Chapter 2: 36E (page 5)
How fast must be a plane 50 m long travel to be found by observer on the ground to be 0.10 nm shorter than 50 m?
Short Answer
The value of derived expression for the travel at a speed .
Chapter 2: 36E (page 5)
How fast must be a plane 50 m long travel to be found by observer on the ground to be 0.10 nm shorter than 50 m?
The value of derived expression for the travel at a speed .
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Get started for freeExercise 117 gives the speed u of an object accelerated under a constant force. Show that the distance it travels is given by
A pole-vaulter holds a pole, A barn has doors at both ends, apart. The pole-vaulter on the outside of the barn begins running toward one of the open barn doors, holding the pole level in the direction he's running. When passing through the barn, the pole fits (barely) entirely within the barn all at once. (a) How fast is the pole-vaulter running? (b) According to whom-the pole-vaulter or an observer stationary in the barn--does the pole fit in all at once? (c) According to the other person, which occurs first the front end of the pole leaving the bam or the back end entering, and (d) what is the time interval between these two events?
Anna and Bob are both born just as Anna's spaceship passes Earth at . According to Bob on Earth planet Z is a fixed away. As Anna passes planet Z on her continuing onward journey, what will be
(a) Bob's age according to Bob
(b) Bob's age according to Anna
(c) Anna's age according to Anna
(d) Anna's age according to Bob
Equation (2-30) is an approximation correct only if the gravitational time-dilation effect is small. In this exercise, it is also assumed to be small. but we still allow for a nonuniform gravitational field. We start with (2-29), based on the Doppler effect in the accelerating frame. Consider two elevations, the lower at r1 and the upper at . Equation (2·29) becomes
Similarly, if we consider elevationsdata-custom-editor="chemistry" and data-custom-editor="chemistry" , we have
We continue the process, incrementing r by dr, until we reach r2.
Now imagine multiplying the left sides of all the equations and setting the product equal to the product of all the right sides. (a) Argue that the left side of the product is simply . (b) Assuming that the term in each individual equation is very small. so that productsof such termscan be ignored, argue that the right side of the product is
(c) Deduce from Newton’s universal law of gravitation, then argue that equation (2-31) follows from the result, just as (2-30) does from (2-29).
(a) Determine the Lorentz transformation matrix giving position and time in framefromthose in framein the classical limitlocalid="1657533931071" . (b) Show that it yields equations (2-1).
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