An astronomical telescope in normal adjustment has objective focal length and eyepiece focal length . Calculate the magnitude of its angular magnification.
Astrophysics (A-level only)
Notes and three levels of exam-style practice for each registered specification leaf in this section.
Open the printable packAstronomical telescope consisting of two converging lenses
- In normal adjustment the objective forms a real intermediate image at the eyepiece focal plane, so the final image is virtual and at infinity; the lens separation is .
- The magnitude of the angular magnification is .
- A ray diagram should show parallel incident rays, an inverted intermediate image, and parallel emergent rays; mark both principal foci and use ruled rays.
- Keep and in the same units. A common error is to use image-height magnification or to subtract the focal lengths in normal adjustment.
Tier 1 · Easy
Tier 2 · Standard
A distant crater subtends at the unaided eye. It is viewed through a normal-adjustment telescope with and . Determine the angle subtended at the eye and the lens separation.
Tier 3 · Hard
A telescope is to make an object that subtends appear to subtend at least . The objective focal length is . Determine the greatest acceptable eyepiece focal length and the corresponding maximum telescope length in normal adjustment.
Reflecting telescopes
- A Cassegrain telescope uses a parabolic concave primary mirror and a convex secondary mirror; the secondary returns converging rays through a central hole in the primary to the eyepiece.
- Reflection is independent of wavelength, so mirrors do not produce chromatic aberration. A spherical mirror can produce spherical aberration, whereas an on-axis parabolic primary brings parallel rays to one focus.
- A large mirror can be supported from behind and can be made thinner than a comparable objective lens, so large-aperture reflectors are more practical than refractors.
- In a ray diagram, show the primary and secondary reflections before the eyepiece. Do not draw rays passing through the secondary as if it were a lens.
Tier 1 · Easy
State one aberration that a reflecting telescope avoids because its primary element is a mirror rather than a lens.
Tier 2 · Standard
Describe the path of initially parallel rays through a Cassegrain reflecting telescope up to the eyepiece.
Tier 3 · Hard
A research group must choose between a large refracting telescope and a Cassegrain reflector of the same aperture. Discuss why the reflector is usually preferred, including aberrations and construction.
Single dish radio telescopes, I-R, U-V and X-ray telescopes
- A single-dish radio telescope uses a concave reflecting surface to direct radio waves to a receiver near the focus; as with an optical telescope, collecting power grows as , so a large dish gathers more of a weak signal.
- Because radio wavelengths are much longer than visible wavelengths, a radio dish needs a much larger diameter for comparable angular resolution through .
- Infrared observatories favour high, dry sites and cooled detectors; most ultraviolet and X-ray astronomy must be carried out above the atmosphere because those bands are strongly absorbed.
- Radio observations can be made from the ground and through cloud, but human-made radio interference matters. Do not claim that every non-visible telescope can operate at sea level or uses a glass lens.
Tier 1 · Easy
State why most X-ray telescopes used for astronomy are placed on satellites.
Tier 2 · Standard
An optical telescope of diameter observes at . Estimate the diameter of a radio dish observing at that would have the same Rayleigh angular resolution.
Tier 3 · Hard
Discuss suitable observing locations for radio, infrared, ultraviolet and X-ray astronomy, and explain why a radio dish generally has a much larger diameter than an optical telescope.
Advantages of large diameter telescopes
- The Rayleigh criterion gives the minimum resolvable angle in radians, so increasing diameter improves angular resolution at fixed wavelength.
- Collecting power is proportional to ; a larger aperture gathers more energy per unit time and makes faint sources easier to detect.
- A CCD generally has higher quantum efficiency than the eye, can integrate and store an exposure, and gives a permanent electronic record; small CCD pixels can improve detector resolution, although the aperture still sets the diffraction limit.
- State ratios carefully: doubling halves the diffraction-limited angle but multiplies collecting power by four. Do not claim that collecting power is proportional to .
Tier 1 · Easy
A telescope aperture is increased from to . Determine the factor by which its collecting power increases.
Tier 2 · Standard
Calculate the Rayleigh minimum angular resolution of a telescope at wavelength . State the effect of increasing the diameter.
Tier 3 · Hard
Two telescopes have diameters and and observe at . A pair of faint stars is separated by . Determine which telescope can resolve the pair, compare their collecting powers, and explain one advantage of recording with a CCD rather than the eye.
Classification by luminosity
- Apparent magnitude is the brightness scale of Hipparchus as seen from Earth; smaller and more negative magnitudes mean brighter objects.
- A difference of one magnitude corresponds to an intensity ratio of , so a difference corresponds to in the opposite brightness direction.
- Under dark conditions the dimmest stars visible to the unaided eye have apparent magnitude about .
- Brightness on this scale is subjective and logarithmic. A common error is to say that a magnitude- star is brighter than a magnitude- star because .
Tier 1 · Easy
Two stars have apparent magnitudes and . State which appears brighter.
Tier 2 · Standard
Star P has apparent magnitude and star Q has apparent magnitude . Calculate the ratio .
Tier 3 · Hard
Interstellar dust reduces the received intensity from a star by a factor of . Before the dimming, its apparent magnitude was . Determine its new apparent magnitude and whether it should remain visible to the unaided eye under dark conditions.
Absolute magnitude, M
- Absolute magnitude is the apparent magnitude a star would have at a distance of , so it compares intrinsic luminosities on the magnitude scale.
- For distance in parsecs, . Rearrange before substituting and use base-10 logarithms.
- One parsec is about light years. A parsec is a distance, not a time, and the distance-modulus equation does not take in metres.
- A more negative means a greater intrinsic luminosity. Do not infer intrinsic power from alone because distance also affects apparent brightness.
Tier 1 · Easy
A star is exactly from Earth and has apparent magnitude . State its absolute magnitude.
Tier 2 · Standard
A star has apparent magnitude and absolute magnitude . Calculate its distance from Earth in parsecs.
Tier 3 · Hard
A supergiant has apparent magnitude and absolute magnitude . Determine its distance in parsecs and in light years. Use .
Classification by temperature, black-body radiation
- Treating a star as a black body, Wien's law estimates its surface temperature from the peak wavelength.
- Stefan's law is ; for a spherical star , so comparisons use .
- For isotropic radiation with negligible absorption, the received intensity follows . State these assumptions when applying the inverse-square law.
- A hotter black-body curve peaks at a shorter wavelength and has greater area. Convert nanometres to metres and use kelvin, not degrees Celsius.
Tier 1 · Easy
The black-body spectrum of a star peaks at . Estimate its surface temperature using Wien's law.
Tier 2 · Standard
Star B has twice the radius of star A but times its surface temperature. Using Stefan's law, calculate .
Tier 3 · Hard
A star away produces an intensity of at Earth and has peak wavelength . Assuming isotropic emission and black-body behaviour, determine its surface temperature and radius. Use and .
Principles of the use of stellar spectral classes
- The sequence OBAFGKM runs from hottest to coolest; intrinsic colours are O/B blue, A blue-white, F white, G yellow-white, K orange and M red.
- Temperature ranges are O -, B -, A -, F -, G -, K - and M below .
- Prominent absorption features progress from , He and H in O stars; He and H in B; strongest H plus ionised metals in A; ionised metals in F; ionised and neutral metals in G; neutral metals in K; and neutral atoms plus TiO in M.
- Hydrogen Balmer absorption requires hydrogen atoms in the state and is strongest in class A: cooler stars have too few excited atoms, while hotter stars have much of their hydrogen ionised.
- Line strength does not directly measure elemental abundance. Do not conclude that a weak Balmer line means that the star contains little hydrogen.
Tier 1 · Easy
Three stars have spectral classes B, G and M. State which has the highest surface temperature.
Tier 2 · Standard
A star's continuous spectrum peaks at . Estimate its temperature and hence identify its most likely spectral class. Use Wien's constant .
Tier 3 · Hard
Explain why hydrogen Balmer absorption lines can be weak in both a very hot class O star and a cool class M star but strongest in a class A star.
The Hertzsprung-Russell (HR) diagram
- An HR diagram plots absolute magnitude vertically, usually from about at the top to at the bottom, against temperature decreasing left to right from about to or classes OBAFGKM.
- The main sequence runs from hot, luminous upper-left stars to cool, faint lower-right stars; giants lie mainly upper right and white dwarfs lower left.
- The Sun is a class G main-sequence star with surface temperature about and absolute magnitude about .
- A Sun-like star moves from formation to the main sequence, then to the red-giant region and finally to the white-dwarf region. Do not reverse the temperature axis or put white dwarfs among cool faint stars.
Tier 1 · Easy
State the region of an HR diagram occupied by the Sun and give its approximate spectral class.
Tier 2 · Standard
A star has surface temperature and absolute magnitude . Deduce its region on an HR diagram and justify your answer.
Tier 3 · Hard
Describe the path of a star with a mass similar to the Sun on an HR diagram from formation until its white-dwarf stage. Refer to changes in temperature and absolute magnitude where appropriate.
Supernovae, neutron stars and black holes
- A typical type Ia supernova light curve rises steeply to about to and then declines more slowly; this standardisable peak makes type Ia supernovae useful standard candles.
- Neutron stars are extremely dense compact remnants composed mainly of neutrons. Collapse of a supergiant to a neutron star or black hole can produce a gamma-ray burst with enormous energy output.
- For a black hole the escape velocity exceeds inside the event horizon; its Schwarzschild radius is . Supermassive black holes occur at galactic centres.
- Type Ia distances helped reveal an accelerating Universe and motivate dark energy. Keep the observation separate from the interpretation, and do not describe absolute magnitude as a physical power unit.
Tier 1 · Easy
A newly identified black hole has mass . Determine its event-horizon radius using and .
Tier 2 · Standard
A type Ia supernova has absolute magnitude and peak apparent magnitude . Use the distance modulus to estimate its distance in parsecs.
Tier 3 · Hard
The collapse of a supergiant produces a gamma-ray burst of energy and leaves a compact object of mass . Calculate the object's Schwarzschild radius and the time for the Sun, at constant power , to emit the burst energy. Give the time in years and use , and .
Doppler effect
- For speeds much smaller than , the fractional wavelength shift is in magnitude; a positive redshift means recession when is taken as the recession speed.
- For frequency, with the same recession-positive convention, so a receding source has a lower observed frequency.
- In an edge-on binary system, each star's spectral lines shift periodically between red and blue as its radial velocity reverses; the shift is zero when its motion is transverse to the line of sight.
- Use the unshifted laboratory wavelength or frequency in the denominator and check that . Do not use the non-relativistic approximation for a large redshift without qualification.
Tier 1 · Easy
A spectral line of laboratory wavelength is observed at . Calculate the redshift .
Tier 2 · Standard
Radiation emitted at is received from a gas cloud at . Determine the cloud's radial speed and state whether it is approaching or receding. Use .
Tier 3 · Hard
In an equal-mass binary system viewed in the plane of its circular orbit, a line of rest wavelength alternates between and for one star. The orbital period is . Estimate the speed of that star, its orbital radius about the centre of mass, and the separation of the stars. Use .
Hubble's law
- Hubble's law is : on large scales, a galaxy's recession speed is proportional to its distance, which is interpreted as expansion of the Universe.
- If has remained constant, the age estimate is . Convert into before taking the reciprocal.
- The Big Bang model is supported by all-sky microwave background radiation, interpreted as relic radiation redshifted and cooled by expansion, and by the roughly hydrogen-to-helium mass ratio produced by early fusion before the Universe cooled.
- Nearby peculiar velocities can obscure the Hubble trend, and the constant- age is an estimate rather than an exact history. Keep distance units consistent with those used for .
Tier 1 · Easy
Use to calculate the recession speed of a galaxy away.
Tier 2 · Standard
Estimate the age of the Universe for . Assume is constant and use and .
Tier 3 · Hard
A galaxy's hydrogen line has laboratory wavelength and is observed at . Use the non-relativistic Doppler approximation and to estimate the galaxy's distance. Check whether , taking .
Quasars
- Quasars were discovered as bright radio sources and have very large optical redshifts, placing them among the most distant measurable objects.
- Their enormous power output is produced by matter accreting onto an active supermassive black hole, not by an unusually luminous ordinary star.
- For modest redshift, use and ; if the received flux is and emission is isotropic, estimate power with .
- State the isotropic-emission and low-redshift assumptions. A common error is to compare flux at Earth directly with luminosity without allowing for inverse-square spreading.
Tier 1 · Easy
State the central engine believed to power a quasar.
Tier 2 · Standard
A quasar at distance produces a flux of at Earth. Estimate its power output assuming isotropic emission. Use .
Tier 3 · Hard
A low-redshift quasar has and measured flux . Estimate its distance, power output and power in units of the Sun's luminosity. Use , , and . Assume isotropic emission.
Detection of exoplanets
- Direct detection is difficult because a planet is faint compared with its host star and has a very small angular separation from it.
- The radial-velocity method detects periodic red and blue Doppler shifts in the star's spectral lines as the star orbits the system's centre of mass.
- The transit method detects a repeated decrease in stellar brightness when an aligned planet crosses the stellar disc; approximately, transit depth .
- A transit light curve has a steady baseline, a fall, a nearly flat or curved minimum, and a rise, repeated once per orbit. Transits require favourable alignment, while radial velocity measures only line-of-sight motion.
Tier 1 · Easy
A star's brightness shows equal, regularly repeated dips. Name the exoplanet-detection method indicated by this observation.
Tier 2 · Standard
During a transit, a star's detected intensity falls by . Estimate the radius of the planet if the star's radius is .
Tier 3 · Hard
A star has radius . Every its intensity falls by , while a absorption line shifts with the same period by up to to either side of its mean. Calculate the planet's radius and the star's maximum radial speed, then explain why the combined observations are stronger evidence for an exoplanet than either observation alone. Use .