Path integral examples
Example 1
Let
| c(t) = (3t - 2,t + 1), 1 ≤ t ≤ 2 |
| f(x,y) = x + y. |
Solution: Mass is the integral of the density along the wire. So we must compute ∫ cfds. Since,
| c'(t) | = (3, 1), | ||
| ||c'(t)|| | = = , | ||
| f(c(t)) | = (3t - 2) + (t + 1) = 4t - 1, |
| ∫ cfds | = ∫ abf(c(t))||c'(t)||dt | ||
= ∫
12(4t - 1) dt | |||
= (2t2 - t)![]() | |||
= = 5![]() |
So, if f were given in grams/cm and c(t) were given in cm, then the mass of the
wire would 5
grams.
Example 2
Neither the length of the wire nor its mass can depend on parametrization. Check that you get the same answer with the parametrization
| p(t) = (9t - 2, 3t + 1), 1∕3 ≤ t ≤ 2∕3. |
Solution: We repeat the same calculations as in Example 1. (Recall that f(x,y) = x + y.) Since
| p'(t) | = (9, 3), | ||
| ||p'(t)|| | = = = 3 , | ||
| f(p(t)) | = (9t - 2) + (3t + 1) = 12t - 1, |
| ∫ pfds | = ∫ 1∕32∕3f(p(t))||p'(t)||dt | ||
= ∫
1∕32∕3(12t - 1)3 dt | |||
= (6t2 - t)![]() | |||
= 3![]() | |||
= 3 = 3 = 5 , |
Note that the “speed” of the parametrization ||p'(t)|| = 3
was three times
greater than the speed ||c'(t)|| =
of Example 1. But the range of
integration 1∕3 ≤ t ≤ 2∕3 was one third the range of integration from Example
1.
Example 3
Here’s another parametrization of the same straight-line wire from (1, 2) to (4, 3). This time, the “speed” of the parametrization is not constant, but depends on t:
q(t) = (3t2 - 2,t2 + 1), 1 ≤ t ≤ . |
Solution: Since
| q'(t) | = (6t, 2t), | ||
| ||q'(t)|| | = = = 2t , | ||
| f(q(t)) | = (3t2 - 2) + (t2 + 1) = 4t2 - 1. |
| ∫ qfds | = ∫
1 f(q(t))||q'(t)||dt | ||
= ∫
1 (4t2 - 1)2t dt | |||
= ∫
1 (8t3 - 2t) dt | |||
= (2t4 - t2)![]() | |||
= ![]() = 5 , |
= 


= 5
=
= 3


3
3
=
3
= 5

=
= 2

(4
(8

![[ ]
2(√2-)4 - (√2-)2 - 2 + 1](pathintex32x.png)
= 5