Rankine Cycle (Simple and Basic)

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Language: en

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00:00:10.799 00:00:10.809 today's engineering topic is funking
00:00:13.770 00:00:13.780 cycle so what are we waiting for it
00:00:16.350 00:00:16.360 started right away Rankine cycle was
00:00:20.070 00:00:20.080 named after Scottish polymath and
00:00:22.230 00:00:22.240 Glasgow University professor William
00:00:24.690 00:00:24.700 John McCone Rankin it is a vapour power
00:00:27.389 00:00:27.399 cycle for a little definition power
00:00:30.269 00:00:30.279 cycle is a cycle which is heat to
00:00:32.339 00:00:32.349 generate work and since it's a vapour
00:00:34.709 00:00:34.719 cycle it uses the vapor phase or in this
00:00:38.130 00:00:38.140 case steam to rotate the blades of the
00:00:39.990 00:00:40.000 turbine it actually utilizes the heat
00:00:44.040 00:00:44.050 energy contained in coal oil for natural
00:00:52.979 00:00:52.989 gas and it converts it into mechanical
00:00:56.700 00:00:56.710 energy and eventually electrical energy
00:00:59.130 00:00:59.140 which of course provides electricity in
00:01:01.739 00:01:01.749 our city and in our homes one of the
00:01:04.560 00:01:04.570 best definitions for the cycle is that
00:01:06.780 00:01:06.790 it closely describes the process of
00:01:09.000 00:01:09.010 steam turbine systems and it's derived
00:01:11.280 00:01:11.290 from the Carnot cycle the most efficient
00:01:14.219 00:01:14.229 thermodynamic cycle which tells us that
00:01:16.859 00:01:16.869 power is dependent on the temperature
00:01:18.990 00:01:19.000 difference between a heat source and
00:01:20.819 00:01:20.829 cold source the higher the difference
00:01:23.429 00:01:23.439 the more mechanical power can be
00:01:24.959 00:01:24.969 efficiently extracted out of heat energy
00:01:27.859 00:01:27.869 so now let's talk about the variance are
00:01:30.779 00:01:30.789 the types of Rankine cycle we have a
00:01:33.330 00:01:33.340 reheat Rankine cycle it is a cycle which
00:01:36.420 00:01:36.430 we introduce the exhausted steam back
00:01:38.340 00:01:38.350 into the boiler to reheat it we also
00:01:40.830 00:01:40.840 have a regenerative Rankine cycle we
00:01:43.349 00:01:43.359 bleed apart the steaming two heat
00:01:44.969 00:01:44.979 exchangers to preheat the feed water
00:01:46.920 00:01:46.930 before entering the boiler
00:01:48.510 00:01:48.520 there is also an organic rankine cycle
00:01:51.149 00:01:51.159 it uses an organic high molecular mass
00:01:54.510 00:01:54.520 fluid with a boiling point occurring at
00:01:56.819 00:01:56.829 lower temperature than the water steam
00:01:58.800 00:01:58.810 phase change a supercritical Rankine
00:02:01.800 00:02:01.810 cycle is also one of the types
00:02:03.480 00:02:03.490 just like we heat and regenerative
00:02:05.190 00:02:05.200 Rankine cycle water is the working fluid
00:02:08.090 00:02:08.100 but it is operated at above this
00:02:10.980 00:02:10.990 critical pressure
00:02:13.000 00:02:13.010 so those are the types of ranking cycle
00:02:16.190 00:02:16.200 but here on this video we will only
00:02:18.680 00:02:18.690 discuss the most basic and fundamental
00:02:20.420 00:02:20.430 of the cycle the ideal Rankine cycle we
00:02:24.350 00:02:24.360 must be aware first that this operates
00:02:26.360 00:02:26.370 slightly different in the real Rankine
00:02:28.430 00:02:28.440 cycle this is a reversible cycle common
00:02:32.300 00:02:32.310 source of irreversibilities are
00:02:33.860 00:02:33.870 neglected such as frictional pressure
00:02:35.360 00:02:35.370 drops and undesired heat transfer with
00:02:37.910 00:02:37.920 the surroundings a constant pressure or
00:02:40.460 00:02:40.470 isobaric process and constant entropy
00:02:47.150 00:02:47.160 for isentropic process are used for the
00:02:50.300 00:02:50.310 equipment's involved in the cycle the
00:02:52.640 00:02:52.650 working fluid is water and it will
00:02:54.890 00:02:54.900 undergo a closed loop and will be reused
00:02:57.440 00:02:57.450 constantly so why do you use water as
00:03:01.220 00:03:01.230 the working fluid well simply because it
00:03:05.090 00:03:05.100 is not toxic not reactive highly
00:03:14.300 00:03:14.310 abundant love cost and good
00:03:22.340 00:03:22.350 thermodynamic properties to make a
00:03:26.990 00:03:27.000 Rankine cycle we need four processes
00:03:29.270 00:03:29.280 process 1 to 2 for the boiler process 2
00:03:34.670 00:03:34.680 to 3 for the turbine
00:03:37.540 00:03:37.550 process three to four for the condenser
00:03:41.100 00:03:41.110 and finally passes for you one for the
00:03:43.810 00:03:43.820 pump and that is what we are going to
00:03:46.600 00:03:46.610 discuss for the next part okay so let's
00:03:49.090 00:03:49.100 get started four passes wants you to
00:04:02.650 00:04:02.660 boiler these are the things that we need
00:04:04.870 00:04:04.880 to remember since boiler is a heat
00:04:07.270 00:04:07.280 exchanger equipment heat is added into
00:04:10.060 00:04:10.070 the boiler through a fuel which may be
00:04:12.310 00:04:12.320 coal oil or natural gas here water is
00:04:17.289 00:04:17.299 converted into steam or superheated
00:04:19.930 00:04:19.940 steam this is an isobaric process or a
00:04:23.200 00:04:23.210 constant pressure process the
00:04:26.620 00:04:26.630 temperature and entropy for this process
00:04:29.500 00:04:29.510 in pieces and we can solve the heat
00:04:32.110 00:04:32.120 addition by using the formula we've
00:04:35.200 00:04:35.210 added equals with energy administered
00:04:38.260 00:04:38.270 energy Inc or enthalpy out minus
00:04:41.950 00:04:41.960 enthalpy in for boiler note that this
00:04:46.480 00:04:46.490 equation is formed by using mass and
00:04:48.670 00:04:48.680 energy rig balance for control building
00:04:50.740 00:04:50.750 at steady-state neglecting pressure drop
00:04:53.050 00:04:53.060 so those are the important things that
00:04:55.210 00:04:55.220 you should remember it understanding the
00:04:57.340 00:04:57.350 boiler passes
00:04:58.770 00:04:58.780 00:05:07.379 00:05:07.389 now steam can be used in the next
00:05:09.969 00:05:09.979 process which is the process to the trip
00:05:12.249 00:05:12.259 turbine turbine is a rate generator
00:05:16.119 00:05:16.129 equipment
00:05:16.839 00:05:16.849 it contains series of stages are a set
00:05:19.779 00:05:19.789 of stationary and moving blades to
00:05:21.939 00:05:21.949 perform its function by using the steam
00:05:24.820 00:05:24.830 work is generated through the expansion
00:05:27.339 00:05:27.349 of vapor which may then be converted
00:05:29.799 00:05:29.809 into electricity through generator
00:05:31.860 00:05:31.870 compared to the previous process here
00:05:34.839 00:05:34.849 since we have an equipment that involves
00:05:36.850 00:05:36.860 work isentropic process or constant
00:05:39.670 00:05:39.680 integral process is assumed
00:05:41.170 00:05:41.180 yes it is a shame because in real world
00:05:43.299 00:05:43.309 there is no such thing as ideal on this
00:05:47.739 00:05:47.749 process the temperature and pressure
00:05:49.329 00:05:49.339 decreases and the formula for the work
00:05:52.149 00:05:52.159 is fluid energy in - fluid energy out
00:05:55.839 00:05:55.849 are the enthalpy - - and topic 3
00:05:59.399 00:05:59.409 note that question is formed by using
00:06:01.989 00:06:01.999 mass and energy weight balance for a
00:06:04.329 00:06:04.339 control volume at steady state and
00:06:06.129 00:06:06.139 lifting heat transfer with the
00:06:08.050 00:06:08.060 surroundings steam is now already
00:06:10.689 00:06:10.699 exhausted and so we need to take dark
00:06:13.480 00:06:13.490 against the boiler but there is no pump
00:06:15.550 00:06:15.560 that can pump steam so we need to
00:06:17.889 00:06:17.899 convert it first into water through
00:06:19.510 00:06:19.520 condensation so this is where our next
00:06:22.570 00:06:22.580 process comes in
00:06:25.220 00:06:25.230 00:06:32.429 00:06:32.439 process three to four condenser in order
00:06:36.070 00:06:36.080 to condense the steam a heat rejection
00:06:38.499 00:06:38.509 must occur most of the power plants
00:06:43.420 00:06:43.430 utilize the seawater as a cooling medium
00:06:45.369 00:06:45.379 to cool down and condense the steam
00:06:47.909 00:06:47.919 condenser consists of tubes to
00:06:49.989 00:06:49.999 accommodate the heat transfer of steam
00:06:51.640 00:06:51.650 and cooling water where cooling water is
00:06:53.860 00:06:53.870 in a separate stream this is a heat
00:06:57.459 00:06:57.469 exchange equipment so we assume that
00:06:59.080 00:06:59.090 this is an isobaric process or constant
00:07:02.050 00:07:02.060 pressure passes the entropy decreases
00:07:05.019 00:07:05.029 and the quality of the fluid changes
00:07:07.779 00:07:07.789 until it reaches a saturated liquid
00:07:09.969 00:07:09.979 state
00:07:10.659 00:07:10.669 so from steam to liquid the equation is
00:07:14.350 00:07:14.360 heat rejected because fluid energy in -
00:07:17.320 00:07:17.330 fluid energy out or enthalpy 3 -
00:07:20.010 00:07:20.020 enthalpy for not again that this
00:07:23.379 00:07:23.389 equation is formed by using a mass and
00:07:25.240 00:07:25.250 energy rate balance for a control volume
00:07:27.429 00:07:27.439 in steady state neglecting pressure drop
00:07:33.400 00:07:33.410 00:07:38.110 00:07:38.120 last process is passes for two one pump
00:07:42.010 00:07:42.020 00:07:44.950 00:07:44.960 pumps main purpose is to convey and
00:07:48.020 00:07:48.030 introduce back the condensed into the
00:07:49.969 00:07:49.979 boiler here work is needed that means
00:07:53.149 00:07:53.159 work is negative some plants name this
00:07:55.730 00:07:55.740 pump as boiler feed pump and it can be
00:07:58.459 00:07:58.469 either steam driven for electric
00:08:00.290 00:08:00.300 motor-driven
00:08:00.980 00:08:00.990 again since this is a work involve
00:08:03.619 00:08:03.629 equipment we assume that this is an
00:08:05.570 00:08:05.580 isentropic process or constant entropy
00:08:08.119 00:08:08.129 process the temperature slightly
00:08:11.749 00:08:11.759 increases and the fluid is in a sub
00:08:14.809 00:08:14.819 cooled region in the TS diagram the
00:08:17.779 00:08:17.789 formula for the pump is work it was
00:08:20.480 00:08:20.490 fluid energy add - fluid energy in work
00:08:23.480 00:08:23.490 enthalpy one - input before fluid energy
00:08:27.170 00:08:27.180 add our improper at is greater than the
00:08:29.149 00:08:29.159 enthalpy as the pump have imparted
00:08:30.830 00:08:30.840 energy to the fluid note again that
00:08:34.219 00:08:34.229 00:08:36.440 00:08:36.450 energy rate balance for control volume a
00:08:38.899 00:08:38.909 steady state neglecting heat transfer
00:08:41.029 00:08:41.039 with the surroundings and one more
00:08:44.089 00:08:44.099 important thing please remember that the
00:08:46.340 00:08:46.350 pump has the highest pressure in the
00:08:47.780 00:08:47.790 whole cycle
00:08:49.880 00:08:49.890 00:08:57.660 00:08:57.670 okay
00:08:58.810 00:08:58.820 so let's have a recap starting from the
00:09:01.030 00:09:01.040 boiler we convert the liquid water into
00:09:03.130 00:09:03.140 steam introduce it into the turbine to
00:09:08.560 00:09:08.570 generate work and then we condense it
00:09:10.480 00:09:10.490 into the condenser and pump the liquid
00:09:12.730 00:09:12.740 water back to the boiler through a
00:09:14.830 00:09:14.840 high-pressure pump so that's it
00:09:19.570 00:09:19.580 Engineering is a fun thing I always
00:09:21.760 00:09:21.770 suspend see you again for our other easy
00:09:24.040 00:09:24.050 and fun engineering topics is
00:09:26.010 00:09:26.020 engineering engineering topics made easy
00:09:29.470 00:09:29.480 and fun for you
00:09:34.550 00:09:34.560 00:09:38.430 00:09:38.440 you
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