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Finding a potential function

Find a potential function for F ( x , y ) = 2 x y 3 , 3 x 2 y 2 + cos ( y ) , thereby showing that F is conservative.

Suppose that f ( x , y ) is a potential function for F . Then, f = F , and therefore

f x = 2 x y 3 and f y = 3 x 2 y 2 + cos y .

Integrating the equation f x = 2 x y 3 with respect to x yields the equation

f ( x , y ) = x 2 y 3 + h ( y ) .

Notice that since we are integrating a two-variable function with respect to x , we must add a constant of integration that is a constant with respect to x , but may still be a function of y . The equation f ( x , y ) = x 2 y 3 + h ( y ) can be confirmed by taking the partial derivative with respect to x :

f x = x ( x 2 y 3 ) + x ( h ( y ) ) = 2 x y 3 + 0 = 2 x y 3 .

Since f is a potential function for F ,

f y = 3 x 2 y 2 + cos ( y ) ,

and therefore

3 x 2 y 2 + g ( y ) = 3 x 2 y 2 + cos ( y ) .

This implies that h ( y ) = cos y , so h ( y ) = sin y + C . Therefore, any function of the form f ( x , y ) = x 2 y 3 + sin ( y ) + C is a potential function. Taking, in particular, C = 0 gives the potential function f ( x , y ) = x 2 y 3 + sin ( y ) .

To verify that f is a potential function, note that f = 2 x y 3 , 3 x 2 y 2 + cos y = F .

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Find a potential function for F ( x , y ) = e x y 3 + y , 3 e x y 2 + x .

f ( x , y ) = e x y 3 + x y

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The logic of the previous example extends to finding the potential function for any conservative vector field in 2 . Thus, we have the following problem-solving strategy for finding potential functions:

Problem-solving stragegy: finding a potential function for a conservative vector field F ( x , y ) = P ( x , y ) , Q ( x , y )

  1. Integrate P with respect to x . This results in a function of the form g ( x , y ) + h ( y ) , where h ( y ) is unknown.
  2. Take the partial derivative of g ( x , y ) + h ( y ) with respect to y , which results in the function g y ( x , y ) + h ( y ) .
  3. Use the equation g y ( x , y ) + h ( y ) = Q ( x , y ) to find h ( y ) .
  4. Integrate h ( y ) to find h ( y ) .
  5. Any function of the form f ( x , y ) = g ( x , y ) + h ( y ) + C , where C is a constant, is a potential function for F .

We can adapt this strategy to find potential functions for vector fields in 3 , as shown in the next example.

Finding a potential function in 3

Find a potential function for F ( x , y ) = 2 x y , x 2 + 2 y z 3 , 3 y 2 z 2 + 2 z , thereby showing that F is conservative.

Suppose that f is a potential function. Then, f = F and therefore f x = 2 x y . Integrating this equation with respect to x yields the equation f ( x , y , z ) = x 2 y + g ( y , z ) for some function g . Notice that, in this case, the constant of integration with respect to x is a function of y and z .

Since f is a potential function,

x 2 + 2 y z 3 = f y = x 2 + g y .

Therefore,

g y = 2 y z 3 .

Integrating this function with respect to y yields

g ( y , z ) = y 2 z 3 + h ( z )

for some function h ( z ) of z alone. (Notice that, because we know that g is a function of only y and z , we do not need to write g ( y , z ) = y 2 z 3 + h ( x , z ) . ) Therefore,

f ( x , y , z ) = x 2 y + g ( y , z ) = x 2 y + y 2 z 3 + h ( z ) .

To find f , we now must only find h . Since f is a potential function,

3 y 2 z 2 + 2 z = g z = 3 y 2 z 2 + h ( z ) .

This implies that h ( z ) = 2 z , so h ( z ) = z 2 + C . Letting C = 0 gives the potential function

f ( x , y , z ) = x 2 y + y 2 z 3 + z 2 .

To verify that f is a potential function, note that f = 2 x y , x 2 + 2 y z 3 , 3 y 2 z 2 + 2 z = F .

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Find a potential function for F ( x , y , z ) = 12 x 2 , cos y cos z , 1 sin y sin z .

f ( x , y , z ) = 4 x 3 + sin y cos z + z

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We can apply the process of finding a potential function to a gravitational force . Recall that, if an object has unit mass and is located at the origin, then the gravitational force in 2 that the object exerts on another object of unit mass at the point ( x , y ) is given by vector field

Practice Key Terms 6

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Source:  OpenStax, Calculus volume 3. OpenStax CNX. Feb 05, 2016 Download for free at http://legacy.cnx.org/content/col11966/1.2
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