Cosmological model, geodesics question

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SUMMARY

The discussion focuses on the geodesic equation in the context of cosmological models, specifically addressing the conservation of quantities associated with independent metric components. The user demonstrates understanding by deriving the geodesic equation, identifying that certain Christoffel symbols are zero, and questioning the implications of constant coordinates on geodesics. The conversation highlights the need to consider the temporal component of the geodesic equation and the definition of an affine parameter, ultimately leading to the conclusion that the user must explore whether the second derivative of time is zero.

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  • Understanding of geodesic equations in general relativity
  • Familiarity with Christoffel symbols and their role in differential geometry
  • Knowledge of the Euler-Lagrange equations
  • Concept of affine parameters in the context of geodesics
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binbagsss
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Homework Statement



I am unsure of Q3 but have posted my solutions to other parts

cosmomodoel.png


Homework Equations

The Attempt at a Solution



3)
ok so it is clear that because the metric components are independent of ##x^i## each ##x^i## has an associated conserved quantity ##d/ds (\dot{x^i})=0##. (1)

The geodesic equation can be written as ##\frac{d^2x^i}{ds^2}+\Gamma^i_{ab}\dot{x}^a\dot{x}^b=0 ##

I look at the Euler-Lagrange equations and I can quickly show that all Christoffel symbols with an upper index ##^i## are zero and so the above is zero (via comparing the the form above of a geodesic equation and identifying the Christoffel symbols from the e-l equations this way). so the first term is zero i have shown by the KVF and the second term zero. so the geodesic equation is obeyed.

Now here is my probably very stupid question, how is this constant ##x^i ## geodesics that the above geodesic equation describes. . the above geodesic equation would hold for ##\dot{x^i}## constant which implies that ##x^i## is constant ofc, but here I see my thoughts are way of track and i have clearly misunderstood something as just using this line of reasoning the geodesic equation is trivially satisfied...

thanks.
 

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The spatial equations yes. You replaced them by the correspondig first integral. You still need to solve the temporal one.
 
Orodruin said:
The spatial equations yes. You replaced them by the correspondig first integral. You still need to solve the temporal one.

okay many thanks.
I am unsure what you mean by 'integral ' however.
But I see clearly I have missed out the time -component equation of ##\ddot{x^u}+\Gamma^u_{ab}\dot{x^a}\dot{x^b}=0 ##

I have found that the Christoffel Symbols ##\Gamma^x_{xt} , \Gamma^t_{xt} \neq 0 ## , and ##\Gamma^t_{tt}=0##
And so for there to be a chance of a geodesic, from my above workings, I assume the quesion means to hold all ##x^i## constant and not just one?

This leaves me to look at whether ##\ddot{t}=0##?

To this I check whether there is an affine parameter ##s## such that this is possible. The definition of affine parameter is that ##dL/ds=0##

and so if I write

##L=-\dot{t^2} + K_{x_1} + K_{x_1} + K_{x_1} ##; where ##K_{x_1}## is the KvF associated with the ##x_i## coordinate.
and then differentiate wrt s to get
##0=\ddot{t}##

is this ok?
have I took a long-winded approach?
 
binbagsss said:
I am unsure what you mean by 'integral ' however
Not ”integral”, ”first integral”.
 
Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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