Using a line integral to find the work done by a vector field example | Khan Academy
TLDRThis video script delves into the concept of work done by a vector field on a moving particle along a path, specifically a counterclockwise circle. The vector field is defined in the x-y plane with a function associating a force vector with every point. The particle's path is parameterized by cosine and sine functions, creating a circular motion. Through mathematical analysis, it's demonstrated that the work done by the field is negative, indicating the field opposes the particle's motion. The script effectively illustrates the application of vector calculus in physics.
Takeaways
- ๐ The concept being discussed is the work done by a vector field on an object moving along a path within the field.
- ๐ฑ The vector field is defined over the x-y plane, associating a vector with every point, specifically y times i minus x times j.
- ๐ผ๏ธ The vector field is visualized as force vectors at various points, such as (1,0) resulting in a vector of -1j and (2,0) resulting in a vector of -2j.
- ๐ The example path of the object is a counterclockwise circle described by the parameterization x(t) = cos(t) and y(t) = sin(t) from t = 0 to t = 2ฯ.
- ๐ฃ๏ธ The work done by the vector field is calculated using a line integral, which involves the dot product of the vector field and the differential of the path's movement.
- ๐ฏ The derivative of the position vector function with respect to time (dr/dt) is determined to facilitate the calculation of the line integral.
- ๐ข The dot product of the vector field and dr results in an expression that can be integrated over the path of the object.
- ๐ The field is observed to oppose the motion of the object at every point, suggesting that the work done by the field will be negative.
- ๐ The integral simplifies to the integral of 1 with respect to t from 0 to 2ฯ, which evaluates to -2ฯ, confirming the field's opposition to the object's motion.
- ๐ก The result of the work done calculation reinforces the concept that negative work corresponds to a force opposing the motion of an object.
Q & A
What is the vector field described in the script defined over?
-The vector field is defined over R^2 for the x-y plane.
What is the specific vector field given in the example?
-The vector field is given by y times the unit vector i minus x times the unit vector j.
How is the force vector represented at the point (1, 0) in the x-y plane?
-At the point (1, 0), the force vector is represented as 0i - 1j, which looks like a vector pointing straight down along the negative y-axis.
What is the parameterization of the curve c that describes the path of the particle?
-The parameterization of the curve c is x(t) = cos(t) and y(t) = sin(t), where t ranges from 0 to 2ฯ.
What does the parameterization of the curve c represent?
-The parameterization represents a counterclockwise circle with a radius of 1 unit.
How is the work done by the vector field on the curve defined?
-The work done by the vector field on the curve is defined as the line integral over the contour of the field, which is the dot product of the vector field and the differential of the movement dr.
What is the expression for the differential of the position vector dr in terms of t?
-The differential of the position vector dr in terms of t is given by dr = -sin(t)dt * i + cos(t)dt * j.
How is the vector field f(t) expressed in terms of the parameterization of the curve c?
-The vector field f(t) is expressed as f(t) = sin(t)i - cos(t)j, using the values of y(t) and x(t) from the curve's parameterization.
What is the result of the line integral for the work done by the field on the particle?
-The result of the line integral for the work done by the field on the particle is -2ฯ.
What does the negative result of the work done indicate?
-The negative result indicates that the field is doing work against the direction of the particle's motion, hindering its movement around the circle in a counterclockwise direction.
How does the script relate the concept of work done by a field to everyday experiences?
-The script relates the concept by comparing it to lifting an object against gravity, where gravity does negative work while the person applies a force to do positive work.
Outlines
๐ Introduction to Vector Field Work
This paragraph introduces the concept of work done by a vector field on a moving object. It describes a vector field defined over the x-y plane, associating a vector with every point. The vector field is given by y times the unit vector i minus x times the unit vector j. The paragraph then sets up a scenario where a particle moves along a path described by a curve c, with its parameterization given by x(t) = cos(t) and y(t) = sin(t), from t = 0 to t = 2ฯ, representing a counterclockwise circle. The goal is to calculate the work done by the vector field on the moving curve.
๐ Negative Work Intuition
In this paragraph, the speaker discusses the intuition behind negative work in the context of the vector field. It is observed that the vector field seems to oppose the motion of the particle at every point along its path. The speaker uses the analogy of lifting an object against gravity, where positive work is done by the person and negative work is done by gravity. The paragraph sets the stage for a mathematical calculation to confirm this intuition and further explore the concept of negative work in the given scenario.
๐งฎ Calculating the Work Done
The final paragraph focuses on the calculation of the work done by the vector field on the moving particle. It begins by finding the derivative of the position vector function with respect to time, dr/dt, and then proceeds to calculate the differential dr. The vector field is then rewritten in terms of t to find the force from the field along the path. The line integral is set up as an integral from 0 to 2ฯ of the dot product of the field and the differential movement. After performing the dot product and integrating, the result simplifies to the integral of 1 with respect to t from 0 to 2ฯ, which evaluates to -2ฯ. This confirms the negative work done by the field, as it opposes the particle's motion.
Mindmap
Keywords
๐กVector Field
๐กWork Done
๐กLine Integral
๐กParameterization
๐กCounterclockwise Circle
๐กDifferential dr
๐กDot Product
๐กUnit Vectors i and j
๐กNegative Work
๐กTrigonometric Functions
๐กAntiderivative
Highlights
The application of vector field work on a particle moving along a path is discussed.
The vector field is defined over the x-y plane with a function of x and y.
The vector field associates a force vector with every point on the plane.
A specific vector field is given, where y times the unit vector i is subtracted by x times the unit vector j.
The force vector at the point (1, 0) is described as -1 j.
The vector field is visualized across the x-y plane with varying points.
A particle's path is described by a curve c, parameterized by x(t) = cos(t) and y(t) = sin(t).
The path of the particle is a counterclockwise circle from t=0 to t=2ฯ.
The work done by the vector field on the curve is calculated using a line integral.
The differential dr is derived from the parameterization of the path.
The vector field is rewritten in terms of t to match the path's parameterization.
The dot product of the vector field and the differential dr is calculated.
The work done by the field is found to be negative, indicating opposition to the particle's movement.
The negative work is analogous to gravity doing negative work when lifting an object.
The line integral is simplified to an integral of 1 with respect to t from 0 to 2ฯ.
The final result of the work done by the field is -2ฯ, confirming the field's oppositional force.
The process provides a concrete example of the theoretical concepts discussed in the previous video.
The mathematical derivation and visualization help to understand the interaction between the vector field and the particle's motion.
Transcripts
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