AP Physics 2 · Topic 9.5

Topic 9.5: Specific Heat and Thermal Conductivity

Unit 9: Thermodynamics15-18% of the multiple-choice section

Specific heat c is the energy one kilogram of a material needs to warm by one kelvin, so the energy transferred is mass times c times the temperature change. Thermal conductivity k sets the conduction rate: k times area times the temperature difference, divided by thickness.

AP Physics: Unit 9 (topics 9.5 Specific Heat and Thermal Conductivity). AP Physics 2 Unit 9, Topic 9.5. Two learning objectives. 9.5.A asks students to describe the energy required to change the temperature of an object by a certain amount, supported by 9.5.A.1 (the amount of energy required to change the temperature of a material is related to the material's specific heat, relevant equation Q = mc times the change in temperature) and 9.5.A.2 (the specific heat of a material is an intrinsic property of that material that depends on the arrangement and interactions of the atoms that make up the material). 9.5.B asks students to describe the rate at which energy is transferred by conduction through a given material, supported by 9.5.B.1 (the rate at which energy is transferred by conduction through a given material is related to the thermal conductivity, the physical dimensions of the material, and the temperature difference across the material, relevant equation Q over delta t equals k A times the temperature difference divided by L) and 9.5.B.2 (the thermal conductivity of a material is an intrinsic property of that material that depends on the arrangement and interactions of the atoms that make up the material). The topic's boundary statement reads in full: AP Physics 2 will model specific heat as independent of temperature. The CED's suggested skills here are 1.B, 2.B, 2.D, 3.A, and 3.B, and 9.5 is the only Unit 9 topic listing 2.B. Unit 9 carries 15 to 18 percent of the multiple-choice section and a suggested 10 to 16 class periods.

What Topic 9.5 requires

Topic 9.5 sits in Unit 9, Thermodynamics, weighted at 15 to 18 percent of the multiple-choice section with a suggested 10 to 16 class periods. It carries two learning objectives, four essential knowledge statements, and one boundary statement.

9.5.A, describe the energy required to change the temperature of an object by a certain amount.

  • 9.5.A.1 states that the amount of energy required to change the temperature of a material is related to the material's specific heat, and prints the relevant equation Q=mcΔTQ = mc\Delta T.
  • 9.5.A.2 states that the specific heat of a material is an intrinsic property of that material that depends on the arrangement and interactions of the atoms that make up the material.

9.5.B, describe the rate at which energy is transferred by conduction through a given material.

  • 9.5.B.1 states that the rate at which energy is transferred by conduction through a given material is related to the thermal conductivity, the physical dimensions of the material, and the temperature difference across the material, and prints the relevant equation QΔt=kAΔTL\dfrac{Q}{\Delta t} = \dfrac{kA\Delta T}{L}.
  • 9.5.B.2 states that the thermal conductivity of a material is an intrinsic property of that material that depends on the arrangement and interactions of the atoms that make up the material.

Boundary statement, in full: "AP Physics 2 will model specific heat as independent of temperature." That is the entire boundary statement, one sentence. Note that 9.5.A.2 and 9.5.B.2 are the same sentence with one noun swapped: cc and kk are both intrinsic properties of the material.

The CED lists five suggested skills here, more than any Unit 9 topic except 9.2: 1.B, create quantitative graphs with appropriate scales and units, including plotting data; 2.B, calculate or estimate an unknown quantity with units from known quantities, by selecting and following a logical computational pathway; 2.D, predict new values or factors of change of physical quantities using functional dependence between variables; 3.A, create experimental procedures that are appropriate for a given scientific question; and 3.B, apply an appropriate law, definition, theoretical relationship, or model to make a claim.

Topic 9.5 is the only one of Unit 9's six topics with 2.B listed, a fair signal that this is the unit's calculation topic. One caveat the CED adds is worth carrying: Progress Check questions are built on that content-and-skill pairing, but "AP Exam questions can pair the content with any of the skills." Treat the list as emphasis, not a fence.

Q = mc(deltaT), symbol by symbol (9.5.A.1)

Q=mcΔTQ = mc\Delta T

Every symbol is defined by the AP Physics 2 equation sheet itself: the Thermal Physics column's symbol list reads QQ as "energy transferred to a system by heating", mm as mass, cc as specific heat, and TT as temperature. Three things follow.

QQ carries a sign, and the sheet's wording fixes which one. Energy transferred to the system is positive. Warm something up and ΔT>0\Delta T > 0, so Q>0Q > 0. That is the same convention as ΔU=Q+W\Delta U = Q + W in Topic 9.4, and it is the same QQ: the first law's heating term, priced for a particular object.

The units of cc come out of the equation. Rearranged, c=QmΔTc = \dfrac{Q}{m\Delta T}, so specific heat is measured in joules per kilogram per kelvin, J/(kgK)\mathrm{J/(kg \cdot K)}. Read that off the rearrangement rather than memorizing it.

ΔT\Delta T is a difference, so kelvin and degrees Celsius give the same number. The two intervals are the same size, so a change of 25 K and a change of 25 degrees Celsius are the same change. This is the one place in Unit 9 where the distinction does not bite. Wherever an absolute temperature appears, including PV=nRTPV = nRT in Topic 9.2, Kavg=32kBTK_{\text{avg}} = \frac{3}{2}k_B T in Topic 9.1, and U=32nRTU = \frac{3}{2}nRT in Topic 9.4, it must be in kelvin.

Solve for the temperature change instead and the comparison questions answer themselves:

ΔT=Qmc\Delta T = \frac{Q}{mc}

Give two objects the same QQ and the one with the larger mcmc warms less. That product is the object's energy cost per kelvin, and it decides a calorimetry problem. The CED never names it, and the phrase "heat capacity" appears nowhere in the AP Physics 2 course description, so write it as mcmc and keep "specific heat" for cc alone.

Specific heat is a property of the material, not of the sample (9.5.A.2)

Essential knowledge 9.5.A.2 calls specific heat an intrinsic property, and that word does precise work. An intrinsic property does not change when you take more or less of the substance: cut a copper block in half and each half has the same specific heat as the whole, just as each half has the same density. What changes is QQ, because mm halved. A question that hands you a specific heat is handing you a fact about a substance, and the number you compute from one experiment is the one you use in the next.

The rest of 9.5.A.2 says where the property comes from: the arrangement and interactions of the atoms that make up the material. The CED stops there and builds no microscopic model, so neither should an answer. The nearest the course comes is essential knowledge 9.4.A.1, which makes internal energy the sum of the kinetic energy of the objects in a system and the potential energy of their configuration. Energy you add can land in either place, and temperature tracks only the motion. No question will ask you to compute a specific heat from atomic structure.

The consequence you are asked about directly is the comparison: two 1.0 kg samples given 5000 J each end at different temperatures, and the one with the larger cc moves less.

Neither the equation sheet nor the CED prints a table of specific heat values. Any question that needs one supplies it, exactly as the CED's own sample multiple-choice set does when it gives the specific heat of water as 4184J/(kgK)4184 \, \mathrm{J/(kg \cdot K)} inside the question stem. Do not carry remembered values into an exam, and do not treat a missing cc as something to look up: if it is not in the stem, the question wants you to solve for it.

The boundary statement: specific heat is modeled as independent of temperature

"AP Physics 2 will model specific heat as independent of temperature."

Short, and load-bearing. What it grants you:

  • cc is a constant you can pull out of any calculation. You never have to ask what the specific heat was at 290 K versus at 350 K.
  • Q=mcΔTQ = mc\Delta T is exact within the course model, not an approximation over a small range. A 200 K change takes the same one-line calculation as a 2 K one.
  • The graphs are straight. Plot QQ against ΔT\Delta T for a fixed sample and you get a line through the origin with slope mcmc. Skill 1.B lives on that linearity, and the boundary statement is what guarantees it.

What it does not say: it does not say specific heat is the same for every material, because 9.5.A.2 says the opposite; it does not say cc is independent of anything other than temperature; and it does not say a substance has the same specific heat in every phase.

On phases: there is no latent-heat or phase-change equation anywhere on the AP Physics 2 equation sheet, and Unit 9's required course content contains no phase-change essential knowledge statement. The Thermal Physics column holds exactly eight equations, and none of them describes melting or boiling.

The conduction rate, Q over delta t equals kA delta T over L (9.5.B.1)

QΔt=kAΔTL\frac{Q}{\Delta t} = \frac{kA\Delta T}{L}

The left-hand side is not an energy, it is a rate: joules per second, which is watts. That makes it the same kind of quantity as power, and the same sheet prints Pavg=ΔEΔtP_{\text{avg}} = \dfrac{\Delta E}{\Delta t} in its mechanics column. If your answer to a conduction question came out in joules, you answered a different question.

Essential knowledge 9.5.B.1 says the rate is related to "the thermal conductivity, the physical dimensions of the material, and the temperature difference across the material". The CED does not spell out which dimension goes where. The equation does, and swapping them is the standard error.

  • AA is the area of the face the energy crosses, the broad side of the slab.
  • LL is the length of the path through the material, measured along the direction the energy travels: the thickness of the window, not its width.
  • ΔT\Delta T is the temperature difference across the material, between the two faces. Another difference, so either scale works.
  • kk is the thermal conductivity, and its units follow from the equation: watts per meter per kelvin, W/(mK)\mathrm{W/(m \cdot K)}.

Every dependence is first order, which makes this a natural home for skill 2.D. Hold everything else fixed and:

ChangeEffect on the rate
double kkrate doubles
double AArate doubles
double ΔT\Delta Trate doubles
double LLrate halves
double both AA and LLrate unchanged

One reading questions probe: the equation contains a single ΔT\Delta T, so it gives the rate for that temperature difference. If the two sides are free to equilibrate, ΔT\Delta T shrinks as energy moves and the rate shrinks with it, so multiplying an initial rate by a long time overestimates the energy transferred.

Topic 9.3 supplies the context: essential knowledge 9.3.A.2 names conduction, convection, and radiation as the three thermal processes by which energy may be transferred between systems at different temperatures. Topic 9.5 puts a rate equation on exactly one of them. The sheet does print P=AσT4P = A\sigma T^4 for radiated power, but in the Modern Physics column, and no Unit 9 essential knowledge statement uses it. Convection gets no equation at all.

The k problem: one letter, three quantities, one equation sheet

Say this once and then never be caught by it. The AP Physics 2 equation sheet uses the letter kk for three unrelated quantities, and its own symbol lists are where you find out which is which.

Where on the sheetWhat kk meansWhere it shows up
Constants and Conversion Factorsthe Coulomb constant, k=14πε0=9.0×109Nm2/C2k = \dfrac{1}{4\pi\varepsilon_0} = 9.0 \times 10^9 \, \mathrm{N \cdot m^2/C^2}Coulomb's law and the point-charge field, both in the Electricity column
Thermal Physics symbol listthermal conductivityonly in QΔt=kAΔTL\dfrac{Q}{\Delta t} = \dfrac{kA\Delta T}{L}
Mechanics and Fluids symbol listspring constantFs=kΔx\vec{F}_s = -k\Delta\vec{x} and Us=12k(Δx)2U_s = \frac{1}{2}k(\Delta x)^2

Two near misses sit alongside them. kBk_B, with the subscript, is Boltzmann's constant, 1.38×1023J/K1.38 \times 10^{-23} \, \mathrm{J/K}, and it appears in PV=NkBTPV = Nk_B T and Kavg=32kBTK_{\text{avg}} = \frac{3}{2}k_B T in this same unit. And κ\kappa, lowercase kappa, in the Electricity column is the dielectric constant, not a kk at all despite looking like one in handwriting.

The dangerous one is the Coulomb constant, for a specific reason: it is the only kk on the sheet with a number printed next to it, so a student who has drilled "kk is 9.0×1099.0 \times 10^9" can walk that value straight into a conduction problem. Thermal conductivity has no sheet value and never will, because 9.5.B.2 makes it an intrinsic property: it differs for glass and for copper, and a question that needs it states it. If you are reaching for a kk the problem did not supply, you are in the wrong column.

Thermal conductivity is intrinsic too (9.5.B.2), and why the tile floor feels colder

The Unit 9 opener lists four essential questions, which the CED calls thought-provoking questions that motivate students and inspire inquiry. The first is: "Why does the tile floor in the bathroom feel so much colder than the bathroom mat?" It is Topic 9.5's question, and the two essential knowledge statements above answer it completely.

Start with what is not different. The tile and the mat have been in the same room all night. By essential knowledge 9.3.A.4, thermal equilibrium results when no net energy is transferred by thermal processes between two systems in thermal contact, and that is what the room has settled into. A thermometer reads the same on both. The tile is not colder.

What differs is kk. Your foot is warmer than the floor, so energy conducts out of it into whatever you stand on, at the rate kAΔTL\dfrac{kA\Delta T}{L}. The contact area and the temperature difference are about the same either way, so the rate scales with the thermal conductivity, and tile conducts far better than a fabric mat. "Feels cold" reports the rate at which your skin is losing energy, not the temperature of the surface. It is why a metal railing and a wooden one on the same porch feel so different on a winter morning.

Essential knowledge 9.5.B.2 supplies the same sentence the CED used for specific heat: thermal conductivity is an intrinsic property of the material, set by the arrangement and interactions of its atoms. Neither property depends on how much material you have, and both are things the exam gives you rather than things you memorize.

One caution, because the course does not support the shortcut. Specific heat and thermal conductivity are independent: a large cc does not imply a large kk. When a question asks which of two objects warms faster, decide first whether it is about the energy required, which is cc, or the rate of supply, which is kk.

Measuring c and k: experimental design and the graphs (skills 3.A, 1.B)

Skill 3.A, create experimental procedures appropriate for a given scientific question, appears on exactly two of Unit 9's six topic pages: 9.2 and 9.5. Skill 1.B, create quantitative graphs with appropriate scales and units, appears on the same two.

Two standard designs measure a specific heat. Steady heating: warm a known mass with a heater of known power PP and plot temperature against time, giving c=P/(m×slope)c = P/(m \times \text{slope}), as in the third worked example. That line is straight because of the boundary statement, not because the data were kind. Mixing: bring a hot sample into an insulated container with a known mass of water, wait for equilibrium, and solve Qhot+Qcold=0Q_{\text{hot}} + Q_{\text{cold}} = 0, as in the first. Every choice there is aimed at making that zero true, which is what the insulation is for.

For a thermal conductivity, hold a slab between a source and a sink at a fixed temperature difference and measure the rate at which energy crosses it. The 1.B move is to choose axes that linearize the relationship before you plot:

To find kk, varyPlotSlope is
thickness LLrate against 1/L1/LkAΔTkA\Delta T
area AArate against AAkΔT/Lk\Delta T / L
temperature differencerate against ΔT\Delta TkA/LkA/L

Plotting rate against LL itself gives a curve you cannot read a slope off; against 1/L1/L it is a line through the origin. That linearizing step is the graded part of a 1.B question more often than the plotting is.

Every one of these designs assumes all the energy you supply goes where you think it goes. If some leaks away, the temperature rises more slowly than it should and a specific heat calculated as if nothing leaked comes out too large.

How Topic 9.5 is tested, and where it leads

The routines are narrow enough to list, and rehearsing them is most of the preparation.

  1. One object, one equation. Find QQ, mm, cc, or ΔT\Delta T from Q=mcΔTQ = mc\Delta T (skill 2.B). Watch the sign, and watch that ΔT\Delta T is a difference and not a temperature.
  2. Two objects reaching a common temperature. An insulated container, a hot thing and a cold thing, and Qhot+Qcold=0Q_{\text{hot}} + Q_{\text{cold}} = 0. Solve for an unknown specific heat, mass, or final temperature (skill 2.B).
  3. Conduction rate through a slab (skill 2.B), or a comparison of two slabs differing in one variable.
  4. Factor-of-change questions on either equation (skill 2.D). Both are products and quotients of first powers, so set them up as ratios rather than recomputing.
  5. Design or critique an experiment to measure cc or kk (skill 3.A), including saying what the insulation is for.
  6. Justify a claim with one of the two relationships as evidence (skill 3.B). The tile-floor question is the archetype.

The CED's sample multiple-choice set is fifteen questions long, and its answer key aligns question 9 to learning objective 9.5.A, essential knowledge 9.5.A.1, and skill 2.B. That question drops a hot metal sample into water in an insulated container and asks for the metal's specific heat: routine 2 above, and the shape of the first worked example below. Those questions illustrate the format of the exam, so read the alignment as a shape worth practising, not as a claim about how often anything appears.

The unit opener also flags the fourth free-response question, the Qualitative/Quantitative Translation, which "first requires students to make a claim and provide evidence and reasoning to support their claim without reference to equations" before asking for an equation and then for the connection between the two. Rehearse the verbal form of both relationships: more energy for a bigger temperature change, faster conduction through a thinner slab.

Where the topic sits:

  • Topic 9.3 says energy moves spontaneously from hot to cold, that conduction is one of three ways it moves, and that equilibrium is where it stops. Topic 9.5 puts numbers on two of those.
  • Topic 9.4 supplies ΔU=Q+W\Delta U = Q + W, and its QQ is this QQ. The PV diagrams guide walks that bookkeeping end to end.
  • Topic 9.6 takes the equilibrium temperature a calorimetry calculation produces and asks what the first law cannot: why the process runs that way and not the other.
  • The full sheet is at the AP Physics 2 formula sheet, the course overview at AP Physics 2.

A hot metal block in water: finding an unknown specific heat

A 0.500 kg block of an unknown metal is heated to 420.0 K and dropped into 0.200 kg of water at 290.0 K inside an insulated container. The mixture settles at 315.0 K. Take the specific heat of water as 4184J/(kgK)4184 \, \mathrm{J/(kg \cdot K)}. (a) Find the specific heat of the metal. (b) Predict the final temperature if the same block were dropped into 0.400 kg of water instead, everything else unchanged.

  1. Declare the sign convention and keep it: QQ is positive when energy is transferred into an object, as the sheet's Thermal Physics symbol list defines it. The container is insulated, so no energy crosses its wall and Qmetal+Qwater=0Q_{\text{metal}} + Q_{\text{water}} = 0.

  2. Water: ΔT=315.0290.0=25.0K\Delta T = 315.0 - 290.0 = 25.0 \, \mathrm{K}, so Qwater=(0.200)(4184)(25.0)=20,920JQ_{\text{water}} = (0.200)(4184)(25.0) = 20{,}920 \, \mathrm{J}, positive as it must be for something that warmed up. Metal: ΔT=315.0420.0=105.0K\Delta T = 315.0 - 420.0 = -105.0 \, \mathrm{K}, so Qmetal=(0.500)(c)(105.0)=52.5cQ_{\text{metal}} = (0.500)(c)(-105.0) = -52.5c.

  3. Set the sum to zero: 20,92052.5c=020{,}920 - 52.5c = 0, so c=20,92052.5=398.5J/(kgK)c = \dfrac{20{,}920}{52.5} = 398.5 \, \mathrm{J/(kg \cdot K)}, which is 398J/(kgK)398 \, \mathrm{J/(kg \cdot K)} to three significant figures.

  4. Plausibility check: the metal's specific heat is roughly a tenth of the water's, the right direction, since the metal fell 105.0 K while the water rose 25.0 K despite being more than twice as massive.

  5. (b) With 0.400 kg of water and an unknown final temperature TT: (0.500)(398)(T420.0)+(0.400)(4184)(T290.0)=0(0.500)(398)(T - 420.0) + (0.400)(4184)(T - 290.0) = 0, so 1872.6T=568,9241872.6\,T = 568{,}924 and T=303.8KT = 303.8 \, \mathrm{K}.

  6. Read the 2.D lesson off that answer. The water's rise fell from 25.0 K to 13.8 K, more than half rather than exactly half. Doubling mm halves ΔT\Delta T only when QQ is held fixed, and here it is not: the lower final temperature means the metal cools further and releases about 2.2×103J2.2 \times 10^{3} \, \mathrm{J} more. Check what is actually held constant before you scale.

(a) c=398J/(kgK)c = 398 \, \mathrm{J/(kg \cdot K)}. (b) 303.8 K, a water temperature rise of 13.8 K rather than 25.0 K. Doubling the water does not halve the rise, because the metal then cools further and gives up more energy.

Conduction through a window pane, and what changing the material does

A glass pane of area 1.5m21.5 \, \mathrm{m^2} and thickness 4.0 mm has its inside face held 18 K warmer than its outside face. The problem gives the glass a thermal conductivity of 0.80W/(mK)0.80 \, \mathrm{W/(m \cdot K)}. (a) Find the rate at which energy is conducted through the pane. (b) Find the energy conducted in one hour at that rate. (c) The pane is replaced by a 4.0 mm panel with k=0.040W/(mK)k = 0.040 \, \mathrm{W/(m \cdot K)}, same area and temperature difference. Find the new rate and the factor by which it changed.

  1. Convert the thickness first: L=4.0mm=4.0×103mL = 4.0 \, \mathrm{mm} = 4.0 \times 10^{-3} \, \mathrm{m}. Leaving it in millimetres inflates the answer by a thousand, and it is the most common arithmetic failure on this equation.

  2. Sort the dimensions: the energy travels through the 4.0 mm direction, so that is LL; the 1.5m21.5 \, \mathrm{m^2} face is what it crosses, so that is AA.

  3. (a) QΔt=(0.80)(1.5)(18)4.0×103=21.64.0×103=5.4×103W\dfrac{Q}{\Delta t} = \dfrac{(0.80)(1.5)(18)}{4.0 \times 10^{-3}} = \dfrac{21.6}{4.0 \times 10^{-3}} = 5.4 \times 10^{3} \, \mathrm{W}. Units check: W/(mK)×m2×K÷m=W\mathrm{W/(m \cdot K)} \times \mathrm{m^2} \times \mathrm{K} \div \mathrm{m} = \mathrm{W}, a rate, as required.

  4. (b) Energy is rate times time, and one hour is 3600 s: Q=(5400)(3600)=1.9×107JQ = (5400)(3600) = 1.9 \times 10^{7} \, \mathrm{J}. This step is only valid because the problem holds the temperature difference at 18 K; if the two sides equilibrated, the rate would fall as they did.

  5. (c) (0.040)(1.5)(18)4.0×103=1.084.0×103=2.7×102W\dfrac{(0.040)(1.5)(18)}{4.0 \times 10^{-3}} = \dfrac{1.08}{4.0 \times 10^{-3}} = 2.7 \times 10^{2} \, \mathrm{W}.

  6. The factor: 5400/270=205400/270 = 20, and 0.80/0.040=200.80/0.040 = 20. With AA, ΔT\Delta T and LL unchanged, the rate is directly proportional to kk, so the factor of change in the rate is exactly the factor of change in kk. You could have written that down without recomputing, which is the point of skill 2.D.

  7. Sanity check: 5.4 kW through one pane is large, and it is why real windows are not a single thin sheet of glass. Doubling the thickness only halves it; the low-kk layer is what changes the order of magnitude.

(a) 5.4×103W5.4 \times 10^{3} \, \mathrm{W}. (b) 1.9×107J1.9 \times 10^{7} \, \mathrm{J} in one hour. (c) 2.7×102W2.7 \times 10^{2} \, \mathrm{W}, smaller by a factor of 20, exactly the factor by which kk fell.

Reading c off a heating graph, and what a leak does to the answer

A student puts 0.250 kg of a liquid in an insulated cup with a 60.0 W immersion heater, stirs continuously, and records temperature against time. The data fall on a straight line of slope 0.0600K/s0.0600 \, \mathrm{K/s}. (a) Find the specific heat of the liquid. (b) A second student points out that 8.0 percent of the heater's output is lost to the surroundings rather than reaching the liquid. Recalculate, and say whether the first answer was too high or too low.

  1. The heater supplies Q=PΔtQ = P\Delta t, and that energy does Q=mcΔTQ = mc\Delta T to the liquid, on the assumption that all of the output reaches it. Equating them gives P=mcΔTΔtP = mc\dfrac{\Delta T}{\Delta t}, and ΔTΔt\dfrac{\Delta T}{\Delta t} is exactly the graph's slope.

  2. (a) c=Pm×slope=60.0(0.250)(0.0600)=60.00.0150=4.00×103J/(kgK)c = \dfrac{P}{m \times \text{slope}} = \dfrac{60.0}{(0.250)(0.0600)} = \dfrac{60.0}{0.0150} = 4.00 \times 10^{3} \, \mathrm{J/(kg \cdot K)}.

  3. Check over a 200 s stretch: the heater supplies (60.0)(200)=12,000J(60.0)(200) = 12{,}000 \, \mathrm{J}, the temperature rises (0.0600)(200)=12.0K(0.0600)(200) = 12.0 \, \mathrm{K}, and mcΔT=(0.250)(4000)(12.0)=12,000Jmc\Delta T = (0.250)(4000)(12.0) = 12{,}000 \, \mathrm{J}. Consistent. The line is straight because the boundary statement models cc as independent of temperature; a curved graph here would point at the apparatus, not the liquid.

  4. (b) Only 92.0 percent of the output reaches the liquid, so Pin=(0.920)(60.0)=55.2WP_{\text{in}} = (0.920)(60.0) = 55.2 \, \mathrm{W}, and c=55.20.0150=3.68×103J/(kgK)c = \dfrac{55.2}{0.0150} = 3.68 \times 10^{3} \, \mathrm{J/(kg \cdot K)}.

  5. So the first answer was too high by a factor of 4000/3680=1.0874000/3680 = 1.087, about 8.7 percent. The logic generalizes: the measured slope is fixed, and crediting the liquid with more energy than it received forces cc upward to explain the same rise. Unaccounted losses here bias the specific heat high, never low.

(a) c=4.00×103J/(kgK)c = 4.00 \times 10^{3} \, \mathrm{J/(kg \cdot K)} if all the heater's output reaches the liquid. (b) With 8.0 percent lost, c=3.68×103J/(kgK)c = 3.68 \times 10^{3} \, \mathrm{J/(kg \cdot K)}. Ignoring the loss overestimates cc by about 8.7 percent, because it credits the liquid with energy it never received.

Frequently asked questions

What is the specific heat formula in AP Physics 2?

Q = mc times the change in temperature, printed on the AP Physics 2 equation sheet in the Thermal Physics column and given as the relevant equation for essential knowledge 9.5.A.1. Q is the energy transferred to the object by heating, m is its mass, and c is its specific heat. Because the last factor is a difference, kelvin and degrees Celsius give the same number for it. Rearranging shows the units of c are joules per kilogram per kelvin.

Do you use Celsius or Kelvin in Q = mc delta T?

Either works, because the equation contains a temperature difference rather than a temperature. A one-kelvin interval and a one-degree-Celsius interval are the same size, so a 25 K change and a 25 degree Celsius change are the same change. This is the exception, not the rule: every AP Physics 2 equation containing an absolute temperature, including PV = nRT and the internal energy of a monatomic ideal gas, requires kelvin.

What is the equation for the rate of heat conduction?

The rate is Q divided by the time interval, and it equals k times A times the temperature difference, all divided by L. It is printed on the AP Physics 2 equation sheet and is the relevant equation for essential knowledge 9.5.B.1. Here k is the thermal conductivity, A is the area of the face the energy crosses, L is the thickness along the direction of travel, and the temperature difference is between the two faces. The left side is a rate in watts, not an energy, so multiply by a time if a question asks for total energy.

Is the k in thermal conductivity the same as Coulomb's constant?

No. They are unrelated quantities that share a letter on the same equation sheet. The AP Physics 2 sheet defines k as thermal conductivity in the Thermal Physics symbol list, as the Coulomb constant equal to 9.0 x 10^9 N m^2 / C^2 in the Constants and Conversion Factors box, and as the spring constant in the Mechanics and Fluids symbol list. Only the Coulomb constant has a numerical value printed. Thermal conductivity is an intrinsic property of a material, so it differs from substance to substance and a question that needs it will state it.

Why does a tile floor feel colder than a rug at the same temperature?

Because your skin reports the rate at which it is losing energy, not the temperature of what it is touching. The tile and the rug have been in the same room long enough to reach thermal equilibrium, so a thermometer reads the same on both. Your foot is warmer than either, so energy conducts out of it at a rate of k times area times temperature difference divided by thickness, and tile has a far larger thermal conductivity than fabric. This is the first essential question in the AP Physics 2 Unit 9 opener.

Does the AP Physics 2 equation sheet give specific heat values?

No. The Thermal Physics column prints eight equations and a symbol list, and no table of material properties appears anywhere on the sheet or in the Course and Exam Description. Specific heat and thermal conductivity are intrinsic properties of individual materials, per essential knowledge 9.5.A.2 and 9.5.B.2, so any question needing a value supplies it. A value missing from a problem is a signal that you are meant to solve for it.