MODULE 7 IQ 4 Flashcards
what is a frame of reference
- a set of coordinate axes and a dimension of time, and we use these sets/dimensions to make observations from our point of view
- if frame of reference is not accelerating, it is known as an inertial frame of reference
inertial frames of reference (IFOR)
- not accelerating
- in these frames, newton’s laws of motion hold
- observers in inertial frames can make predictions about motion of objects with relative ease
galilean relativity
- describes how the laws of mechanics are the same in all inertial frames of reference
- if you’re in a closed room moving at a constant velocity, you cannot perform any experiment to determine that you’re moving
special theory of relativity
- the laws of physics are the same for all observers in inertial frames of reference, regardless of their relative motion
- leads to time dilation, length contraction and the equivalence of mass and energy ( E = mc^2)
einstein’s postulates
- the speed of light in a vacuum remains constant in all inertial frames of reference
- the laws of physics are invariable in all inertial frames of reference
implications of einstein’s 1st postulate
- light is invariant at 1/√ε(0)μ(0) for ALL frames of reference
- relative velocity between the light source and the observe does not alter the measure velocity of light
implications of einstein’s 2nd postulate
- experiments conducted within inertial frames will yield consistent results
- it is not possible to determine experimentally whether an inertial frame is stationary or in motion
- time and distance are not absolute quantities
proper time
time an event takes to occur, as measured by an observer with the same frame of reference as the event itself
proper length
length of an object, measured in a frame of reference that observes the object at rest (not moving)
time dilation
- velocity of object increases, the factor by which its time dilates increases
- for outside observer: light needs to travel a longer distance (longer time observed)
- for inside observer: no change in distance (shorter time)
time dilation equation
t = t(0)/√1-v^2/c^2
t: dilated time
t(0): proper time
length contraction
- length appears shorter for a moving observer
- length appears longer for stationary observer
length contraction equation
l = l(0)√1-(v^2/c^2)
l: contracted length while in motion (observer moving with respect to distance’s endpoints)
l(0): proper length (observer at rest in reference to distance’s endpoints
simultaneity
- reality is not different for 2 observers in different frames
evidence for special relativity
hafele-keating experiment, muons