Identification of an unknown liquid using refraction Theory Refraction is the bending of light as it propagates through one medium to another. Light refracts whenever it enters another substance at an angle and this change in direction is caused by a change in speed. (Science Learning Hub, 2012) The refractive index is characterised as the quotient of the speed of light as it travels between two mediums. It describes the speed of a light ray as it propagates through media. (Mettler Toledo, n.d.). The refractive index of all media should be greater than one as if it is less than one, it will indicate that light is travelling faster than the speed of light in a vacuum (The Social Select, 2022). This is not possible as nothing can go faster than the speed of light in a vacuum (Siegel, 2018) The angle of incidence is the angle between the ray incident on a surface (Ashish, 2018). Likewise, the angle of refraction is the angle that is created at the boundary between two mediums when light changes direction (PhysicsClassroom, n.d.). Snell’s Law is an equation that relates the angle of incidence and angle of refracted light at the boundary of two mediums. Snell’s Law can be applied to all materials in any state of matter. Snell’s Law is as follows (Flens, 2021): Equation 1: ππ π ππ π = ππ π ππ π Where ππ is refractive index of incident medium, π is incident angle, ππ is refractive index of refracted medium and π is the angle of refracted ray. The angle of incidence can be altered using a refraction dish with a light box emitting a light ray into an unknown solution. A protractor was used to measure the angle of refraction and the refractive index was calculated using Snell’s law to identify the unknown solution. The refraction dish was used to alter the angle of incidence and therefore, the angle of refraction through turning the dish as these values are directly proportional as seen in Equation 1. ππ π ππ π = ππ π ππ π ∴ ππ ∝ π π Since angle of incidence was the independent variable, this angle was determined before and the angle of refraction was measured using the protractor on the refraction dish. The refractive index was calculated using a derived formula of Equation 1. Equation 2: ππ = ππ sin π sin π Aim: To explore how the angle of incidence affects the refractive index and how it can be used to identify unknown solutions Hypothesis: As the angle of incidence increases then the refractive index will also increase as seen in Equation 2: ππ = ππ sin π sin π ∴ ππ ∝ π Therefore, the refractive index should be consistent as angle of incidence is increased and with a list of known refractive indexes, can be identified. Variables: Independent variable: The angle of incidence (Λ). The angle of incidence was altered by turning the refraction dish. 7 angles of incidence were utilized in the experiment. Dependent variable: The refractive index Table 1: An arrangement identifying and addressing the multiple controlled variables within the experiment Controlled variable How was this variable controlled? Why was it controlled? Voltage of electricity This variable was controlled by setting the power bank to the maximum voltage of 12 volts for the entire experiment. Concentration of solution This variable was controlled by pouring an adequate amount of solution into the refractive dish and not altering the concentration by pouring more each trial. This variable was controlled by aiming the light ray into the curved section of the refractive dish. This variable was controlled as it would affect the light’s brightness which can affect how visible the light ray was. (RIC, n.d.) Since brightness depends on power which is directly proportional to voltage as seen in: P= ππΌ ∴π∝π Where P is power, and V is voltage. (Eugen, 2019). Therefore, the voltage of the bank needed to be consistent. Concentration has a directly proportional relationship with refractive index. (Adnan et al. 2017). Therefore, if this variable was not controlled and concentration was not consistent throughout the trials, then refractive index would not be consistent as the angle of incidence is altered. When light hits the refractive dish at the flat surface, the change in direction will be drastically different than the light hitting the curved surface. (Wolfgang n.d.). If different sides were used, this would result in imprecise data. Same side of refractive dish Table 2: An arrangement identifying and addressing the uncontrollable variables within the experiment Uncontrolled variables Why was this variable uncontrollable? Why and how would this variable affect the dependant variable? (Would the implication be significant?) Temperature The temperature in the room could not be controlled as the participants had no access to a thermostat to keep the temperature at a constant value. The temperature could affect the refractive index by evaporating the solution if the temperature is high enough. This would affect the concentration of the solution and since concentration is directly to refractive index (Adnan et al. 2017), this would lead to inaccurate results. However, this variable would not affect the refractive index significantly as the temperature did not alter drastically. Light arising from different sources made the light ray of the light box slightly dim. This made it difficult for the participants to accurately measure the angle of refraction. This would result in inaccurate data. However, this would not impact the dependant variable significantly, as for most of the time, it was sufficiently dark. Light coming from alternate sources. Materials & apparatus ο· ο· ο· ο· 1x Light box 1x Power bank 1x Refractive dish 1x Protractor The room where the experiment took place was not completely dark due to the T.V being on and light coming from the hall as light was required for other groups to continue with work. The light box was set next to a window which produced light towards the experiment. ο· 300ml 3-4 unknown liquids Diagram: Protractor that will allow measurement of angle of incidence and refraction. Light box which produces angle of incidence Slit former Procedure: 1. 2. 3. 4. 5. 6. 7. 8. 9. Refractive dish where solution is placed An unknown solution was poured into the refractive dish with an approximate volume of 250ml The refractive dish was placed on the protractor and secured with two nails. The light box was connected to a power bank that was set at 12 volts to maintain intensity of light. A slit former was placed in front of the light box. The lights of the room were turned off and the light box was turned on. The protractor was rotated to allow the light ray to create an angle of incidence of 0o The angle of refraction was observed and recorded in a data table Steps 6-7 was repeated with 6 more different angles of incidence such as 10o, 20o, etc. The angle of refraction was averaged to minimise random error. Table 3: A table of the relevant safety and risk assessment factors within the experiment Safety Hazard (equipment) Light ray Power bank Bags (Tripping Hazard) Ingestion of liquids Hazard Risks The light ray could be a blinding hazard if a participant stares directly into the light box either accidently or through carelessness. Since wires are used to connect the light box to a power bank which can be dangerous if mishandled or if the solution is spilled on the wires or the outlet. Bags could be a tripping hazard and hurt participants if left carelessly around the testing benches. Due to hygiene and potential health risk, if the unknown How to prevent hazard/ what to do if hazard occurs All participants should not stare at the light ray directly and only use to create and alter angles of incidence as required. The wires should be handled with care and only used to connect the power bank to the light box. The solution should remain as far from the wires as possible to prevent any spillage on the wires causing electrical hazard. Bags should be kept under the tables or all in one corner of the room to prevent any participant from being able to trip and potentially injuring themselves. Participants should not be ingesting any of the unknown solutions and should only be used to solutions are ingested either accidentally or carelessly could be a health hazard and dangerous due to constant usage by other participants. further progress in the experiment. When finished with the solution, it should be poured back into its beaker and the top should be covered. Results: Table 4: An arrangement measuring the angles of incidence and angle of refraction for Solution A Angle of incidence (Λ) π½π 0 10 20 30 40 50 60 Trial number (Λ) ππ1 2.0 17.0 33.0 49.0 75.0 N/A N/A ππ2 3.0 16.5 34.0 50.5 75.5 N/A N/A ππ3 2.5 18.0 34.5 50.0 76.0 N/A N/A Solution A Sample mean (Λ) πππ₯Μ 2.5 17.2 33.8 49.8 75.3 N/A N/A sin ππ sin πππ₯Μ 0 0.174 0.342 0.5 0.643 N/A N/A 0.0436 0.296 0.556 0.764 0.967 N/A N/A Table 5: An arrangement measuring the angles of incidence and angle of refraction for Solution B Angle of incidence (Λ) π½π 0 10 20 30 40 50 60 Trial number (Λ) ππ1 3.0 17.5 32.5 48.0 68.0 N/A N/A ππ2 3.5 17.5 32.0 48.5 68.5 N/A N/A ππ3 3.0 18.0 32.5 48.0 68.0 N/A N/A Solution B Sample mean (Λ) πππ₯Μ 3.17 17.7 32.3 48.2 68.2 N/A N/A sin ππ sin πππ₯Μ 0 0.174 0.342 0.5 0.643 N/A N/A 0.0553 0.304 0.534 0.745 0.928 N/A N/A Table 6: An arrangement measuring the angles of incidence and angle of refraction for Solution C Angle of incidence (Λ) π½π 0 10 20 30 40 50 60 Trial number (Λ) ππ1 3.0 12.0 29.0 43.5 61.0 N/A N/A ππ2 2.5 15.5 26.0 41.5 58.5 N/A N/A ππ3 2.5 12.0 29.0 44.0 61.5 N/A N/A Solution C Sample mean (Λ) πππ₯Μ 2.67 13.2 28 43 60.3 N/A N/A sin ππ sin πππ₯Μ 0 0.174 0.342 0.5 0.643 N/A N/A 0.0466 0.228 0.469 0.682 0.869 N/A N/A Table 7: An arrangement measuring the angles of incidence and angle of refraction for Solution D Angle of incidence (Λ) π½π 0 10 20 30 40 50 60 Trial number (Λ) ππ1 2.0 12.0 26.0 41.0 58.5 N/A N/A ππ2 2.0 12.0 26.0 41.0 58.5 N/A N/A ππ3 2.0 12.0 26.0 41.0 58.5 N/A N/A Solution D Sample mean (Λ) πππ₯Μ 2 12 26 41 58.5 N/A N/A sin ππ sin πππ₯Μ 0 0.174 0.342 0.5 0.643 N/A N/A 0.0349 0.208 0.438 0.656 0.853 N/A N/A The sine of the incident angle against the sine of the refracted angle of Solution A 1,2 y = 1,4369x + 0,0486 1 Sin r 0,8 0,6 0,4 0,2 0 0 0,1 0,2 0,3 0,4 0,5 0,6 0,7 Sin i Figure 1: A line graph of the sine of the incident angle against the sine of the refracted angle for Solution A. Sin r The sine of incident ray against the sine of the refracted ray for Solution B 1 0,9 0,8 0,7 0,6 0,5 0,4 0,3 0,2 0,1 0 y = 1,3574x + 0,0629 0 0,1 0,2 0,3 0,4 0,5 0,6 0,7 Sin i Figure 2: A line graph of the sine of the incident angle against the sine of the refracted angle for Solution B. Sin r The sine of the incident angle against the sine of the refracted angle in Solution C 1 0,9 0,8 0,7 0,6 0,5 0,4 0,3 0,2 0,1 0 y = 1,3007x + 0,0273 0 0,1 0,2 0,3 0,4 0,5 0,6 0,7 Sin i Figure 3: A line graph of the sine of the incident angle against the sine of the refracted angle for Solution C. Sin r The sine of the incident angle against the sine of the refracted angle of Solution D 0,9 0,8 0,7 0,6 0,5 0,4 0,3 0,2 0,1 0 y = 1,2906x + 0,0098 0 0,1 0,2 0,3 0,4 0,5 0,6 0,7 Sin i Figure 4: A line graph of the sine of the incident angle against the sine of the refracted angle for Solution D. Table 8: A table for the calculated refractive index of each solution Solution Refractive Index (Identification) A B C D 1.505 1.444 1.351 1.326 Identification based on calculated refractive index Cedar Oil Ethylene glycol Ether Methanol Sample calculations: The slope for the ratio between the sine of incident angle and the sine of refracted angle for Solution B: (0.643, 0.928) (0, 0.0533) π= π¦2 − π¦1 π₯2 − π₯1 0.928 − 0.0533 0.643 − 0 π= π= 0.8747 0.643 π = 1.36 Refractive index of Solution A: ππ sin π = ππ sin π (1.00)π ππ75.3 = ππ π ππ40 (1.00)π ππ75.3 π ππ40 ππ = ππ = 1.505 Error percentage: Solution A was Vegetable Oil πΈππππ% = 1.505 − 1.47 × 100 1.47 ∴ πΈππππ% = 2.38% Solution B was Distilled Water πΈππππ% = 1.444 − 1.33346 × 100 1.33346 ∴ πΈππππ% = 8.29% Solution C was 30% Glucose πΈππππ% = 1.351 − 1.38 × 100 1.38 ∴ πΈππππ% = 2.10% Solution D was 30% citric acid solution πΈππππ% = 1.326 − 1.498 × 100 1.498 ∴ πΈππππ% = 11.48% Analysis: The data obtained such as Figure 3 and Figure 4 demonstrated that the sine of the incident ray and the sine of the refracted ray have a linearly dependent relationship, which is expected given Equation 1 where: ππ sin π = ππ sin π ∴ sin π = ππ sin π ππ ∴ sin π ∝ sin π Each of the trendlines in all figures demonstrated that as the sine of the angle of incidence increased the sine of the angle of refraction increased. This supports the hypothesis as the angle of refraction increased due to increased angle of incidence. The trendlines in all figures are linear lines and are extremely similar. Scatter points (0.174, 0.228) and (0, 0.0466) in Figure 3 are not on the trendline indicating the presence of random errors. This is further supported by scatter points (0.174, 0.208) and (0, 0.0349) in Figure 4 which are not on the trendline indicating random error. A random error is the rotation of the protractor. When the participant was rotating the protractor to different angles of incidence, it was possible that the light ray was not exactly on the line of the protractor and so this would result in imprecise data as seen in Table 6 where for the angle of incidence of 10o, there is a large range of 3.5Λ while other tables have no such range. This would have a significant impact on the data as the angle of incidence is the independent variable. Another random error was instrument resolution of the refractive dish that impacted the concentration of each solution that was tested. Since the refractive dish had no measurement markings or no method was utilised to keep the concentration of each solution the same was used, the concentration of each solution was not equal. Since concentration has a directly proportional relationship with refractive index, this would have created imprecise data and the impact would be significant as it affects the dependent variable directly. A systematic error was the weak light ray from the light box. The light ray that was produced was weak throughout the experiment and so made it harder for participants to measure angle of refraction. This would have resulted in inaccurate data and would have had a significant impact as it affects the dependent variable. Another systematic error was failure to account for the material of the refractive dish. The light ray from the light box travelled from the solution into the material of the refractive dish first before propagating into the air and so the material of the refractive dish may have altered the angle of refraction. This can be seen in Table 8 where the calculated refractive index led to all incorrect identification of the solutions. The precision of the data is high which can be seen in Table 7 where the range of each set of trials is 0Λ and is further endorsed by Table 5 which only has a range of 0.5Λ across all trials. Precision was also high as 3 trials was done for 7 angles of incidence reducing the effect of random errors, however precision was lessened given the resolution of the protractor was in divisions of 1Λ. The scatter points in Figure 2 are all on the trendline, indicating a high amount of precision, however in Figure 3, there is a considerable amount of scatter around the trendline, notably scatter points (0, 0.0466) and (0.174, 0.228). This is also present in Figure 4 with points (0, 0.0349) and (0.174, 0.208) are not on the trendline. This indicates less precision which affect the reliability of the experiment; however, these results should be reproducible given the smaller number of factors that affected precision. The accuracy of the experiment is low. This is seen in Table 8 as the calculated refractive index led to incorrect identification of each solution. This indicates a low level of accuracy. Low accuracy is also seen in the error percentage such as the Error% of Solution D was 11.48% and the Error% of Solution B was 8.29% which indicates a moderate level of inaccuracy. Therefore, the validity is moderate, as the experiment did address the aim and the expected trend was demonstrated by a linearly dependent relationship between sin i and sin r, however the low accuracy reduces the validity significantly. Conclusion: The proportional relationship between angle of incidence and refraction was discovered and supported Equation 1, however the unknown solutions was incorrectly identified due to the calculated refractive index in Table 8. The hypothesis was not supported as despite supporting Equation 1, the unknown solutions were not able to be identified using this method. The results did not lead to a definite conclusion as the results were particularly inaccurate. Limitations included that it was assumed that angle of incidence was measured accurately, and that the glass boundary of the refractive dish was not considered. 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