Give step-by-step solution with explanation and final answer:(5.2) Exercise 3.4.14 Determine the Mayer equation for the isoperimetric problem with the functional . Ila] = [ [p® + gi?) dt. Jo with auxiliary and boundary conditions [ raldt =1, (0) =0, x(a) =0, o where p,q, are given class C? functions of ¢.
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Give step-by-step solution with explanation and final answer:
(5.2) Exercise 3.4.14 Determine the Mayer equation for the isoperimetric problem with the
functional .
Ila] = [ [p® + gi?) dt.
Jo
with auxiliary and boundary conditions
[ raldt =1, (0) =0, x(a) =0,
o
where p,q, are given class C? functions of ¢.
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Asked by: Test User 100252
Created at: 2025-05-22 04:33:26
Asked by: Test User 100252
Created at: 2025-05-22 04:33:26
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Let's break down the steps to **determine the Mayer equation** for the isoperimetric problem given:
### **Step 1: State the Problem**
Given the functional:
\[
I[x] = \int_0^a \left[ p x^2 + q \dot{x}^2 \right] dt
\]
with the **isoperimetric (auxiliary) constraint**:
\[
\int_0^a r x^2 \, dt = 1
\]
and boundary conditions:
\[
x(0) = 0, \quad x(a) = 0
\]
where \( p, q, r \) are given \( C^2 \) functions of \( t \).
---
### **Step 2: Formulate the Augmented Functional**
Introduce a Lagrange multiplier \( \lambda \) for the constraint. The augmented functional becomes:
\[
J[x] = \int_0^a \left[ p x^2 + q \dot{x}^2 + \lambda r x^2 \right] dt - \lambda
\]
Or usually written:
\[
J[x] = \int_0^a \left[ (p + \lambda r) x^2 + q \dot{x}^2 \right] dt
\]
---
### **Step 3: Euler–Lagrange Equation**
The integrand is:
\[
L = (p + \lambda r) x^2 + q \dot{x}^2
\]
The Euler–Lagrange equation is:
\[
\frac{\partial L}{\partial x} - \frac{d}{dt} \left( \frac{\partial L}{\partial \dot{x}} \right) = 0
\]
Compute the derivatives:
- \( \frac{\partial L}{\partial x} = 2(p + \lambda r)x \)
- \( \frac{\partial L}{\partial \dot{x}} = 2q\dot{x} \)
- \( \frac{d}{dt}\left(2q\dot{x}\right) = 2q\ddot{x} + 2q'\dot{x} \)
Plug into the equation:
\[
2(p + \lambda r)x - \left[2q\ddot{x} + 2q'\dot{x}\right] = 0
\]
Divide by 2:
\[
(p + \lambda r)x - q\ddot{x} - q'\dot{x} = 0
\]
Or:
\[
q\ddot{x} + q'\dot{x} - (p + \lambda r)x = 0
\]
---
### **Step 4: Final Mayer Equation**
The **Mayer equation** for this isoperimetric problem is:
\[
\boxed{
q(t)\ddot{x} + q'(t)\dot{x} - \left[ p(t) + \lambda r(t) \right] x = 0
}
\]
with auxiliary condition:
\[
\int_0^a r(t)x^2(t)\,dt = 1
\]
and boundary conditions:
\[
x(0) = 0, \quad x(a) = 0
\]
---
## **Summary**
### The Mayer equation is:
\[
\boxed{
q(t)\ddot{x} + q'(t)\dot{x} - (p(t) + \lambda r(t)) x = 0
}
\]
with:
- Boundary: \( x(0) = x(a) = 0 \)
- Constraint: \( \int_0^a r(t)x^2(t)\,dt = 1 \)
- \( p,q,r \) given \( C^2 \) functions, \( \lambda \) to be determined.
---
If you need more details on solving for \( \lambda \), let me know!
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