Kit Library / Science / Thermodynamics & Modern Physics

⚡ Topic Learning Kit

Thermal Physics

English 15 leveled MCQs 17 flashcards 6 games Free

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💡 Key Idea

The Perfect Absorber

Black bodies absorb everything.

A black body is an idealized object that absorbs all incident electromagnetic radiation, regardless of frequency or angle of incidence. It reflects nothing.

↳ A black body is a perfect absorber, not necessarily black in color.

📖 Definition

Cavity Radiator Model

A hole in a box.

The best practical approximation of a black body is a cavity radiator: a hollow metal box with a tiny hole. Radiation entering the hole undergoes multiple reflections and is almost completely absorbed.

↳ A small hole in a cavity acts as a near-perfect black body.

⭐ Important Fact

Kirchhoff's Law

Good absorbers are good emitters.

Kirchhoff's law of thermal radiation states that at thermal equilibrium, the emissivity of a body equals its absorptivity at a given wavelength and temperature: $e_\lambda = a_\lambda$.

↳ A perfect absorber is also a perfect emitter.

➗ Formula

Stefan-Boltzmann Law

Power scales with T to the fourth.

This law gives the total power radiated across all wavelengths. Doubling temperature increases radiated power by $2^4 = 16$ times.

↳ Total radiated power is proportional to the fourth power of absolute temperature.

➗ Formula

Wien's Displacement Law

Hotter bodies glow bluer.

As temperature increases, the peak wavelength shifts to shorter wavelengths (higher frequencies). This explains why heated objects first glow red, then yellow, then white.

↳ Peak wavelength is inversely proportional to temperature.

⚖️ Comparison

Black Body vs Real Body

Ideal vs actual emitters.

↳ Real bodies are grey or selective emitters, never perfect black bodies.

✏️ Example

Sun as a Black Body

Our star approximates a black body.

The Sun's spectrum closely resembles a black body curve at about 5800 K. Its peak wavelength is in the visible range (green-blue), which is why our eyes evolved to see this region.

↳ The Sun is a near-perfect black body at 5800 K.

🌍 Real World

Earth's Energy Balance

Our planet radiates infrared.

Earth absorbs solar radiation (mostly visible) and re-emits it as infrared radiation (around 255 K). This balance determines our climate.

↳ Black body radiation governs planetary temperatures.

⚠️ Common Mistake

Black Body Isn't Always Black

Color is misleading.

A black-painted surface is a good absorber in visible light but may not be a perfect black body across all wavelengths.

↳ Black body means perfect absorber, not visually black.

⚙️ Process

Spectral Distribution

Intensity vs wavelength curves.

↳ The black body spectrum is a universal curve shape that shifts with temperature.

🛠️ Application

Pyrometry

Measuring temperature remotely.

Optical pyrometers measure the radiation from a hot object to determine its temperature without contact. Used in furnaces, molten metals, and stars.

↳ Non-contact temperature measurement uses black body radiation.

❓ Did You Know

Cosmic Microwave Background

The universe is a black body.

The Cosmic Microwave Background (CMB) radiation is the most perfect black body spectrum ever observed, at a temperature of 2.725 K. It is remnant radiation from the early universe.

↳ The CMB is the best natural black body spectrum known.

🎯 Exam Tip

Remember the Constants

Don't mix up b and σ.

↳ Memorize b and σ with their units.

Smart notes

What you'll study, topic by topic

1

Black Body Radiation

8 min

Black body radiation is the electromagnetic radiation emitted by an idealized perfect absorber and emitter in thermal equilibrium. Its spectrum depends only on temperature, described by Stefan-Boltzmann law (total power)…

  • A black body is a perfect absorber and emitter of radiation.
  • Kirchhoff's law: emissivity equals absorptivity at thermal equilibrium.
  • Stefan-Boltzmann law: total radiated power $E = \sigma T^4$.

Full explanation, worked examples & memory tricks in the app

Leveled MCQ practice

Try the smart MCQs from this kit

All 15 questions, laddered from warm-up to topper-level, each with its answer and the reasoning behind it.

Warm-up · 5 questions

Q1. What is a black body?

Beginner
A An object that absorbs all incident radiation and emits it perfectly
B An object that reflects all incident radiation
C An object that transmits all incident radiation
D An object that only emits radiation at high temperatures
Show the answer

A · An object that absorbs all incident radiation and emits it perfectly

A black body is an idealized object that absorbs all incident electromagnetic radiation and emits radiation perfectly at all wavelengths.

Q2. Which of the following is a real-world approximation of a black body?

Beginner
A A glass window
B A mirror
C A small hole in a cavity
D A white wall
Show the answer

C · A small hole in a cavity

A small hole in a cavity acts as a near-perfect black body because any radiation entering is absorbed after multiple reflections.

Q3. Which scientist proposed that energy is emitted or absorbed in discrete quanta to explain black body radiation?

Beginner
A Niels Bohr
B Albert Einstein
C Isaac Newton
D Max Planck
Show the answer

D · Max Planck

Max Planck introduced the quantum hypothesis in 1900 to explain the black body spectrum.

Q4. A black body emits radiation only at a single wavelength.

Beginner
A True
B False
Show the answer

B · False

A black body emits a continuous spectrum of radiation across all wavelengths, with a peak that depends on temperature.

Q5. The total energy radiated by a black body is proportional to the fourth power of its absolute temperature.

Beginner
A True
B False
Show the answer

A · True

This is the Stefan-Boltzmann law: $E = \sigma T^4$.

Building up · 10 questions

Q6. Which law describes how the wavelength of peak emission from a black body shifts with temperature?

Intermediate
A Stefan-Boltzmann law
B Planck's law
C Wien's displacement law
D Kirchhoff's law
Show the answer

C · Wien's displacement law

Wien's displacement law states that the peak wavelength is inversely proportional to temperature: $\lambda_{\text{max}} T = b$.

Q7. According to the Stefan-Boltzmann law, the total power radiated per unit area of a black body is proportional to:

Intermediate
A $T^4$
B $T^3$
C $T$
D $T^2$
Show the answer

A · $T^4$

The Stefan-Boltzmann law states that the power radiated per unit area is $P = \sigma T^4$, where $\sigma$ is the Stefan-Boltzmann constant.

Q8. What does Planck's radiation law describe?

Intermediate
A The spectral energy density of black body radiation
B The total energy radiated by a black body
C The absorption spectrum of a black body
D The shift in wavelength due to motion
Show the answer

A · The spectral energy density of black body radiation

Planck's law gives the spectral radiance of a black body as a function of wavelength and temperature, resolving the ultraviolet catastrophe.

Q9. The ultraviolet catastrophe refers to:

Intermediate
A The failure of classical physics to explain the black body spectrum at short wavelengths
B The absorption of ultraviolet light by the atmosphere
C The excessive emission of ultraviolet light by black bodies
D The rapid cooling of black bodies due to UV emission
Show the answer

A · The failure of classical physics to explain the black body spectrum at short wavelengths

Classical Rayleigh-Jeans law predicted infinite energy at short wavelengths, which was resolved by Planck's quantum hypothesis.

Q10. What is the value of Wien's displacement constant $b$ approximately?

Intermediate
A $3.00 \times 10^8 \, \text{m/s}$
B $6.626 \times 10^{-34} \, \text{J·s}$
C $5.67 \times 10^{-8} \, \text{W·m}^{-2}\text{K}^{-4}$
D $2.898 \times 10^{-3} \, \text{m·K}$
Show the answer

D · $2.898 \times 10^{-3} \, \text{m·K}$

Wien's displacement constant $b$ is approximately $2.898 \times 10^{-3} \, \text{m·K}$.

Q11. If the temperature of a black body is doubled, the total radiated power per unit area increases by a factor of:

Intermediate
A 4
B 16
C 2
D 8
Show the answer

B · 16

Since $P \propto T^4$, doubling $T$ gives $2^4 = 16$ times the power.

Q12. The emissive power of a black body depends on:

Intermediate
A Its surface area only
B Its material only
C Its color only
D Its temperature only
Show the answer

D · Its temperature only

For a black body, emissive power depends solely on temperature, as described by Planck's law and Stefan-Boltzmann law.

Q13. What is the shape of the black body radiation spectrum at a given temperature?

Intermediate
A A constant value across all wavelengths
B A straight line
C A curve with a single peak
D A curve with multiple peaks
Show the answer

C · A curve with a single peak

The spectrum is a continuous curve that rises to a peak at a certain wavelength and then falls off, with the peak shifting with temperature.

Q14. Which law states that the ratio of emissive power to absorptive power is constant for all bodies at the same temperature?

Intermediate
A Kirchhoff's law
B Wien's law
C Planck's law
D Stefan-Boltzmann law
Show the answer

A · Kirchhoff's law

Kirchhoff's law of thermal radiation states that good absorbers are good emitters, and the ratio is the same for all bodies at a given temperature.

Q15. The Sun's spectrum approximates that of a black body at about 5800 K. What is the peak wavelength of its radiation?

Intermediate
A 2000 nm
B 250 nm
C 500 nm
D 1000 nm
Show the answer

C · 500 nm

Using Wien's law: $\lambda_{\text{max}} = b/T = (2.898 \times 10^{-3})/5800 \approx 5 \times 10^{-7} \, \text{m} = 500 \, \text{nm}$.

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