Heat moves three ways — conduction, convection and radiation — and only radiation crosses empty space. Drag the sliders below to change the temperatures, conductivity, thickness and emissivity, and compare the three transfer rates in real time.

Heat Transfer: Three Ways

Set a hot temperature and a cool/surroundings temperature, then tune each mode's controls. Conduction, convection and radiation each compute their own rate — watch which one wins as you change the slab, the airflow and the glow.

Conduction kAΔT/d
Convection hAΔT
Radiation εσA(T4−Ts4)
Dominant
Hot temperature T200 °C
Cool / surroundings Ts20 °C
Conductivity k50.00 W/m·K
Slab thickness d0.050 m
Convection h25 W/m²·K
Emissivity ε0.90
Surface area A = 1 m² (fixed) · σ = 5.67 × 10-8 W/m²·K4 · radiation uses kelvin.
Thin, conductive slabs make conduction huge; strong airflow favours convection; very hot bodies make radiation climb steeply (∝ T4). Set T = Ts and every rate falls to zero.

What Is the Heat Transfer Simulator?

The heat transfer simulator is a free interactive physics lab that runs in your browser — nothing to install and no sign-up. Change the temperatures, conductivity, thickness and emissivity and compare conduction, convection and radiation. It reports conduction kAΔT/d, convection hAΔT and radiation εσa as you drag the sliders.

What you can change in the heat transfer simulator
ControlRangeStep
Hot temperature Celsius50 – 500 °C1
Cool or surroundings temperature Celsius0 – 100 °C1
Thermal conductivity per metre kelvin0.02 – 400 W/m·K0.01
Slab thickness0.001 – 0.20 m0.001
Convective heat transfer coefficient per square metre kelvin2 – 100 W/m²·K1
Emissivity0 – 10.01

Three Routes for Heat, One That Needs Nothing

You feel heat travel three different ways, but only one of them can cross empty space. When you touch a warm mug, conduction carries energy through the solid ceramic, particle to particle. The sim reports that rate as kAΔT/d: a bigger thermal conductivity k, a wider area A, or a larger temperature gap ΔT all speed it up, while a thicker slab d slows it down. That is exactly why a fluffy jacket, thick and barely conductive, keeps you warm. Slide the Thermal conductivity and Slab thickness controls and watch the conduction readout swing.

Now let a fluid do the work. Convection moves heat by physically carrying warm material away, so its rate hAΔT climbs with the Convection coefficient h and the temperature difference. The third path abandons matter entirely. Radiation leaves every warm surface as electromagnetic waves at rate εσAT^4, where T is the absolute temperature in kelvin. That fourth power bites hard: double the absolute temperature and radiated power jumps sixteen-fold. Push the Hot temperature slider high and the radiation figure runs away from the others.

Only radiation needs no medium at all, which is how sunlight pours across the vacuum of space to warm the Earth. Test each mode yourself, then size a real wall with the thermal conduction calculator or branch into another hands-on experiment in the physics simulation collection.

Frequently asked questions

What are the three ways heat is transferred?

Conduction (through a solid, particle to particle), convection (carried by a moving fluid), and radiation (as electromagnetic waves). Only radiation can cross a vacuum.

What does the rate of conduction depend on?

On Q/t = k·A·ΔT/d — the thermal conductivity k, the area A, the temperature difference ΔT and the thickness d. Thicker or less conductive materials conduct more slowly, which is why they insulate.

Why does radiation matter so much at high temperature?

Radiated power follows Stefan's law, ε·σ·A·T^4, with T the absolute temperature. Because of the fourth power, doubling the absolute temperature raises the radiated power sixteen-fold.

How does heat from the Sun reach the Earth?

By radiation. Conduction and convection both need matter, but radiation travels as electromagnetic waves and crosses the vacuum of space, so sunlight can warm the Earth.

References & formula source

  • Halliday, Resnick & Walker — Fundamentals of Physics, Chapter 18 (Heat Transfer Mechanisms).
  • Young & Freedman — University Physics with Modern Physics, §17.7 (Mechanisms of Heat Transfer).
  • R. Nave — HyperPhysics, Georgia State University, "Heat Transfer" section.
  • Further reading: Heat transfer — Wikipedia