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28.4 Relativistic Addition of Velocities

28.4 Relativistic Addition of Velocities

  • The signal is different when the particle goes through a coil.
  • A particle is traveling through the Earth's atmosphere.
    • It travels 2.50 km to an Earth-bound observer.
  • The total velocity of a kayak, like this one on the Deerfield River in Massachusetts, is its speed relative to the water as well as the water's speed relative to the riverbank.
    • The kayak is being pulled by the river current.
    • Pushing the oars against the water can move the kayak forward in the water, but it only accounts for part of the speed.
    • Classical addition of velocities can be seen in the kayak's motion.
    • In classical physics, the velocities add up.
    • The kayak's velocity is the sum of the water's and the riverbank's velocities.
  • We only consider velocity addition to one-dimensional motion.
    • In one-dimensional motion, velocities add like regular numbers.
    • A girl is riding a sled at a speed of 1.0 m/s relative to an observer.
    • She throws a snowball at a speed of 1.5 m/s relative to the sled.
    • In this example, forward is positive and direction is plus and minus signs.
    • The velocities of the sled relative to the Earth, the snowball relative to the observer, and the snowball relative to the sled should be considered.
  • In one-dimensional motion, velocities add like ordinary numbers.
    • The girl throws a snowball from a sled.
    • The sled's speed is relative to the Earth.
    • The snowball's speed relative to the sled is, while its speed relative to the Earth is.
  • The girl throws the snowball.
    • The snowball will head towards the observer faster because it is thrown from a moving vehicle.
    • The girl throws the snowball backwards.
    • The snowball moves away from the observer.
  • Classical velocity addition does not apply to light according to the second postulate of relativity.
    • If classical velocity addition was applied to light, the light from the car's headlights would approach the observer on the sidewalk at a speed.
    • Light will move away from the car at speed relative to the driver of the car, and light will move towards the observer on the sidewalk at the same time.
  • Light from the car's headlights moves away from the car at speed and towards the observer on the sidewalk.
    • Classical velocity addition is not valid.
  • Light is an exception, or the classical velocity addition formula only works at low speeds.
    • The latter is true.
  • The velocity of an object relative to one observer is what is known as the relative velocity.
    • The term becomes very small at low velocities, and gives a result very close to classical velocity addition.
    • Classical velocity addition is an excellent approximation to the correct formula for small velocities.
    • It seems correct to us in our experience.
  • A spaceship heading towards the Earth at half the speed of light emits a beam of light.
    • Determine the speed at which the light leaves the ship and approaches the Earth from there.
  • Simple velocity addition is not possible because the light and spaceship are moving at very fast speeds.
    • We can use the speed at which the light approaches the Earth to determine the light's speed.
  • The knowns should be identified.
  • The appropriate equation can be chosen.
  • The knowns should be plugged into the equation.
  • The correct result is given by extrapolation velocity addition.
    • Light leaves the ship and approaches the Earth.
    • The relative motion of source and observer does not affect the speed of light.
  • If the speed of light is less than and does not exceed, velocities cannot add to it.
    • The following example shows the difference between classical and relativistic velocity addition.
  • The spaceship in the previous example is approaching the Earth at half the speed of light and shooting a canister.
  • We need to determine the speed of the canister by an Earth-bound observer using a different method than simple velocity addition.
  • The knowns should be identified.
  • The appropriate equation can be chosen.
  • The knowns should be plugged into the equation.
  • The knowns should be identified.
  • The appropriate equation can be chosen.
  • The knowns should be plugged into the equation.
  • The canister is heading towards the Earth in part and away in part, as expected, because of the minus sign.
    • Residual velocities do not add as much as they do classically.
    • The canister does approach the Earth faster, but not at the simple sum.
    • The total velocity is not as high as it could be.
    • The canister moves away from the Earth at a faster pace than you would expect.
    • The velocities are not symmetrical.
    • The canister moves faster than the ship relative to the Earth, but slower than the ship.
  • The frequencies and wavelength of light do not change with relative velocity.
    • When there is relative motion between source and observer, a Doppler shift occurs.
  • When the source moves away from the observer, the red shift is longer than the blue shift, which is when the source moves towards the observer.
  • The observed wavelength, the source wavelength, and the relative velocity of the source to the observer are all part of the equation.
    • Positive for motion away from an observer and negative for motion toward an observer.
  • The - and + signs are different from the wavelength equation.
  • If you're interested in a career that requires a knowledge of special relativity, astronomy is probably the best place to start.
    • Calculating distances, times, and speeds of black holes, galaxies, quasars, and all other astronomy objects must take into account relativistic effects.
    • If you want to work in astronomy, you need at least an undergraduate degree in either physics or astronomy, but a Master's or doctorate degree is often required.
    • A good background in high-level mathematics is required.
  • A universe is moving away from the Earth at a fast pace.
    • It emits radio waves.
  • The classical Doppler shift can't be used because the galaxy is moving at a relativistic speed.
  • The knowns should be identified.
  • The appropriate equation can be chosen.
  • The knowns should be plugged into the equation.
  • The wavelength of radiation the galaxy emits is expected to be redshifted because it is moving away from the Earth.

28.4 Relativistic Addition of Velocities

  • The signal is different when the particle goes through a coil.
  • A particle is traveling through the Earth's atmosphere.
    • It travels 2.50 km to an Earth-bound observer.
  • The total velocity of a kayak, like this one on the Deerfield River in Massachusetts, is its speed relative to the water as well as the water's speed relative to the riverbank.
    • The kayak is being pulled by the river current.
    • Pushing the oars against the water can move the kayak forward in the water, but it only accounts for part of the speed.
    • Classical addition of velocities can be seen in the kayak's motion.
    • In classical physics, the velocities add up.
    • The kayak's velocity is the sum of the water's and the riverbank's velocities.
  • We only consider velocity addition to one-dimensional motion.
    • In one-dimensional motion, velocities add like regular numbers.
    • A girl is riding a sled at a speed of 1.0 m/s relative to an observer.
    • She throws a snowball at a speed of 1.5 m/s relative to the sled.
    • In this example, forward is positive and direction is plus and minus signs.
    • The velocities of the sled relative to the Earth, the snowball relative to the observer, and the snowball relative to the sled should be considered.
  • In one-dimensional motion, velocities add like ordinary numbers.
    • The girl throws a snowball from a sled.
    • The sled's speed is relative to the Earth.
    • The snowball's speed relative to the sled is, while its speed relative to the Earth is.
  • The girl throws the snowball.
    • The snowball will head towards the observer faster because it is thrown from a moving vehicle.
    • The girl throws the snowball backwards.
    • The snowball moves away from the observer.
  • Classical velocity addition does not apply to light according to the second postulate of relativity.
    • If classical velocity addition was applied to light, the light from the car's headlights would approach the observer on the sidewalk at a speed.
    • Light will move away from the car at speed relative to the driver of the car, and light will move towards the observer on the sidewalk at the same time.
  • Light from the car's headlights moves away from the car at speed and towards the observer on the sidewalk.
    • Classical velocity addition is not valid.
  • Light is an exception, or the classical velocity addition formula only works at low speeds.
    • The latter is true.
  • The velocity of an object relative to one observer is what is known as the relative velocity.
    • The term becomes very small at low velocities, and gives a result very close to classical velocity addition.
    • Classical velocity addition is an excellent approximation to the correct formula for small velocities.
    • It seems correct to us in our experience.
  • A spaceship heading towards the Earth at half the speed of light emits a beam of light.
    • Determine the speed at which the light leaves the ship and approaches the Earth from there.
  • Simple velocity addition is not possible because the light and spaceship are moving at very fast speeds.
    • We can use the speed at which the light approaches the Earth to determine the light's speed.
  • The knowns should be identified.
  • The appropriate equation can be chosen.
  • The knowns should be plugged into the equation.
  • The correct result is given by extrapolation velocity addition.
    • Light leaves the ship and approaches the Earth.
    • The relative motion of source and observer does not affect the speed of light.
  • If the speed of light is less than and does not exceed, velocities cannot add to it.
    • The following example shows the difference between classical and relativistic velocity addition.
  • The spaceship in the previous example is approaching the Earth at half the speed of light and shooting a canister.
  • We need to determine the speed of the canister by an Earth-bound observer using a different method than simple velocity addition.
  • The knowns should be identified.
  • The appropriate equation can be chosen.
  • The knowns should be plugged into the equation.
  • The knowns should be identified.
  • The appropriate equation can be chosen.
  • The knowns should be plugged into the equation.
  • The canister is heading towards the Earth in part and away in part, as expected, because of the minus sign.
    • Residual velocities do not add as much as they do classically.
    • The canister does approach the Earth faster, but not at the simple sum.
    • The total velocity is not as high as it could be.
    • The canister moves away from the Earth at a faster pace than you would expect.
    • The velocities are not symmetrical.
    • The canister moves faster than the ship relative to the Earth, but slower than the ship.
  • The frequencies and wavelength of light do not change with relative velocity.
    • When there is relative motion between source and observer, a Doppler shift occurs.
  • When the source moves away from the observer, the red shift is longer than the blue shift, which is when the source moves towards the observer.
  • The observed wavelength, the source wavelength, and the relative velocity of the source to the observer are all part of the equation.
    • Positive for motion away from an observer and negative for motion toward an observer.
  • The - and + signs are different from the wavelength equation.
  • If you're interested in a career that requires a knowledge of special relativity, astronomy is probably the best place to start.
    • Calculating distances, times, and speeds of black holes, galaxies, quasars, and all other astronomy objects must take into account relativistic effects.
    • If you want to work in astronomy, you need at least an undergraduate degree in either physics or astronomy, but a Master's or doctorate degree is often required.
    • A good background in high-level mathematics is required.
  • A universe is moving away from the Earth at a fast pace.
    • It emits radio waves.
  • The classical Doppler shift can't be used because the galaxy is moving at a relativistic speed.
  • The knowns should be identified.
  • The appropriate equation can be chosen.
  • The knowns should be plugged into the equation.
  • The wavelength of radiation the galaxy emits is expected to be redshifted because it is moving away from the Earth.