ANALYTICAL AND GRAPHICAL SOLUTIONS TO PROBLEMS IN DESCRIPTIVE GEOMETRY INVOLVING PLANES AND LINES

Similar documents
FINDING THE TRACES OF A GIVEN PLANE: ANALYTICALLY AND THROUGH GRAPHICAL CONSTRUCTIONS

MATH CALCULUS I 2.1: Derivatives and Rates of Change

Introduction to Derivatives

Bob Brown Math 251 Calculus 1 Chapter 3, Section 1 Completed 1 CCBC Dundalk

qwertyuiopasdfghjklzxcvbnmqwerty uiopasdfghjklzxcvbnmqwertyuiopasd fghjklzxcvbnmqwertyuiopasdfghjklzx cvbnmqwertyuiopasdfghjklzxcvbnmq

Some Review Problems for First Midterm Mathematics 1300, Calculus 1

Differentiation. Area of study Unit 2 Calculus

Average Rate of Change

Chapter 2 Limits and Continuity

The derivative function

Definition of the Derivative

Numerical Analysis MTH603. dy dt = = (0) , y n+1. We obtain yn. Therefore. and. Copyright Virtual University of Pakistan 1

Eva Stanová 1. mail:

lim 1 lim 4 Precalculus Notes: Unit 10 Concepts of Calculus

Section 15.6 Directional Derivatives and the Gradient Vector

Logarithmic functions

1 1. Rationalize the denominator and fully simplify the radical expression 3 3. Solution: = 1 = 3 3 = 2

2.11 That s So Derivative

Exponentials and Logarithms Review Part 2: Exponentials

ON THE CONSTRUCTION OF REGULAR A-OPTIMAL SPRING BALANCE WEIGHING DESIGNS

1 Calculus. 1.1 Gradients and the Derivative. Q f(x+h) f(x)

SECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY

f a h f a h h lim lim

Mathematics 5 Worksheet 11 Geometry, Tangency, and the Derivative

1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point

Solve exponential equations in one variable using a variety of strategies. LEARN ABOUT the Math. What is the half-life of radon?

The algebra of functions Section 2.2

1. State whether the function is an exponential growth or exponential decay, and describe its end behaviour using limits.

LIMITS AND DERIVATIVES CONDITIONS FOR THE EXISTENCE OF A LIMIT

4.2 - Richardson Extrapolation

2.8 The Derivative as a Function

Click here to see an animation of the derivative

Derivatives. By: OpenStaxCollege

Differential Calculus (The basics) Prepared by Mr. C. Hull

158 Calculus and Structures

1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t).

(4.2) -Richardson Extrapolation

Numerical Differentiation

Derivatives of Exponentials

5.1 We will begin this section with the definition of a rational expression. We

Moments and Product of Inertia

1. Which one of the following expressions is not equal to all the others? 1 C. 1 D. 25x. 2. Simplify this expression as much as possible.

lecture 26: Richardson extrapolation

Derivative as Instantaneous Rate of Change

pancakes. A typical pancake also appears in the sketch above. The pancake at height x (which is the fraction x of the total height of the cone) has

DEFINITION OF A DERIVATIVE

Chapter 2. Limits and Continuity 16( ) 16( 9) = = 001. Section 2.1 Rates of Change and Limits (pp ) Quick Review 2.1

INTRODUCTION AND MATHEMATICAL CONCEPTS

Section 2.7 Derivatives and Rates of Change Part II Section 2.8 The Derivative as a Function. at the point a, to be. = at time t = a is

MANY scientific and engineering problems can be

Cubic Functions: Local Analysis

Chapter 2 Limits and Continuity. Section 2.1 Rates of Change and Limits (pp ) Section Quick Review 2.1

A = h w (1) Error Analysis Physics 141

Chapter. Differentiation: Basic Concepts. 1. The Derivative: Slope and Rates. 2. Techniques of Differentiation. 3. The Product and Quotient Rules

1.5 Functions and Their Rates of Change

Recall from our discussion of continuity in lecture a function is continuous at a point x = a if and only if

Midterm #1B. x 8 < < x 8 < 11 3 < x < x > x < 5 or 3 2x > 5 2x < 8 2x > 2

These errors are made from replacing an infinite process by finite one.

Practice Problem Solutions: Exam 1

Combining functions: algebraic methods

We name Functions f (x) or g(x) etc.

= 0 and states ''hence there is a stationary point'' All aspects of the proof dx must be correct (c)

WYSE Academic Challenge 2004 Sectional Mathematics Solution Set

MODEL FOR FLEXIBLE PLATES SUPPORTED ON PILES

MA2264 -NUMERICAL METHODS UNIT V : INITIAL VALUE PROBLEMS FOR ORDINARY DIFFERENTIAL. By Dr.T.Kulandaivel Department of Applied Mathematics SVCE

UNIT #6 EXPONENTS, EXPONENTS, AND MORE EXPONENTS REVIEW QUESTIONS

= h. Geometrically this quantity represents the slope of the secant line connecting the points

Math Module Preliminary Test Solutions

Tangent Lines-1. Tangent Lines

Diffraction. S.M.Lea. Fall 1998

11.6 DIRECTIONAL DERIVATIVES AND THE GRADIENT VECTOR

The total error in numerical differentiation

Chapter XI. Solution of Ordinary Differential Equations

ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER /2019

Space Coordinates and Vectors in Space. Coordinates in Space

REVIEW LAB ANSWER KEY

Lines, Conics, Tangents, Limits and the Derivative

Continuity and Differentiability of the Trigonometric Functions

Derivative at a point

Continuity and Differentiability

SECTION 1.10: DIFFERENCE QUOTIENTS LEARNING OBJECTIVES

In Leibniz notation, we write this rule as follows. DERIVATIVE OF A CONSTANT FUNCTION. For n 4 we find the derivative of f x x 4 as follows: lim

INTRODUCTION TO CALCULUS LIMITS

Lesson 6: The Derivative

Lesson 4 - Limits & Instantaneous Rates of Change

Outline. MS121: IT Mathematics. Limits & Continuity Rates of Change & Tangents. Is there a limit to how fast a man can run?

11-19 PROGRESSION. A level Mathematics. Pure Mathematics

Polynomial Interpolation

A.P. CALCULUS (AB) Outline Chapter 3 (Derivatives)

Polynomial Functions. Linear Functions. Precalculus: Linear and Quadratic Functions

Financial Econometrics Prof. Massimo Guidolin

Outline. Seepage Analysis. Soil Mechanics. Laplace Equation of Continuity

The Derivative The rate of change

The Verlet Algorithm for Molecular Dynamics Simulations

Function Composition and Chain Rules

CHAPTER (A) When x = 2, y = 6, so f( 2) = 6. (B) When y = 4, x can equal 6, 2, or 4.

Sample Problems for Exam II

June : 2016 (CBCS) Body. Load

Polynomial Interpolation

MATH1151 Calculus Test S1 v2a

Transcription:

ULETINUL INSTITUTULUI POLITENI DIN IŞI Publicat de Uniersitatea Tenică George saci din Iaşi Tomul LVII (LXI) Fasc 3 0 Secţia ONSTRUŢII DE MŞINI NLYTIL ND GRPIL SOLUTIONS TO PROLEMS IN DESRIPTIVE GEOMETRY INVOLVING PLNES ND LINES Y PUL GEORGESU bstract Seeral common situations wic occur wen soling problems in descriptie geometr including finding te intersection of two planes passing troug points wit coordinates of a certain form and finding te intersections between particular lines and planes are inestigated troug analtical and grapical metods e words: planes lines traces analtic geometr descriptie geometr Te statement of te problem Of concern in tis paper is te following problem encompassing seeral situations commonl occuring in concrete applications of descriptie geometr Gien te points (00030) (60500) (60040) M(0080) N(60800) R (000) I(80) find: a) te coordinates of I knowing tat tis point is situated on te () line; b) te traces of te plane [P] defined b te lines (I) and (); c) te intersection between te planes [P] and [Q] were [Q] is a plane parallel to (O) wic as traces at distance 5 and eleation 65 respectiel; d) te intersection point between te line ( ) and te plane [ Q ] We sall sole tis problem first b means of analtic geometr briefl discussing te main teoretical points and te formulae concerned and ten b means of descriptie geometr

Paul Georgescu Te analtical approac We first discuss seeral properties of a plane [ Q ] wic is parallel to ( O ) and passes troug Q (0 d0) of distance d and Q (00 e) of eleation e respectiel Namel we sall find te equation of [ Q ] and determine its intersection wit gien lines and planes Te equation of [Q] plane Since two ectors parallel to [ Q ] are i and QQ = dj+ ek te ector nq = i QQ = dk ej is normal to [ Q ] Te equation of [ Q ] is ten d e + D = 0 te constant D being determined troug te condition tat Q belongs to [ Q ] onsequentl te equation of [ Q ] can be written as: () [ Q]: e+ d de= 0 Te intersections of [ Q ] wit lines and planes We find now te intersection of a line determined b two of its points ( ) ( ) and te plane [ Q ] One sees tat te parametric equation of te line ( ) is = = = t tat is [] [5]: () ) : = + t( ) = + t( ) = + t( ) ( t being a real parameter To find te intersection between ( ) and [ Q ] we sole te sstem consisting in Eqs () and () substituting and gien b Eq () into Eq () we find tat: (3) de e d t = e d ( ) + ( ) onsequentl te point of intersection between ( ) and [ Q ] as coordinates: (4) de e d = + e ( ) ( ) ( ) + d

ul Inst Polit Iaşi t LVII (LXI) f 3 0 3 (5) (6) de e d = + e ( ) ( ) ( ) + d de e d = + e ( ) ( ) ( ) + d We find now te intersection between te [ Q ] plane and a [ P] plane determined b ( ) ( ) and ( ) Tis line can be tougt as being determined b te point aboe te intersection between ( ) and [ Q ] and te point te intersection between () and [ Q ] similarit wit Eqs (4)-(6) it is seen tat te coordinates of are gien b: () (8) (9) de e d = + e ( ) ( ) ( ) + d de e d = ( ) ( ) ( ) + e + d de e d = + e + d ( ) ( ) ( ) Ten te intersection ( ) ( D) between [ P] and [ Q ] as te parametric equation: (0) = = = t t R and being gien b Eqs (4)-(6) and ()-(9) 3 Te traces of a plane [P] In wat follows we sall determine te traces of a plane determined b tree of its points on te coordinate planes It can be sown [] tat te traces of a plane [ P ] determined b ( ) ( ) and ( ) ae te following equations: () ( P ) : Δ + Δ = Δ; = 0 () ( P): Δ + Δ =Δ ; = 0 l (3) ( P ): Δ + Δ =Δ ; = 0

4 Paul Georgescu lso [P] intersects te coordinate aes in te points P P P gien b: (4) Δ P = P 00 Δ Δ P Δ = P 0 0 P = P Δ 0 0 Δ (5) Δ = Δ = Δ = (6) Δ = We are now read to sole te problem stated in Section S o l u t i o n a) Since I is situated on te line ( ) its coordinates I I I erif Eq () for a alue of t wic is to be determined From te first part of Eq () it follows tat t = and consequentl tat I = 30 and I = 0 b) Te plane [ P ] can be tougt as being determined b and onsequentl since Δ = 08000 Δ = 600 Δ = 00 and Δ = 00 it follows ten from Eq (4) tat te intersections of [ P ] wit te coordinate aes are P ( 8000) P ( 0900) P ( 0090) O is ( P ) : 90; 0 It also follows from Eqs ()-(3) tat te trace of te plane [ P ] on ( ) + = = te trace of [ P ] on ( O ) is ( P ):+ = 90; = 0 and te trace of [ P ] on ( O ) is ( P): + = 90; = 0 l 5 c) Using Eqs (4)-(6) and Eqs ()-(9) it follows tat = 90 = 65 60 00 95 = and = = = From Eq (0) one ma deduce tat te intersection between te plane [ P ] and te plane [ Q ] is te line ( ) wic as te parametric equation:

ul Inst Polit Iaşi t LVII (LXI) f 3 0 5 () 60 6 = 00 5 95 = 3 = t t R 5 For = 0 it follows tat t = and consequentl te intersection between ( ) and te plane (O) is te point (3050 ) Similarl for = 0 it 0 follows tat t = and te intersection between ( ) and te plane (O) is te point V (50065 ) 60 00 95 d) s seen aboe = = = 3 Descriptie Geometr approac a) ecause te point I is ling on te straigt line () its projections are located on te corresponding projections of te straigt line (Fig ) [4] ence if a point I () it follows tat i (ab) i ( a b ) and i ( a b ) Z(-Y) X a' a i' b' a'' i'' b'' Y(-X) i b Y(-Z) Fig Projections of te point I [3]

l 6 Paul Georgescu Z(-Y) ' P X P ' a' ' a i' c c' b' ' l Y(-X) P i b Y(-Z) P Fig Traces of te plane [P] b) We determine first te projections and b etending te projections (ab) (ci) and (a'b') (c'i') respectiel up to te (O) ais and ten b using te projecting lines we find te traces of gien straigt lines: on (ab) on (ci) and ' on (a'b') on (c'i') respectiel (Fig ) Z(-Y) P ' l X P ' (d) (d') (d") Q Y(-X) P Y(-Z) Fig 3 (D)(dd'd'') te intersection line of planes [P] and [Q] P

l ul Inst Polit Iaşi t LVII (LXI) f 3 0 c) Two concurrent planes [P] and [Q] intersect along a straigt line (D)(dd'd'') (Fig 3) wose traces lie at te intersection of corresponding traces of bot planes (R ) ' 3 (δ ) Q Z(-Y) X R a' 3 a k' a'' k" k ' 3 b' (δ ) b'' Y(-X) 3 Q b (R ) (δ) Y(-Z) Fig 4 te intersection point of ()-[Q] intersection d) We draw an auiliar cutting plane [R] wic contains te gien straigt line and we find te line of intersection of te cutting plane [R] and te gien plane [Q] (Fig 4) Te required point ( k k k ) is at te intersection of te straigt lines ( )( ab a b a b ) and ( Δ )( δ δ δ ) common to bot planes [P] and [R] 4 onclusions s we can see from a comparatie iew of bot solutions presented aboe te one emploing Descriptie Geometr offers a quick and elegant reasoning wic appeals to one s intuition wile te approac based on naltic Geometr altoug more computational offers general formulas wic can be applied to a large class of problems wic are reductible to te ones discussed in tis paper 00 George saci Tecnical Uniersit Department of Matematics Iaşi Romania e-mail: pgeorgescu@gmailcom

8 Paul Georgescu R E F E R E N E S ă r ă u ş u Vector algebra analtic & differential geometr Ed PIM Iaşi 003 G e o r g e s c u P î n c u G Finding te traces of a gien plane: analticall and troug grapical constructions Proceedings of IEGD0 Sustainable Eco-Design -4 june 0 Iaşi ul Inst Polit Iaşi LVII (LXI) Facultatea de onstrucţii de Maşini (0) 3 î n c u G Infografică utod Ed Societăţii cademice Matei Teiu ote Iaşi 009 4 î n c u G Geometrie descriptiă urs şi aplicaţii Ed PIM Iaşi 009 5 * * * Mica Enciclopedie Matematică Ed Tenică ucureşti 985 SOLUŢII NLITIE ŞI GRFIE LE UNOR PROLEME DIN GEOMETRI DESRIPTIVĂ ÎN RE INTERVIN PLNE ŞI DREPTE (Reumat) Lucrarea de faţă abordeaă câtea probleme de intersecţie ale unor drepte şi plane particulare prin metodele geometriei analitice şi respecti ale geometriei descriptie Un studiu comparati al celor două metode atestă faptul că raţionamentul baat pe geometrie descriptiă este mai intuiti mai rapid în reme ce raţionamentul analitic deşi mai laborios poate fi adaptat pentru reolarea unei clase largi de probleme înrudite