We will now explore the discussion section of the report. This section includes your critical interpretation of the results you obtained. You may also include a critique of the approach you took or a brief note on the limitations of your methods. Remember that a critique is a detailed evaluation.
The following table can help you develop a substantial discussion section as it combines analysis and interpretation of the data provided.
Analysis | Interpretation | |
Questions to ask yourself |
Explain what you know with certainty based on your results and draw conclusions. |
Find logical explanations for problems in the data. |
Example | Since none of the samples reacted to the Silver foil test, therefore sulfide, if present at all, does not exceed a concentration of approximately 0.025 g/l. It is therefore unlikely that the water main pipe break was the result of sulfide-induced corrosion. | Although the water samples were received on 14 August 2000, testing could not be started until 10 September 2000. It is normally desirable to test as quickly as possible after sampling in order to avoid potential sample contamination. The effect of the delay is unknown. |
Adapted from University of Toronto (2005)
In this section, you should address the following elements:
If your report does not include a conclusion, then in the discussion you should also:
Task 8:
Read an extract from the discussion section of the lab report we looked at earlier. Find examples of the following elements:
Discussion
The natural frequency of the bungee cord for each applied load was calculated from the spring constant values using Equation 4 (see sample calculation in the Results section). This data can be seen in Table 1. The predicted value of natural frequency for an applied mass of 250g (applied load of 2.45N) was 0.96 Hz. The natural frequency measured by experiment was 0.97 Hz, showing excellent agreement (approximately 1% different).
There were a number of sources of error in this experiment. The deflection of the cord could only be measured to ± 1mm and the scale could only be originally placed to the same degree of accuracy. This led to an inaccuracy of up to 20% for the smaller deflection measurements (around 10mm). For larger deflections (up to 740 mm), this inaccuracy reduced to 0.3%. Further error could have been introduced by deflection of the loading frame and slippage of the attachments at each end of the cord.
Another error arose from the assumption shown in Equation 3, that the gradient of the force-deflection graph can be approximated using the finite difference between consecutive data points. This error may be reduced by using more data points and a more accurate method of gradient approximation.
The main error in the measurement of the natural frequency was caused by the human reaction time of operating the stop watch and assessing the point at which four oscillations had occurred. These sources of error may be reduced by using a longer piece of cord, which would oscillate more slowly and by averaging over a large number of measurements.
Adapted from Beagles et al. (no date)
Discussion
The natural frequency of the bungee cord for each applied load was calculated from the spring constant values using Equation 4 (see sample calculation in the Results section). This data can be seen in Table 1. The predicted value of natural frequency for an applied mass of 250g (applied load of 2.45N) was 0.96 Hz. The natural frequency measured by experiment was 0.97 Hz, showing excellent agreement (approximately 1% different).
There were a number of sources of error in this experiment. The deflection of the cord could only be measured to ± 1mm and the scale could only be originally placed to the same degree of accuracy. This led to an inaccuracy of up to 20% for the smaller deflection measurements (around 10mm). For larger deflections (up to 740 mm), this inaccuracy reduced to 0.3%. Further error could have been introduced by deflection of the loading frame and slippage of the attachments at each end of the cord.
Another error arose from the assumption shown in Equation 3, that the gradient of the force-deflection graph can be approximated using the finite difference between consecutive data points. This error may be reduced by using more data points and a more accurate method of gradient approximation.
The main error in the measurement of the natural frequency was caused by the human reaction time of operating the stop watch and assessing the point at which four oscillations had occurred. These sources of error may be reduced by using a longer piece of cord, which would oscillate more slowly and by averaging over a large number of measurements.
Like in the results section, the discussion section uses verb forms in a similar way.
The predicted value of natural frequency for an applied mass of 250g (applied load of 2.45N) was 0.96 Hz.
This led to an inaccuracy of up to 20% for the smaller deflection measurements (around 10mm).
Further error could have been introduced by deflection of the loading frame and slippage of the attachments at each end of the cord.
These sources of error may be reduced by using a longer piece of cord, …
… the gradient of the force-deflection graph can be approximated using the finite difference between consecutive data points.
This error may be reduced by using more data points and a more accurate method of gradient approximation.
The natural frequency of the bungee cord for each applied load was calculated from the spring constant values using Equation 4 (see sample calculation in the Results section).
This error may be reduced by using more data points and a more accurate method of gradient approximation.
The main error in the measurement of the natural frequency was caused by the human reaction time of…