Vector fields assign vectors to points in space, representing physical quantities like force or velocity. They're visualized using arrow plots in 2D or 3D, with components defined by scalar functions in each direction.
Line integrals measure accumulated effects along curves in vector fields. They're computed by parameterizing curves and evaluating single-variable integrals. The Fundamental Theorem of Line Integrals simplifies calculations for conservative fields, while work in force fields is calculated using line integrals.
Vector Fields
Vector fields in multiple dimensions
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Conservative Vector Fields · Calculus View original
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Vector field assigns vector to each point in space representing physical quantities (force, velocity, electric field)
Two-dimensional vector fields expressed as F ( x , y ) = P ( x , y ) i + Q ( x , y ) j \mathbf{F}(x, y) = P(x,y)\mathbf{i} + Q(x,y)\mathbf{j} F ( x , y ) = P ( x , y ) i + Q ( x , y ) j visualized using arrow plots on 2D plane
Three-dimensional vector fields expressed as F ( x , y , z ) = P ( x , y , z ) i + Q ( x , y , z ) j + R ( x , y , z ) k \mathbf{F}(x, y, z) = P(x,y,z)\mathbf{i} + Q(x,y,z)\mathbf{j} + R(x,y,z)\mathbf{k} F ( x , y , z ) = P ( x , y , z ) i + Q ( x , y , z ) j + R ( x , y , z ) k visualized using arrow plots in 3D space
Components of vector fields defined by scalar functions in each direction
Continuity and smoothness of vector fields ensure no abrupt changes or discontinuities
Vector fields applied in physics and engineering (electromagnetic fields, fluid flow, gravitational fields)
Line Integrals
Line integrals along curves
Line integrals integrate along curve or path in vector field measuring accumulated effect
Curves parameterized as function of parameter t t t to describe path mathematically
Line integral formulas: scalar fields ∫ C f ( x , y , z ) d s \int_C f(x,y,z) ds ∫ C f ( x , y , z ) d s , vector fields ∫ C F ⋅ d r \int_C \mathbf{F} \cdot d\mathbf{r} ∫ C F ⋅ d r
Computation process:
Parameterize curve
Express integrand in terms of parameter
Evaluate resulting single-variable integral
Line integrals independent of parameterization choice
Orientation of curves affects sign of line integral result
Fundamental theorem of line integrals
Theorem states ∫ C ∇ f ⋅ d r = f ( b ) − f ( a ) \int_C \nabla f \cdot d\mathbf{r} = f(b) - f(a) ∫ C ∇ f ⋅ d r = f ( b ) − f ( a ) for conservative vector fields
Conservative vector fields have path-independent line integrals
Potential functions found for conservative fields by integrating components
Theorem applications simplify calculations and prove path independence
Curl test in two and three dimensions determines if field is conservative
Work in force fields
Work calculated as line integral W = ∫ C F ⋅ d r W = \int_C \mathbf{F} \cdot d\mathbf{r} W = ∫ C F ⋅ d r in force fields
Force fields in physics include gravitational, electromagnetic, and spring forces
Calculation process involves identifying force field and curve, setting up line integral, evaluating using parameterization or Fundamental Theorem
Positive work increases energy of system, negative work decreases energy
Work path-dependent in non-conservative fields (friction)
Energy conserved in conservative force fields (gravitational potential energy)