Home » 2011
Yearly Archives: 2011
Harry Hill and Professor Brian Cox
Actually Harry, it is just a bit more complex than that!
Where:
T is the gravitational time dilation of an object at a distance of r.
dt is the change in coordinate time, or the interval of coordinate time.
G is the gravitational constant
M is the mass generating the field
is the change in proper time dτ, or the interval of proper time.