describes how motion looks from different viewpoints. It works well for everyday speeds but falls short when things move super fast. This concept is crucial for understanding why we needed a new way to think about motion.
Einstein's came to the rescue, fixing the problems with Galilean relativity. It changed our view of space and time, showing that they're not as fixed as we thought. This shift was a big deal in physics.
Galilean Relativity
Coordinate Transformations and Relative Motion
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Galilean transformations describe the relationship between coordinates in two inertial frames moving at constant velocity relative to each other
Consists of a translation in space and time
Allows for the conversion of coordinates from one to another
Inertial frames are reference frames in which Newton's laws of motion hold
An object at rest or moving at constant velocity remains at rest or moving at constant velocity unless acted upon by an external force
Experiments performed in one inertial frame will yield the same results as in any other inertial frame ()
Relative motion refers to the motion of an object as observed from different inertial frames
The velocity of an object depends on the choice of the reference frame
An object at rest in one frame may appear to be moving in another frame
Velocity Addition and Invariance
Velocity addition is a consequence of Galilean transformations
The velocity of an object in one inertial frame is the sum of its velocity in another frame and the between the two frames
Formula for velocity addition: v′=v+u, where v′ is the velocity in the new frame, v is the velocity in the original frame, and u is the relative velocity between frames
Galilean relativity implies the invariance of mechanical laws under Galilean transformations
The laws of mechanics have the same form in all inertial frames
Examples include Newton's laws of motion and the conservation of momentum
Invariance and Absolute Time
Acceleration and Its Invariance
Acceleration is the rate of change of velocity over time
Mathematically, acceleration is the second derivative of position with respect to time: a=d2x/dt2
Acceleration is invariant under Galilean transformations
The acceleration of an object is the same in all inertial frames
This invariance is a consequence of the absolute nature of time in Galilean relativity
Absolute Time and Simultaneity
Galilean relativity assumes the existence of
Time is considered to flow at the same rate for all observers, regardless of their motion
The time interval between two events is the same in all inertial frames
Absolute time implies the notion of absolute simultaneity
If two events are simultaneous in one inertial frame, they are simultaneous in all inertial frames
The order of events is preserved across all inertial frames
Limitations of Galilean Relativity
Inconsistencies at High Velocities
Galilean relativity breaks down when objects move at speeds comparable to the speed of light
The invariance of the speed of light, as observed in experiments such as the Michelson-Morley experiment, cannot be explained by Galilean transformations
The addition of velocities in Galilean relativity would imply that the speed of light should vary depending on the observer's motion, which contradicts experimental evidence
The limitations of Galilean relativity led to the development of special relativity by Albert Einstein
Special relativity postulates the invariance of the speed of light and the relativity of simultaneity
It introduces Lorentz transformations, which replace Galilean transformations, to describe the relationship between coordinates in different inertial frames moving at high velocities relative to each other