theme 5 – the doppler shift astr 101 prof. dave hanes

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Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

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Page 1: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

Theme 5 – The Doppler Shift

ASTR 101Prof. Dave Hanes

Page 2: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

The Surfer’s Experience

Waves come in to shore perfectly regularly.

If you float in place, you bob up and down as each wave passes – say, once every 5 sec

If you paddle out towards the incoming waves, you meet each wave sooner than expected, so your frequency of bobbing up and down increases – perhaps once every 4 seconds

Page 3: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

Think of Sound

The ‘wavefronts’ reach your ear with a regular frequency.

But if you walk towards the speaker, successive waves hit your eardrum a little sooner than expected, so they arrive with a higher frequency than expected.

Your eardrum is set vibrating at a higher frequency than if you were at rest! The tone sounds higher in pitch than if you were at rest.

Page 4: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

Turn The Thinking Around

If the surfer now paddles towards the shore, the waves affect her with reduced frequency. (In the limit, she ‘rides a wave’ and experiences no up and down motion at all!)

If the listener walks away from the speaker, the sound waves arrive less frequently, producing a lower-pitched sound.

Moreover, it does not matter if the listener is moving and the speaker at rest, or vice versa. Relative motion is the key! If the distance between them is shrinking, the perceived frequency is increased; if it’s growing, the perceived frequency drops.

Page 5: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

The Doppler Effect in Words

Any periodic effect will be:

Perceived at higher frequency if the distance between the source and the receiver is decreasing

Perceived at reduced frequency if the distance between the source and the receiver is increasing

Page 6: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

A Direct Test: Sound

Doppler proposed a test: an open train car with trumpeters playing a note of constant pitch.

Other musicians with ‘perfect pitch’ stood beside the tracks to see if the note sounded ‘too high’ as the train approached.

This was successful!

http://www.planetseed.com/relatedarticle/doppler-effect-train

Page 7: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

Common Misunderstandings

If you know the expected pitch, and you hear a note that is “too high,” you know instantly that the source is approaching. You don’t need to hear it again later to see if anything changes. One hearing is enough!

The familiar up-and-down wailing of a siren is not the Doppler shift! (Is the source alternately coming towards you and moving away? No!) But here’s a link where we hear that wailing (produced by the siren itself) and then an overall drop in pitch as the fire engine passes by (so it is no longer approaching you but receding).

https://www.youtube.com/watch?v=imoxDcn2Sgo

Page 8: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

What is Light?

You are right: it’s a wave, the crests of which reach you with a certain frequency.

By Doppler’s reasoning, if you are moving towards a source of (say) red light, you should perceive a higher frequency – the light should look somewhat bluer.

And conversely: a receding source should look somewhat redder. (This is true whether it is you or the source that is ‘actually moving.’ Relative motion is the key.)

Page 9: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

A Losing Argument

You run a red light, but tell the traffic policeman that you perceived it as green because you were approaching it.

This would require you to be travelling at a considerable fraction of the speed of light! So you get charged with speeding instead.

Page 10: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

One Problem

Doppler first applied this reasoning to stars. Some binary stars have a red and a blue star side by side. He proposed that the colours might be due to their motions – the blue one approaching us, the red one moving away.

But the speed of light is so high, and the velocities of the stars so small, that only imperceptible colourchanges could ever arise. (As you now know, the difference is because of different stellar temperatures.)

Page 11: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

Apparently Hopeless As noted, the colours of stars are too little

affected by the Doppler shift to be noticeable, since their velocities though space are so small (perhaps a few hundred km/sec) compared to ‘c’ (300,000 km/sec).

Moreover, even if blue light in the spectrum were to be shifted to (say) green, previously invisible ultraviolet light will be shifted to blue, making up the loss.

All in all, you expect no pronounced effect, and indeed this is hopeless for determining velocities.

Page 12: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

Easy With Emission Lamps!Someone turns on an emission lamp. The spectrum might look like this (one blue, one green, one red line):

Suddenly, in a fit of rage, they hurl it at your head at very high speed. To you, the spectrum now looks like this:

Because you can identify several discrete lines, the shift towards the blue/violet end is actually noticeable! (even for modest velocities).

Page 13: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

Towardsand Away

Page 14: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

Same Principle for the Stars

Instead of looking at the overall colours of the stars, we look for displacements in the absorption lines. Measuring those displacements gives us the velocities of the stars relative to us.

Note that one measurement only is required to figure out the instantaneous velocity – there’s no need to “do it again later and look for changes.”

Note also that this does not tell you anything about the sideways motion of a star – only its motion along the line of sight (the so-called radial velocity).

Page 15: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

Applied Here First, we use an emission lamp at rest in the

observatory to tell us what colour / wavelength / frequency each line should be, then compare the star’s spectrum to that.

We don’t need to see the colours, by the way! We note that the absorption lines are shifted to the blue end (shorter wavelengths, higher frequencies.) This tells us that the star is approaching (or that we are moving towards it). And we can determine that velocity!

Page 16: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

Arcturus Remember that the radial velocity signifies only the relative motion – it could be the Earth or the star moving (or both).

Here’s the spectrum of Arcturus in June

And here it is in December

Page 17: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

Compare These in Detail

We see a change in the Doppler shift, implying a change in velocity from June to December. This behaviour repeats, year after year. Is Arcturus moving back-and-forth in our direction?

NO! In this case, we are noticing the back-and-forth motion of the Earth towards and away from Arcturus as we orbit the Sun. The Doppler shift told us about the relative motion.

Page 18: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

Radar Guns and Sunlight

In the Solar System, we can use the Doppler effect as well, in one of two ways:

Like a policeman, send out actual radar signals. This is a radio wave of a fixed frequency that gets shifted to a higher or lower frequency if the object off of which it reflects is moving towards or away from us

Use the Sun as a source (a ‘radar gun’)! When its light reflects from an object, we see a Doppler shift in the absorption lines in the solar spectrum depending on how the object is moving.

Page 19: Theme 5 – The Doppler Shift ASTR 101 Prof. Dave Hanes

Applied to Saturn’s RingsLook at the sunlight reflected from various parts of Saturn.

The planet itself rotates as a whole, with the outer edges moving fast (one towards us, the other away)

The rings are different. The inner edge of the ring moves faster than the outer edge! This would not be possible if it were solid, like a frisbee. The rings are evidently made of small lumps, like millions of tiny moons in parallel orbits.