Attention Central Business District Residents. This is a community notification of a new sexually violent predator in your area. Please stay tuned to the following short program for more information. Hi, I'm Technician Ron Hackett with the Denver Police Department. The Sex Offender Registration and Compliance Unit at DPD is responsible for the registration, monitoring and tracking of all registered sex offenders and sexually violent predators who live in the city and county of Denver. Here's a brief history of sex offender legislation in Colorado. Our state laws trickle down from federal government mandates. In 1994, we had the Jacob Wetterling Act, which mandated that states would establish a sex offender list. Megan's law of 1996 said that the public would have access to those sex offender registration lists. The Pam Litchner Act of 1996 stated that some offenders might have to have lifetime registrations. And the Adam Walsh Act of 2006 unified sex offender laws across the country. In Colorado, the legislature has determined that sexually violent predators, by definition, pose a higher risk to the community at large and therefore mandated that upon their release from the Department of Corrections, the community must be notified. Sex offender notification in Colorado happens in two ways. The first is passive and ongoing through the sex offender registration process, which is a list maintained by local police departments. The second way is active via community notification for those offenders determined to be sexually violent predators by the courts or by the parole board. Most sex offenders in Colorado are supervised by the criminal justice system in our communities. Most sex offenders engage in crossover behavior, which means they may have been arrested for one type of crime, but be apt to commit another.  There is no typical sex offender, but all tend to be deceptive, manipulative, and secretive. 80 to 93% of sex offenses are committed by someone known to the victim. Sexual deviancy begins in mid to late adolescence. Sex offenses are not impulsive.  The community has a vested interest in helping offenders to be successfully managed in the community. Sex offenders have the same need for housing and employment as any other citizen. Any citizen who uses sex offender information to harass, threaten, or intimidate an offender will be subject to criminal prosecution. There are approximately 16,500 registered sex offenders in the state of Colorado. About 65% of convicted sex offenders are placed in the community on probation. The remainder are in the Department of Corrections or Community Corrections. Offenders may be caught for one type of offense, but be at a high risk to commit another type. Crime of conviction is only one indicator of risk.  The offender's residence must be verified quarterly by the Denver Police Department. The full Sex Offender Registration List is available by calling the Denver Police Department Identification Bureau at<PHONE_NUMBER>. Convicted felons and those with multiple convictions are posted online at denvergov.org-police.   Now, here's a look at the newest sexually violent predator living in Denver. Here's an overview of the registered sex offenders currently living in Denver. There are 2,484 total living within city limits. In Denver Police District 6, there are 488. Precinct 611 has 168 registered sex offenders. Of those, 111 have felony convictions and 57 have misdemeanor convictions. Sydney Leon Smith is a sexually violent predator currently living in Denver. He's 52 years old and was born on February 27, 1967.  He's currently living at 1955 Arapaho Street, No. 404, in the central business district neighborhood of Denver. Schools located within one mile of this offender include University Prep School at 2409 Arapaho Street, Downtown Denver Expeditionary School and Emily Griffith High School, both at 1860 Lincoln Street, Rise Up Community School at 2342 Broadway, Whittier Elementary at 2480 Downing Street, Denver Language School Gilpin K-8 at 2949 California Street, Polaris Elementary at 410 Park Avenue West, Montessori Academy of Colorado at 2500 Curtis Street. Parks located within one mile of this offender include Mestizo Curtis Park, McIntosh Park, Railroad Dog Park, Benedict Fountain Park, Skyline Park, Broadway Triangles, Civic Center Park, Pioneer Monument Park, Confluence Park, Creekfront Park, Park Avenue Parks, Sculpture Park, Centennial Gardens, Spear Boulevard Park, Downtown Playground, Sunny Lawson Park, Denver Skate Park, Cuernavaca Park, Stout Street Children's Park, Miastas Park, Commons Park, Quick Park. Recreation centers located within one mile of this offender include Glenarm Rec Center at 2800 Glenarm Place, 20th Street Rec Center at 1011 Twentieth Street. Bus routes located within one mile of this offender include Routes 122X, FF4 and FF7 at 19th and Lawrence Street, Routes 38 and 52 at 18th and Lawrence Street, Routes 120 at 18th and Lawrence Street, Routes 9, 38 and 52 at 20th and Larimer Streets. A brief history of charges against this offender, sexual assault on a child, position of trust. He's not currently on parole and registered with the Denver Police Department on November 12, 2019 to 1955 Arapahoe Street number 404 in the Central Business District neighborhood of Denver. Past charges against this offender include drugs, escape, petty theft, trespassing, drug paraphernalia, parole violation, assault, disturbing the peace, burglary, aggravated vehicle theft. Sydney Leon Smith has been determined as sexually violent predator after meeting the following criteria. Criteria 1, age 18 or older on the date of the offense or under 18 and tried as an adult. The offender was age 35 at the time of the offense. Criteria 2, the crime must have been committed on or after July 1, 1997 and convicted on or after July 1, 1999.  The offender was convicted on December 16, 2002 for sexual assault on a child position of trust. Criteria 3, the relationship to the victim was one of the following. Victim was a stranger to the offender or the offender established or promoted a relationship with the victim primarily for the purpose of sexual victimization. The victim was a nine-year-old female. The offender was known to the victim. Criteria 4, positive results are the passing of a risk assessment instrument administered by probation parole staff and a qualified treatment evaluator. Positive results include an assessment for the presence of a mental abnormality, a level of denial regarding the offense, treatment appropriateness and motivation, presence of sexual deviant interests. The offender was evaluated by the Colorado State Board of Parole with positive results, determining him to be a sexually violent predator.


We have been learning about melting the charge and also how to treat the molten metal. Now in this lecture, let us see the fluidity of molten metal. The fluidity of molten metal is very important, because we may melt the metal, we may treat the metal, but after all it is going to occupy the cavity and it has to fill the entire cavity. It has to fill the entire thin sections of the mould cavity. If the molten metal does not possess enough fluidity, then the molten metal cannot fill the entire cavity. May be it may partly fill the cavity, but it may not fill the thin sections or the complex sections. That is why the fluidity of the molten metal has highest importance. Let us see in this lecture, let us learn about the factors that are governing the fluidity of the molten metal and how to improve the fluidity. Before that, let us see the definition for the fluidity. Fluidity may be defined as an empirical measure of the distance a liquid metal can flow in a specific channel before being stopped by solidification. So this is the definition for fluidity. Again physicists define fluidity as the reciprocal of the coefficient of its viscosity. Viscosity and fluidity, these will be always inversely proportional. If the viscosity is higher, fluidity will be lesser. If the viscosity is lesser, fluidity will be higher. Again metallurgists define it as the ability of a liquid metal or alloy to flow freely and thus to feed a mould cavity and produce the desired contour before freezing occurs. So this is the definition given by the metallurgists. Now most important thing is pure metals act with good fluidity. Now let us see the factors affecting the fluidity. Now there are two categories. One is the factors relating to the melt and the other category is the factors relating to the casting parameters. First let us see the casting factors related to the melt. First one is the freezing range of alloy. Fluency is inversely proportional to the freezing temperature range. In some alloys, the freezing temperature range will be longer. In some alloys, the freezing temperature will be shorter. For example, let us take the magnesium aluminum alloy. The aluminum's melting temperature of the freezing temperature is 660 degree centigrade whereas the freezing temperature of magnesium is only 650 degree centigrade. The difference is only 10 degree centigrade. So that is a short freezing range alloy whereas if we consider aluminum and tin alloy, aluminum freezes at 660 degree centigrade and tin freezes at 232 degree centigrade. Here the freezing range is longer than 400 degree centigrade. So that is a long freezing alloy. Now the question is the fluidity is inversely proportional to the freezing temperature range. Longer the freezing range, the shorter will be the fluidity or shorter the freezing range higher will be the fluidity. Next one alloy composition eutectic composition has higher fluidity. In any alloy system, there will be at a particular composition, there will be eutectic composition where there is no mushy zone. So that particular composition has the highest fluidity or the higher fluidity. Next one inclusions insoluble particles can increase viscosity and reduce fluidity. When there are insoluble inclusions, what happens? They increase the viscosity and also they reduce the fluidity. Next one surface tension, it decreases the fluidity and often caused by oxide films. Next one viscosity, higher the viscosity, lesser the fluidity. This we have already seen. Next one latent heat of fusion of alloy. What is this latent heat of fusion? When you alloy is freezing, heat is liberated during the phase transformation. Now higher the latent heat of fusion, higher will be the fluidity. Now all these we will be analyzing and discussing later. Next one there is another set of what say parameters. These are the factors related to the casting parameters. Now first one is the modulus. Fluidity length increases as the modulus of the casting increases. Now what is modulus? Modulus is the ratio of volume to surface area. Now as the modulus is increasing, fluidity is also increasing. What does it mean? When the what say this modulus is increasing, the surface area is decreasing. That is the meaning. When the surface area is decreasing, less heat is dissipated to the mould wall. When less heat is dissipated to the mould wall, it will stays in the liquid state for a longer time. Then what happens? The fluidity will be increasing. Next one section thickness, larger thickness of the section results in higher fluidity. Next one heat transfer coefficient. A reduction in the rate of heat transfer will increase the fluidity. What is this heat transfer coefficient? It stands for the amount of heat what say that is transferred from the casting to the mould wall. Now when this heat transfer coefficient is smaller, then what happens? Less heat is transmitted from the casting to the mould wall. Then what happens? The molten metal will be in liquid state for a longer time. That is how its fluidity will be increasing. Next one super heating. What is this super heating? For example, if an alloy or a metal freezes or melts at a particular temperature. For example, let us take aluminum, pure aluminum melts at 660 degree centigrade. But we never pour the what say aluminum at 660 degree centigrade. We always keep a higher temperature for pouring may be at 700 or 750 degree centigrade. So we always pour the alloy or the metal at a temperature higher than its melting point. This is known as the pouring temperature. So for a casting alloy or a casting metal there are two temperatures. One is the pouring temperature, another one is the melting temperature. Melting temperature is the temperature at which the alloy or the metal actually melts. Whereas pouring temperature is such a temperature it is a somewhat higher temperature at where will be pouring. Now the super heating is the difference of these two temperatures. It is the difference between the melting temperature and the pouring temperature. So as the super heating is increasing what happens? The fluidity will be increasing. Next one, mould temperature. Higher mould temperature increases fluidity. When the temperature of the mould is higher than what will happen? The temperature difference between the molten metal and the mould is lesser. Lesser the temperature difference means that is the temperature gradient lesser will be the heat transfer means the molten metal continues to be in liquid state for a longer time. That be the case the fluidity will be increasing. Next one pouring rate. Lower pouring rates decrease fluidity because of larger cooling. Now let us see the first category of factors. These are the factors affecting fluidity related to the melt. First one is the freezing range of alloys. Now there are two what say alloys primarily one is the short freezing range alloys and the other one is the long freezing range alloys. Now first let us analyze the short freezing range alloys. These alloys solidify at a narrow range of temperature for example, aluminium and magnesium alloy. Aluminium freezes at 660 degrees centigrade and magnesium freezes at 650 degrees centigrade only 10 degrees difference in the freezing. So there is a narrow range of temperature. Next one solidification starts from the mould wall and grows inside. Solidification needs to be 100 percent complete at one location for the flow to stop. As long as the solidification is continuing and until and unless the solidification becomes 100 percent the liquid metal continues to flow. Total fluidity length for these materials is equal to is given by Lf is equal to v t f where v is the velocity of flow. Most of the times this velocity may not be uniform but assuming it is the constant then t f is the time for solidification. Now here we can see this is the mould a cylindrical mould and it sees for a short freezing range alloy. This is the cylindrical mould and this is the molten metal. Now what happens earlier we have discussed the solidification starts from the mould wall and it slowly progresses inside. Here we can see that this is this deep blue coloured one is the solidified metal. Now the solidification has started here and slowly it is becoming larger and larger like this. And here also from this side also the solidification starts and it is becoming larger and larger. Now what happens till the entire section is blocked by the molten metal the molten metal will be flowing to the other direction. Now that is how we have seen Lf is equal to v t f where v is the velocity of flow and t f is the time for solidification. Now let us see the long freezing range alloys. Freezing over a wide range of temperature means the freezing starts at a particular temperature and freezing continues for a long what is a freezing temperature means for example best thing is aluminium tin, aluminium freezes at what is a 660 degree centigrade and tin freezes at 232 degree centigrade. Now the freezing range is very long. Next one dendritic mode of solidification during the solidification dendrites will be forming and these will be hindering the flow of molten metal. Next one these dendritic crystals offer resistance to the flow of liquid metal. Then what happens at some point of solidification in the range of 20 to 50% solid the flow ceases because of the obstruction caused by the dendritic crystals. Then here the total fluidity length for these materials is equal to Lf is equal to x v t f. Here x is coming additionally when we compare the what is a fluidity length for the short freezing range alloys here x is extra. What is this x? x is the fraction of solids in melt when solidification ceases. Now here you can see this is the what is a solidification pattern for a long freezing alloy. Now you can see here this is the initial stage of solidification as the solidification is advancing and here we can see these are the dendrites dendrites and these dendrites will be increasing and at a particular stage they will be causing obstruction to the flow of metal. Now the total fluidity length Lf is equal to x v t f v is the velocity of flow t f is the time for solidification and x is the fraction of solids in melt when the solidification ceases. Now we need to consider this x what is the nature of x? Now a comparison between short freezing range alloys and long freezing range alloys. In the case of the short freezing range alloys Lf is equal to v t f where Lf is the total fluidity length v is the velocity of flow and t f is the time for solidification and in the case of the long freezing range alloys almost it is same Lf is equal to x v t f this x is coming additionally. Now where Lf is the total fluidity length v is the velocity of flow t f is the time for solidification and x is the fraction of solids in the melt when the solidification ceases and it is always less than 1 then what happens in which case the fluidity will be longer naturally because this x is less than 1 the fluidity in long freezing range alloys will be lesser than that of the fluidity in short freezing range alloys thus the fluidity length in long freezing range alloys is always less. Now what is our conclusion longer freezing range of an alloy what say reduces the fluidity next one let us consider the next factor that is the alloy composition effect of alloying elements effect of small concentrations of tin on the fluidity of pure aluminum we are considering the fluidity of pure aluminum and when there are small what say traces of tin now here this graph depicts the effect of alloying element on the fluidity. Now here you can see the x axis indicates the what say percentage of tin and y axis indicates the fluidity now as the tin proportion is increasing the fluidity is decreasing what we can say the alloying elements will be reducing the fluidity here we can see another graph right so this is a this is the phase diagram and here we can see this is metal A and this is metal B this side it is only pure metal A and this side it is pure metal B in between the what say as we what say progress from left to right the proportion of B metal is increasing gradually starting from 0 now here we can see this is the phase diagram and here this is the eutectic composition means there is no mushy zone now here we can see now let us see this is the what say graph which reflects as the fluidity of this alloy system now here at the point A it is a pure metal A and 0 of B 100 percent of A now what happen fluidity is very high let us come to the other side this is metal B only B and 0 of A you see this fluidity and this axis y axis indicates the fluidity fluidity is very high now let us see this is the eutectic point means there is no mushy zone here also fluidity is very high now this is what we can what say conclude the fluidity is between the three peaks are lower by a factor of 2 to 16 more typically 2 to 4 the fluidity between these three peaks is lower you see here it is lower and here it is lower again what we can conclude the fluidity is highest for pure metals and here it is pure metal A fluidity is very high here it is pure metal B here the fluidity is very high next one for an alloy the fluidity is also higher at the eutectic composition so this is the eutectic point you see here this is the fluidity means at the eutectic point also fluidity is very higher and here the fluidity of aluminum silicon alloys and here we can see here the fluidity is higher next one effect of alloying elements right the fluidity of aluminum zinc alloys let us consider another alloy that is the aluminum zinc alloys. Now this is the phase diagram of aluminum zinc this is the phase diagram and here we can see this is the solidus means below solidus there is only solid and here we can see this is the liquidus line means above that liquidus there is only liquid between liquidus and solidus there is a mushy zone so this is the what is the phase diagram and here we can see this is the eutectic point means there is no mushy zone above the eutectic point only liquid and below the eutectic point only solid no mushy zone. Now let us consider how the fluidity will be changing in this system now let us consider constant pouring temperature that will be the case how the fluidity will be now for example yes in the same alloy it is what is a freezing point is about 650 degree centigrade if it is pure aluminum 660 degree centigrade. Now generally we add another 50 degrees for super heating may be at 710 or at 725 we start pouring if it is the constant pouring what happens may be when the composition is this much when the composition is pure aluminum when the freezing point is 660 we are keeping constant pouring temperature may be at 700 degree centigrade. Now as we move to the right side then what happens slowly zinc's proportion is increasing as the zinc's proportion is increasing what is happening to the melting temperature of the alloy here it may be some 600 and here it may be some 500 and here it may be some 400 as the zinc proportion is increasing the melting point of that alloy will be decreasing but the pouring temperature we are keeping constant that is the 700 degree centigrade whether the what is a alloy is of a pure metal or whether it is zinc is say some 25 percent or 50 percent the pouring temperature is 700 only then what will happen yes here when it is pure aluminum yes the difference or the difference between the pouring temperature and the melting temperature is only about some 40 degree centigrade but as the zinc's concentration is increasing that difference is also increasing what is the difference the difference is the super heat. Super heat is the difference between the pouring temperature and the melting temperature as the super heat is increasing fluidity is also increasing we are not altering the pouring temperature pouring temperature is 700 only then what happens here 700 is somewhere here this is the difference this is the difference this is the difference as the zinc concentration is increasing this difference or the super heat is also increasing that is how the fluidity will be increasing at constant pouring temperature. So, this curve indicates the what is the fluidity of the system at constant pouring temperature you see as the zinc concentration is increasing at constant pouring temperature the fluidity is increasing. Now, this is the eutectic point at eutectic point fluidity is very high. Now, let us consider a what is a liquid is temperature plus 50 degree centigrade. Now, we are not considering a constant pouring temperature constant pouring temperature means we consider 700 degree centigrade constant whatever be the what is a melting temperature or the freezing temperature. Now, we are considering we are choosing such a pouring temperature such that the pouring temperature will be liquid is temperature plus 50 degree centigrade means what is happening the liquid is temperature is slowly coming down as the zinc concentration is increasing. But, we are not a what is a we are keeping the pouring temperature just 50 degrees above the liquid is temperature whatever it is. Now, may be here it may be say right may be in a 710 degree centigrade and the as the zinc concentration is increasing even the pouring temperature will be just 50 degrees above the liquid is temperature that be the case what happens the super heat will be constant all through then what happens the fluidity also will be constant. Now, this line reflects the fluidity when the pouring temperature is just 50 degrees plus liquid is temperature the pouring temperature is constant. But, however at the eutectic point again it is very high that is how the fluidity of aluminum and zinc alloy will be changing. Next one inclusions effect of inclusions sand inclusions are mainly caused by bulk turbulence in gating channels or mould cavity which dislodges sand particles from the mould wall inclusions can obstruct the flow of metal stream and reduce the fluidity. Once these inclusions coming to picture what happens they can obstruct the fluidity of metal and they can reduce the fluidity. Next one let us see the surface tension. What is this surface tension back pressure experienced by the liquid metal due to surface tension resisting entry into a narrow mould. Now, this is here we can see this equation delta p is equal to gamma 1 by r x plus 1 by r y where delta p is the difference pressure difference known as the laplace pressure. Gamma is the surface tension r x and r y are ready of curvature in each of the axis that are parallel to the surface. Now, for cylindrical mould r x is equal to r y that be the case delta p is equal to 2 gamma divided by r and for thin and wide mould r y is equal to infinity that be the case delta p is equal to gamma by r. Now, this back pressure must be overcome by the metal head pressure otherwise the liquid will not enter into the mould. In larger mould or square sections where the ready r x and r y both become large in the range of 10 to 20 mm the effects of surface tension become too small to be neglected. Large sections are therefore filled easily. Next one let us consider the effect of viscosity. As the viscosity increases the fluidity decreases since the resistance to flow for the molten metal increases and the molten metal cannot pass through the mould cavity successfully. So, this is a what is a fundamental fact as the viscosity is increasing what happens the molten metal what say becomes thicker and thicker then what happens its fluidity will become smaller and smaller. Next one let us see the latent heat of fusion of the alloy. The latent heat given up on solidification will take time to diffuse away thereby delaying solidification and extending the fluidity. What is this? Every alloy or every metal during freezing releases latent heat. Now, what happens this latent heat causes the metal to be in liquid state for a longer time. Now, what happens silicon has a latent heat of solidification 4 to 6 5 times greater than that of pure aluminium that is why the hyper eutectic aluminium silicon alloys have higher fluidity. Now, here we can see this is the aluminium silicon phase diagram and here we can see this is the eutectic point means above the eutectic point only liquid and below the eutectic point only solid no mushy zone and this side means to the left of this eutectic point is the hypo eutectic alloy system and to the right of this eutectic point is the hyper eutectic alloy systems. Now, what happens in this case? Yes in the hyper eutectic alloys what happens the silicon content is increasing because of the higher silicon content during freezing what happens this silicon releases much what is a heat that is the latent heat of solidification because of that the fluidity will be increasing. Now, let us see the other category of factors these are the factors affecting fluidity related to casting parameters among them first one is the modulus what is modulus? Modulus is the ratio of volume to surface area of the casting that is the modulus. Now, this is the Chorinov's rule Chorinov's rule states that TST is equal to Cm multiplied by V by a to the power of n where TST is the total solidification time a is the surface area of the casting v is the volume of the casting n is the an exponent usually it is 2 and Cm is the constant it is a mould constant and depends upon the mould material. Now, as the modulus increases what happens total solidification time also increases if the total solidification time increases what will happen the fluidity also increases. Next one the section thickness effect of section thickness let us consider the fluidity of JTA 27 alloy in this case n exponent has been conducted now this x axis indicates the strip thickness and the y axis indicates the strip length means the fluidity length. Now, what happens these are all the pouring temperatures at 525, 45, 550, 570 and 600 degree centigrade. Now, in all these cases as the section thickness increases the fluidity also increases whatever be the pouring temperature when the section thickness is increasing it right the fluidity is also increasing. Next one heat transfer coefficient a reduction in the rate of heat transfer will benefit the fluidity right this coefficient of heat transfer reflects the amount of heat transfer from the casting to the mould wall. If the heat transfer coefficient is smaller less heat will be dissipated from the casting to the mould wall. So, for this reason insulating ceramic coatings are applied to all gravity and low pressure dyes and for sand moulds acetylene black is applied from a sooty flame giving very substantial increase in fluidity by a factor of 2 to 3. Now, a black flame or a black coating is given to the mould what is a cavity by a using this acetylene black what is the purpose so that the heat transfer coefficient becomes smaller means less heat will be dissipated from the casting to the mould because of that the fluidity will be increasing. This dramatic improvement in fluidity is used in some precision sand foundries alloying thin walled castings to be filled successfully. So, when the casting is a having larger thickness is no problem, but when a casting has very thin sections that time it is very difficult for the molten metal to flow into those thin sections it is that time we need to take some measures to improve the fluidity. So, we can decrease the heat transfer coefficient by doing this kind of techniques one is the if it is a die casting right we can always use ceramic coatings or if it is a sand mould we can apply acetylene black coating. Next we will see the influence of super heating on fluidity first of all we should know what is meant by super heating it is defined as the excess of casting temperature over liquid temperature. So, that is the super heat. So, for example, let us see the aluminum zinc phase diagram here you can see here. So, this is the liquid as temperature and this is the solidus line and this is the liquidus line means everything above this line is in liquid state and everything below this line is in solid state and this is the mushy zone. Now fluidity increases linearly with the super heat. So, as the super heat is increasing the fluidity will be increasing. So, at constant super heat the fluidity of the eutectic is almost exactly that expected from the rule of the mixtures. Now when determined at a constant temperature the eutectic has the advantage of a large effective super heat hence the fluidity of the eutectic is correspondingly enhanced. The fluidity of the eutectic becomes significantly higher than that of either of the pure metals. Next one let us see the effect of mould temperature on the fluidity. For the most casting process moulding temperature is fixed at or close to room temperature little or no effect of moulding temperature on fluidity because most of the times the moulding temperature is fixed at the room temperature. But you see in investment casting or die casting the increase in moulding temperatures do contribute modestly to the increase of the fluidity. When the mould temperature is raised to the melting point of the alloy the fluidity becomes infinite means the melt will run forever. Example nickel based single crystal for the turbine blade. So, here the melting point is 1450 degrees centigrade. Next let us see the influence of pouring rate on fluidity. The slower the rate of pouring the molten metal into the mould the lower the fluidity becomes because of the faster rate of cooling. Now so far we have completed the effect of the casting parameters. So, under these we have seen effect of modulus effect of section thickness effect of heat transfer coefficient effect of super heating effect of mould temperature and finally we have seen the effect of pouring rate on the fluidity. Next let us see other factors influencing the fluidity. What are these other factors? Flow characteristics. Turbulence can oppose the lamellar flow of the liquid metal. Lamellar flow is very good whereas, turbulence can oppose the lamellar flow of the liquid. The Reynolds number RE is equal to inertia forces divided by viscous forces is used to quantify this aspect of the fluid flow. RE is equal to V d rho divided by mu right. Here V is equal to velocity of the liquid, rho is the density of the liquid, d is the diameter of the channel and the other parameter is the viscosity of the liquid. The higher the RE the Reynolds number the greater the tendency for turbulent flow to occur. So, in gating systems lamellar flow we will get when the Reynolds number is between 0 to 2000 and we get transition flow when the Reynolds number is between 2000 and 20000 and we get the turbulent flow when the Reynolds number is more than 20000. Now what happens if there is a turbulent flow? Turbulent flow leads to inclusions and hence there will be reduction in fluidity. Next other factor is the moulding material. Now you see here this is the pouring temperature and this is the zircon sand and this is the silica sand. Now as the pouring temperature is increasing fluidity is also increasing, but you see in case of the silica sand the fluidity is higher for the same temperature whereas in zircon sand for the same temperature the fluidity will be less. So, this is another factor which will be influencing the fluidity and again we can see another aspect coming to the moulding material that is whether it is fine sand or the coarse sand. For the same what is a type of sand whether you take silica sand or you take the zircon sand. So, here we have the two types one is the fine sand we have taken and the other thing is we have taken the coarse sand in which case there will be better fluidity for the same temperature. What is a coarse sand will have the better fluidity compared to the fine sand. Why? Because fine sand so many what is a particles will be coming in contact with the molten material because of there what is a fineness. So, more what is a heat is extracted by this fine sand particles that is how it becomes more viscous as it is flowing that is how the fluidity will be coming down in case of the fine sand. Now, next other parameter is the mould coating mould coating also influences the fluidity. Now, you see here so this is the time x axis we can see the time and on the y axis we can see the flow distance means the fluidity. Fluidity is measured in terms of a in terms of the flow distance in a channel. Now, here we can see there are two cases in one case there is no coating uncoated means the fluidity will be enhancing and at one stage it will come and it will be stagnating. On the other hand when the moulding material is given a certain coating then what is happening it is the fluidity is increasing. So, we can conclude like this when there is a mould coating the fluidity will be enhanced why it is enhancing you see here we can see this is the what say we can see here there are the uncoated grains and here there are coated grains. Let us examine now what happens when the molten metal is flowing above uncoated grains and also above the coated grains. When it is flowing above the coated grains uncoated grains what is happening it is fully occupying or flowing around the grains. So, this is a grain and this is a grain. So, it is fully occupying and fully going in contact with the what say grain sand grains then it is flowing. Whereas, in the case of the coated grains the mould what say molten metal is not going in full contact with the sand grains. Now, what happens in these two cases in the case of the uncoated grains because it is going in full contact with the sand grains it is what say extract liberating more heat or it is dissipating more heat to the sand grains. In the case of the coated grains because it is partly going in contact with the sand grains it will be dissipating lesser amount of heat to the grains sand grains. So, as it in the case of the coated grains because it is dissipating lesser amount of heat its fluidity will be enhanced or it will be what say having higher what say what say lesser viscosity that is how the fluidity will be increased. Now, we have another topic that is the methods for determining the fluidity. So, far we have seen the importance of fluidity in casting and different parameters that will be influencing the fluidity. Now, how to measure the fluidity? Let us see few methods that are available. One method is fluidity spiral tube method, another method is section tube method and another method is long stripes of different thicknesses. So, these are the three methods available for determining the fluidity of a molten metal. Now, let us see the first one that is the fluidity spiral tube method. The fluidity index of a material is the length of the solidified metal in the spiral process.  You can see. So, this is the pouring cup and this is the sprue and at the bottom there is a sprue well. Now, this is a thin tube a metallic tube that is all that is all about this what say spiral tube what say apparatus. Now, this is the thin tube this whole apparatus will be kept inside the mould box the drag then it will be compacted then this will be withdrawn. Once it is withdrawn yes naturally there will be what say passes sprue passes then here you can see this is the thin wire spiral wire. So, there also a mould cavity created a spiral cavity will be created then you put the cope box over that then you pour the molten metal then the molten metal will be flowing like this it will be flowing then it will be flowing along this spiral passes then as the molten metal is flowing inside it will be flowing and flowing and it all depends upon the fluidity. If the fluidity is more and it will be flowing more distance and if or if the fluidity is less and it will be flowing to a lesser distance. So, now when we stretch it yes we can measure what is the distance it has flown. So, that is how we can measure the fluidity using the spiral tube method. So, the greater the length of the solidified metal greater is the fluidity sometimes it may flow for 20 inches or sometimes that is that is a lesser fluidity sometimes it may flow for 30 inches means it is a higher fluidity. Next one is the suction tube method. So, it is based on the application of the vacuum. So, here there is a simple tube is there. So, this tube will be immersed inside the molten metal. So, this is the molten metal. Now, on the other side the tube will apply vacuum then what happens because of the application of the vacuum the molten metal will be flowing through this tube. Now, what will happen depends upon the fluidity of the molten metal it will be flowing inside the tube. If the fluidity of the molten metal is very good it will be flowing to a longer distance maybe it may flow up to even here or if the fluidity is very less it may flow up to here or if the fluidity is moderate it may flow up to here. So, that is how the fluidity of the molten metal can be measured using the suction tube method using the vacuum. Next one next method is the long strips of different thicknesses. So, here we can see. So, this is another what say method which is similar to the what say spiral tube method. In the case of the spiral tube method we see a thin spiral wave is there, but here long what say sections are there. So, this is the what say sprue what say pouring cup and this is the sprue the tapered sprue and this is the runner you can see there is a central runner is there here. Now, to this runner different what say sections are attached these sections are what say cross sections of these what say plates is they are rectangle rectangles. You can see here here the thickness is more and the here the thickness is moderate and the here the thickness is very less likewise you can see different thicknesses may be 1 mm here 5 mm 3 mm 6 mm 8 mm 0.5 mm you can see 2 mm likewise different thicknesses what say sections will be attached. Now, the when you pour the molten metal into this the molten metal will be flowing then it will be flowing into this runner then it will be flowing through different sections and depends depending upon the fluidity of that molten metal it will be flowing into these different sections and stopping at a particular place. Next one let us see the problems related to fluidity what are the problems associated with the fluidity one is the sledge formation and another one is the die shouldering what are these first let us see the sledge formation. So, the sledge is made up of oxides such as alumina Al2O3 and magnesium MgO and primary crystals that contain aluminum, silicon, iron, manganese, magnesium and r chromium. So, all these together will be forming a sledge. Now, this will be affecting the flow of the molten metal sometimes this sledge will be obstructing the flow of the molten metal. Now, what are the factors affecting sledge formation one is the alloy composition second one is the melting and holding temperatures and the third one is the cooling rate. Sledge factor Sf is equal to 1 into percentage weight of iron plus 2 into percentage weight of manganese plus 3 into percentage weight of chromium. So, with an increase in cooling rate the size of the sledge particles and the volume fraction of the sledge decreases sledge form at the low cooling rate as large plate plates and polyhedral particles at the high cooling rate sledge is in the form of plate plates and star like particles. Next problem associated with the fluidity is the dye-shouldering. So, this arises in the case of the dye castings when we are making castings using the dye casting process. So, it takes place in aluminum dye castings especially the molten metal sticks to the surface of the what is a dye material and remains there even after rejection of the casting. So, this dye-shouldering is the result of interface reaction between the molten aluminum and the dye material during the impact of the high velocity molten metal into the dye surface. It is also due to the intimate contact between the alloy and dye at high temperature. So, what happens in the case of the dye casting we inject the molten metal into the metallic dyes. Now, there inside the metallic dyes the molten metal solidifies and the casting has to be taken out, but in this process it can so happen that the molten metal will be sticking to the dye material inside the cavity. So, that is how this dye-shouldering problem arises. Now, factors influencing the dye-shouldering one is the temperature of the metal and dye. Next one nature and constituents of casting alloy and inter metallic layers. Next one dilubrication and coating. Next one nature of the dye and operating parameters. Now, mechanisms of the dye-shouldering. Let us see the mechanisms of the dye-shouldering. It takes place at different stages. At stage one erosion of grain boundaries on the dye surface. At second stage what happens pitting of the dye surface. At the third stage formation of iron aluminum compounds. Fourth stage formation of pyramid shaped inter metallic phases. And at fifth stage adherence of aluminum on to the pyramids of inter metallic phases. And finally, merging and straightening of erosion pits and inter metallic phases. So, these are the mechanisms of the dye-shouldering. So, friends in this lecture we have seen the fluidity its importance and the factors affecting the fluidity. We have seen that factors related to the melt that affect the fluidity or the freezing range of alloy, alloy composition, inclusions, surface tension, viscosity, latent heat of fusion of the alloy. And what are the other factors related to casting parameters? They are the modulus, section thickness, heat transfer coefficient, super heating, cold temperature and pouring rate. Now, also we have seen the methods for determining the fluidity. Now, then we have seen the problems related to the fluidity. So, with this we are completing this lecture and we will meet in the next lecture. Thank you.


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