Production of X-rays (AQA A Level Physics): Revision Note

Exam code: 7408

Katie M

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Production of X-rays

  • When the fast-moving electrons collide with the target, X-rays are produced by one of two methods:

    • Method 1: Bremsstrahlung

    • Method 2: Characteristic Radiation

Method 1: Bremsstrahlung

  • When high-speed electrons collide with a metal target (often tungsten), they undergo a steep deceleration

    • When a charged particle decelerates quickly, some of the energy released is converted into a photon

  • A small amount of the kinetic energy (~ 1%) from the incoming electrons is converted into X-rays as the electrons decelerate in the tungsten, due to conservation of energy 

    • The rest of the energy heats up the anode, which usually requires some form of cooling

  • The energy of the X-ray photon can be of any value, up to the original kinetic energy of the electron, giving a range of possible X-ray energies

    • These X-rays cause the continuous or ‘smooth hump shaped’ line on an intensity wavelength graph

Ranges of wavelengths in Bremsstrahlung radiation

Graph of relative intensity against wavelength shows smooth curves for 20, 30, 40 and 50 kilovolts. Higher voltage increases intensity and reduces the minimum wavelength. An electron is decelerated by a nucleus, emitting an X-ray photon.
The continuous spectra of Bremsstrahlung radiation at different acceleration potentials. As wavelength decreases, the energy of the X-ray photons increases
  • When an electron is accelerated, it gains energy equal to the product of its charge and the accelerating potential, V

  • This energy can be calculated using:

Emax = eV

  • This is the maximum energy that an X-ray photon can have

  • The smallest possible wavelength is equivalent to the highest possible frequency and therefore, the highest possible energy

    • This is assuming all of the electron’s kinetic energy has turned into electromagnetic energy

  • Therefore, the maximum X-ray frequency fmax, or the minimum wavelength λmin, that can be produced is calculated using the equation:

Emax = eV = hfmax = hcλmin

  • The maximum X-ray frequency, fmax, is therefore equal to:

fmax = eVh

  • The minimum X-ray wavelength, λmin, is therefore equal to:

λmin = hceV

  • Where:

    • e = elementary charge (C)

    • V = potential difference between the anode and cathode (V)

    • h = Planck's constant (J s)

    • c = the speed of light (m s−1)

Method 2: Characteristic radiation

  • Some of the incoming fast electrons cause inner shell electrons of the tungsten to be ‘knocked out’ of the atom, leaving a vacancy

    • This vacancy is filled by an outer electron moving down and releasing an X-ray photon as it does (equal in energy to the difference between the two energy levels)

    • Because these X-rays are caused by energy level transitions, they have only specific discrete energies

    • They cause sharp spikes on an intensity wavelength graph

    • The number of spikes depends on the element used for the target - there are two sets of spikes for a tungsten target, representing two sets of possible energy transitions

Characteristic discrete X-Ray wavelengths

A graph of relative intensity against X-ray energy has sharp peaks at 17 and 19.5 keV. An incoming electron creates a vacancy. Electrons move down energy levels, emitting photons with discrete energies.
Electron transitions emit photons with discrete energies. An incoming electron can cause these transitions, making tungsten emit characteristic photons

Combined X-Ray spectra of Bremsstrahlung and characteristic photons

Combined X-ray spectrum graph of relative intensity against photon energy, showing smooth Bremsstrahlung curves and sharp characteristic X-ray peaks.
A real X-ray spectrum combines the continuous Bremsstrahlung curve with the sharp peaks of characteristic radiation

Worked Example

X-rays are a type of electromagnetic wave with wavelengths in the range 10−8 to 10−13 m

If the accelerating potential difference in an X-ray tube is 60 kV, determine if the photons emitted fall within this range.

[3]

Answer:

Step 1: Write out known quantities

  • Charge on an electron, e = 1.6 × 10−19 C

  • Accelerating potential difference, V = 60 000 V

  • Planck’s constant, h = 6.63 × 10−34 J s

  • Speed of light, c = 3 × 108 m s−1

Step 2: Determine the maximum possible energy of a photon

  • The maximum possible energy of a photon corresponds to the maximum energy an electron could have:

Emax = eV

Step 3: Determine an expression for minimum wavelength

Planck relation: E = hf

Wave equation: c = fλ

  • When energy is a maximum:

Emax = eV = hfmax

  • Maximum energy corresponds to a minimum wavelength:

eV = hcλmin

  • Rearrange for minimum wavelength, λmin:

λmin = hceV

Step 4: Calculate the minimum wavelength λmin

λmin = (6.63 × 10−34)(3 × 108)(1.6 × 10−19)(60 000) [1 mark]

λmin = 2.1 × 10−11 m [1 mark]

Step 5: Comment on whether this is within the range for the wavelength of an X-ray 

  • X-ray wavelengths are within 10−8 to 10−13 m

  • The minimum wavelength for a 60 kV supply is 2.1 × 10−11 m, which means the photons produced will be X-rays [1 mark]

Worked Example

A typical spectrum of the X-ray radiation produced by electron bombardment of a metal target is shown below.

Graph of X-ray intensity against wavelength, showing a continuous spectrum that rises from a short-wavelength cut-off, peaks, then falls, with several sharp characteristic-radiation peaks superimposed.

Explain why:

(a) A continuous spectrum of wavelengths is produced. [2]

(b) The gradient is steeper at shorter wavelengths. [2]

(c) The spectrum has a sharp cut-off at short wavelengths. [2]

 Answer:

Part (a)

Step 1: Consider the path of the electrons from the cathode to the anode

  • Photons are produced whenever a charged particle undergoes a large acceleration or deceleration

  • X-ray tubes fire high-speed electrons at a metal target

  • When an electron collides with the metal target, it loses energy in the form of an X-ray photon as it decelerates [1 mark]

Step 2: Consider the relationship between the energy of the electron and the wavelength of the photon

  • The wavelength of a photon depends on the energy transferred by a decelerating electron

  • The electrons don't all undergo the same deceleration when they strike the target

  • This leads to a distribution of energies, hence, a range, or continuous spectrum, of wavelengths is observed [1 mark]

Part (b)

Step 1: Identify the significance of the intensity 

  • The intensity of the graph signifies the proportion of photons produced with a specific energy, or wavelength

  • The higher the intensity, the more photons of a particular wavelength are produced

  • In other words, the total intensity is the sum of all the photons with a particular wavelength [1 mark]

Step 2: Explain the shape of the graph

  • When a single electron collides with the metal target, a single photon is produced

  • Most electrons only give up part of their energy, and hence there are more X-rays produced at wavelengths higher than the minimum (or energies lower than the maximum)

  • At short wavelengths, there is a steeper gradient because only a few electrons transfer all, or most of, their energy [1 mark]

Part (c)

Step 1: Identify the relationship between minimum wavelength and maximum energy

  • The minimum wavelength of an X-ray is equal to

λmin = hcEmax

  • The equation shows the maximum energy of the electron corresponds to the minimum wavelength, they are inversely proportional 

λmin ∝ 1Emax

  • Therefore, the higher the energy of the electron, the shorter the wavelength of the X-ray produced [1 mark]

Step 2: Explain the presence of the cut-off point

  • The accelerating voltage determines the kinetic energy which the electrons have before striking the target

  • The value of this accelerating voltage, therefore, determines the value of the maximum energy

  • This corresponds to the minimum, or cut-off, wavelength [1 mark]

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Katie M

Author: Katie M

Expertise: Curriculum Expert

Katie has always been passionate about the sciences, and completed a degree in Astrophysics at Sheffield University. She decided that she wanted to inspire other young people, so moved to Bristol to complete a PGCE in Secondary Science. She particularly loves creating fun and absorbing materials to help students achieve their exam potential.

Tim

Reviewer: Tim

Expertise: Content Creator

Timothy graduated with a first class degree in Mathematics and Physics from the University of Warwick. After working as a postgraduate researcher, Timothy has worked as a content creator for various online revision platforms, creating physics resources for a range of levels and exam boards.