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yanalaym [24]
3 years ago
15

Spaceship A is 10 meters long and approaching you from the south at a speed of.7c while spaceship B, which is also 10 meters lon

g, is approaching you from the north at a speed of.7c. a. What is the relative speed of A as measured by B? b. What is the length of A as measured by you? c. What is the length of A as measured by B? d. An event on A lasts 1 second as measured by A. How long does the event last as measured by you? e. An event on A lasts 1 second as measured by A. How long does the event last as measured by B?
Physics
1 answer:
Valentin [98]3 years ago
3 0

Answer:

a) 0.94 C

b) 7.14 m

c) 3.11 m

d) 1.40 s

e) 2.93 s

Explanation:

First we need to set up a coordinate system. This will have the positive X axis pointing north. So spaceship A has positive speed, and spaceship B has negative speed.

The Lorentz transformation for speed is:

u' = \frac{u - v}{1 - \frac{u*v}{c^2}}

u: speed of spaceship A as observed by you

v: speed of spaceship B as observed by you

In the case of the speed of spaceship A as observed by spaceship B:

u' = \frac{0.7c - (-0.7c)}{1 - \frac{0.7c*(-0.7c)}{c^2}} = 0.94c

The transform for lengths is:

L = L0 * \sqrt{1 - \frac{v^2}{c^2}}

For the case of spaceship A as observed by you:

L = 10 m * \sqrt{1 - \frac{(0.7c)^2}{c^2}} = 7.14 m

For the case of spaceship A as observed by spaceship B:

L = 10 m * \sqrt{1 - \frac{(0.94c)^2}{c^2}} = 3.12 m

The time dilation equation is:

T = \frac{T0}{\sqrt{1-\frac{v^2}{c^2}}}

For the case of the event as observed by you:

\frac{1 s}{\sqrt{1-\frac{(0.7c)^2}{c^2}}} = 1.40 s

For the case of the event as observed by spaceship B:

\frac{1 s}{\sqrt{1-\frac{(0.94c)^2}{c^2}}} = 2.93 s

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Answer:

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State and prove bessel inequality​
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Statement :- We assume the orthagonal sequence {{\{\phi\}}_{1}^{\infty}} in Hilbert space, now {\forall \sf \:v\in \mathbb{V}}, the Fourier coefficients are given by:

{\quad \qquad \longrightarrow \sf a_{i}=(v,{\phi}_{i})}

Then Bessel's inequality give us:

{\boxed{\displaystyle \bf \sum_{1}^{\infty}\vert a_{i}\vert^{2}\leqslant \Vert v\Vert^{2}}}

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So that, {\bf v_n} is projection of {\bf v} onto the surface by the first {\bf n} of the {\bf \phi_{i}} . For any event, {\sf (v-v_{n})\perp v_{n}}

Now, by Pythagoras theorem:

{:\implies \quad \sf \Vert v\Vert^{2}=\Vert v-v_{n}\Vert^{2}+\Vert v_{n}\Vert^{2}}

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Now, we can deduce that from the above equation that;

{:\implies \quad \displaystyle \sf \sum_{i=1}^{n}\vert a_{i}  \vert^{2}\leqslant \Vert v\Vert^{2}}

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FrozenT [24]

Answer:

t = 4 s

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As we know that the particle A starts from Rest with constant acceleration

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on solving above kinematics equation we have

t = 4 s

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