Study Notes on Vector Calculus and Analytical Geometry - Code 198701008

Core Vector Properties and Operations

  • Unit Normal Vectors to a Plane     - A unit normal to the plane defined by two vectors, a\vec{a} and b\vec{b}, is calculated by taking the cross product a×b\vec{a} \times \vec{b} and dividing by its magnitude.     - Given vectors:         - a=i+2j+3k\vec{a} = \vec{i} + 2\vec{j} + 3\vec{k}         - b=i+j+2k\vec{b} = \vec{i} + \vec{j} + 2\vec{k}     - Potential solutions provided:         - a) i+jk\vec{i} + \vec{j} - \vec{k}         - b) 13(i+2jk)\frac{1}{\sqrt{3}}(\vec{i} + 2\vec{j} - \vec{k})         - c) 13(i+2j+k)\frac{1}{\sqrt{3}}(\vec{i} + 2\vec{j} + \vec{k})         - d) 13(i+j+k)\frac{1}{\sqrt{3}}(\vec{i} + \vec{j} + \vec{k})         - e) 13(i+jk)\frac{1}{\sqrt{3}}(\vec{i} + \vec{j} - \vec{k})

  • Scalar Projection     - The scalar projection of vector b\vec{b} on vector a\vec{a} is defined as compab=aba\text{comp}_{\vec{a}}\vec{b} = \frac{\vec{a} \cdot \vec{b}}{|\vec{a}|}.     - Given vectors:         - a=i+jk\vec{a} = \vec{i} + \vec{j} - \vec{k}         - b=2i+4j+3k\vec{b} = 2\vec{i} + 4\vec{j} + 3\vec{k}     - Possible values for the scalar projection:         - a) 3\sqrt{3}         - b) 13\frac{1}{\sqrt{3}}         - c) 3-\sqrt{3}         - d) 13-\frac{1}{\sqrt{3}}         - e) 11

  • Relationships Between Vectors and Angles     - If several vectors sum to zero (a+b+c=0\vec{a} + \vec{b} + \vec{c} = \vec{0}), the law of cosines for vectors can be applied to find internal angles.     - Specific magnitudes provided:         - a=3\left|\vec{a}\right| = 3         - b=5\left|\vec{b}\right| = 5         - c=7\left|\vec{c}\right| = 7     - The angle between a\vec{a} and b\vec{b} is queried among options:         - a) 6060^{\circ}         - b) 4545^{\circ}         - c) 3030^{\circ}         - d) 9090^{\circ}         - e) none of these

  • Vector Linear Combinations     - Analysis of non-collinear vectors a\vec{a} and b\vec{b}.     - Given equations for vectors v\vec{v} and w\vec{w} involving variables xx and yy:         - v=xa+(yx)b\vec{v} = x\vec{a} + (y - x)\vec{b}         - w=(2x+y+3)a(x+2y)b\vec{w} = (2x + y + 3)\vec{a} - (x + 2y)\vec{b}     - If the condition 3v=w3\vec{v} = \vec{w} is met, the values of xx and yy can be solved by comparing coefficients of a\vec{a} and b\vec{b}.     - Options for solutions:         - a) x=10,y=3x = 10, y = 3         - b) x=15,y=4x = 15, y = -4         - c) x=5,y=2x = 5, y = 2         - d) x=4,y=5x = 4, y = -5         - e) none of these

Analytical Geometry of Lines and Planes

  • Intersection of a Line and a Plane     - A line r=(1+2t)i+tj+(1t)k\vec{r} = (1 + 2t)\vec{i} + t\vec{j} + (1 - t)\vec{k} (where tRt \in \mathbb{R}) intersects a plane defined by 2x+yz=72x + y - z = 7.     - The intersection point is found by substituting the parametric components (x=1+2tx=1+2t, y=ty=t, z=1tz=1-t) into the plane equation and solving for tt.     - Point options:         - a) (3,1,0)(-3, 1, 0)         - b) (1,7,0)(1, 7, 0)         - c) (3,1,0)(3, 1, 0)         - d) (3,1,0)(3, -1, 0)         - e) (3,1,0)(-3, -1, 0)

  • Deriving the Equation of a Plane     - A plane passing through the point (1,1,3)(1, -1, 3) and perpendicular to the vector i+3j4k\vec{i} + 3\vec{j} - 4\vec{k}.     - The standard equation of the plane follows the form A(xx0)+B(yy0)+C(zz0)=0A(x - x_0) + B(y - y_0) + C(z - z_0) = 0.     - Formula options:         - a) x3y4z=14x - 3y - 4z = 14         - b) x3y4z=14x - 3y - 4z = -14         - c) x+3y+4z=14x + 3y + 4z = -14         - d) x+3y4z=14x + 3y - 4z = -14         - e) x+3y4z=14-x + 3y - 4z = 14

  • Condition for a Line to Lie within a Plane     - Consider the line r(t)=t(2i+cj+3k)\vec{r}(t) = t(2\vec{i} + c\vec{j} + 3\vec{k}) and the plane x+3y+5z=0x + 3y + 5z = 0.     - For the line to lie entirely within the plane, the dot product of the direction vector of the line and the normal vector of the plane must be zero, and the line must contain a point on the plane (in this case, the origin (0,0,0)(0,0,0)).     - Values for cc to satisfy the condition:         - a) 13/3-13/3         - b) 11/5-11/5         - c) 17/317/3         - d) 17/3-17/3         - e) none of these

  • Tetrahedron Volume Calculations     - The volume VV of a tetrahedron with vertices A,B,C,A, B, C, and DD is given by 16(AB×AC)AD\frac{1}{6} |(\vec{AB} \times \vec{AC}) \cdot \vec{AD}|     - Coordinates provided:         - A=(1,0,2)A = (1, 0, 2)         - B=(1,2,2)B = (-1, 2, 2)         - C=(1,1,3)C = (1, 1, -3)         - D=(4,0,3)D = (4, 0, 3)     - Volume options:         - a) 16/316/3         - b) 1/31/3         - c) 55         - d) 11/311/3         - e) 32/332/3

Advanced Vector Calculus Operators

  • Vector Field Operations     - Cross multiplication of vector sums: (v+p)×w(\vec{v} + \vec{p}) \times \vec{w}.     - Components:         - v=i2j+3k\vec{v} = \vec{i} - 2\vec{j} + 3\vec{k}         - w=i+j+2k\vec{w} = -\vec{i} + \vec{j} + 2\vec{k}         - p=2i+2j3k\vec{p} = 2\vec{i} + 2\vec{j} - 3\vec{k}     - Possible result vectors:         - a) 7i+10j+3k-7\vec{i} + 10\vec{j} + 3\vec{k}         - b) 7i+3k7\vec{i} + 3\vec{k}         - c) 6j+3k-6\vec{j} + 3\vec{k}         - d) 3-3         - e) 6j+3k6\vec{j} + 3\vec{k}

  • Divergence and Gradient Identities     - Calculation of div(grad r3)\text{div}(\text{grad } r^3), where r=xi+yj+zk\vec{r} = x\vec{i} + y\vec{j} + z\vec{k} and r=rr = |\vec{r}|.     - Possible identities:         - a) 00         - b) 9r9r         - c) 12r12r         - d) 6r6r         - e) 3r3r

  • Combinations of Operators (Divergence, Curl, Gradient)     - Discussion of which operator combinations resulting in meaningful expressions where F\vec{F} is a vector field and ff is a scalar function:         - a) div(div F)\text{div}(\text{div } \vec{F}) (meaningless as divergence results in a scalar, and you cannot take the divergence of a scalar).         - b) curl(div F)\text{curl}(\text{div } \vec{F}) (meaningless for the same reason).         - c) grad(grad F)\text{grad}(\text{grad } \vec{F}).         - d) grad(grad f)\text{grad}(\text{grad } f).         - e) curl(curl F)\text{curl}(\text{curl } \vec{F}).

  • Solenoidal Vector Fields     - A vector field F\vec{F} is solenoidal if div F=0\text{div } \vec{F} = 0.     - Vector field: F=(x+3y)i+(y3z)j+(y+mz)k\vec{F} = (x + 3y)\vec{i} + (y - 3z)\vec{j} + (y + mz)\vec{k}.     - The condition for F\vec{F} being solenoidal determines the constant mm:         - a) 00         - b) 11         - c) 1-1         - d) 22         - e) 2-2

  • Curl Calculation at a Point     - Determining curl F\text{curl } \vec{F} for F=ze2xyi+2xycos(y)j+(x+2y)k\vec{F} = ze^{2xy}\vec{i} + 2xy\cos(y)\vec{j} + (x + 2y)\vec{k}.     - Specifically evaluated at point (2,0,3)(2, 0, 3).     - Options:         - a) 2i12k2\vec{i} - 12\vec{k}         - b) 2i12k-2\vec{i} - 12\vec{k}         - c) 3k-3\vec{k}         - d) 3i12k3\vec{i} - 12\vec{k}         - e) 3i12k-3\vec{i} - 12\vec{k}

Multi-Variable Calculus and Surfaces

  • Functions and Domains     - Function: f(x,y,z)=x11y+ln(4x2y2z2)f(x, y, z) = \frac{\sqrt{x - 1}}{\sqrt{1 - y}} + \ln(4 - x^2 - y^2 - z^2).     - Domain constraints:         - The numerator x1\sqrt{x - 1} requires x1x \geq 1.         - The denominator 1y\sqrt{1 - y} requires 1 - y > 0 (since it is in the denominator, it cannot be zero), hence y<1y < 1.         - The natural logarithm ln(4x2y2z2)\ln(4 - x^2 - y^2 - z^2) requires the argument to be positive: x2+y2+z2<4x^2 + y^2 + z^2 < 4.     - Domain sets:         - a) (x,y,z)R3:y1(x, y, z) \in \mathbb{R}^3 : y \neq 1         - b) (x,y,z)R3:x<1,2<y<1(x, y, z) \in \mathbb{R}^3 : x < 1, -2 < y < 1 and x2+y2+z2>4x^2 + y^2 + z^2 > 4         - c) (x, y, z) \in \mathbb{R}^3 : -1 < x < 2 and -1 < y < 0         - d) (x, y, z) \in \mathbb{R}^3 : 1 < x < 2, -2 < y < 1 and x2+y2+z24x^2 + y^2 + z^2 \leq 4         - e) (x, y, z) \in \mathbb{R}^3 : 1 \leq x < 2, -2 < y < 1 and x^2 + y^2 + z^2 < 4

  • Tangent Plane to a Surface     - Surface equation: x2+2y2+3z2=36x^2 + 2y^2 + 3z^2 = 36.     - Evaluation point P=(1,2,3)P = (1, 2, 3).     - The gradient f\nabla f at the point provides the normal vector to the tangent plane.     - Plane equation options:         - a) 2x+8y+18z=722x + 8y + 18z = -72         - b) x4yz=10x - 4y - z = 10         - c) 2x+8y+18z=722x + 8y + 18z = 72         - d) x+4yz=10x + 4y - z = 10         - e) x+4y+z=10x + 4y + z = 10

  • Directional Derivatives     - Function: f(x,y,z)=2x2+3y2+z2f(x, y, z) = 2x^2 + 3y^2 + z^2.     - Calculation point: P=(2,1,3)P = (2, 1, 3).     - Direction vector: i2k\vec{i} - 2\vec{k}.     - The directional derivative is f(P)u\nabla f(P) \cdot \vec{u}, where u\vec{u} is the unit vector in the specified direction.     - Result options:         - a) 25-\frac{2}{\sqrt{5}}         - b) 45\frac{4}{\sqrt{5}}         - c) 25\frac{2}{\sqrt{5}}         - d) 205\frac{20}{\sqrt{5}}         - e) 45-\frac{4}{\sqrt{5}}

Kinematics and Curve Properties

  • Acceleration Components     - Particle position function: r(t)=cos(t)i+sin(t)j+cos2(t)k\vec{r}(t) = \cos(t)\vec{i} + \sin(t)\vec{j} + \cos^2(t)\vec{k}.     - Goal: Find the tangential component of acceleration (aTa_T) at time t=π4t = \frac{\pi}{4}.     - Defined as aT=vava_T = \frac{\vec{v} \cdot \vec{a}}{|\vec{v}|}.     - Options: 0,1,2,3,40, 1, 2, 3, 4.

  • Osculating Plane     - Curve definition: r(t)=(t32sin(t))i+(132cos(t))j+tk\vec{r}(t) = (t - \frac{3}{2}\sin(t))\vec{i} + (1 - \frac{3}{2}\cos(t))\vec{j} + t\vec{k}.     - Point of interest: (π,52,π)(\pi, \frac{5}{2}, \pi).     - The osculating plane contains the velocity vector r(t)\vec{r}'(t) and the acceleration vector r(t)\vec{r}''(t).     - Cartesian equation options:         - a) 2x5z=3π2x - 5z = -3\pi         - b) 2y+z=1π2y + z = 1\pi         - c) 2x+5z=3π2x + 5z = 3\pi         - d) 2x+5z=1π2x + 5z = 1\pi         - e) 2x5z=3π2x - 5z = 3\pi

  • Line Integrals and Arc Length     - Conservative Fields:         - F=(yz)i+(zx)j+(xy)k\vec{F} = (yz)\vec{i} + (zx)\vec{j} + (xy)\vec{k}.         - Line integral result for any path joining A=(1,1,1)A = (1, 1, 1) and B=(1,2,0)B = (-1, 2, 0).         - Integral output options: 1,0,5,5,11, 0, 5, -5, -1.     - Arc Length Formula:         - For curve r(t)=ti+t2j+t3k\vec{r}(t) = t\vec{i} + t^2\vec{j} + t^3\vec{k} for 0t10 \leq t \leq 1.         - Formula options:             - a) 01t2+t4+t6dt\int_0^1 \sqrt{t^2 + t^4 + t^6} dt             - b) 011+4t2+9t4dt\int_0^1 \sqrt{1 + 4t^2 + 9t^4} dt             - c) 011+2t2+3t6dt\int_0^1 \sqrt{1 + 2t^2 + 3t^6} dt             - d) 01t+t2+t6dt\int_0^1 \sqrt{t + t^2 + t^6} dt             - e) 011+2t+3t2dt\int_0^1 \sqrt{1 + 2t + 3t^2} dt

Descriptive Geometry and Vector Fields

  • Analysis of Plane Alpha (α\alpha)     - Vector equation: r=(3i+3j+2k)+λ(i+2j+k)+μ(2i+k)\vec{r} = (3\vec{i} + 3\vec{j} + 2\vec{k}) + \lambda(-\vec{i} + 2\vec{j} + \vec{k}) + \mu(2\vec{i} + \vec{k}).     - Perpendicularity check: Show that vector 2i+3j4k2\vec{i} + 3\vec{j} - 4\vec{k} is perpendicular to plane α\alpha (calculated via the cross product of direction vectors d1×d2\vec{d_1} \times \vec{d_2}).     - Cartesian form derivation of plane α\alpha.     - Shortest distance application:         - Line l:r=(4i5j+2k)+t(i+6j3k)l: \vec{r} = (4\vec{i} - 5\vec{j} + 2\vec{k}) + t(\vec{i} + 6\vec{j} - 3\vec{k}).         - Point AA lies on line ll.         - The shortest distance from AA to α\alpha is exactly 2292\sqrt{29}.         - Task involves finding possible coordinates of AA.

  • Work and Flux Theorems     - Work Done:         - Force field F(x,y,z)=y2i+(3x6y)j\vec{F}(x, y, z) = y^2\vec{i} + (3x - 6y)\vec{j}.         - Displacement: Line segment from (3,7)(3, 7) to (0,12)(0, 12).         - Calculated as W=CFdrW = \int_C \vec{F} \cdot d\vec{r}.     - Divergence Theorem Verification:         - Field F(x,y,z)=(x3yz)i2x2yj+zk\vec{F}(x, y, z) = (x^3 - yz)\vec{i} - 2x^2y\vec{j} + z\vec{k}.         - Volume: Cube bounded by planes x=y=z=ax = y = z = a and the coordinate planes (x=0,y=0,z=0x=0, y=0, z=0).         - Requires computing the surface integral SFdS\iint_S \vec{F} \cdot d\vec{S} and comparing it to the volume integral Vdiv FdV\iiint_V \text{div } \vec{F} dV.