Give step-by-step solution with explanation and final answer:1. Hubble expansion has an analogy with baking a loaf of raisin bread with the
raisins in the dough playing the part of galaxies. Imagine viewing the expansion
from one raisin’s pont of view. Clearly the distance between raisins expand while
the density of the dough decreases. The loaf expands into the surrounding space
‘because it has a boundary. But if the loaf is infinite in extent in all directions,
‘without a boundary, then it is exactly homogeneous and it would make no sense to
talk about whatit is expanding into. The expansion looks the same from every
raisin and so the expansion has no “center”, and we have no evidence that there js
‘boundary to the universe. Initially the raisins can be located by Cartesian
‘coordinates (x,y,z) in flat Euclidean space. Continue o label the coordinates with
the same values (x,y,z) thatare co-moving
a. Express theline element of flat Euclidean space in terms of these
commoving coordinates and a scale factor afr) (note that the line.
element includes a” (1).
b. Sketcha possible curve for the scale factor between start of baking.
and the end of baking.
. What would the curve look like after the end of baking if the.
dough was a badly behaved spherical soufflé?
d. Ifthe dough was contained in a spherical boundary of initial radius
R, what would be the equation of the boundary as a function of
time and the area of the boundary at the end of baking?
Question:
Give step-by-step solution with explanation and final answer:1. Hubble expansion has an analogy with baking a loaf of raisin bread with the
raisins in the dough playing the part of galaxies. Imagine viewing the expansion
from one raisin’s pont of view. Clearly the distance between raisins expand while
the density of the dough decreases. The loaf expands into the surrounding space
‘because it has a boundary. But if the loaf is infinite in extent in all directions,
‘without a boundary, then it is exactly homogeneous and it would make no sense to
talk about whatit is expanding into. The expansion looks the same from every
raisin and so the expansion has no “center”, and we have no evidence that there js
‘boundary to the universe. Initially the raisins can be located by Cartesian
‘coordinates (x,y,z) in flat Euclidean space. Continue o label the coordinates with
the same values (x,y,z) thatare co-moving
a. Express theline element of flat Euclidean space in terms of these
commoving coordinates and a scale factor afr) (note that the line.
element includes a” (1).
b. Sketcha possible curve for the scale factor between start of baking.
and the end of baking.
. What would the curve look like after the end of baking if the.
dough was a badly behaved spherical soufflé?
d. Ifthe dough was contained in a spherical boundary of initial radius
R, what would be the equation of the boundary as a function of
time and the area of the boundary at the end of baking?
This is AI generated Response.
Asked by: srrr
Created at: 2025-06-05 21:10:46
Final Answer:
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Let's solve each part step by step:
### 1a. **Express the line element in terms of comoving coordinates and a scale factor \( a(t) \)**
---
#### **Explanation:**
- In cosmology, the expansion of the universe is described by the scale factor \( a(t) \).
- **Comoving coordinates** (\(x, y, z\)) remain fixed for objects moving with the "flow" of the universe (like the raisins in the dough).
- The **physical distance** between two points grows as \( a(t) \) increases.
#### **Flat Euclidean space (in Cartesian coordinates):**
\[ ds^2 = dx^2 + dy^2 + dz^2 \]
#### **With scale factor \( a(t) \):**
The physical distance at time \( t \) is given by:
\[ ds^2 = a^2(t) \left( dx^2 + dy^2 + dz^2 \right) \]
#### **Including time:**
The spacetime interval is:
\[
ds^2 = -c^2 dt^2 + a^2(t) \left( dx^2 + dy^2 + dz^2 \right)
\]
where \( c \) is the speed of light (can be set to 1 in cosmological units).
#### **Final answer for (a):**
\[
\boxed{
ds^2 = -c^2 dt^2 + a^2(t) \left( dx^2 + dy^2 + dz^2 \right)
}
\]
---
### 1b. **Sketch a possible curve for the scale factor \( a(t) \) between the start and end of baking**
---
#### **Explanation:**
- At the start of baking (\( t = 0 \)), the scale factor is smallest, say \( a(0) = 1 \).
- As the bread expands, \( a(t) \) increases.
- The curve should be smooth and monotonically increasing.
#### **Possible Curve:**
- For a simple rising (exponential expansion, like a well-behaved dough):
\[
a(t) = 1 + \alpha t \quad \text{(linear growth)}
\]
or
\[
a(t) = e^{\beta t} \quad \text{(exponential growth, for more rapid expansion)}
\]
where \( \alpha, \beta > 0 \) are constants.
#### **Sketch:**
- Y-axis: \( a(t) \), X-axis: \( t \)
- Curve starts at \( a(0) = 1 \), increases smoothly over time.
---
### 1c. **What would the curve look like after the end of baking if the dough was a badly behaved spherical soufflé?**
---
#### **Explanation:**
- A "badly behaved" soufflé might rise rapidly, then collapse (deflate).
- So, the scale factor would **increase**, reach a **maximum**, then **decrease**.
#### **Possible Curve:**
- Looks like a "hill" or "bump."
- Mathematically: \( a(t) = 1 + \alpha t - \gamma t^2 \) for some small \( t \), with \( \gamma > 0 \), so \( a(t) \) rises then falls.
- Or as a sketch: an up-and-down curve (rise and collapse).
---
### 1d. **Equation for the boundary as a function of time and area at the end of baking**
---
#### **Explanation:**
- Initial radius: \( R \)
- As dough expands, all lengths scale by \( a(t) \).
- So at time \( t \), new radius: \( a(t) R \).
#### **Equation for boundary:**
\[
\text{Radius at time } t: \quad r(t) = a(t) R
\]
#### **Area of the boundary (sphere):**
\[
A(t) = 4\pi [r(t)]^2 = 4\pi [a(t) R]^2 = 4\pi R^2 [a(t)]^2
\]
#### **Final answers for (d):**
\[
\boxed{
\text{Radius: } r(t) = a(t) R
}
\]
\[
\boxed{
\text{Area: } A(t) = 4\pi R^2 [a(t)]^2
}
\]
---
## **Summary Table of Answers**
| Part | Answer |
|------|--------|
| a | \( ds^2 = -c^2 dt^2 + a^2(t)(dx^2 + dy^2 + dz^2) \) |
| b | \( a(t) \) is a monotonically increasing curve (linear or exponential) |
| c | \( a(t) \) rises then falls (hill-shaped curve) |
| d | \( r(t) = a(t) R \), \( A(t) = 4\pi R^2 [a(t)]^2 \) |
Let me know if you want the sketches for (b) and (c) or any further explanation!
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