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Single-Effect Evaporator - Heat Transfer Area
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00:00:03.210 --> 00:00:10.620 In this video I am going to show an example where we calculate the heat transfer area 00:00:10.620 --> 00:00:16.950 for a single effect evaporator that is being used to concentrate a salt solution. 00:00:16.950 --> 00:00:26.730 the feed salt solution is 1.5 % salt in water and the exit is 4% salt in water. 00:00:26.730 --> 00:00:33.920 And the feed rate is given and the temperature of the evaporator is at 1 bar and we are using 00:00:33.920 --> 00:00:41.739 saturated steam at 170 kPa to provide the heat for vaporization. 00:00:41.739 --> 00:00:50.960 And the question is, if we know the heat transfer coefficient 2500 W/m^2 per degree K, what 00:00:50.960 --> 00:00:57.449 is the heat transfer area and what assumptions do we have to make to do this calculation 00:00:57.449 --> 00:01:03.800 if this is the only information that we have available to us. 00:01:03.800 --> 00:01:11.350 So the first thing we do in a problem like this is to draw a diagram and define our variables. 00:01:11.350 --> 00:01:18.469 So here is a diagram and the single effect evaporator is explained in more detail in 00:01:18.469 --> 00:01:20.670 another video. 00:01:20.670 --> 00:01:28.070 Feeding in saturated steam to the evaporator through some sort of heat transfer coil, so 00:01:28.070 --> 00:01:34.630 the steam leaving, is condensed liquid at saturated conditions. 00:01:34.630 --> 00:01:41.930 Feed is 1.5% and the feed flow rate is 7500 kg/hr. 00:01:41.930 --> 00:01:47.890 One of the assumptions we make is there is no salt in the vapor which is certainly what 00:01:47.890 --> 00:01:49.330 we would expect. 00:01:49.330 --> 00:01:55.310 So the other assumptions, one is that the evaporating liquid is well mixed. 00:01:55.310 --> 00:02:02.460 And so that means the temperature for the vapor, temperature inside the temperature 00:02:02.460 --> 00:02:05.450 liquid, all the same temperature. 00:02:05.450 --> 00:02:16.640 it also means the concentration, this weight percent leaving is the same as the weight 00:02:16.640 --> 00:02:19.440 percent inside our evaporator. 00:02:19.440 --> 00:02:24.780 The second assumption we are going to make is that the heat of vaporization is going 00:02:24.780 --> 00:02:29.010 to be calculated based on the heat of vaporization of water. 00:02:29.010 --> 00:02:34.750 The fact that it is a solution, we could still use the steam tables to get the heat of vaporization. 00:02:34.750 --> 00:02:42.280 We also assume there is no heat of mixing or unmixing, and the salt is added to the 00:02:42.280 --> 00:02:44.450 water, water is removed from the salt. 00:02:44.450 --> 00:02:50.040 This may or may not be a good assumption based on information we have not knowing the salt. 00:02:50.040 --> 00:02:52.240 This is a reasonable first approximation. 00:02:52.240 --> 00:02:59.430 We are also going to assume that the boiling point temperature increase, namely the fact 00:02:59.430 --> 00:03:04.950 that we add salt, lowers the water fugacity if you like, and therefore raises the boiling 00:03:04.950 --> 00:03:05.950 point. 00:03:05.950 --> 00:03:08.520 We are going to assume for now that that is zero. 00:03:08.520 --> 00:03:14.930 That the concentration is low on a molar basis such that we don't get much of a temperature 00:03:14.930 --> 00:03:15.930 increase. 00:03:15.930 --> 00:03:20.640 This may not be a good assumption depending on the system and this can have a significant 00:03:20.640 --> 00:03:25.260 effect on the heat transfer area because looking at the temperature difference between this 00:03:25.260 --> 00:03:33.060 steam and the temperature TE.Our next step now is to write down mass balances for this 00:03:33.060 --> 00:03:40.010 system because we need to know the flow rates of the liquid and the vapor leaving in order 00:03:40.010 --> 00:03:43.150 to calculate the energies. 00:03:43.150 --> 00:03:48.420 And there is the overall mass balance, the flow coming in, the molar flow rate is leaving 00:03:48.420 --> 00:03:50.310 as liquid or as vapor. 00:03:50.310 --> 00:03:52.960 And then there is a balance on the salt. 00:03:52.960 --> 00:03:59.241 So if we take the mole fraction of the salt and the feed, times the molar flow rate, all 00:03:59.241 --> 00:04:03.000 of the salt appears in the liquid leaving. 00:04:03.000 --> 00:04:12.280 so this is 7500 kg/hr and we don't know L, but of course we can solve this to determine 00:04:12.280 --> 00:04:16.590 L. So this is the total liquid flow rate. 00:04:16.590 --> 00:04:20.890 Which means the vapor flow rate is 7500-2812. 00:04:20.890 --> 00:04:27.960 So the vapor flow rate 4688 kg/hr. 00:04:27.960 --> 00:04:35.830 Now that we have the mass balances, the next step is to do energy balance on the stream 00:04:35.830 --> 00:04:37.300 that we are evaporating. 00:04:37.300 --> 00:04:41.319 Apply the first law, steady state system, a flow system. 00:04:41.319 --> 00:04:42.319 No accumulation. 00:04:42.319 --> 00:04:52.110 The energy coming in is the mass flow rate times the enthalpy per kg entering the system. 00:04:52.110 --> 00:04:57.930 And then the energy leaving is the mass flow rate of the vapor times the enthalpy of the 00:04:57.930 --> 00:05:06.039 vapor per kg, minus the mass flow rate of the liquid times the enthalpy of the liquid 00:05:06.039 --> 00:05:08.060 per kg. 00:05:08.060 --> 00:05:10.629 And then the other term that we have is the heat transfer. 00:05:10.629 --> 00:05:17.889 So it is a heat transfer coefficient times the heat transfer area times the temperature 00:05:17.889 --> 00:05:24.220 difference, the temperature of the steam, saturated steam coming in, saturated liquid 00:05:24.220 --> 00:05:25.220 leaving. 00:05:25.220 --> 00:05:31.819 So everything is at water vapor and liquid TS- minus the temperature in the evaporator. 00:05:31.819 --> 00:05:32.919 so this is the first law. 00:05:32.919 --> 00:05:36.280 We can use steam tables to look up values. 00:05:36.280 --> 00:05:42.740 So what I have listed is flow rate, steam coming in 85 degrees we will assume that the 00:05:42.740 --> 00:05:49.900 1.5 wt% solution can be modeled as pure water at 85 decrees C. 00:05:49.900 --> 00:05:57.379 We will use the enthalpy of saturated steam at 85 degrees C, that is a pretty good approximation 00:05:57.379 --> 00:06:07.650 to the steam at 1 bar and 85 degrees C. Vapor at 1 bar, so 100 degrees C, and then liquid 00:06:07.650 --> 00:06:16.430 also at 1 bar, 100 degrees C. And then we look up for 170 kPa the saturation temperatures 00:06:16.430 --> 00:06:24.159 around 115 degrees C. So we can substitute the values for mass flow rates and our enthalpies 00:06:24.159 --> 00:06:25.280 into this equation. 00:06:25.280 --> 00:06:33.529 We are also given the heat transfer coefficients so our only unknown is the heat transfer area 00:06:33.529 --> 00:06:35.349 and that is what we are going to solve for. 00:06:35.349 --> 00:06:37.680 So let's substitute the numbers in. 00:06:37.680 --> 00:06:41.990 So here are the values substituted in that we looked up in the steam table and we calculated 00:06:41.990 --> 00:06:43.960 from the mass balances. 00:06:43.960 --> 00:06:48.960 And then we have to be aware of a Watt is a J/s. 00:06:48.960 --> 00:06:53.530 We have to keep units consistent and that is why it is valuable to write the units with 00:06:53.530 --> 00:06:54.530 each of the numbers. 00:06:54.530 --> 00:07:01.240 So we convert time to hours, convert J to kJ for the heat transfer coefficient. 00:07:01.240 --> 00:07:07.020 And then the temperature difference is the same as the temperature difference in K. 00:07:07.020 --> 00:07:15.110 Now certainly two significant figures is probably more than we can justify since we made a number 00:07:15.110 --> 00:07:16.110 of assumptions. 00:07:16.110 --> 00:07:21.190 And one of the big assumptions that affects things is the fact that the temperature difference 00:07:21.190 --> 00:07:27.340 here is going to affect the heat transfer area a lot is temperature is going to be higher 00:07:27.340 --> 00:07:31.850 for a 4% solution than the temperature difference is less the heat transfer area would have 00:07:31.850 --> 00:07:31.853 to be more.
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