Jesper
Haglund
*a,
Staffan
Andersson
a and
Maja
Elmgren
b
aDepartment of Physics and Astronomy, Uppsala University, Sweden. E-mail: jesper.haglund@physics.uu.se
bDepartment of Chemistry, Uppsala University, Sweden
First published on 15th April 2015
Thermodynamics, and in particular entropy, has been found to be challenging for students, not least due to its abstract character. Comparisons with more familiar and concrete domains, by means of analogy and metaphor, are commonly used in thermodynamics teaching, in particular the metaphor ‘entropy is disorder’. However, this particular metaphor has met major criticism. In the present study, students (N = 73) answered a questionnaire before and after a course on chemical thermodynamics. They were asked to: (1) explain what entropy is; (2) list other scientific concepts that they relate to entropy; (3) after the course, describe how it had influenced their understanding. The disorder metaphor dominated students' responses, although in a more reflective manner after the course. The view of entropy as the freedom for particles to move became more frequent. Most students used particle interaction approaches to entropy, which indicates an association to the chemistry tradition. The chemistry identification was further illustrated by enthalpy and Gibbs free energy being the concepts most often mentioned as connected to entropy. The use of these two terms was particularly pronounced among students at the Chemical Engineering programme. Intriguingly, no correlation was found between the qualitative ideas of entropy and the results of the written exam, primarily focusing on quantitative problem solving. As an educational implication, we recommend that students are introduced to a range of different ways to interpret the complex concept entropy, rather than the use of a single metaphor.
log
W, in commemoration of his ground-breaking formula, which relates entropy to the number of microstates of a system.
In the early 1980s, science educators came to realise that doing well on paper-and-pencil problem-solving exams is no guarantee for a deep conceptual understanding of the topic at hand. Early focus was on investigating students' understanding of Newtonian mechanics (Clement, 1982; McCloskey, 1983), but has later expanded to other fields, including thermodynamics (e.g.Yeo and Zadnik, 2001). In this tradition, science education research has shown that thermodynamics is challenging to grasp – see Bain et al. (2014) and Dreyfus et al. (2015) for recent reviews on teaching and learning in the field. Consequently, in an international questionnaire study, Ugursal and Cruickshank (2014) concluded that engineering students found thermodynamics to be more difficult than most other engineering subjects, and – unfortunately – not very interesting to learn. This challenge in learning is particularly pronounced for the concept of entropy (e.g.Sözbilir, 2003; Sözbilir and Bennett, 2007), not least due to its abstract nature. We cannot readily probe the entropy of a system with our senses, and there is no ‘entropymeter’; rather we derive its value from measurements of a set of other quantities.
In the present study, we set out to explore how engineering students interpret and understand the entropy concept and its role in thermodynamics, before and after a course in chemical thermodynamics. In particular, we attended to what metaphors students use, what other concepts they associate with entropy, and how this relates to their exam results on the course. In what follows, we first review the literature of students' understanding of entropy, and teaching approaches to come to terms with students' challenges in relation to entropy.
Carson and Watson (2002) interviewed students in order to probe their qualitative understanding of entropy and Gibbs free energy before and after a first-year course in chemical thermodynamics. The students were presented with three chemical reactions, asked to explain what happened and why, and to describe how they understood the concepts entropy and Gibbs free energy. Few of the students had been introduced to entropy in their prior secondary chemistry education, but many ideas had formed after the course. The majority of students had grasped that the entropy of a system and its surroundings cannot decrease, along with ways in which the entropy of a system can increase, e.g. through change of state from solid to liquid to gas. Other aspects of entropy were found to be more challenging, including its relation to the number of microstates or energy distribution across energy levels, or differentiating between the system and its surroundings. Some explanations involved entropy as a ‘form of energy’, which was hard to disambiguate from enthalpy or Gibbs free energy. The term was also vaguely identified with disorder or randomness. Overall, Carson and Watson argue that the course focused on teaching quantitative problem solving through symbol manipulation, as reflected in the problem solving exercises and the nature of the exam. In this way, the students were given little opportunity to develop a conceptual understanding of involved concepts, such as entropy and Gibbs free energy.
In a similar vein, Sözbilir and Bennett (2007) studied third-year chemistry undergraduates' understanding and misconceptions of entropy before and after courses in physical chemistry. They gathered data from pre- and post-tests with conceptual questions – some of which involved entropy – and interviews before and after the course. The results reveal that students have many challenges with regard to entropy, due to, e.g.: identification of entropy with disorder, interpreted as movement, collisions and ‘mixed-upness’, and disambiguation of the system and its surroundings. Some identified misunderstandings were actually more prevalent after the course than before, and the rather discouraging conclusion is that after the course most of the students were still unable to explain the change in entropy of a system using thermodynamic principles.
Turning to studies of physics students' understanding of entropy, Brosseau and Viard (1992) interviewed physics PhD students regarding what happens to the entropy of a thermally isolated gas during reversible expansion. Although the majority of the students mentioned that the relation dS = dQ/T applies to the situation, only one of them concluded that the entropy remains unchanged. Instead, the dominating line of reasoning built on the idea of entropy as disorder: as the volume increases, the disorder increases; hence the entropy increases. In their interpretation, seeing entropy as disorder made the students focus exclusively on spatial configuration, but ignore the decrease in internal energy. Similarly, physics teacher students concluded, in small-group exercises, that the entropy of an ideal gas should increase during reversible adiabatic expansion (Haglund and Jeppsson, 2014), while a pair of physical chemistry PhD students arrived at constant entropy, but found it to be counterintuitive (Jeppsson et al., 2013). Furthermore, physics undergraduate students have been found to have difficulties applying the second law of thermodynamics in assessing the feasibility of given thermal processes (Cochran and Heron, 2006), and believe that the entropy of a system and its surroundings typically remains unchanged throughout thermal processes (Christensen et al., 2009).
As part of a course in engineering thermodynamics, Gustavsson et al. (2013) studied students' conceptions of entropy. The students were given a questionnaire where they were asked to rate how strongly, on a 0–5 scale, they related entropy to a list of notions: probability, temperature, work, disorder, heat, and energy. The result was that the students associated entropy most strongly with disorder, and least strongly with work. There was further a strong correlation between relating entropy to heat and relating it to temperature (indicating an awareness of the formula dS ≥ dQ/T), but also between relating it to disorder and to probability. The students were further asked to read four short texts involving entropy and summarise them in groups of 4–5 students. The texts represented different aspects of the topic, including a microscopic approach, macroscopic cyclic processes, and relating entropy to human, social matters. Out of these, the students' summaries of the microscopic, statistical accounts, some of which involved disorder, reflected a more complex understanding of entropy.
Eventually, however, students would need both a foundational, microscopic understanding of entropy, and practical skills in applying it in calculations of thermal processes and chemical reactions. There remains a particular challenge for students to see how such diverse aspects of entropy relate to one single physical quantity (Baierlein, 1994; Kozliak, 2004). For instance, Baierlein (1994) sees a risk that students do not get an in-depth understanding of what entropy is with macroscopic approaches to the topic. In the light of Johnstone's (1991) triangle model of levels of thought in chemistry and chemistry education, at the macroscopic level, we find heat engine and chemical reaction applications, while notions such as microstates and probabilities which may be interpreted in terms of disorder are introduced at the submicroscopic level. However, this divide across the macro and submicro levels is also inherited at the symbolic level, where it is hard for students to see how macroscopic quantities, such as heat, temperature, enthalpy or Gibbs free energy, relate to microstates and probabilities from the world of statistical mechanics.
The metaphor that has dominated teaching is entropy is disorder, often exemplified by the analogy to an untidy room, where scattered toys and clothes are assigned high entropy, in contrast to the tidy room's low entropy. The analogy is meant to illustrate Boltzmann's microscopic approach to entropy, in that there are more disordered configurations of the child's belongings – corresponding to a system's microstates – than there are ordered ones; hence higher entropy. The use of the disorder metaphor has, however, met with considerable criticism (e.g.Styer, 2000; Lambert, 2002). Styer (2000) points out a range of weaknesses of the disorder metaphor, including that disorder is vague and emotionally charged. Most importantly, the messy room analogy focuses on a snapshot view of a system's spatial configuration, and fails to recognise the importance of the energy involved. As we have seen above, empirical findings that students have difficulties in problem solving involving entropy have often been explained by overreliance on disorder. Wei et al. (2014, p. 330) even see the use of the disorder metaphor and the confusion it has induced as the main cause of the marginalised position of the second law of thermodynamics in K-12 teaching:
“Ultimately, however, it is the pervasive yet inappropriate use of the disorder metaphor for entropy that has prevented more widespread incorporation of the second law into student thinking. /…/ Because the metaphor of entropy as disorder has been so pervasive, most of students' misconceptions – that have documented regarding entropy, the second law and spontaneous processes – are directly or indirectly related to this metaphor.”
The personal engagement vested in this issue may be illustrated by Lambert's (2014) list of textbooks (36, and counting!), from which the disorder metaphor has been removed.
Realising the need for conceptualising entropy beyond mathematical formalism, but finding the disorder metaphor “entirely mysterious” in relation to Clausius' macroscopic interpretation, Leff (1996, p. 1260) instead proposes the introduction of entropy in terms of spreading of energy. He argues that “entropy is a function that represents a measure of spatial spreading of energy and a temporal spreading over energy states” (Leff, 2007, p. 1760) and concludes that “it is appropriate to view entropy's symbol S as shorthand for spreading” (p. 1744). Consequently, Wei et al. (2014) propose that we replace the disorder metaphor with the idea of entropy as energy dispersal also in K-12 teaching of energy. In contrast, Jeppsson et al. (2011) argue that, like all metaphors, the spreading metaphor is not unproblematic. For instance, ‘spreading’ as a verb in the gerund form may lead students to think that it is a process variable, parallel to for instance ‘heating’. Although more neutral than disorder, spreading is also likely to be given primarily spatial interpretations. Furthermore, it would not be unreasonable to interpret the ‘spreadoutness’ of energy mathematically in terms of a derivative of the internal energy with respect to the volume: dU/dV, which relates closer to an ‘energy density’ or the pressure of a system than its entropy. Such merits and shortcomings have to be pointed out explicitly to students for every metaphor that is engaged in teaching.
Similar to Leff (1996), Styer (2000) argues that we need qualitative, metaphorical ways to introduce entropy. However, in line with the reasoning above, where Leff and Wei et al. (2014) suggest wholesale replacement of the disorder metaphor with entropy as spreading, Styer recognises that every metaphor – including, but not only, entropy as disorder – has shortcomings. Consequently, he thinks that the disorder metaphor may be retained, as long as we acknowledge its drawbacks. Furthermore, as a way to counteract the idiosyncrasies of the disorder metaphor, Styer suggests that we complement it with another: entropy is freedom, which admittedly is just as vague as disorder, but positively charged emotionally, and better at capturing the range of microstates a system can be in. The merit of the freedom metaphor in going beyond the typical snapshot view of the disorder metaphor is emphasised also by Amin et al. (2012). The approach of deliberately combining the freedom metaphor with other metaphors in the teaching of entropy is adopted also by Brissaud (2005), even though he settles for entropy is information, relating to its use in information theory.
A quite different qualitative interpretation, entropy as heat, has been suggested within macroscopic approaches to thermal physics (Fuchs, 1987; Herrmann, 2000) and in engineering thermodynamics (Gaggoli, 2010). Here, entropy is seen as a substance-like (although not conserved) entity that may be contained in and flow between objects, i.e. corresponding to how we typically use ‘heat’ in everyday language. Note, however, that this approach may entail problems for students who later encounter more traditional interpretations of heat as a process variable in thermodynamics (Strnad, 2000).
Taber and Watts (1996) investigated students' use of anthropomorphic language in relation to chemical bonding, and identified two different classes of anthropomorphism. In the case of ‘weak’ anthropomorphism, a student realises that an atom does not actually ‘want’ or ‘feel’ anything, but uses such language metaphorically as if the atom were a sentient being. Weak anthropomorphism might be a powerful communicative device, in breaking the rules of the otherwise impersonal, detached language in science class (Lemke, 1990). However, in the case of ‘strong’ anthropomorphism, typically expressed as teleological reasoning, such desires are actually ascribed to inanimate entities. In chemistry, this sometimes results in misunderstandings, for example in the context of the ‘full outer shell’ heuristic, i.e. that atoms ‘try’ to achieve stable noble-gas electronic configurations. As part of their further investigation of students' ideas of chemical bonds, Taber and Watts (2000) have developed a framework of students' explanations. They bring forward teleology and anthropomorphism as examples of pseudoexplanations, i.e. statements that look like explanations on the surface, but do not logically fit the studied phenomenon. Relating to the anthropomorphism example of a student who says that an atom is trying to become stable, they argue that: “Such language has explanatory currency only when the implied actor is actually animate and capable of ‘trying’” (Taber and Watts, 2000, pp. 347–348).
Talanquer (2007) identified and analysed teleological explanations in chemistry textbooks. He found that teleological lines of reasoning are used to explain rules and laws, which have been found empirically to have high generality. According to these rules and laws, chemical changes occur in order to optimise some characteristic or quantity. As an example, Talanquer also refers to the full outer shell heuristic, in the form of the octet rule, according to which bonds form in order to achieve increased stability. Novice students are often not aware that the octet rule is a quite rough rule-of-thumb, and tend to overgeneralise it in situations where it does not apply. Other examples relate to the second law of thermodynamics, where students are told that changes occur in order to maximise the entropy of the universe, or minimise the Gibbs free energy of the studied system; teleological explanations of causes, in reference to their effects. Here, in contrast to the case of the octet rule, however, the teleological reasoning gains force and educational legitimacy from the generality and consistency of the second law of thermodynamics. The confidence in the second law of thermodynamics has been expressed eloquently by Eddington (1928, p. 74):
“The law that entropy always increases, holds, I think, the supreme position among the laws of Nature. If someone points out to you that your pet theory of the universe is in disagreement with Maxwell's equations – then so much the worse for Maxwell's equations. If it is found to be contradicted by observation – well, these experimentalists do bungle things sometimes. But if your theory is found to be against the second law of thermodynamics I can give you no hope; there is nothing for it but to collapse in deepest humiliation.”
Once we are convinced that the second law of thermodynamics holds universally, we may see the increase of entropy as a ‘driving force’, a ‘tendency’, or giving directions for change along ‘time's arrow’. From this perspective, anthropomorphic reasoning represents another step in understanding the second law of thermodynamics, as expressed, for example, in “nature abhors a gradient” (Schneider and Sagan, 2005). Indeed, such anthropomorphic language was also adopted by Clausius (1865, p. 400), as he ended the seminal paper in which he coined ‘entropy’ by stating the laws of thermodynamics in terms of:
(1) Die Energie der Welt ist Constant.
(2) Die Entropie der Welt strebt einem Maximum zu.†
Then again, we seek for deeper explanations, and would prefer to understand the underlying mechanical causation. Why does the entropy tend to increase? Explanations of the underlying mechanisms are provided probabilistically in statistical mechanics. But this does not automatically discredit the educational legitimacy of teleological explanations at earlier stages in the educational system. The question is whether teleological explanations are valuable for helping students to understand aspects of the second law of thermodynamics, without introducing obstacles for grasping more fundamental explanations, should they decide to specialise in the subject.
As recognised by Amin et al. (2012) and Wei et al. (2014), this search for teaching approaches that fit a particular age group and prepare for further studies also applies to the issue of the relative merits and shortcomings of different metaphors for entropy – in particular the still widely used, yet contended disorder metaphor. So far, however, this pedagogical debate has been largely limited to theoretical arguments, and we believe that empirical study of how students respond to different teaching approaches is required to cast further light on these matters.
In particular, the study served to respond to the following research questions:
• What scientific concepts do engineering students relate to entropy, prior to and after a chemical thermodynamics course, and how are these concepts related to one another?
• How do engineering students explain what entropy is, prior to and after a chemical thermodynamics course?
• How do engineering students' explanations of and associations to entropy relate to their exam results on a chemical thermodynamics course?
Atkins' physical chemistry, 9th edn (Atkins and De Paula, 2010) was used as course literature, and the course had a traditional structure with lectures, problem-solving sessions, and laboratory exercises. The lecturer told – in a subsequent interview – that emphasis was placed on students' development of conceptual understanding, for instance by use of qualitative problems to be discussed in small-group settings, as well as quantitative problem-solving skills. Furthermore, adhering to the chemistry disciplinary tradition (Christensen and Rump, 2008), students' development of microscopic explanations was given priority, rather than the relation to macroscopic examples, such as heat engine cycles. In particular, Boltzmann's approach to entropy, involving the number of microstates, was adopted more commonly than Clausius' macroscopic approach. When teaching about entropy, the lecturer explained that there are limitations to the disorder metaphor that students had encountered in previous courses. For example, crystals may form into layers where molecules have high freedom to move in the layer (high ‘order’ going together with high entropy).
After the course, the students took a paper-and-pencil problem-solving exam in Swedish, where some of the items involved entropy. Most items were of a predominately quantitative character, but some involved qualitative reasoning, such as whether the entropy in a given reaction is likely to increase, decrease, or remain the same. The seven items were graded from 1 to 10, based on the correctness and justifications given, and an overall score of 35 out of a maximum 70 was required to pass the exam. English translations of the exam items that relate explicitly to entropy are provided in Appendix A.
For ethical reasons, students were introduced orally to the purpose of the study and how data would be used and reported, informed that participation was voluntary, and that the teachers of the course would not have access to individual students' responses. By signing their questionnaires, students provided written consent to participation.
In both questionnaires, the students were asked two open-answer questions:
• What is entropy? Give a brief explanation that reflects your understanding.
• Which are the most important other scientific concepts that relate to entropy, according to you?
In the questionnaire after the course, the following item was added:
• How has the course influenced your understanding of the entropy concept? Please give concrete examples.
Research on students' conceptual understanding of a broad range of science topics, including thermodynamics and entropy, has typically been performed by use of clinical interviews or multiple choice questions. Interviews have the benefit that an in-depth understanding can be gained of the interviewed student's line of reasoning, but involves an asymmetrical power relationship between the interviewer and the interviewee. In addition, since conducting interviews and analysing the outcome is time consuming, there are practical constraints on how many interviews can be conducted. With multiple choice questions, in turn, many more students can be included, but the students' qualitative understanding can only be inferred indirectly. By asking the students to write down their explanations of what entropy is, we strived to approach all students of the course in order to be able to say something about how prevalent different ideas were among them, and to gain some insight into their qualitative understanding of entropy. This exploratory approach was adopted in the light of the scarcity of empirical studies on the metaphors students use in relation to entropy. We also considered that the approach should be reasonable for practicing teachers to adopt in getting an overview of their students' understanding of a particular topic or concept, based on positive experience from asking students in a similar population to provide free-text explanations (Gustavsson et al., 2013).
The second item was used against the background of previous research on the connection between students' achievement and their responses to word association tests in physics. High school students who are currently taking a physics course have been found to generate more concepts and more strongly interrelated concepts, when asked to associate freely to a word when given a list of 18 terms from the topic of mechanics, in comparison to students who took the course a year ago, or have not taken the course (Johnson, 1964). Similarly, Shavelson (1972) found that high school students' achievement increases from a pretest to a posttest after instruction in mechanics came together with increased interrelation between key concepts at word association tests. As mentioned above, Gustavsson et al. (2013) have used word association tasks for engineering thermodynamics students, although with a given set of concepts to choose from.
The students' answers to what entropy is (before and after) and how the course had changed their ideas (after) were first categorised by one of the researchers, deductively as the categories were formed against the background of previous research described in the Theoretical framework, but also inductively as new patterns of reasoning were identified (e.g. coming to problematise one's previous understanding). These ideas vary in the degree to which they align with the current view in science. Next, two of the researchers refined the categories, gave them descriptions in English, and coded the students' responses. The resulting classification scheme, with relative frequencies and examples of students' answers, which have been translated into English, are detailed in Table 1. These categories are not mutually exclusive, and many student responses were classified as involving several of them. Suitable grain sizes of the categories were also discussed. For instance, we chose to form one category of teleological and anthropomorphic reasoning since many expressions involved both, such as systems ‘striving’ for disorder. Lastly, the categories were grouped into overarching themes.
| Category | Percentage of students (%) (before/after) | Description | Example student explanations |
|---|---|---|---|
| Microscopic interpretation of entropy (38/68) | |||
| Microscopic | 34/59 | Relating to the state of a system's particles, atoms, molecules, etc. |
How many ways the particles can distribute across different energy levels… (after).
Probabilities for molecules to move in a particular way (after). |
| Movement | 10/19 | Connection to the movement of particles | The disorder of molecules, how much they move (before). |
| Freedom | 3/30 | The freedom or possibility for a system or its particles to change states, move, etc. | Entropy is the molecules' possibility to move freely. E.g. gas has high entropy, solids have lower (after). |
| Probability | 7/7 | The probability for a system or its particles to be in a particular state | ΔS, it deals with how probable it is that a certain substance will be in a certain state (before). |
| The disorder metaphor for entropy (67/77) | |||
| Disorder | 67/77 | Relating entropy to disorder |
Entropy describes the disorder in a system (after).
Entropy is a measure of disorder. How free the molecules are to move (after). |
| Problematising | 0/19 | Reflection on or questioning own understanding of entropy prior to the course (in responses after the course) |
Last time I answered that I thought it was order. Apparently, that was a dumb way to see things. How atoms distribute (after).
In the beginning of the course I saw entropy as ‘disorder’. Now I have a more nuanced view on entropy [in terms of the possibility for molecules to move and spread out] (after). |
| The spreading metaphor for entropy (7/30) | |||
| Spatial configuration | 7/25 | The location, mixing or spreading of particles |
Order, high entropy → high disorder, i.e. the molecules are spread out in a room, a beaker, etc. (before).
Entropy is disorder, how “messy” or mixed up it is in a gas/liquid (before). |
| Spreading of energy | 0/5 | The spreading or distribution of energy in space or across particles | A measure of how energy is distributed among molecules in a system (after). |
| Problematic connection between entropy and energy (26/7) | |||
| Energy | 26/7 | Identification of entropy with energy, or a part or form of it | Entropy is the heat in a system that does not transform into work (before). |
| Teleological understanding of the second law of thermodynamics (26/20) | |||
| Second law of thermodynamics | 25/18 | Entropy as an increasing quantity | Everything strives for high entropy (before). |
| Teleology/anthropomorphism | 23/11 | Attribution of purposefulness, sentience or volition to physical phenomena |
Entropy – disorder. All systems strive for disorder in all processes. The entropy is thereby the driving force for reactions to happen (before).
Atoms/molecules strive to reach disorder, since they want most to be as spread out from each other as possible (before). |
| Other categories | |||
| Literal | 15/19 | Statements that entropy is a state function, use of denotations (e.g. S, ΔS) or formulae (e.g. dS = dQrev/T) |
A physical state function. Denoted with S (before).
You can calculate it like this: S = U/T + k dS = dQrev/T. S increases for every spontaneous process in an isolated system (after). |
| Concrete examples | 14/22 | Specific physical processes, or the third law of thermodynamics |
A measure of order/disorder, e.g. a gas has higher entropy than a solid, as the molecules in the gas are free (before).
A substance at 0 K and with perfect crystalline structure cannot be ordered in different ways and the entropy is then 0 (after). |
In order to describe how the classification was done, we provide an example of the coding of a student's explanation of what entropy is:
“Order, high entropy → high disorder, i.e. the molecules are spread out in a room, vessel, etc. The universe strives for, like, high entropy…”
This statement was coded as involving microscopic explanations and spatial configuration, since it relates to the relative locations of molecules. It further makes use of the disorder metaphor, which is used to express the second law of thermodynamics. Since the word ‘strives’ was used, the expression was also coded as making use of teleology/anthropomorphism.
Following Johnson (1964) and Shavelson (1972), we took interest in the interrelations that the students attributed to scientific concepts. The concepts associated to entropy and our categorisation of the student explanations of entropy were uploaded into SPSS, and descriptive statistics (absolute frequencies) were generated. An overview of correlations between the categories was provided by means of Spearman's rho, and individual pairs singled out for one-tailed Fisher's exact tests, for which the significances are given in the results. The correlations were calculated in order to identify clusters of ideas that tended to come together. Some of the responses were further subjected to qualitative analysis, with a particular focus on how individual students had developed their understanding of entropy between the pre- and post-tests.
In a second round of analysis, the students' responses to the questionnaires were matched with their overall exam results. Correlations were calculated between the exam results on one hand, and the concepts students relate to entropy and categories of students' explanations on the other, in order to identify patterns of qualitative understanding of entropy that are useful or detrimental to problem solving.
After the data analysis, preliminary results were shared with the lecturer of the course, in order to check whether our interpretations were reasonable, and might be useful for the teaching practice.
![]() | ||
| Fig. 1 Number of students that relate entropy to certain concepts, before or after the course, or both. | ||
This connection to enthalpy and Gibbs free energy is further reinforced by the correlation analysis. Students who relate entropy to Gibbs free energy prior to the course tend to relate it also to enthalpy prior to the course (p = 0.0004, significance of one-tailed Fisher's exact test), and to Gibbs free energy after the course (p = 0.0007). Relating entropy to enthalpy and Gibbs free energy was found to be particularly common among students at the Chemical Engineering programme, which has the most extensive chemistry content prior to the course.
Whereas 18 of the students relate entropy to energy before the course, their responses are more differentiated after the course, distributed between internal energy, temperature, heat, and heat capacity. Out of these, relating entropy to energy before the course is significantly positively correlated to relating entropy to heat after the course (p = 0.005). Similarly, relating entropy to energy (undifferentiated) and Gibbs free energy after the course is significantly negatively correlated (p = 0.003).
A remarkable finding was that none of the students (before or after) bring up disorder as a scientific concept that is related to entropy. This is interesting for many reasons. First, there is the international research pointing to dominance of the disorder metaphor in teaching (e.g.Lambert, 2002). Second, there is a stark contrast with the results of Gustavsson et al. (2013), where engineering thermodynamics students connected entropy most strongly with disorder, when given a list of notions to choose from. Third, as we will see, the majority of the students in the present study mention disorder in their explanations of what entropy is to them. In our view, this unwillingness to bring up disorder as a scientific concept connected to entropy suggests that the students were aware that the notion should be interpreted figuratively rather than literally.
Another identified category within the microscopic theme, which is more common in the answers after the course than before, is the connection between entropy and movement of particles. Prior to the course, this connection is typically quite direct, for instance: “The disorder of molecules, how much they move”. As we have seen, such an interpretation of disorder as a microscopic movement in relation to entropy has been reported previously (Sözbilir and Bennett, 2007), and may indicate confusion between entropy and kinetic energy (Johnstone et al., 1977). After the course, however, entropy is not typically connected to movement as such, but to the potential or freedom for particles to move about: “Entropy is the molecules' possibility to move freely. E.g. gas has high entropy. Solids have lower”, or “The ability for atoms/molecules to move/change places/how locked they are”. Indeed, in the responses after the course, there is a significant positive correlation between the movement and freedom categories (p = 0.00004). Overall, responses involving freedom are much more prevalent after the course than before (from 3% to 30%). Styer (2000) suggests using entropy as freedom in conjunction with the disorder metaphor. In our data, however, even though many of the descriptions involve both freedom and disorder, there is a significant negative correlation between these categories after the course (p = 0.005).
Overall, several of the qualitative, figurative descriptions of entropy we have come across in the literature are mentioned by one or more of the students, including disorder, freedom to move about, spreading of energy, teleological striving, etc. The chemistry profile of these engineering students is once again emphasised by the fact that only one of them indirectly alludes to entropy as information (“how ‘well’ we can know where molecules are located”), and none sees entropy as a substance-like entity that flows into and out of a system, which could have been expected in other scientific disciplines (Christensen and Rump, 2008).
We can further follow the change that some of the students undergo in relation to the disorder metaphor from before to after the course, in terms of problematising their previous understanding. In their responses, some of the students relate explicitly to the lecturer's given limitations of the disorder metaphor. In the light of examples where visual order goes along with high entropy, some of these students draw the same conclusion as Lambert (2002): the disorder metaphor is no good. For instance, Lisa, who wrote that entropy is disorder prior to the course, relates to her previous response after the course: “Last time I answered that I thought it was order. Apparently, that was a dumb way to see things. How atoms distribute.” Still, her feeling that she has not quite grasped the concept remains: “Now, I know how to do calculations with it, but I still feel that it's not very clear to me.” Similarly Anna has come to abandon the disorder metaphor, where the course has “clarified, taken away ‘disorder’ explanations”.
However, more students express that they have now a more nuanced view on the disorder metaphor. There are cases when it does not work very well: “I have realised that entropy cannot always be described as the degree of disorder in a system”, or “That entropy cannot be described only as a measure of disorder”. In particular, Karolina adopted the idea of entropy as the possibility for molecules to move and spread out. She reflects: “In the beginning of the course I saw entropy as ‘disorder’. Now I have a more nuanced view on entropy, according to [her description].” In all these cases, the disorder metaphor is problematised, and the students have developed an awareness that it does not always apply. There are good reasons to provide other, complementary explanations, but in line with Styer (2000), that does not necessarily mean that the disorder metaphor has to be avoided and completely abandoned.
As we have seen, Leff (1996, 2007) has proposed the introduction of entropy in terms of spreading of energy, which is adopted in the course literature (Atkins and De Paula, 2010). However, only four of the students make use of descriptions relating to entropy as spreading of energy in terms of the distribution or dispersal of energy across energy levels after the course. In fact, all cases where students use expressions involving “spread” or “spreading” relate to the spreading of particles rather than energy, supporting the view that it is tempting to give the metaphor a spatial interpretation (Jeppsson et al., 2011); these instances were thus coded in the spatial configuration category. It may be the case that the interpretation of entropy as spreading of particles is particularly tempting within chemistry, with its focus on particle interactions (Becker et al., 2013).
In the analysis of the concepts the students relate to entropy, we also found many of them associating entropy with enthalpy. A closer look at the descriptions of what entropy means to them reveals a variety of the nature of the connection to enthalpy prior to the course. Some of the students admit to mixing them up: “I mix it up with enthalpy, but I think it is disorder”, and one of them sees the concepts as contrary: “A measure of disorder, the opposite of enthalpy”. In these examples, the fact that the students merely do not remember which label comes with which concept does not preclude that they may have an adequate understanding of the concepts themselves. In contrast, none of the descriptions of entropy after the course involve enthalpy.
If teleological and anthropomorphic language were seen as an indication of a more primitive understanding or of limited explanatory value, its decreasing prevalence would be welcome. In this case, we would rather side with Talanquer (2007), in his argumentation that the idea of teleological striving may be useful in grasping the second law of thermodynamics. Our data show that the teleological/anthropomorphic category is significantly positively correlated with relating to the second law of thermodynamics, both before (p < 0.00001) and after the course (p = 0.0002). In fact, 18 of the 19 students who relate to the second law of thermodynamics before the course also involve teleological or anthropomorphic reasoning in their responses. In other words, without recourse to teleological expressions, students are less likely to connect entropy to the second law of thermodynamics, which we think is a central aspect of the concept. Furthermore, before the course, both mentioning of the second law of thermodynamics (p = 0.0002) and the use of teleological/anthropomorphic reasoning (p = 0.0004) are positively correlated to the use of the disorder metaphor, forming a cluster of three categories, as captured in statements like: “Entropy – disorder. All systems strive for disorder in all processes.” These significant correlations to disorder are not retained in the responses after the course (p = 0.32 and p = 0.47, respectively). In addition, there was no significant correlation between the teleology/anthropomorphic category and the microscopic category.
ln
Q”, in reference to the partition function formalism presented in the course, or “dS = dQrev/T. S increases for every spontaneous process in an isolated system” (after course). However, surprisingly few answers relate to Clausius's (or Boltzmann's) formalism explicitly in this way.
Finally, many of the students admitted, before and after the course, that they found entropy to be a difficult and abstract concept – particularly in the responses to the item “How has the course influenced your understanding of the entropy concept? Please give concrete examples.” –. For instance: “Now, I know how to do calculations with it, but I still feel it's not entirely clear to me.” This view of thermodynamics, and particularly entropy, as abstract and restricted to mathematical formalism, is recognised from previous research (e.g.Carson and Watson, 2002).
As for the overall purpose of the study, the students provided evidence of a broad range of explanations of what entropy is, and other scientific concepts they associate with entropy. We also see clear evidence of the involved students adopting a chemistry-specific perspective on thermodynamics. This is expressed in the phenomena and scientific concepts they bring up, but most characteristically, however, with a focus on microscopic, particle-based explanations (Becker et al., 2013; Christensen and Rump, 2008). When it comes to our ambition to evaluate the usefulness of different ideas of and metaphors for entropy, our results are less clear cut and require some elaboration.
When comparing the responses from the questionnaires before and after the course, there is a trend towards abandoning a connection between entropy and an undifferentiated energy, and instead mentioning its connection to heat, heat capacity, internal energy and temperature.
It should further be noted that no students related entropy to disorder as a scientific concept, which points to their awareness of the metaphorical interpretation of the idea of entropy as disorder. This stands in stark contrast to the students' own interpretations of what entropy is and prior research where students were found to associate entropy strongly with disorder, when it was given in a list of concepts related to entropy found in the literature (Gustavsson et al., 2013).
As the course was framed in chemistry education (Christensen and Rump, 2008), it comes as no surprise that a large and increasing proportion of the students make use of microscopic, molecular interpretations of entropy. In particular, several of the participants come to adopt the view of entropy as particles' freedom to move about, relying on but also elaborating on the metaphor of entropy as freedom (Styer, 2000; Brissaud, 2005).
The proportion of students employing teleological reasoning (e.g. the universe strives for maximum entropy or disorder) decreases from the pre- to the post-questionnaire. However, the fact that reduced teleological reasoning comes along with fewer students pointing out the relevance of entropy in relation to the second law of thermodynamics – which we regard as a central aspect of entropy – confirms its usefulness for this particular topic (Talanquer, 2007).
Only a few students adopt the idea of entropy as in some way related to spreading after the course, and those who do relate it to spreading of particles, rather than spreading of energy, as suggested by Leff (1996). In other words, the spreading metaphor – just like the disorder metaphor – easily invites a focus on the spatial configuration of the constituent particles of a system, rather than constraining the focus to energy distributions.
One possible interpretation aligns with the findings of Carson and Watson (2002) that thermodynamics courses tend to focus on algebraic problem-solving, and that the connection between problem-solving skills and conceptual understanding in science courses is weak (Clement, 1982); in fact, in the current study problem-solving and conceptual understanding come across as completely orthogonal dimensions. An alternative, possibly more provocative interpretation, also consistent with our findings, is that the different conceptions or metaphors of entropy are potentially equally useful or likely to be misinterpreted. For each metaphor, students need to become aware of its shortcomings as well as its merits. What is perhaps most puzzling with our findings is that problematisation of an earlier understanding of entropy has no correlation with exam results.
Then again, given the nature of the exam and the method of data collection, we should be cautious in reading too much into the lack of correlations. As seen in Appendix A, most exam items did not involve entropy explicitly. It may well be that a more fine-grained analysis of the responses to the individual test items would show correlational patterns, but they do not emerge at the aggregate score level.
First of all, we would like to emphasise that metaphor is a ubiquitous feature of language (Lakoff and Johnson, 1980). We use metaphors frequently – and often unconsciously – in many different contexts, including everyday language, the science classroom, and scientific texts. Metaphor is not merely an ornamental rhetorical device, but something that we cannot do without in science learning and communication. The questions are whether a particular metaphor is apt, and whether our students have understood it in the way that it was intended by an author or teacher.
As we have seen above, Taber and Watts (2000) argue that students' language involving entities ‘trying’, ‘wanting’, or ‘liking’ has explanatory power only so long as these entities literally are animate; such use of anthropomorphic or teleological lines of reasoning can only provide pseudoexplanations. From another perspective, Boyer (1996) points to research that has found that infants are able to distinguish between animate and inanimate objects and that pre-schoolers are able to make reasonable inferences based on such categories. Since even young children do not tend to confuse animate and inanimate entities, Boyer sees the prevalence of animistic and anthropomorphic reasoning across cultures as counter-intuitive and puzzling at first glance. However, he argues that it is precisely this counter-intuitive character that makes anthropomorphic reasoning attractive and attention grabbing. In this regard, he resonates with Duit's (1991, p. 650) take on the use of metaphors in science education: “Metaphors always have an aspect of surprise; they provoke anomaly”, and Lemke's (1990) view that metaphorical language in the science classroom is attractive just because of its rule-breaking character.
In our view, when one of the student writes: “The universe strives for, like, high entropy…”, we think that he is aware of the figurative nature of the expression, in relation to an inanimate quality of nature, i.e. a case of ‘weak’ anthropomorphism (Taber and Watts, 1996). In fact, this may help to remind students that entropy is not a conserved quantity, a mistake many students have been found to make (Christensen et al., 2009). In this regard, we argue that anthropomorphic and teleological reasoning may be useful for students' understanding of science, in particular in relation to theoretically and empirically well-grounded ideas as the second law of thermodynamics (Talanquer, 2007).
On the other hand, in line with Taber and Watts (1996), we acknowledge that the enticement of anthropomorphic and teleological reasoning makes novices vulnerable to overgeneralisation. For instance, from our human experience at the macroscopic scale, it is tempting to infer – erroneously – that heat is generated and accumulated when atoms collide with each other, or that energy is needed as an ingredient, rather than released, when a chemical bond is formed. In this regard, we find some problematic student statements in our data, such as: “Atoms/molecules strive to reach disorder, since they want most to be as spread out from each other as possible.” From this sentence, we suspect that the student has not fully grasped the randomness of the spatial distribution of the particles, implying that the particles are repelled from each other, as if they were equally charged particles. Students also have to be made aware of the difference between ‘weak’ anthropomorphism used as a pedagogical tool, and ‘strong’ anthropomorphism, which might be relevant for instance in a biological context. More fundamentally, from the point of view of the nature of science, students need to understand the relation between cause and effect, and thereby the difference between teleological and properly causal explanations. Teleological explanation may serve as a useful intermediate stepping stone in education, but students should be encouraged to eventually grasp the underlying causal mechanisms.
In contrast to these ambiguous cases of metaphorical language, some of the students' explanations involving the relation between entropy and aspects of energy are more unequivocally inaccurate. For instance, the statement: “Entropy is the heat in a system that does not transform into work”, provided before the course, reveals a poor understanding of entropy, but also of heat and work as process variables. Confusion of entropy and energy may be an underlying reason for believing that entropy is a conserved quantity (Christensen et al., 2009). In this regard, we were happy to see that the prevalence of such statements decreased considerably in the responses after the course.
As we have seen, the disorder metaphor has received considerable criticism in science education research (Leff, 1996; Lambert, 2002; Wei et al., 2014), and there is a deliberate effort to convince textbook authors and teachers not to use it (Lambert, 2014). Although acknowledging many of the drawbacks of identifying entropy as disorder, we would like to call for some moderation. Data from the present study show that students' use of the disorder metaphor or not in coming to understand entropy has no correlation with problem-solving ability in a chemical thermodynamics course. This does not support the view that the metaphor is detrimental for thermodynamics teaching (Lambert, 2002; Wei et al., 2014), but it is not very useful in its own right either.
In our view, the disorder metaphor serves well in early introductions of entropy. In particular, it may be used to explain the possibility of spontaneous endothermic reactions, or that a substance typically increases in entropy as it changes from solid, through liquid, to gas phase, although as emphasised by Styer (2000) and others not without exceptions. In addition, we found that students' connection of entropy to the second law of thermodynamics before the course was positively correlated to seeing entropy in terms of disorder, and the use of teleological reasoning; a valuable contribution of the otherwise criticised ways of approaching the concept. In fact, in the interview with the lecturer where we presented the main outcomes of the study, he found it valuable to get to know that fewer students connected entropy to the second law of thermodynamics after the course than before it. He explained this as a consequence of the microscopic focus of the course, and thought, in line with Baierlein (1994), that more effort might be spent towards the end of the course to connect the microscopic interpretations to the macroscopic level.
Admittedly, as pointed out by Leff (1996), the disorder metaphor may seem mysterious from the point of view of macroscopic thermodynamics, in relation to Clausius's formalism: dS = dQrev/T. However, the metaphor is probably less cryptic within a chemistry tradition, with its inherent focus on molecular interactions (Christensen and Rump, 2008). Furthermore, in order to encourage a more nuanced interpretation of the disorder metaphor, Pflug (1983) proposes distinguishing between a static, configurational ‘desk type disorder’ and a more dynamic ‘disco type disorder’. With the disco type disorder in mind, there is a better opportunity to illustrate the influence of a system's energy on its entropy.
Some of the students express that they have come to problematise the disorder metaphor as they engaged with the course, in response to the lecturer pointing out its limitations. This is encouraging. As pointed out by Glynn (1989), analogies and metaphors are double-edged swords, and every metaphor breaks down at some point. As some of these students realise, however, awareness of a metaphor's limitations does not mean that it has to be abandoned altogether. It is also interesting to note that the students bring up limitations only of the disorder metaphor. Ideally, all metaphors or models that are introduced in teaching should undergo the same type of scrutiny with regard to the scope of their applicability.
As a final word, previous recommendations for teaching about entropy have sometimes focused on finding the best metaphor, be it freedom, spreading or something else. The present study, in contrast, shows that students are able to coordinate several metaphors simultaneously, including entropy as disorder, freedom and movement. Each of these metaphors has the potential to illustrate different aspects of the topic at hand. In this way, we would encourage the introduction of several ways to conceive the highly complex concept of entropy, rather than using one approach only.
| Na2SO4·10H2O(s) → Na2SO4(s) + 10H2O(g) |
3. (a) 0.750 moles of hexane evaporates at its normal boiling point (69 °C). The enthalpy of vaporization is 331.8 J g−1 and the vapour phase is assumed to be ideal. Calculate ΔH, ΔS, and ΔG.
7. For the gas phase reaction
| 2HBr ↔ H2 + Br2 |
Use this expression to calculate ΔHθ, ΔSθ, ΔGθ, and ΔCθp for the reaction at 80 °C.
Footnote |
| † This translates literally into: “(1) The energy of the world is constant. (2) The entropy of the world strives towards a maximum”, although the formulation “The entropy of the universe tends to a maximum” is more widely spread. |
| This journal is © The Royal Society of Chemistry 2015 |