340 00:26:58.350 22 and at 69 psi G which is right about
00:27:02.479 00:27:02.489 here if we read it over to our
00:27:05.239 00:27:05.249 temperature column you can see that at
00:27:11.049 00:27:11.059 when we have saturated refrigerant at
00:27:15.279 00:27:15.289 for the sake of argument 69 psi G it is
00:27:19.940 00:27:19.950 a it is 40 degrees
00:27:26.159 00:27:26.169 and you can see here the gauge our gauge
00:27:29.039 00:27:29.049 reads 69 psig
00:27:32.520 00:27:32.530 and we have our thermometer on we can't
00:27:35.550 00:27:35.560 really measure this in the coil but for
00:27:37.560 00:27:37.570 the sake of our class we do if you could
00:27:41.490 00:27:41.500 measure that coil we would read 40
00:27:43.260 00:27:43.270 degrees and as this
00:27:46.550 00:27:46.560 saturated refrigerant pass is passes
00:27:48.920 00:27:48.930 through the evaporator coil it is
00:27:51.080 00:27:51.090 starting to change state more and more
00:27:53.870 00:27:53.880 and more and we're going from changing
00:27:56.360 00:27:56.370 state from liquid to liquid to vapor
00:27:57.860 00:27:57.870 picking up more
00:28:01.580 00:28:01.590 heat in the form of latent heat again
00:28:04.100 00:28:04.110 that's changing of state and
00:28:07.430 00:28:07.440 at this point we're at about 50 50 50
00:28:10.639 00:28:10.649 percent vapor 50% liquid and we are
00:28:15.379 00:28:15.389 still at 69 PSIG and still at 40 degrees
00:28:18.740 00:28:18.750 Fahrenheit because we're still at the
00:28:21.080 00:28:21.090 saturation point remember any heat
00:28:23.210 00:28:23.220 that's picked up is not measurable
00:28:25.269 00:28:25.279 measurable when we're at the saturation
00:28:28.249 00:28:28.259 point it changes the state of the
00:28:30.080 00:28:30.090 refrigerant so it's changing state from
00:28:33.139 00:28:33.149 liquid to vapor as we move through the
00:28:35.419 00:28:35.429 evaporator coil and it's sucking the
00:28:36.980 00:28:36.990 heat out of the indoor air
00:28:39.330 00:28:39.340 now at a certain point that where it is
00:28:43.669 00:28:43.679 where the engineers design this coil we
00:28:47.820 00:28:47.830 are now going to change this refrigerant
00:28:50.249 00:28:50.259 is now no longer going to be at a
00:28:52.350 00:28:52.360 saturation point although it's still at
00:28:54.600 00:28:54.610 69 psi G we are now at
00:28:59.900 00:28:59.910 don't 100% vapor point and from here on
00:29:06.010 00:29:06.020 we are no longer picking up sensible
00:29:09.130 00:29:09.140 heat we are excuse me we're no longer
00:29:11.620 00:29:11.630 picking up latent heat we're picking up
00:29:13.630 00:29:13.640 sensible heat and if we put our
00:29:15.940 00:29:15.950 thermometer on the line after we have
00:29:18.760 00:29:18.770 changed the state of that refrigerant
00:29:21.570 00:29:21.580 completely from liquid to vapor we can
00:29:25.419 00:29:25.429 now start to measure the sensible heat
00:29:30.440 00:29:30.450 of the refrigerant remember when we
00:29:32.690 00:29:32.700 talked about our sensible heat let's
00:29:36.530 00:29:36.540 take a look at that in this chart here
00:29:40.539 00:29:40.549 so
00:29:44.340 00:29:44.350 here's our here's the point where the
00:29:46.350 00:29:46.360 refrigerant enters the evaporator coil
00:29:49.530 00:29:49.540 it's it's at 75 percent liquid 25
00:29:54.900 00:29:54.910 percent vapor and as it travels through
00:29:58.080 00:29:58.090 the
00:29:59.660 00:29:59.670 evaporator coil it's picking up all of
00:30:02.120 00:30:02.130 the heat and changing state and that's
00:30:04.520 00:30:04.530 where all the heat energy is absorbed
00:30:06.200 00:30:06.210 into the refrigeration system and at
00:30:08.900 00:30:08.910 this point in our evaporator coil that
00:30:11.240 00:30:11.250 we just looked at we're now at a hundred
00:30:13.640 00:30:13.650 percent vapor and any heat that's gained
00:30:17.540 00:30:17.550 00:30:19.479 00:30:19.489 sensible heat and that is our
00:30:21.430 00:30:21.440 superheating point right here
00:30:23.799 00:30:23.809 there is really no cooling that happens
00:30:26.169 00:30:26.179 with the super heat
00:30:28.500 00:30:28.510 we have super heat
00:30:33.390 00:30:33.400 to make sure that we have 100% vapor
00:30:37.520 00:30:37.530 going back to the compressor so we're
00:30:40.650 00:30:40.660 going to go through this quickly again
00:30:43.380 00:30:43.390 so we have
00:30:48.030 00:30:48.040 solid column of sub cooled refrigerant
00:30:51.299 00:30:51.309 hits our metering device metering device
00:30:53.220 00:30:53.230 drops the pressure which drops the
00:30:55.200 00:30:55.210 temperature it changes us into the
00:30:57.000 00:30:57.010 saturation state where we have 75%
00:31:00.150 00:31:00.160 liquid and 25% vapor that refrigerant is
00:31:03.419 00:31:03.429 flowing through the evaporator coil and
00:31:07.430 00:31:07.440 the heat energy from the indoor room
00:31:11.460 00:31:11.470 again to 75 degrees in the room we're at
00:31:14.250 00:31:14.260 40 degrees Fahrenheit here heat travels
00:31:16.289 00:31:16.299 from the sub substance with more heat to
00:31:19.289 00:31:19.299 a substance with less heat and those
00:31:22.110 00:31:22.120 molecules of motion and all that heat
00:31:24.240 00:31:24.250 energy is used to change the state of
00:31:27.409 00:31:27.419 from liquid to vapor in the evaporator
00:31:30.210 00:31:30.220 at a certain point designed by the
00:31:32.730 00:31:32.740 engineers we hit 100% vapor and any heat
00:31:37.770 00:31:37.780 that's gained is the form is in the form
00:31:41.010 00:31:41.020 of sensible heat which is our super heat
00:31:43.860 00:31:43.870 and that makes sure that we have 100%
00:31:47.100 00:31:47.110 vapor going back to the outdoor unit to
00:31:49.799 00:31:49.809 the compressor because we all know you
00:31:51.000 00:31:51.010 can't compress liquid
00:31:54.980 00:31:54.990 all right so we hit we hit the
00:31:58.039 00:31:58.049 evaporator we hit the compressor with
00:32:05.420 00:32:05.430 100% vapor that has 20 degrees of
00:32:08.600 00:32:08.610 superheat
00:32:10.900 00:32:10.910 added to its 100% vapor now remember our
00:32:13.840 00:32:13.850 gas laws so when you come when this
00:32:16.060 00:32:16.070 compressor compresses the refrigerant
00:32:20.060 00:32:20.070 it increases the pressure which
00:32:22.700 00:32:22.710 increases the temperature now we we have
00:32:27.320 00:32:27.330 20 degrees of superheat in this vapor
00:32:29.630 00:32:29.640 and after it comes out of the out of the
00:32:32.750 00:32:32.760 compressor it is still it still contains
00:32:36.320 00:32:36.330 that 20 degrees of superheat
00:32:41.789 00:32:41.799 and as that refrigerant travels out of
00:32:44.310 00:32:44.320 the compressor it is beginning to cool
00:32:47.549 00:32:47.559 down and it's D super heating and it is
00:32:50.999 00:32:51.009 just letting off the sensible heat as it
00:32:54.720 00:32:54.730 enters in the into the condenser coil so
00:32:58.499 00:32:58.509 we're at 278 psi G and at a certain
00:33:02.460 00:33:02.470 point in the condenser coil we are going
00:33:04.649 00:33:04.659 to hit the saturation point of this
00:33:08.600 00:33:08.610 refrigerant and if we take a look
00:33:17.000 00:33:17.010 right here 278 PSIG here's our r22
00:33:22.370 00:33:22.380 column here's our temperature column
00:33:25.460 00:33:25.470 this is such the saturation point 278
00:33:29.049 00:33:29.059 psig for r22 means it's at 125 degree
00:33:35.770 00:33:35.780 temperature
00:33:38.840 00:33:38.850 now
00:33:41.000 00:33:41.010 we know that
00:33:45.270 00:33:45.280 heat travels from a substance with more
00:33:47.940 00:33:47.950 heat more molecules emotion to us to one
00:33:51.180 00:33:51.190 with less molecules of motion so our
00:33:53.760 00:33:53.770 outdoor air is 95 degrees Fahrenheit our
00:33:58.520 00:33:58.530 saturated refrigerant
00:34:02.720 00:34:02.730 at 125 degrees Fahrenheit so that heat
00:34:06.919 00:34:06.929 is traveling and leaving the 125 degree
00:34:12.409 00:34:12.419 condenser and is being dumped into the
00:34:15.950 00:34:15.960 95 degree air so we're from this point
00:34:20.480 00:34:20.490 on we are now
00:34:23.510 00:34:23.520 condensing back from vapor 100% vapor
00:34:28.639 00:34:28.649 and then we start to travel through the
00:34:30.889 00:34:30.899 evaporator coil and we are condensing
00:34:33.109 00:34:33.119 back down into liquid so all the heat
00:34:35.510 00:34:35.520 that we picked up over here has been
00:34:37.609 00:34:37.619 carried outside and we're dumping it
00:34:41.180 00:34:41.190 outside remember that all that heat
00:34:45.200 00:34:45.210 energy in this evaporator coil is now
00:34:49.249 00:34:49.259 being released outside so now we're
00:34:53.059 00:34:53.069 condensing back from
00:34:58.120 00:34:58.130 from vapor to liquid and as it travels
00:35:02.289 00:35:02.299 through the evaporate or the condensing
00:35:03.999 00:35:04.009 coil all that tremendous amount of heat
00:35:06.789 00:35:06.799 energy is being released and and again
00:35:09.400 00:35:09.410 if we have a thermometer at any point in
00:35:11.799 00:35:11.809 the condensing coil as long as we're at
00:35:13.809 00:35:13.819 the saturation point it's 125 degree
00:35:17.229 00:35:17.239 fahrenheit now I just saw a question pop
00:35:20.469 00:35:20.479 up there let me let me take a look at
00:35:23.380 00:35:23.390 that here and I'll answer that question
00:35:32.070 00:35:32.080 00:35:38.330 00:35:38.340 okay Andrew I'll get back with you on
00:35:40.640 00:35:40.650 that on that question okay so we have
00:35:48.090 00:35:48.100 we are at the saturation point through
00:35:50.820 00:35:50.830 the condensing coil we're dumping the
00:35:53.730 00:35:53.740 heat to the outside air and at a certain
00:35:56.460 00:35:56.470 point we are now back to 100% liquid
00:36:02.830 00:36:02.840 now any oh now the heat that is being
00:36:06.100 00:36:06.110 released from this liquid is in the form
00:36:10.810 00:36:10.820 of sub cooled liquid and let's take a
00:36:12.970 00:36:12.980 look at that take a look at our chart
00:36:16.420 00:36:16.430 here real quick
00:36:20.830 00:36:20.840 all right so let's take a look what we
00:36:22.420 00:36:22.430 what we just talked about
00:36:25.770 00:36:25.780 so here's our sensible heat remember
00:36:28.620 00:36:28.630 this is our superheated vapor point
00:36:32.070 00:36:32.080 right here
00:36:34.950 00:36:34.960 it enters the condensing coil and we are
00:36:38.940 00:36:38.950 changing from 100% vapor back down to
00:36:42.089 00:36:42.099 100% liquid at the point where it's 100%
00:36:46.010 00:36:46.020 liquid we start to pick up sensible heat
00:36:50.760 00:36:50.770 so this is our sub cooling
00:36:54.180 00:36:54.190 point so if we took our refrigeration
00:36:56.730 00:36:56.740 cycle and we started
00:36:59.420 00:36:59.430 right here at the
00:37:04.510 00:37:04.520 well we're going to start right here
00:37:08.839 00:37:08.849 we'll start right here with subcooled
00:37:10.400 00:37:10.410 liquid that hits our
00:37:13.310 00:37:13.320 metering device it goes immediately from
00:37:17.690 00:37:17.700 sub-cooled liquid to a saturation point
00:37:22.450 00:37:22.460 to the evaporator
00:37:24.910 00:37:24.920 boils off the refrigerant which is
00:37:27.370 00:37:27.380 changing state it takes tons of heat to
00:37:30.430 00:37:30.440 do that absorbs all that heat till is
00:37:33.370 00:37:33.380 100% vapor and then it goes into the
00:37:37.809 00:37:37.819 super heating part where it's picking up
00:37:39.609 00:37:39.619 sensible heat at that point it hits the
00:37:42.039 00:37:42.049 compressor it gets compressed
00:37:46.190 00:37:46.200 and the first part of the condensing
00:37:49.460 00:37:49.470 coil D superheats removes the heat we
00:37:52.250 00:37:52.260 hit the saturation point it comes back
00:37:54.770 00:37:54.780 down as it condenses back down from the
00:37:58.460 00:37:58.470 saturation point in two hundred percent
00:38:00.079 00:38:00.089 liquid goes through the evaporator by
00:38:02.900 00:38:02.910 the condenser excuse me and it becomes
00:38:05.720 00:38:05.730 sub cooled liquid again then it hits the
00:38:08.270 00:38:08.280 metering device goes back through the
00:38:11.349 00:38:11.359 evaporator coil and that is our
00:38:13.460 00:38:13.470 refrigeration cycle so
00:38:20.100 00:38:20.110 what we do is we take actually in
00:38:24.330 00:38:24.340 refrigeration as we take
00:38:28.210 00:38:28.220 heat from a place where it's not needed
00:38:30.910 00:38:30.920 which is the your home
00:38:34.579 00:38:34.589 and we take it and release it to a place
00:38:39.440 00:38:39.450 where it really doesn't matter which is
00:38:42.069 00:38:42.079 outside and it's all done through
00:38:47.360 00:38:47.370 do the refrigeration process so let's go
00:38:49.880 00:38:49.890 through this one more time then we'll
00:38:53.210 00:38:53.220 get we'll have about 10 or 15 minutes
00:38:56.840 00:38:56.850 for questions and to wrap this up
00:38:59.910 00:38:59.920 all right so we're going to start we
00:39:02.880 00:39:02.890 hate we hit our metering device with a
00:39:05.660 00:39:05.670 solid column of sub cold refrigerant the
00:39:09.599 00:39:09.609 metering device immediately drops the
00:39:13.970 00:39:13.980 refrigerant from sub cooled into the
00:39:17.309 00:39:17.319 saturation point where it's 25% vapor
00:39:20.519 00:39:20.529 and 75 percent liquid travels through
00:39:23.039 00:39:23.049 the evaporator coil where the indoor
00:39:25.890 00:39:25.900 room air is blown across the evaporator
00:39:29.880 00:39:29.890 coil and the heat is from the indoor
00:39:33.089 00:39:33.099 room air is transferred from the room
00:39:36.059 00:39:36.069 air and is used to change the state of
00:39:38.460 00:39:38.470 that refrigerant and that requires tons
00:39:41.549 00:39:41.559 and tons of heat energy to do that so we
00:39:45.000 00:39:45.010 are changing state changing state
00:39:46.680 00:39:46.690 changing state all the way through the
00:39:48.900 00:39:48.910 evaporator coil till we hit the certain
00:39:51.630 00:39:51.640 point where we have is designed by the
00:39:53.910 00:39:53.920 engineers all over all of the
00:39:56.460 00:39:56.470 refrigerant is boiled off and we are now
00:39:59.700 00:39:59.710 100% vapor and any heat that is picked
00:40:02.700 00:40:02.710 up doesn't really cool anything but it
00:40:05.819 00:40:05.829 does ensure that we have 100 percent
00:40:07.910 00:40:07.920 vapor heading back to the compressor so
00:40:11.190 00:40:11.200 we have superheated vapor coming back to
00:40:14.339 00:40:14.349 the compressor the compressor uses the
00:40:17.519 00:40:17.529 compression cycle to increase the
00:40:19.740 00:40:19.750 pressure which in turns increase the
00:40:22.259 00:40:22.269 temperature and we have superheated
00:40:25.049 00:40:25.059 vapor leaving the compressor as it
00:40:28.349 00:40:28.359 travels through the evaporator coil it
00:40:31.200 00:40:31.210 is shedding all of the superheat that's
00:40:32.849 00:40:32.859 called de-superheating until we hit the
00:40:35.190 00:40:35.200 saturation point again of the
00:40:37.410 00:40:37.420 refrigerant and we're changing state
00:40:38.910 00:40:38.920 back from liquid to vapor as it travels
00:40:43.589 00:40:43.599 through the evaporator coil all of that
00:40:46.019 00:40:46.029 heat that is picked up inside the house
00:40:48.779 00:40:48.789 is now released outside as it changes
00:40:51.569 00:40:51.579 state at a certain point in the
00:40:53.460 00:40:53.470 condensing coil we have now changed all
00:40:56.819 00:40:56.829 of the refrigerant back into liquid and
00:40:59.880 00:40:59.890 we have sub cooled liquid we have the
00:41:03.359 00:41:03.369 sub cooling process which makes sure
00:41:05.460 00:41:05.470 that we have 100% liquid
00:41:08.670 00:41:08.680 coming back to the evaporator coil now
00:41:12.180 00:41:12.190 that is and that is our refrigeration
00:41:14.330 00:41:14.340 process that's the basic refrigeration
00:41:17.250 00:41:17.260 process now if we're it if you're in one
00:41:20.550 00:41:20.560 of my students in the HVAC class we're
00:41:23.130 00:41:23.140 going to go through this again using a
00:41:26.420 00:41:26.430 txp will talk about overcharging and
00:41:28.980 00:41:28.990 undercharged systems and how that
00:41:30.900 00:41:30.910 affects the the refrigeration cycle and
00:41:35.220 00:41:35.230 system performance as well so I saw we
00:41:38.730 00:41:38.740 had a couple of questions so let's see
00:41:45.460 00:41:45.470 if we have any
00:41:51.770 00:41:51.780 in Andrew if you just want to hang on
00:41:53.450 00:41:53.460 there let me know but and then I'll chat
00:41:57.290 00:41:57.300 with here in just a bit
00:42:04.770 00:42:04.780 00:42:08.280 00:42:08.290 okay I I just had a question about how
00:42:13.080 00:42:13.090 can I get involved in the class I do
00:42:17.490 00:42:17.500 have if you go to HVAC training
00:42:20.640 00:42:20.650 solutions net I do have an HVAC
00:42:24.090 00:42:24.100 technician class commercial
00:42:26.460 00:42:26.470 refrigeration for HVAC technician
00:42:28.290 00:42:28.300 classes and Nate test prep courses and
00:42:35.630 00:42:35.640 if you're really if you're interested in
00:42:37.370 00:42:37.380 doing that you can reach me at H vac
00:42:39.350 00:42:39.360 training solutions at gmail.com thanks
00:42:41.210 00:42:41.220 for that question that wasn't a plug
00:42:42.530 00:42:42.540 that was real that was really a question
00:42:46.760 00:42:46.770 question if is it applicable to
00:42:48.890 00:42:48.900 Canadians as well this HVAC class that I
00:42:51.859 00:42:51.869 have gives you the basic knowledge and
00:42:55.210 00:42:55.220 understanding of the refrigeration
00:42:57.020 00:42:57.030 process as well as electronics and the
00:42:59.930 00:42:59.940 reading schematic diagrams safety tubing
00:43:03.200 00:43:03.210 and piping and so forth this prepares
00:43:05.390 00:43:05.400 you to take an HVAC exam should your
00:43:09.920 00:43:09.930 state or country require that and and
00:43:12.589 00:43:12.599 gives you the basic knowledge needed to
00:43:14.390 00:43:14.400 get it an entry-level position as an
00:43:16.310 00:43:16.320 HVAC technician
00:43:20.859 00:43:20.869 okay last chance for questions
00:43:26.570 00:43:26.580 I'd like to thank everyone for coming if
00:43:31.550 00:43:31.560 you go to HVAC training solutions net we
00:43:34.820 00:43:34.830 do have our online training calendar and
00:43:38.750 00:43:38.760 you can check out our training there and
00:43:42.320 00:43:42.330 Joe I'll ask if you want to if you have
00:43:44.780 00:43:44.790 if you want to stay late and have any
00:43:48.140 00:43:48.150 questions answered please feel free to
00:43:50.000 00:43:50.010 do so the rest of you thank you very
00:43:51.710 00:43:51.720 very much
Office location
Engineering company LOTUS®
Russia, Ekaterinburg, Lunacharskogo street, 240/12

Phone: +7 343 216 77 75

E-mail: info@lotus1.ru

Sales phone

Russia: +7 343 216 77 75

WhatsApp: +79122710308