06.02 Thermal energy

Module 06 — Heat and Particles · quiz worth 15 pts

The big idea Use Q = mcΔT when temperature changes within one phase. Use Q = mL during a phase change, when energy changes particle arrangement while temperature stays constant.

Two equations, one decision

The hardest part is choosing the equation. Start by asking whether temperature or phase is changing.

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Course constants used in this review

Substancec (J/kg·K)Lf (J/kg)Lv (J/kg)
Water 4186 3.33 × 10⁵ 2.26 × 10⁶
Lead 128 2.5 × 10⁴ 8.68 × 10⁵
Copper 387 1.34 × 10⁵ 5.06 × 10⁶
Before you start Use the 06.01 distinction between temperature and transferred energy. Be ready to convert grams to kilograms and calculate ΔT = Tf − Ti.

Heat is energy in transit

Heat is energy transferred because two systems have different temperatures. Spontaneous transfer runs from the higher-temperature system to the lower-temperature system until they reach thermal equilibrium. After the transfer, the energy belongs to the systems' internal energy. The symbol Q records the amount transferred, in joules (J).

Optional three-panel helper: conduction passes energy through neighboring solid particles, convection forms a complete warm-up and cool-down fluid loop, and radiation crosses an empty gap as electromagnetic waves to an absorber.
Optional helper: conduction transfers through neighboring particles, convection circulates fluid, and radiation needs no material medium.

The particle picture

Within one phase, added energy usually raises average particle kinetic energy and temperature. During melting or boiling, added energy instead changes intermolecular arrangement and potential energy. That is why temperature can remain constant even while energy continues to enter. Removing energy reverses the changes: gas condenses and liquid freezes at the same transition temperatures at a given pressure.

Phase-change map

Solid → liquid is melting; liquid → solid is freezing. Liquid → gas is vaporization or boiling; gas → liquid is condensation. Melting and vaporization absorb energy. Freezing and condensation release energy to the surroundings. A melting point equals the freezing point for the same substance and pressure; a boiling point equals the condensation point under the same conditions.

Read a heating curve

Read an ideal heating curve from left to right as energy enters: solid warms on a rising segment, melting occurs on a level segment, liquid warms on the next rise, boiling occurs on the next level segment, and gas warms on the final rise. A rising segment means temperature and average kinetic energy increase within one phase. A level segment means phase and particle arrangement change while energy still enters.

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Heat-transfer formulas

Temperature change
Q=mcΔTQ=mc\Delta T

Q in J, m in kg, c in J/(kg·K), and ΔT = Tf − Ti in K or Celsius degrees.

Fusion or freezing
Q=mLfQ=mL_f

Lf is latent heat of fusion in J/kg. Use its magnitude, then assign the sign from energy direction.

Vaporization or condensation
Q=mLvQ=mL_v

Lv is latent heat of vaporization in J/kg.

Energy conservation
∑Q=0\sum Q=0

For an isolated exchange, energy gained plus energy lost equals zero.

Choose the equation

Mark the starting and ending phase

If both are the same phase and temperature changes, start with Q = mcΔT.

Look for a transition word

Melt, freeze, vaporize, boil, or condense points to Q = mL while the transition occurs.

Split a multi-stage path

Heating ice below 0 °C until it becomes warm water needs separate warming, melting, and warming calculations. Add the Q values.

Assign the sign

With ΔT = Tf − Ti, warming gives positive Q and cooling gives negative Q. A negative result means energy left the chosen system.

Check units

Convert grams to kilograms before using constants written per kilogram.

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Worked heat examples

Warm one kilogram of water

  • Mass. m=1.00 kgm=1.00\,\text{kg}
  • Specific heat. c=4186 J/(kg⋅K)c=4186\,\text{J/(kg·K)}
  • Temperatures. Ti=5.0 ∘C, Tf=40.0 ∘CT_i=5.0\,^{\circ}\text{C},\ T_f=40.0\,^{\circ}\text{C}

How much energy enters the water?

  1. Find the temperature change.
    ΔT=40.0−5.0=35.0 K\Delta T=40.0-5.0=35.0\,\text{K}
  2. Use sensible heat.
    Q=(1.00)(4186)(35.0) JQ=(1.00)(4186)(35.0)\,\text{J}

Q = 1.47 × 10⁵ J.

Cool a copper sample

  • Mass. m=0.349 kgm=0.349\,\text{kg}
  • Specific heat. c=387 J/(kg⋅K)c=387\,\text{J/(kg·K)}
  • Temperature change. ΔT=21.0−87.0=−66.0 K\Delta T=21.0-87.0=-66.0\,\text{K}

How much energy transfers relative to the copper?

  1. Use Q = mcΔT.
    Q=(0.349)(387)(−66.0) JQ=(0.349)(387)(-66.0)\,\text{J}

Q = −8.92 × 10³ J. The negative sign means energy left the copper.

Melt lead at its melting point

  • Mass. m=5.0 kgm=5.0\,\text{kg}
  • Fusion constant. Lf=2.5×104 J/kgL_f=2.5\times10^4\,\text{J/kg}

How much energy is required?

  1. The phase changes at constant temperature.
    Q=mLfQ=mL_f
  2. Multiply mass by latent heat.
    Q=(5.0)(2.5×104) JQ=(5.0)(2.5\times10^4)\,\text{J}

Q = 1.3 × 10⁵ J to two significant figures.

Thermal-energy traps

A plateau does not mean no energy transfer

Energy still enters or leaves. It changes intermolecular potential energy rather than average kinetic energy.

Do not use mcΔT for a completed phase change

The temperature is constant during the transition, so latent heat supplies the missing energy calculation.

Mass must match the constant

A constant in J/kg requires kilograms.

Heat direction belongs to a chosen system

Q is positive for energy entering that system and negative for energy leaving it.

Thermal-energy practice

Choose the physical process first. The arithmetic comes second.