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Green's Theorem

Green’s theorem applies in two dimensions (xy-plane) and relates a line integral around a closed curve to a double integral over the enclosed area. It deals with the circulation or “swirliness” of a vector field. Green’s theorem is a special case of a more general theorem called Stokes’ theorem, which applies in three dimensions. It has various applications in physics and engineering, such as calculating work done by forces, fluid flow and curl.

In this article, You will get to know about Green’s Theorem, What it is, Its Statement, Green’s Theorem Proof, Finding closed curved area using Green’s theorem, Difference between Green Theorem and Strokes Theorem, Green Theorem Example and Problems with Solutions and much more.

What is Green’s Theorem?

Green’s theorem is a fundamental concept in vector calculus. It essentially relates the work done by a vector field around a closed curve (line integral) to the circulation or “swirliness” of the field within the area enclosed by that curve (double integral).

Important aspects of Green’s Theorem include:

  • It applies in two dimensions (think xy-plane).
  • It connects a line integral around a simple closed curve C to a double integral over the flat region D enclosed by C.
  • Line integral represents the total work done by the vector field as you traverse the curve.
  • Double integral captures the net circulation of the vector field within the region D.

Green’s Theorem Statement

The formal statement of Green’s theorem can be expressed mathematically:

Let C be a simple, closed, positively oriented curve bounding a simply connected region D in the xy-plane. If P(x, y) and Q(x, y) have continuous partial derivatives throughout D, then the line integral around C of P dx + Q dy is equal to the double integral over D of ∂Q/∂x – ∂P/∂y dA:

C (P dx + Q dy) = ∫∫D (∂Q/∂x – ∂P/∂y) dA

where,

  • C: Simple, closed curve (a single loop without any holes)
  • D: Simply connected region (no “islands” inside) enclosed by C
  • P(x, y) and Q(x, y): Functions representing the vector field
  • ∂Q/∂x and ∂P/∂y: Partial derivatives of P and Q
  • dA: Area element (infinitesimal area unit)

Note:

  • Curve C is assumed to be traversed in a positively oriented direction, which means counter-clockwise.
  • Double integral represents the difference between the rate of change of Q concerning x and the rate of change of P concerning y across the entire region of D.

Green’s Theorem Proof

Green’s Theorem relates a line integral around a simple closed curve to a double integral over the region it encloses. It is stated as:

C​(Pdx + Qdy) = ∬R​(∂x/∂Q​ − ∂y/∂P​)dA

where:

  • C is a positively oriented, simple closed curve in the plane.
  • R is the region enclosed by C.
  • P and Q are functions of (x,y).
  • ∂y/∂P​ and ∂Q/∂x are the partial derivatives of Pand Q concerning y and x, respectively.
  • dA denotes the area element.
Green's-Theorem

Proof:

Setup Line Integral: Consider the line integral of a vector field F = (P, Q) around the curve C:

C​F⋅dr = ∮C​(Pdx + Qdy)

Divide Region: Divide the region R enclosed by C into small regions ΔAi.

Apply Divergence Theorem in 2D: Use the divergence theorem (also known as Gauss’s theorem in 2D) on each small region ΔAi.

∬ΔAi​​(∂x/∂Q ​− ∂y/∂P​)dA = ∮∂ΔAi​​(Pdx + Qdy)

Sum Over Entire Region: Summing over all small regions ΔAi, the line integrals around the boundaries of these regions cancel out with adjacent regions due to their opposite orientations (assuming C is positively oriented), leaving:

C​(Pdx + Qdy) = ∬R​(∂x/∂Q​ − ∂y/∂P​)dA

This completes the proof of Green’s Theorem. It establishes the equivalence between the line integral of a vector field around a closed curve C and the double integral of the curl (or circulation density) of the vector field over the region R enclosed by C.

Green’s Theorem: Closed Curved Area

To find the area enclosed by a closed curve C using Green’s Theorem, we can use the following approach:

C(P dx + Q dy) = ∬R( ∂Q / ∂x − ∂P / ∂y) dA

where:

  • C is a positively oriented, simple closed curve in the plane.
  • R is the region enclosed by C.
  • P and Q are functions of (x, y)
  • ∂P/∂y​ and ∂Q/∂x are the partial derivatives of P and Q concerning y and x, respectively.
  • dA denotes the area element.

Finding Area:

To find the area A enclosed by the closed curve C:

Choose P and Q: Choose P(x,y)=0 and Q(x,y)=x

Here, P(x, y) = 0 simplifies the dx term in the line integral, making it vanish, while Q(x,y)=x integrates to find the area in the y direction.

Apply Green’s Theorem: According to Green’s Theorem

C​(Pdx+Qdy) =∬R​(∂x/∂Q​ − ∂y/∂P​)dA

Substitute P(x,y) and Q(x,y):

C​(0⋅dx + x⋅dy) = ∬R​(∂x / ∂(x) ​− ∂y/ ∂(0)​)dA

C​xdy = ∬R​1dA

Evaluate Line Integral:

The line integral ∮Cxdy represents the area enclosed by C

Cxdy = Area(R) = A

Therefore, by Green’s Theorem, the area A enclosed by the closed curve C can be found by evaluating the line integral Cxdy.

Difference Between Green’s Theorem and Strokes Theorem

Various difference between Green’s theorem and strokes theorem are added in the table below:

Feature

Green’s Theorem

Stokes’ Theorem

Context

Applies in the plane (2 dimensions)

Applies in three-dimensional space (3 dimensions).

Type of Integral

Relates a line integral around a closed curve to a double integral over the region it encloses.

Relates a line integral of a vector field around a closed curve to a surface integral of the curl of the vector field over the surface of its bounds.

Dimension

2-dimensional theorem.

3-dimensional theorem

Field Type

Typically applied to conservative vector fields (where curl is zero).

Generally applied to any sufficiently smooth vector field.

Formal Statement

C​(Pdx+Qdy) = ∬R​(∂x/∂Q​−∂y/∂P​)dA

C​F⋅dr=∬S​(∇×F)⋅dS

Fields Involved

Involves a vector field F = (P, Q)

Involves a vector field F = (F1, F2, F3)

Curl Condition

Does not require the vector field to have a non-zero curl.

Requires the vector field to have a well-defined curl (non-zero in some regions).

Application Example

Calculation of area enclosed by a curve in the plane.

Calculation of flux through a surface in three-dimensional space.

Physical Interpretation

Relates circulation (or line integral) to area (or double integral).

Relates circulation around a curve to flux through a surface.

Green’s Theorem Example

Example: Use Green’s Theorem to calculate the work done by a force field F(x, y) = (y2, 2xy) around a closed rectangular path in the xy-plane.

Solution:

Step 1: Define Path and Force Field

We’re given a force field F(x, y) = (y2, 2xy) and a rectangular path. Let’s define the rectangle with:

  • Starting point: (x1, y1) = (1, 1)
  • Ending point: (x2, y2) = (2, 3)

This creates a rectangle with side lengths of 1 unit (x2 – x1) and 2 units (y2 – y1). We’ll assume a counter-clockwise direction around the rectangle.

Step 2: Verify Green’s Theorem Requirements

  • Path is a simple, closed curve (rectangle).
  • It encloses a simply connected region (no “holes” inside the rectangle).
  • Force field F(x, y) has continuous partial derivatives throughout the rectangle (y2 and 2xy are both continuous everywhere).

Therefore, Green’s theorem can be applied to this scenario.

Step 3: Apply Green’s Theorem

We can either evaluate the line integral directly or use Green’s theorem to convert it into a double integral. Here, we’ll use Green’s theorem:

C F(x, y) • dr = ∫∫D (∂Q/∂x – ∂P/∂y) dA

Step 4: Find Partial Derivatives

We need ∂Q/∂x and ∂P/∂y:

  • ∂Q/∂x = 2y (partial derivative of 2xy w.r.t. x)
  • ∂P/∂y = 2y (partial derivative of y^2 w.r.t. y)

Step 5: Convert Line Integral to Double Integral

Plugging the partial derivatives into Green’s theorem:

∫∫D (2y – 2y).dA = 0.dA

Since ∂Q/∂x – ∂P/∂y cancels out, the double integral becomes zero across the entire area.

Step 6: Interpretation

Green’s theorem tells us that in this case, the work done by the force field F around the closed rectangular path is zero.

Green’s Theorem Applications

Green’s theorem has various applications in physics, engineering, and mathematics. Here are some key examples:

  • Calculating Work Done by Forces: Imagine a force field acting on an object along a closed path. Green’s theorem can be used to relate the line integral of the force (work done) around the path to the double integral of a quantity related to the circulation of the force field within the enclosed area.
  • Fluid Flow: Green’s theorem can be applied to analyze two-dimensional fluid flow. By considering a velocity field representing the fluid’s motion, the theorem can help calculate the net circulation of the fluid around a closed curve or the total outward flux across the curve.
  • Area Enclosed by a Curve: In a simpler form, Green’s theorem can be used to calculate the area enclosed by a simple closed curve. By setting one of the component functions in the line integral to zero and using a specific circulation property, the double integral reduces to calculating the area.

Green’s Theorem Problems and Solutions

Problem 1: Calculating Work Done: A force field F(x, y) = (2xy, y2) acts in the xy-plane. Calculate the work done by this force field along a positively oriented square path with a of side length 1 unit, starting at the point (0, 0).

Solution:

C F • dr

where C is the square path. Green’s theorem allows us to convert this into a double integral:

∫∫D (∂Q/∂x – ∂P/∂y) dA

where D is the area enclosed by the square path (unit square), P(x, y) = 2xy (from F’s first component), Q(x, y) = y2 (from F’s second component), and dA is the area element.

Find Partial Derivatives:

∂Q/∂x = 2y (partial derivative of y2 w.r.t. x) ∂P/∂y = 2x (partial derivative of 2xy w.r.t. y)

Evaluate Double Integral:

∫∫D (2y – 2x) dA

Since the square path is from (0, 0) to (1, 1) with constant side length, we can directly evaluate the double integral:

[Tex]∫_0^1 [/Tex][Tex]∫_0^1[/Tex] (2y – 2x) dy dx = 0

Interpretation:

Work done by the force field around the closed square path is zero. This could be because the force field is conservative in this scenario, or because the square path itself creates cancelling effects along opposite sides.

Problem 2: Findin Area Enclosed by a Curve: Find the area enclosed by the curve C defined by x^2 + y^2 = 4 (circle centred at the origin with radius 2) using Green’s theorem.

Solution:

Green’s Theorem for Area: We can use a special case of Green’s theorem where one function in the line integral is zero. Here, we set P(x, y) = 0 and Q(x, y) = x. The double integral then becomes:

∫∫D ∂Q/∂x dA = ∫∫D dA

which essentially calculates the area enclosed by the curve C.

Line Integral and Double Integral: The line integral becomes:

C 0 dx + x dy

Partial Derivative:

∂Q/∂x = 1 (partial derivative of x w.r.t. x)

Evaluate Double Integral:

We can use the standard formula for the area of a circle (πr^2) since Green’s theorem essentially converts the line integral into calculating the area:

∫∫D dA = π × 22 = 4π

Interpretation:

Area enclosed by the circle x2 + y2 = 4 is 4π square units.

Problem 3: Fluid Flow: A two-dimensional fluid flow has a velocity field F(x, y) = (y, -2x). Consider a rectangular path in the xy-plane with vertices at (0, 0), (1, 0), (1, 2), and (0, 2).

  • (a) Calculate the circulation of the fluid around the rectangular path using Green’s theorem.
  • (b) Interpret the result in terms of the fluid flow.

Solution:

(a) We can directly apply Green’s theorem. Here’s the breakdown:

  • P(x, y) = y (from F’s first component)
  • Q(x, y) = -2x (from F’s second component)

We need to find ∂Q/∂x – ∂P/∂y = -2 – 1 = -3

Green’s theorem states:

C F • dr = ∫∫D (-3) dA

where C is the rectangular path and D is the area it encloses.

Since the path is a rectangle with constant side lengths, we can directly evaluate the double integral:

[Tex]∫_0^1 [/Tex][Tex]∫_0^2[/Tex] (-3) dy.dx = -6

Interpretation:

(b) Negative value (-6) for the circulation indicates that the fluid has a net counter-clockwise flow around the rectangle.

The circulation represents the total “turning tendency” of the fluid along the closed path. A negative value signifies counter-clockwise circulation in this context.

Also Read:

FAQs on Green’s Theorem

What is the Use of Green’s Theorem?

Green’s Theorem is commonly used for the integration of lines when combined with a curved plane. It is used to integrate the derivatives in a plane. If the line integral is given, it is converted into the surface integral or the double integral or vice versa with the help of this theorem.

Who Invented the Green Theorem?

It is named after George Green, who stated a similar result in an 1828 paper titled An Essay on the Application of Mathematical Analysis to the Theories of Electricity and Magnetism. In 1846, Augustin-Louis Cauchy published a paper stating Green’s theorem as the penultimate sentence.

Where is Green’s theorem used in real life?

Some of applications of Greens’s Theorem include:

  • Calculating the area of irregular shapes.
  • Determining the circulation and flux of fluid across a surface in engineering tasks.
  • Facilitating the analysis of electromagnetism field flux in physics.

What are Both Forms of Green’s Theorem?

There are two primary forms of Green’s Theorem:

  • Circulation Form
  • Flux Form

What is the Unit of Green’s Function?

The unit of a Green’s function depends on the context in which it is used and the specific type of differential equation it is associated with. Generally, Green’s functions are used to solve linear differential equations, and their units are determined by the differential operator they are associated with and the nature of the source term.




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