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ME 533 Introduction to ICF
Assignment 4 Solutions
Problem 1
Starting from hot-spot mass equation
𝒅
𝒅𝒕(
𝑷𝑹𝟑
𝑻𝟎) = 𝟎. 𝟖𝟔 ∗ 𝜿𝟎𝑻𝟎
𝟓/𝟐𝑹
We define normalized variables 𝑷′, 𝑹′, 𝒕′ normalized to no-α stagnation
quantities 𝑷𝒔, 𝑹𝒔 and 𝒕𝒔(𝑹𝒔
𝑽𝒊) as found in assignment 3. Also define
𝑻𝟎′ =
𝑻𝟎
𝑻𝟎𝒔 ( for now 𝑻𝟎𝒔 unknown)
We get
(𝟏
𝒕𝒔𝑻𝟎𝒔)
𝒅
𝒅𝒕′(
𝑷′𝑹′𝟑
𝑻𝟎′ ) 𝑷𝒔𝑹𝒔
𝟑 = 𝟎. 𝟖𝟔 ∗ 𝜿𝟎𝑻𝟎𝒔𝟓/𝟐𝑻𝟎
′𝟓/𝟐𝑹𝒔𝑹′
To simplify this as
𝒅
𝒅𝒕′ (𝑷′𝑹′𝟑) = 𝑹′𝑻𝟎
′𝟓/𝟐 ( ……. Eqn. 1) , we need 𝑻𝟎𝒔 = (
𝑷𝒔𝑹𝒔𝑽𝒊
𝟎.𝟖𝟔∗𝜿𝟎)𝟐/𝟕
Let 𝑿 ≡𝟏
𝑻𝟎′𝑹′𝟐 we can write (1) as 𝑿𝟓/𝟐 𝒅𝑿
𝒅𝒕′ =𝟏
𝑹′𝟒
⟹ 𝒅 (𝑿
𝟕𝟐)
𝒅𝒕′= (
𝟕
𝟐)
𝟏
𝑹′𝟒
⟹ 𝒅 (𝑿
𝟕𝟐)
𝒅𝒕′= (
𝟕
𝟐)
𝟏
(𝟏 + 𝒕′𝟐)𝟐
Integrating in mathematica and using B.C 𝑿 ⟶ ∞ 𝒂𝒔 𝑹′ → 𝟎
⟹ 𝑿 = (𝟕
𝟒(
𝒕′
𝟏 + 𝒕′𝟐+ 𝑻𝒂𝒏−𝟏(𝒕′) +
𝝅
𝟐))𝟐/𝟕
⟹ 𝑻𝟎′ =
𝟏
(𝟏 + 𝒕′𝟐)𝟐(𝟕
𝟒(
𝒕′
𝟏 + 𝒕′𝟐+ 𝑻𝒂𝒏−𝟏(𝒕′) +
𝝅
𝟐))−𝟐/𝟕
Problem 2
Normalization of equation for Newton`s second law for shell
motion is straight forward, and we derived normalized hot-spot
mass/temperature equation in problem 1.
Starting from hot-spot energy equation with alpha heating
𝒅
𝒅𝒕(𝑷𝑹𝟓) = 𝝁𝑷𝟐𝑹𝟓𝑻𝟎
𝟏.𝟏
Expanding the derivative and defining normalized variables as
in problem 1, we get
𝐝𝐏′
𝐝𝐭′+
𝟓𝐏′
𝐑′
𝐝𝐑′
𝐝𝐭′= 𝛍𝐭𝐬𝐏𝐬(𝐓𝟎𝐬𝐓𝟎
′)𝟏.𝟎𝟏𝐏′𝟐
Also, at stagnation 𝑰. 𝑬𝒉𝒐𝒕−𝒔𝒑𝒐𝒕 = 𝑲. 𝑬𝒔𝒉𝒆𝒍𝒍−𝒎𝒂𝒙
⟹ 𝑷𝒔𝑹𝒔𝟑 = (
𝟏
𝟒𝝅)𝑴𝒔𝒉𝑽𝒊𝒎𝒑
𝟐
Also using from problem 1, 𝑻𝟎𝒔 = (𝑷𝒔𝑹𝒔𝑽𝒊
𝟎.𝟖𝟔∗𝜿𝟎)𝟐/𝟕 we get,
𝒅
𝒅𝒕(𝐏′𝐑′𝟓
) = 𝝃𝒏𝒐−𝜶𝐏′𝟐𝐑′𝟓
𝐓𝟎′𝟏.𝟎𝟏
With 𝝃𝒏𝒐−𝜶 = 𝛍𝐭𝐬𝐏𝐬𝐓𝟎𝐬𝟏.𝟎𝟏 =
𝛍𝐑𝐬𝐏𝐬𝐓𝟎𝐬𝟏.𝟎𝟏
𝑽𝒊
𝝃𝒏𝒐−𝜶 = 𝝁(𝟎. 𝟖𝟔𝜿𝟎)−𝟐.𝟎𝟐/𝟕𝑽𝒊
𝟏𝟑.𝟎𝟔/𝟕(𝝆𝚫)𝟗.𝟎𝟐/𝟕
Problem 3
𝜉𝑐𝑟𝑖𝑡 = 1.07 (𝑠𝑒𝑒 𝑎𝑡𝑡𝑎𝑐ℎ𝑒𝑑 𝑚𝑎𝑡ℎ𝑒𝑚𝑎𝑡𝑖𝑐𝑎 𝑛𝑜𝑡𝑒𝑏𝑜𝑜𝑘)
Singular solution at 𝜉𝑛𝑜−𝛼 = 1.07
Problem 4
Plots of hot-spot pressure for various values of 𝜉𝑛𝑜−𝛼
Problem 5
𝝌𝒏𝒐−𝜶 ≡𝜉𝑛𝑜−𝛼
𝜉𝑐𝑟𝑖𝑡
> 1
Substituting for 𝜉𝑛𝑜−𝛼
⟹ 𝝌𝒏𝒐−𝜶 = (𝟏
𝟏. 𝟎𝟕) ∗ (
𝜺𝜶𝑺𝒇𝐓𝟎𝐬𝟏.𝟎𝟏
𝟐𝟒)
Substituting for 𝐓𝟎𝐬, we get
⟹ 𝝌𝒏𝒐−𝜶 = 𝟎. 𝟖𝟖 ∗ 𝜿𝟎𝟏/𝟑 ∗ (
𝜺𝜶𝑺𝒇(𝝆𝚫)𝟐/𝟑𝐓𝟎𝐬𝟐.𝟏𝟖
𝟐𝟒)
Use neutron averaged quantities
< 𝑇 >= 0.53𝐓𝟎𝐬 & < 𝝆𝐑 >= 𝟎. 𝟖𝟖 𝝆𝚫
and 𝜺𝜶 = 𝟑. 𝟓 𝑴𝒆𝒗, 𝑺𝒇 = 𝟕. 𝟓 ∗ 𝟏𝟎−𝟐𝟑 𝒎𝟑
𝒔 𝑲𝒆𝑽𝟑.𝟎𝟏 , 𝜿𝟎 = 𝟑. 𝟕𝟒 ∗ 𝟏𝟎𝟔𝟗 𝑱𝟐/𝟓
𝒎∗𝒔
We finally get
𝝌𝒏𝒐−𝜶 = 𝟎. 𝟎𝟑 < 𝝆𝐑𝒏𝒐−𝜶 >𝟐/𝟑< 𝑻𝒏𝒐−𝜶 >𝟐.𝟏𝟖
Problem 3D[P[t] R[t]^3 / T[t], t]
R[t]3 P′[t]
T[t]+3 P[t] R[t]2 R′[t]
T[t]-P[t] R[t]3 T′[t]
T[t]2
xi = 1.07eps = 10^-2NDSolve[{R''[t] ⩵ R[t]^2 P[t], P'[t] + 5 P[t] / R[t] R'[t] ⩵ xi P[t]^2 T[t]^1.01,
D[P[t] R[t]^3 / T[t], t] ⩵ T[t]^5 / 2 R[t], R[0] ⩵ 1 / eps, P[0] ⩵ eps^5,R'[0] ⩵ -1, T[0] ⩵ eps}, {R[t], P[t] , T[t]}, {t, 0, 500}]
1.07
1
100
NDSolve::ndsz : At t == 100.53605397419585` , step size is effectively zero; singularity or stiff system suspected.
R[t] → InterpolatingFunctionDomain: {{0., 101.}}Output: scalar
[t],
P[t] → InterpolatingFunctionDomain: {{0., 101.}}Output: scalar
[t],
T[t] → InterpolatingFunctionDomain: {{0., 101.}}Output: scalar
[t]
xi = 1.04eps = 10^-1NDSolve[{R''[t] ⩵ R[t]^2 P[t], P'[t] + 5 P[t] / R[t] R'[t] ⩵ xi P[t]^2 T[t]^1.01,
D[P[t] R[t]^3 / T[t], t] ⩵ T[t]^5 / 2 R[t], R[0] ⩵ 1 / eps, P[0] ⩵ eps^5,R'[0] ⩵ -1, T[0] ⩵ eps}, {R[t], P[t] , T[t]}, {t, 0, 50}]
1.04
1
10
R[t] → InterpolatingFunctionDomain: {{0., 50.}}Output: scalar
[t],
P[t] → InterpolatingFunctionDomain: {{0., 50.}}Output: scalar
[t],
T[t] → InterpolatingFunctionDomain: {{0., 50.}}Output: scalar
[t]
Problem 4xiCrit = 1.05getRandP[xi_, eps_] :=
NDSolve[{R''[t] ⩵ R[t]^2 P[t], P'[t] + 5 P[t] / R[t] R'[t] ⩵ xi P[t]^2 T[t]^1.01,D[P[t] R[t]^3 / T[t], t] ⩵ T[t]^5 / 2 R[t], R[0] ⩵ 1 / eps, P[0] ⩵ eps^5,R'[0] ⩵ -1, T[0] ⩵ eps}, {R[t], P[t] , T[t]}, {t, 0, 50}]
1.05
2 assn_4 (1).nb
S = getRandP[0 / xiCrit, 10^-1];Plot[Evaluate[{R[t]} /. S], {t, 0, 20}, PlotStyle → Automatic]a = Plot[Evaluate[{P[t]} /. S], {t, 0, 20}, PlotRange → {{5, 15}, {0, 2.5}}]Plot[Evaluate[{T[t]} /. S], {t, 0, 20}, PlotRange → All]
5 10 15 20
2
4
6
8
10
6 8 10 12 14
0.5
1.0
1.5
2.0
2.5
5 10 15 20
0.2
0.4
0.6
0.8
1.0
assn_4 (1).nb 3
S1 = getRandP[0.1 * xiCrit, 10^-1];Plot[Evaluate[{R[t]} /. S], {t, 0, 20}, PlotStyle → Automatic]a1 = Plot[Evaluate[{P[t]} /. S1], {t, 0, 20}, PlotRange → {{5, 15}, {0, 2.5}}]Plot[Evaluate[{T[t]} /. S], {t, 0, 20}, PlotRange → All]
5 10 15 20
2
4
6
8
10
6 8 10 12 14
0.5
1.0
1.5
2.0
2.5
5 10 15 20
0.2
0.4
0.6
0.8
1.0
4 assn_4 (1).nb
S2 = getRandP[0.5 * xiCrit, 10^-1];Plot[Evaluate[{R[t]} /. S], {t, 0, 20}, PlotStyle → Automatic]a2 = Plot[Evaluate[{P[t]} /. S2], {t, 0, 20}, PlotRange → {{5, 15}, {0, 2.5}}]Plot[Evaluate[{T[t]} /. S], {t, 0, 20}, PlotRange → All]
5 10 15 20
2
4
6
8
10
6 8 10 12 14
0.5
1.0
1.5
2.0
2.5
5 10 15 20
0.2
0.4
0.6
0.8
1.0
assn_4 (1).nb 5
S3 = getRandP[0.9 * xiCrit, 10^-1];Plot[Evaluate[{R[t]} /. S], {t, 0, 20}, PlotStyle → Automatic]a3 = Plot[Evaluate[{P[t]} /. S3], {t, 0, 20}, PlotRange → {{5, 15}, {0, 2.5}}]Plot[Evaluate[{T[t]} /. S], {t, 0, 20}, PlotRange → All]
5 10 15 20
2
4
6
8
10
6 8 10 12 14
0.5
1.0
1.5
2.0
2.5
5 10 15 20
0.2
0.4
0.6
0.8
1.0
6 assn_4 (1).nb
S = getRandP[xiCrit, 10^-1];Plot[Evaluate[{R[t]} /. S], {t, 0, 20}, PlotStyle → Automatic]a4 = Plot[Evaluate[{P[t]} /. S], {t, 0, 20}, PlotRange → All,
AxesLabel → {Style["P", Bold, 14], Style["t", Bold, 14]}, PlotStyle → FontSize]Plot[Evaluate[{T[t]} /. S], {t, 0, 20}, PlotRange → All]
NDSolve::ndsz : At t == 10.402023057183255` , step size is effectively zero; singularity or stiff system suspected.
5 10 15 20
-1.5×1054
-1.0×1054
-5.0×1053
5 10 15 20P
5.0×1044
1.0×1045
1.5×1045
2.0×1045
2.5×1045
3.0×1045
t
5 10 15 20
5.0×1039
1.0×1040
1.5×1040
2.0×1040
2.5×1040
assn_4 (1).nb 7
Show[{a1, a2, a3}]
6 8 10 12 14
0.2
0.4
0.6
0.8
1.0
1.2
1.4
Plot[{Evaluate[{P[t]} /. S], Evaluate[{P[t]} /. S1], Evaluate[{P[t]} /. S2],Evaluate[{P[t]} /. S3]}, {t, 0, 20}, PlotRange → {{5, 15}, {0, 2.5}},
AxesLabel → {Style["P'", Bold, 14], Style["t'", Bold, 14]},PlotLegends → Placed[{"0", "0.1", "0.525", "0.945"}, Above]]
0 0.1 0.525 0.945
6 8 10 12 14P'
0.5
1.0
1.5
2.0
2.5t'
1.05 * 0.9
0.945
ealpha = 3.5 * 1.6 * 10^-13; (to Joules)sf = 7.5 * 10^-23;k0 = 3.74 * 10^69;
coeff = (0.88 * k0^(1 / 3) * sf * 0.53^2.18 * 0.88^2 / 3) / 24
0.0276093
8 assn_4 (1).nb