Introduction to Vector Calculus (29) SOLVED EXAMPLES. (d) B. C A. (f) a unit vector perpendicular to both B. = ˆ 2k = = 8 = = 8

Size: px
Start display at page:

Download "Introduction to Vector Calculus (29) SOLVED EXAMPLES. (d) B. C A. (f) a unit vector perpendicular to both B. = ˆ 2k = = 8 = = 8"

Transcription

1 Introduction to Vector Calculus (9) SOLVED EXAMPLES Q. If vector A i ˆ ˆj k, ˆ B i ˆ ˆj, C i ˆ 3j ˆ kˆ (a) A B (e) A B C (g) Solution: (b) A B (c) A. B C (d) B. C A then find (f) a unit vector perpendicular to both B and C Component of A along B. (a) A B (b) A B i ˆ ˆ j k ˆ i ˆ ˆ j 4iˆ j ˆ kˆ i ˆ ˆ j b ˆ i ˆ ˆ j ˆ k (c) A. B C (d) B. C A (e) A B C B A.C C A.B i ˆ ˆj i ˆ ˆj k ˆ. i ˆ 3j ˆ kˆ i ˆ 3j ˆ k ˆ i ˆ ˆ j k ˆ. i ˆ ˆ j iˆ 3kˆ

2 (30) Introduction to Vector Calculus (f) ˆn i ˆ ˆ j ˆ ˆ ˆ i 3j k B C B C 4 ˆi j ˆ 4bˆ (g) A B A cos Bˆ A.B Bˆ ˆ 0i ˆ 5j ˆ 5 i ˆ ˆj Q.: Find the angle between A i ˆ ˆj kˆ Solution : as A.B B B as i ˆ ˆ j k. i ˆ ˆ j i ˆ ˆ j A.B A B cos cos B ˆB B and B ˆi ˆj 3kˆ. i ˆ ˆ j k ˆ ˆ ˆ ˆ. i j 3k A.B A B 3 cos approx. Q.3: If A i ˆ 3j ˆ 7kˆ and B i ˆ ˆj kˆ perpendicular to each other. Solution : so A.B i ˆ 3j ˆ 7k ˆ. i ˆ ˆ j k ˆ A.B A B cos 0, then show that A and B are cos 0

3 Introduction to Vector Calculus (3) 90 so A is perpendicular to B. Q.4: Find the unit vector perpendicular to both A i ˆ 3j ˆ 5kˆ and B i ˆ 3j ˆ kˆ. Also find the angle between them. Solution: As A B ˆ ˆ ˆ i j k iˆ 8j ˆ unit vector perpendicular to both A and B A B ˆn A B Again sin i ˆ 8j ˆ i ˆ 8j ˆ 8 08 A B A B sin Approx. Q.5: A particle is acted upon by two constant forces F ˆ ˆ ˆ i 4j 3k and F ˆ ˆ ˆ 3i j k due to which particle is displaced from ˆi j ˆ 3kˆ to 4i ˆ 5j ˆ kˆ. Calculate the total work done. Solution: Displacement of the particle r 4i ˆ 5j ˆ k ˆ ˆ i j ˆ 3k ˆ

4 (3) Introduction to Vector Calculus Hence total work done 3i ˆ 3j ˆ kˆ Total force. displacement F F.r ˆi 4ˆj 3kˆ 3i ˆ ˆj k ˆ. 3i ˆ 3j ˆ kˆ ˆ ˆ ˆ ˆ ˆ ˆ 4i 5j 4k. 3i 3jk units. Q.6: A rigid body is rotating with angular velocity of 5 rad/s about an axis parallel to 3j ˆ kˆ and passing through the point ˆi ˆj 3kˆ. Find the velocity vector of the particle, when it is at the point i ˆ 4 ˆj kˆ. Solution : Suppose r is the position vector then r i ˆ 4j ˆ k ˆ ˆ i ˆ j 3k ˆ angular velocity linear velocity ˆi 5j ˆ 4kˆ 3j ˆ kˆ 5 5 3j ˆ kˆ 3j ˆ kˆ 0 v 5 ˆ ˆ r 3j k ˆ i 5j ˆ 4k ˆ 0 ˆi ˆj kˆ i ˆ ˆj 3kˆ 0 units. Q.7 : Calculate the torque of a force i ˆ j ˆ 5kˆ about the point 8j ˆ acting through the point 6i ˆ 4j ˆ kˆ. Solution : Here

5 Introduction to Vector Calculus (33) r 8j ˆ 6i ˆ 4j ˆ k ˆ 6i ˆ 4j ˆ kˆ r F 6i ˆ 4j ˆ k ˆ i ˆ j ˆ 5k ˆ torque ˆ ˆ ˆ i j k i ˆ 34ˆj 4kˆ Q.8: A force vector 0ˆi 5ˆj 35kˆ passes through a point (, 5, 7). Prove that force is also passing through the origin. Solution: The position vector r i ˆ 5j ˆ 7k ˆ and moment of the form about this point i.e. torque r F i ˆ 5j ˆ 7k ˆ 0i ˆ 5j ˆ 35k ˆ ˆ ˆ ˆ i j k As the moment is zero, which shows that forces is passing through the origin. Q.9: A force 4i ˆ 3j ˆ kˆ passes through the point ( 9,, ). Find the component of moment of the force about the axis of reference. Sol.: Here so moment of force i.e. torque r F r 9i ˆ j ˆ k ˆ 9i ˆ ˆ j k ˆ 4i ˆ 3j ˆ k ˆ

6 (34) Introduction to Vector Calculus ˆ ˆ ˆ i j k iˆ ˆj 9kˆ Hence components of moment of force are 7 unit, units and 9 units in x, y and z direction respectively. Q.0: A proton is moving with velocity 0 8 cm/s along z-axis through an electric field of intensity volt/cm along x-axis and magnetic field of intensity 000 gauss along y-axis. Calculate the magnitude and direction of total force. Solution: Intensity of electric field E 4 30 iˆ volt / cm 00 iˆ esu/cm Proton charge C 4.80 esu Magnetic field B velocity v ˆ 000 j gauss 8 ˆ 0 k cm / s so total force acting on the proton F v B q E C ˆi 0 kˆ 000ˆj ˆi dyne Hence total force acting on the proton has magnitude dyne along the +ve x- direction. Q.: Find the value of the constant p so that A i ˆ ˆj 3k, ˆ B i ˆ 3j ˆ kˆ and C 3i ˆ pj ˆ kˆ are coplanar. A. B C 0 Solution: We know that three vectors are said to be coplanar if p 0

7 Introduction to Vector Calculus (35) 4p 38 0 or 4p 38 Q.: Evaluate A B C Solution: p where A i ˆ ˆj, B ˆi ˆj kˆ A B C and C 5i ˆ 3j ˆ kˆ. B A.C C A.B ˆi ˆj kˆ i ˆ ˆj 0k ˆ. 5i ˆ 3j ˆ kˆ 5i ˆ 3j ˆ kˆ i ˆ ˆj 0k ˆ. ˆi ˆj kˆ 7 ˆ i ˆ j k ˆ 5i ˆ 3j ˆ k ˆ i ˆ 4j ˆ 8kˆ Q.3: If r si the position vector of any point (x, y, z) and A then show that r.a. A 0 is the equation of a constant plane. (i) (ii) r A.r is the equation of a sphere. is a constant vector Also show that result of (i) is of the form Ax By Cz D 0 where D A B C and that of (ii) is of the from x y z r. [RU 005] Solution: (i) Suppose A A, B, C and r x, y, z r A. A x AA y BB z CC xa A yb B zc C xa yb zc A B C Ax By Cz D

8 (36) Introduction to Vector Calculus where D A B C r A.A so which is an equation of a plane. r A.A (ii) r A.A if x y z 0 Ax By Cz D 0 x Ax y B y z Cz 0 then x y z A B C 0 Which is the equation of sphere whose surface touches the origin. Q.4: A particle moves on the curve x t, y t 4t, z 3t 5 where t is the time. Find the components of velocity and acceleration at time t in the direction ˆi 3j ˆ kˆ. Solution: Position vector so velocity vector acceleration r dr v dt t ˆi t 4t ˆj 3t 5 kˆ d ˆ d ˆ d t i t 4t j 3t 5 kˆ dt dt dt 4t ˆ i t 4 ˆ j 3k ˆ a dv dt d ˆ d ˆ d 4t i t 4 j 3 kˆ dt dt dt 4iˆ j ˆ 0 at` t, velocity v 4iˆ j ˆ 3kˆ acceleration a 4i ˆ j ˆ and the component of v along ˆi 3j ˆ kˆ

9 Introduction to Vector Calculus (37) is 4i ˆ ˆ j 3k ˆ ˆ ˆ ˆ. i 3j k and component of a along i 3j ˆ kˆ is ˆ ˆ ˆ ˆ ˆ 4i j. i 3j k Q.5: Calculate the unit vector, which is normal to the surface Solution : Here At (,, ), x y xy 3xyz at the point (,, ). ˆ ˆ ˆ i j k x y xy 3xyz x y z ˆ x x y xy 3xyz i x y xy 3xyz ˆj y x y xy 3xyz kˆ z ˆ xy y 3yz i x xy 3xz j 3xy kˆ 3 ˆ i 3 ˆ j 3k ˆ 3k ˆ so the unit vector normal to the surface at (,, ) is ˆ 3k 3 ˆk ˆ 3k 3 Q.6: Find the direction derivative of x, y,z x y xy at the point (,, 4) along the direction of the vector (,, ). Solution: as

10 (38) Introduction to Vector Calculus,, 4 x y xy ˆ ˆ ˆ x y z i j k x, y,z x y xy iˆ x y xy ˆj x y xy kˆ x y z ˆ xy y i x xy ˆj ˆ 3i Position vector ˆr ˆi j ˆ kˆ and unit vector along this position vector and direction derivative ˆn ˆn ˆi j ˆ kˆ iˆ j ˆ kˆ 4 6 ˆi j ˆ kˆ 3i ˆ Q.7: Find the equation of the tangent plane and normal line to the surface x y z 3 at the point (,, 3). Solution : Here x,y,z x y z 3 x y z 6 x x y z 4x y x y z y z x y z so the components, and at the point (,, 3) will be x y z

11 Introduction to Vector Calculus (39) x 4 8,, y z Hence the equation of the tangent plane to the surface at the point (,, 3) is X 8 Y Z 3 0 or 4X + y + Z 6 so the equation of normal to the surface at (,, 3) is or X 8 X 4 Y Z 3 Y Z + 3 Q.8: Find the angle between the surfaces x y z 9 and x y z 3 at the (,, ) Solution: Suppose x y z and x y z so x ˆi yˆj z kˆ and x iˆ yˆj kˆ and,,,, iˆ 4j ˆ 4kˆ iˆ 4j ˆ kˆ since and are normal to and then. cos surfaces and. so. cos where is the angle between the cos cos approx. Q.9 (i) Provle that P cos ˆ ˆ ˆ ˆ i sin j and cosi sin j are unit vectors in

12 (40) Introduction to Vector Calculus the xy-plane respectively making and with the x-axis. (ii) By means of dot product, obtain the formula for cos. by similarly formulating P and Q, obtain the formula for cos. (iii) If is the angle between P and Q find P Q in terms of. Solution: (i) Given P cos ˆ ˆ i sin j Q cos ˆ ˆ i sin j y Q P (ii) hence P and Q But P cos sin Q cos sin are unit vectors. P.Q P Q cos. cos...() P.Q cos ˆ i sin ˆ ˆ ˆ j. cosi sin j so cos cos sin sin...() cos cos cos sin sin let P P cos ˆ ˆ i sin j and Q cos ˆ ˆ i sin j then P.Q. cos

13 Introduction to Vector Calculus (4) (iii) P and Q are unit vectors. so P Q cos cos sin sin Q PQ cos cos cos sin W 4x y ˆi 7x z ˆj 4xy z kˆ Q.0: A vector field is given as (i) What is the magnitude of the field at point (. 3, 4). (ii) At what point on z-axis is the magnitude of W equal to unity? [RU 00] Solution: (i) 4x y iˆ 7x z ˆj 4xy z kˆ W 4 3 iˆ 7 4 ˆj kˆ at P(, 3, 4), W 48iˆ ˆj 8kˆ W (ii) As the required point is on z-axis so x 0, y 0 W ˆ z j z k for that point. W so 4 4z 4z 0 taking z as positive z z z 4z 4z z 8 z.07 and 0.07 z ± Q.: Calculate the differential volume to obtain the expression for volume of the (i) sphere of radius 'b'

14 (4) Introduction to Vector Calculus (ii) Semispherical shell of inner radius 'a' and outer radius 'b'. (iii) Cylinder of radius 'b' and height 'h'. Solution: (i) Differential volume in spherical coordinates dv r sin dr d d here r 0 to b, 0 to, 0 to. So volume of sphere V b dv r sin dr d d V b r dr sin d d b r dr cos 0 0 r dr b b 3 so V sphere (ii) For semispherical shell r a, r b 4 b 3 3 so dv r sin dr d d here r a to b, 0 to, 0 to so V b a 0 0 r sin dr d d

15 Introduction to Vector Calculus (43) b a 0 0 r dr sin d d b r drcos a 0 r 3 b a (iii) 3 3 b a Differential volume for a cylinder dv r dr d dz here r 0 to b, z 0 to h, and 0 to. 3 so V dv V V b h a 0 0 r dr d dz b h r dr dz d r.h. b 0 so V cyl. b h Q. : For positive x, y, z let 40 xyz c/m 3. Find the total charge within the region bounded by x 0, y 0, 0 x 3y 0 and 0 z. Solution : Here Q 5 y z xyz dx dydz

16 (44) Introduction to Vector Calculus 0x 5 3 y z 40x dx x 40x 4x dx 40 00x 40x 4x Q C 3 4 Q.3: Given point P in Cartesian coordinate system as P(,, 3). Calculate its coordinates in cylindrical system. Solution: As given x, y, z y x y tan, z z x so 5.36 z 3 tan so P cyl. (.36, 63.43, 3) Q.4: The cooridnate of a point P in cylindrical system is P(, 45, ). find its equivalent in cartesion system. Solution: Here, 45, z and x cos, y sin, z z x. cos y z so P cart. (0.707, 0.707,) Q.5: Find the constant m such that the vector

17 Introduction to Vector Calculus (45) x 3y ˆi y z ˆj x mz kˆ is solenoidal. Solution: The vector will be solenoidal if ˆ ˆ i j kˆ x 3y ˆi y z ˆj x mz kˆ 0 x y z so x 3y y z x mz 0 x y z i.e. or + + m 0 m Q.6: Find div F and curl F if F grad x 3 y 3 z 3 3xyz Solution: Here F grad x 3 y 3 z 3 3xyz. [WBUT 00] ˆ x x y z 3xyz i x y z 3xyz ˆj y x y z 3xyz kˆ z 3x 3yz ˆi 3y 3xz ˆj 3z 3xy kˆ div F 3x 3yz 3y 3xz 3z 3xy x y z 6x y z ˆ ˆ ˆ i j k F x y z 3x 3yz 3y 3xz 3z 3xy 3x 3x ˆi 3y 3y ˆj 3z 3z kˆ 0 Q.7 Show that curl grad f 0 where f x y + xy + z.

18 (46) Introduction to Vector Calculus Solution: grad f f ˆi f ˆj f kˆ x y z xy y ˆi x x ˆj z kˆ curl grad f ˆ ˆ ˆ i j k x y z xy y x x z 0 0 x x k ˆ 0 Q.8: If the scalar function x,y,z xy z,. is its corresponding scalar field is solenoidal or irrotational? Solution : Let so.f So field is not solenoidal. F yˆi x ˆj zkˆ x y z y x z Now F ˆ ˆ ˆ i j k x y z y x z so field is irrotational. 0 Q.9: Verify the divergence theorem for the vector function F ˆ 4xz i y ˆ j yz k ˆ taken over the cube bounded by x 0, y 0,, z 0,. [WBUT (math) 00] Solution.:

19 Introduction to Vector Calculus (47) z y for face 4567; 7 x ˆn ˆi and x 6 F. n ˆ ds 0 0 F. n ˆ ds 4z dydz î dy dz 0 for 30 for and for 3074 for face 345, and total Again 3 56 n ˆ ĵ, y F. n ˆ ds F. n ˆ ds 0 4 F. n ˆ ds 5 F. n ˆ ds 0 for F. n ˆ ds S F x y z 4xz y yz 4z y

20 (48) Introduction to Vector Calculus.F dv 4z ydx dy dz z yz dx dy 3 F. n ˆ ds F dv V s Hence divergence theorem is verified. Q.30: Calculate the line integral of A cos ˆ z sin zˆ wedge defined by 0 4, 0 30, z 0. Solution: Given A cos ˆ z sin zˆ differential length dl y d ˆ d ˆ dzzˆ around the edge L of the (3) () 0 () x Circulation of A around path is A.dl A.dl A.dl A.dl L 3 for () 0, d 0, z 0, dz 0 A.dl cosˆ z sin d ˆ d ˆ dz zˆ

21 Introduction to Vector Calculus (49) 4 4 cos d d 0 0 for () for (3) 4, d z 0, dz 0 A. dl cos d zsin dz 0 / 6, d 0, z 0, dz 0 A. dl cos d cos d 6 4 So total L d A. dl Q.3 Given A x xy, calculate A. ds Solution: So y x, ds dx dy over the region y x, 0 < x <.

22 (50) Introduction to Vector Calculus y 0 A. ds x xy dx dy x x x x dx dy 0 y 0 0 y 0 xy dx dy 5 4 x x dx x 0 x 0 dx x y z Q.3 For a scalar function sin sin e 3. Calculate the magnitude direction of maximum rate of increase of at the point (,, ). Solution: As gradient of a scalar function gives the magnitude and direction of max. rate of change of that So ˆi ˆj kˆ x y z x y z ˆ x y z sin sin e i sin sin e ˆ j x 3 y 3 at (,, ) x y z sin sin e kˆ z 3 z x ˆ x y z e sin j sin sin e kˆ 6 3

23 Introduction to Vector Calculus (5),, and,, ˆ e sin j sin sin e kˆ j kˆ ˆ 0.9 ˆj 0.38 kˆ / and ĵ 0.9j ˆ 0.38kˆ j ˆ 0.86 kˆ Q.33 : Determine the divergence of the following vector fields at given points A yzi ˆ 4 x y ˆ j xyz k ˆ at,, (i) (ii) (iii) B z sin ˆ 5 z cos ˆ z zˆ at 5,, C r sin cos rˆ cos ˆ r ˆ at,, 3 3 Solution: In cartesion (a).a x y z yz 4x 4y xyz.a xy 4 + xy at,,,.a,, 4 + ( ) (b) In cylindrical.b B B Bz z

24 (5) Introduction to Vector Calculus given B z sin B 5z cos, Bz z at 5,,.B z sin 5. zsin 3z sin (c) In spherical system.b (3 ).C C r r r r sin rsin r C sin C cos sin cos r sin r r r sin rsin 3 at,, 3 3 cos cot 6sin cos r.c cos cot 6sin cos Q.34: Find the nature of the vector ˆ ˆ F 30i xy j 5xz kˆ. [RU 003] Solution :.F 30 xy 5xz x y y x + 0xz 0

25 Introduction to Vector Calculus (53) Curl F ˆ ˆ ˆ i j k F x y z 30 xy 5xz 5z ˆj y kˆ 0 as.f 0 fields is not solenoidal and F 0 field is rotational. G 6xy 3 ˆi 8x ˆj xkˆ. Q.35: Given the vector field (i) Is G irrotational (or conservative)? (ii) Find the net flux of G over the cube 0<x, y, z <. (iii) Determine the circulation of G around the edge of the square z 0, 0 < x, y <. Assume anticlockwise direction. [RU 003] Solution: (i) So G is irrotational. G ˆ ˆ ˆ i j k x y z 6xy z 8x x (ii) Net flux of G over the cube. G dv so V. G. G dv 0ˆi ˆj 6x 6x kˆ 0 V x y z 6xy z 8x x 6y 0 0 6y 6y dx dydz 6 dx dz y dy 0 0 0

26 (54) Introduction to Vector Calculus (iii) G. dl 0 y y 0 x 6xy z dx 8x dy x 0 z 0 y 0 z 0 y x xy z dx 8x dy x z 0 y z 0 0 x 0 8 y SUMMARY A vector is with magnitude and direction. In space a quantity is specified by a function. When the result of multiplication of two vectors is a scalar then it is called scalar product or dot product. When product is a vector then it is called vector product. A. B C Multiplication of three vectors can give scalar or a vector A B C Vector differentiation is done using dal () operator the gradient of a scalar field is, divergence as. A and curl by A and laplacian by A. In Cartesion coordinate system dl dx ˆi dy ˆj dz k, ˆ dv dx dy dz. Gradient ˆi ˆj kˆ x y z Divergences. A A A x y A x y z z

27 Introduction to Vector Calculus (55) Curl A ˆ ˆ ˆ i j k x x z A A A x y z Laplacian In cylindrical system dl x y z d ˆ d ˆ dz z, ˆ dv d d dz gradient T T T ˆ T ˆ ẑ z divergence. A A A A z z Curl A ˆ ˆ ẑ z A A A z Laplacian In spherical system z dl dr rˆ rd ˆ r sin d ˆ dv r sin d dr d gradient T T ˆr T ˆ T ˆ r r r sin divergence A r r r sin rsin r Ar A sin

28 (56) Introduction to Vector Calculus Curl A r sin ˆr r ˆ rsin ˆ r A ra rsin A Laplacian r sin r r r sin Gauss Divergence theorem A. ds Stoke's theorem s sin L A. dl V. A dv V A. ds A vector field is solenoidal if Irrotational or conservative if Triple products A. B C B C A C A B A B C B A. C C A. B Second derivatives. A 0 f 0 A. A A EXERCISE

29 Introduction to Vector Calculus (57). Give the basic concepts of transformation of one coordinate system to another. Derive necessary relations for rectangular, cylindrical and spherical systems. [RU 003]. Write short note on "Physical significance of curl, divergence and gradient". 3. State-Gauss divergence theorem. Write its applications, advantages and limitations. [RU 00] 4. State and prove stoke's theorem. [RU 000] 5. Explain how stoke's theorem enables us to obtain the integral form of ampere circuital law. 6. Explain various types of vector fields. (i) (ii) (iii) Solenoidal and irrotational fields. Irrotational but not solenoidal fields Solenoidal but not irrotaitonal fields (iv) Neither irrotational nor solenoidal fields. 7. For the vectors A iˆ 3kˆ and B 5i ˆ j ˆ 6kˆ calculate (i) A B (ii) A B (iii) A. B (iv) A B (v) Angle between A and B (vi) A unit vector parallel to 3A B. (vii) Length of the projection of A on B. i 6i ˆ j ˆ 3k ii 4i ˆ j ˆ 9k iii 3 iv 6i ˆ j ˆ k Ans.: ˆ ˆ 8i ˆ j ˆ 3kˆ v 60 vi vii.6m Use the differential volume dv to find volume of region. (i) 0 x, y, 3 z 3 [Ans.: 6] (ii) 5,, z 4 [Ans.: 0] 3 9. Find area of the region 0 on the spherical shell of radius 'b'. [Ans. b ] 0. Evaluate the gradient of the following scalar fields

30 (58) Introduction to Vector Calculus (a) z [Ans.: z z P e sin x P cos xe ˆi sin xe kˆ ] (b) q zcos ˆ Ans.: q zcos ˆ zsin cosz (c) s 0r sin cos. If f xy + yz + xz then (i) (ii) Ans.: r 0sin cos rˆ 0r cos cos ˆ 0r sin sin ˆ Find the magnitude and direction of the maximum rate of change of the function at point (,, 3) Find the rate of change of the function at the same point in the direction of the vector. and V xyz evaluate. VT. If ˆ ˆ ˆ T x i 3y j 4z k Ans.: i f 4 f i ˆ 3j ˆ kˆ ˆ f f 4 (ii) df f.dl. [Ans.: xyz] 3. If U xz x y y z find div (grad U). [Ans.: ( y + z + y )] 4. Given ˆ ˆ ˆ 3 D 6xyz i 3x z j 6x y k C/m Find the total charge lying within the region bounded by 0 < x <, < y < and z by separately evaluating each side of divergence theorem. A x y ˆ i ˆ j x y k ˆ 5. If A. 0 then prove that A x y z ˆ i y zx ˆ j z xy k ˆ 6. Prove that vector 7. If x y z find. 8. Show that is not solenoidal. [Ans.: 6C] [WBUT 005]. [WBUT 005] ˆ ˆ B xyz i x z y j x ykˆ is irrotational. [WBUT 005] 9. find a unit vector perpendicular to x y z 00 at (,, 3). [WBUT 007]

31 Introduction to Vector Calculus (59) 0. if 3 3x y y z find. Show that ˆi j ˆ 3kˆ Ans.: 4 at (,, ). [WBUT 004] Ans.: i ˆ 9j ˆ 6kˆ 3 ˆ ˆ F xy z i x j 3xz kˆ is a conservative force field. Find also the scalar 3 potential. [WBUT 006, 003] Ans. : x y z x constant. Evaluates F.n ˆ ds where ˆ F 8x zi y ˆ j yzk ˆ and s is the surface of the cube bounded s by x 0,, y 0,, z 0,.

ENGI Gradient, Divergence, Curl Page 5.01

ENGI Gradient, Divergence, Curl Page 5.01 ENGI 94 5. - Gradient, Divergence, Curl Page 5. 5. The Gradient Operator A brief review is provided here for the gradient operator in both Cartesian and orthogonal non-cartesian coordinate systems. Sections

More information

ENGI Gradient, Divergence, Curl Page 5.01

ENGI Gradient, Divergence, Curl Page 5.01 ENGI 940 5.0 - Gradient, Divergence, Curl Page 5.0 5. e Gradient Operator A brief review is provided ere for te gradient operator in bot Cartesian and ortogonal non-cartesian coordinate systems. Sections

More information

ENGI 4430 Surface Integrals Page and 0 2 r

ENGI 4430 Surface Integrals Page and 0 2 r ENGI 4430 Surface Integrals Page 9.01 9. Surface Integrals - Projection Method Surfaces in 3 In 3 a surface can be represented by a vector parametric equation r x u, v ˆi y u, v ˆj z u, v k ˆ where u,

More information

Problem Solving 1: The Mathematics of 8.02 Part I. Coordinate Systems

Problem Solving 1: The Mathematics of 8.02 Part I. Coordinate Systems Problem Solving 1: The Mathematics of 8.02 Part I. Coordinate Systems In 8.02 we regularly use three different coordinate systems: rectangular (Cartesian), cylindrical and spherical. In order to become

More information

Multiple Integrals and Vector Calculus: Synopsis

Multiple Integrals and Vector Calculus: Synopsis Multiple Integrals and Vector Calculus: Synopsis Hilary Term 28: 14 lectures. Steve Rawlings. 1. Vectors - recap of basic principles. Things which are (and are not) vectors. Differentiation and integration

More information

MATH 332: Vector Analysis Summer 2005 Homework

MATH 332: Vector Analysis Summer 2005 Homework MATH 332, (Vector Analysis), Summer 2005: Homework 1 Instructor: Ivan Avramidi MATH 332: Vector Analysis Summer 2005 Homework Set 1. (Scalar Product, Equation of a Plane, Vector Product) Sections: 1.9,

More information

Chapter 6: Vector Analysis

Chapter 6: Vector Analysis Chapter 6: Vector Analysis We use derivatives and various products of vectors in all areas of physics. For example, Newton s 2nd law is F = m d2 r. In electricity dt 2 and magnetism, we need surface and

More information

Multiple Integrals and Vector Calculus (Oxford Physics) Synopsis and Problem Sets; Hilary 2015

Multiple Integrals and Vector Calculus (Oxford Physics) Synopsis and Problem Sets; Hilary 2015 Multiple Integrals and Vector Calculus (Oxford Physics) Ramin Golestanian Synopsis and Problem Sets; Hilary 215 The outline of the material, which will be covered in 14 lectures, is as follows: 1. Introduction

More information

CURRENT MATERIAL: Vector Calculus.

CURRENT MATERIAL: Vector Calculus. Math 275, section 002 (Ultman) Spring 2012 FINAL EXAM REVIEW The final exam will be held on Wednesday 9 May from 8:00 10:00am in our regular classroom. You will be allowed both sides of two 8.5 11 sheets

More information

Contents. MATH 32B-2 (18W) (L) G. Liu / (TA) A. Zhou Calculus of Several Variables. 1 Multiple Integrals 3. 2 Vector Fields 9

Contents. MATH 32B-2 (18W) (L) G. Liu / (TA) A. Zhou Calculus of Several Variables. 1 Multiple Integrals 3. 2 Vector Fields 9 MATH 32B-2 (8W) (L) G. Liu / (TA) A. Zhou Calculus of Several Variables Contents Multiple Integrals 3 2 Vector Fields 9 3 Line and Surface Integrals 5 4 The Classical Integral Theorems 9 MATH 32B-2 (8W)

More information

Chapter 1. Vector Algebra and Vector Space

Chapter 1. Vector Algebra and Vector Space 1. Vector Algebra 1.1. Scalars and vectors Chapter 1. Vector Algebra and Vector Space The simplest kind of physical quantity is one that can be completely specified by its magnitude, a single number, together

More information

Vector Calculus. Dr. D. Sukumar. February 1, 2016

Vector Calculus. Dr. D. Sukumar. February 1, 2016 Vector Calculus Dr. D. Sukumar February 1, 2016 Green s Theorem Tangent form or Ciculation-Curl form c Mdx + Ndy = R ( N x M ) da y Green s Theorem Tangent form or Ciculation-Curl form Stoke s Theorem

More information

EELE 3331 Electromagnetic I Chapter 3. Vector Calculus. Islamic University of Gaza Electrical Engineering Department Dr.

EELE 3331 Electromagnetic I Chapter 3. Vector Calculus. Islamic University of Gaza Electrical Engineering Department Dr. EELE 3331 Electromagnetic I Chapter 3 Vector Calculus Islamic University of Gaza Electrical Engineering Department Dr. Talal Skaik 2012 1 Differential Length, Area, and Volume This chapter deals with integration

More information

Vectors Coordinate Systems VC - Differential Elements VC - Differential Operators Important Theorems Summary Problems.

Vectors Coordinate Systems VC - Differential Elements VC - Differential Operators Important Theorems Summary Problems. S. R. Zinka zinka@vit.ac.in School of Electronics Engineering Vellore Institute of Technology July 16, 2013 Outline 1 Vectors 2 Coordinate Systems 3 VC - Differential Elements 4 VC - Differential Operators

More information

Notes 19 Gradient and Laplacian

Notes 19 Gradient and Laplacian ECE 3318 Applied Electricity and Magnetism Spring 218 Prof. David R. Jackson Dept. of ECE Notes 19 Gradient and Laplacian 1 Gradient Φ ( x, y, z) =scalar function Φ Φ Φ grad Φ xˆ + yˆ + zˆ x y z We can

More information

MAC2313 Final A. (5 pts) 1. How many of the following are necessarily true? i. The vector field F = 2x + 3y, 3x 5y is conservative.

MAC2313 Final A. (5 pts) 1. How many of the following are necessarily true? i. The vector field F = 2x + 3y, 3x 5y is conservative. MAC2313 Final A (5 pts) 1. How many of the following are necessarily true? i. The vector field F = 2x + 3y, 3x 5y is conservative. ii. The vector field F = 5(x 2 + y 2 ) 3/2 x, y is radial. iii. All constant

More information

Problem Solving 1: Line Integrals and Surface Integrals

Problem Solving 1: Line Integrals and Surface Integrals A. Line Integrals MASSACHUSETTS INSTITUTE OF TECHNOLOY Department of Physics Problem Solving 1: Line Integrals and Surface Integrals The line integral of a scalar function f ( xyz),, along a path C is

More information

CURRENT MATERIAL: Vector Calculus.

CURRENT MATERIAL: Vector Calculus. Math 275, section 002 (Ultman) Fall 2011 FINAL EXAM REVIEW The final exam will be held on Wednesday 14 December from 10:30am 12:30pm in our regular classroom. You will be allowed both sides of an 8.5 11

More information

ENGI Duffing s Equation Page 4.65

ENGI Duffing s Equation Page 4.65 ENGI 940 4. - Duffing s Equation Page 4.65 4. Duffing s Equation Among the simplest models of damped non-linear forced oscillations of a mechanical or electrical system with a cubic stiffness term is Duffing

More information

G G. G. x = u cos v, y = f(u), z = u sin v. H. x = u + v, y = v, z = u v. 1 + g 2 x + g 2 y du dv

G G. G. x = u cos v, y = f(u), z = u sin v. H. x = u + v, y = v, z = u v. 1 + g 2 x + g 2 y du dv 1. Matching. Fill in the appropriate letter. 1. ds for a surface z = g(x, y) A. r u r v du dv 2. ds for a surface r(u, v) B. r u r v du dv 3. ds for any surface C. G x G z, G y G z, 1 4. Unit normal N

More information

A Brief Revision of Vector Calculus and Maxwell s Equations

A Brief Revision of Vector Calculus and Maxwell s Equations A Brief Revision of Vector Calculus and Maxwell s Equations Debapratim Ghosh Electronic Systems Group Department of Electrical Engineering Indian Institute of Technology Bombay e-mail: dghosh@ee.iitb.ac.in

More information

Vector Calculus, Maths II

Vector Calculus, Maths II Section A Vector Calculus, Maths II REVISION (VECTORS) 1. Position vector of a point P(x, y, z) is given as + y and its magnitude by 2. The scalar components of a vector are its direction ratios, and represent

More information

Review Sheet for the Final

Review Sheet for the Final Review Sheet for the Final Math 6-4 4 These problems are provided to help you study. The presence of a problem on this handout does not imply that there will be a similar problem on the test. And the absence

More information

Lecture 2: Review of Vector Calculus

Lecture 2: Review of Vector Calculus 1 Lecture 2: Review of Vector Calculus Instructor: Dr. Gleb V. Tcheslavski Contact: gleb@ee.lamar.edu Office Hours: Room 2030 Class web site: www.ee.lamar.edu/gleb/em/in dex.htm 2 Vector norm Foran n-dimensional

More information

ENGI 4430 Gauss & Stokes Theorems; Potentials Page 10.01

ENGI 4430 Gauss & Stokes Theorems; Potentials Page 10.01 ENGI 443 Gauss & tokes heorems; Potentials Page.. Gauss Divergence heorem Let be a piecewise-smooth closed surface enclosing a volume in vector field. hen the net flux of F out of is F d F d, N 3 and let

More information

MATH 228: Calculus III (FALL 2016) Sample Problems for FINAL EXAM SOLUTIONS

MATH 228: Calculus III (FALL 2016) Sample Problems for FINAL EXAM SOLUTIONS MATH 228: Calculus III (FALL 216) Sample Problems for FINAL EXAM SOLUTIONS MATH 228 Page 2 Problem 1. (2pts) Evaluate the line integral C xy dx + (x + y) dy along the parabola y x2 from ( 1, 1) to (2,

More information

Study Guide for Exam #2

Study Guide for Exam #2 Physical Mechanics METR103 November, 000 Study Guide for Exam # The information even below is meant to serve as a guide to help you to prepare for the second hour exam. The absence of a topic or point

More information

is the ith variable and a i is the unit vector associated with the ith variable. h i

is the ith variable and a i is the unit vector associated with the ith variable. h i . Chapter 10 Vector Calculus Features Used right( ), product( ),./,.*, listúmat( ), mod( ), For...EndFor, norm( ), unitv( ),

More information

APPLICATIONS OF GAUSS S LAW

APPLICATIONS OF GAUSS S LAW APPLICATIONS OF GAUSS S LAW Although Gauss s Law is always correct it is generally only useful in cases with strong symmetries. The basic problem is that it gives the integral of E rather than E itself.

More information

Mathematical Concepts & Notation

Mathematical Concepts & Notation Mathematical Concepts & Notation Appendix A: Notation x, δx: a small change in x t : the partial derivative with respect to t holding the other variables fixed d : the time derivative of a quantity that

More information

Summary for Vector Calculus and Complex Calculus (Math 321) By Lei Li

Summary for Vector Calculus and Complex Calculus (Math 321) By Lei Li Summary for Vector alculus and omplex alculus (Math 321) By Lei Li 1 Vector alculus 1.1 Parametrization urves, surfaces, or volumes can be parametrized. Below, I ll talk about 3D case. Suppose we use e

More information

Notes 3 Review of Vector Calculus

Notes 3 Review of Vector Calculus ECE 3317 Applied Electromagnetic Waves Prof. David R. Jackson Fall 2018 A ˆ Notes 3 Review of Vector Calculus y ya ˆ y x xa V = x y ˆ x Adapted from notes by Prof. Stuart A. Long 1 Overview Here we present

More information

18.02 Multivariable Calculus Fall 2007

18.02 Multivariable Calculus Fall 2007 MIT OpenCourseWare http://ocw.mit.edu 18.02 Multivariable Calculus Fall 2007 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. V9. Surface Integrals Surface

More information

EE2007: Engineering Mathematics II Vector Calculus

EE2007: Engineering Mathematics II Vector Calculus EE2007: Engineering Mathematics II Vector Calculus Ling KV School of EEE, NTU ekvling@ntu.edu.sg Rm: S2-B2b-22 Ver 1.1: Ling KV, October 22, 2006 Ver 1.0: Ling KV, Jul 2005 EE2007/Ling KV/Aug 2006 EE2007:

More information

r t t x t y t z t, y t are zero, then construct a table for all four functions. dy dx 0 and 0 dt dt horizontal tangent vertical tangent

r t t x t y t z t, y t are zero, then construct a table for all four functions. dy dx 0 and 0 dt dt horizontal tangent vertical tangent 3. uggestions for the Formula heets Below are some suggestions for many more formulae than can be placed easily on both sides of the two standard 8½"" sheets of paper for the final examination. It is strongly

More information

Q1. A wave travelling along a string is described by

Q1. A wave travelling along a string is described by Coordinator: Saleem Rao Wednesday, May 24, 2017 Page: 1 Q1. A wave travelling along a string is described by y( x, t) = 0.00327 sin(72.1x 2.72t) In which all numerical constants are in SI units. Find the

More information

18.02 Multivariable Calculus Fall 2007

18.02 Multivariable Calculus Fall 2007 MIT OpenourseWare http://ocw.mit.edu 18.02 Multivariable alculus Fall 2007 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. 18.02 Lecture 30. Tue, Nov

More information

Physics 3323, Fall 2016 Problem Set 2 due Sep 9, 2016

Physics 3323, Fall 2016 Problem Set 2 due Sep 9, 2016 Physics 3323, Fall 26 Problem Set 2 due Sep 9, 26. What s my charge? A spherical region of radius R is filled with a charge distribution that gives rise to an electric field inside of the form E E /R 2

More information

x + ye z2 + ze y2, y + xe z2 + ze x2, z and where T is the

x + ye z2 + ze y2, y + xe z2 + ze x2, z and where T is the 1.(8pts) Find F ds where F = x + ye z + ze y, y + xe z + ze x, z and where T is the T surface in the pictures. (The two pictures are two views of the same surface.) The boundary of T is the unit circle

More information

Created by T. Madas VECTOR OPERATORS. Created by T. Madas

Created by T. Madas VECTOR OPERATORS. Created by T. Madas VECTOR OPERATORS GRADIENT gradϕ ϕ Question 1 A surface S is given by the Cartesian equation x 2 2 + y = 25. a) Draw a sketch of S, and describe it geometrically. b) Determine an equation of the tangent

More information

Module 02: Math Review

Module 02: Math Review Module 02: Math Review 1 Module 02: Math Review: Outline Vector Review (Dot, Cross Products) Review of 1D Calculus Scalar Functions in higher dimensions Vector Functions Differentials Purpose: Provide

More information

ENGI 4430 Line Integrals; Green s Theorem Page 8.01

ENGI 4430 Line Integrals; Green s Theorem Page 8.01 ENGI 443 Line Integrals; Green s Theorem Page 8. 8. Line Integrals Two applications of line integrals are treated here: the evaluation of work done on a particle as it travels along a curve in the presence

More information

ENGI 4430 Line Integrals; Green s Theorem Page 8.01

ENGI 4430 Line Integrals; Green s Theorem Page 8.01 ENGI 4430 Line Integrals; Green s Theorem Page 8.01 8. Line Integrals Two applications of line integrals are treated here: the evaluation of work done on a particle as it travels along a curve in the presence

More information

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Spring 2013 Exam 3 Equation Sheet. closed fixed path. ! = I ind.

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Spring 2013 Exam 3 Equation Sheet. closed fixed path. ! = I ind. MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.0 Spring 013 Exam 3 Equation Sheet Force Law: F q = q( E ext + v q B ext ) Force on Current Carrying Wire: F = Id s " B # wire ext Magnetic

More information

(a) The points (3, 1, 2) and ( 1, 3, 4) are the endpoints of a diameter of a sphere.

(a) The points (3, 1, 2) and ( 1, 3, 4) are the endpoints of a diameter of a sphere. MATH 4 FINAL EXAM REVIEW QUESTIONS Problem. a) The points,, ) and,, 4) are the endpoints of a diameter of a sphere. i) Determine the center and radius of the sphere. ii) Find an equation for the sphere.

More information

Final Review Worksheet

Final Review Worksheet Score: Name: Final Review Worksheet Math 2110Q Fall 2014 Professor Hohn Answers (in no particular order): f(x, y) = e y + xe xy + C; 2; 3; e y cos z, e z cos x, e x cos y, e x sin y e y sin z e z sin x;

More information

The Divergence Theorem Stokes Theorem Applications of Vector Calculus. Calculus. Vector Calculus (III)

The Divergence Theorem Stokes Theorem Applications of Vector Calculus. Calculus. Vector Calculus (III) Calculus Vector Calculus (III) Outline 1 The Divergence Theorem 2 Stokes Theorem 3 Applications of Vector Calculus The Divergence Theorem (I) Recall that at the end of section 12.5, we had rewritten Green

More information

UNIT 1. INTRODUCTION

UNIT 1. INTRODUCTION UNIT 1. INTRODUCTION Objective: The aim of this chapter is to gain knowledge on Basics of electromagnetic fields Scalar and vector quantities, vector calculus Various co-ordinate systems namely Cartesian,

More information

Chapter 3 - Vector Calculus

Chapter 3 - Vector Calculus Chapter 3 - Vector Calculus Gradient in Cartesian coordinate system f ( x, y, z,...) dr ( dx, dy, dz,...) Then, f f f f,,,... x y z f f f df dx dy dz... f dr x y z df 0 (constant f contour) f dr 0 or f

More information

MATH Calculus IV Spring 2014 Three Versions of the Divergence Theorem

MATH Calculus IV Spring 2014 Three Versions of the Divergence Theorem MATH 2443 008 Calculus IV pring 2014 Three Versions of the Divergence Theorem In this note we will establish versions of the Divergence Theorem which enable us to give it formulations of div, grad, and

More information

Practice Problems for Exam 3 (Solutions) 1. Let F(x, y) = xyi+(y 3x)j, and let C be the curve r(t) = ti+(3t t 2 )j for 0 t 2. Compute F dr.

Practice Problems for Exam 3 (Solutions) 1. Let F(x, y) = xyi+(y 3x)j, and let C be the curve r(t) = ti+(3t t 2 )j for 0 t 2. Compute F dr. 1. Let F(x, y) xyi+(y 3x)j, and let be the curve r(t) ti+(3t t 2 )j for t 2. ompute F dr. Solution. F dr b a 2 2 F(r(t)) r (t) dt t(3t t 2 ), 3t t 2 3t 1, 3 2t dt t 3 dt 1 2 4 t4 4. 2. Evaluate the line

More information

+ f f n x n. + (x)

+ f f n x n. + (x) Math 255 - Vector Calculus II Notes 14.5 Divergence, (Grad) and Curl For a vector field in R n, that is F = f 1, f 2,..., f n, where f i is a function of x 1, x 2,..., x n, the divergence is div(f) = f

More information

Chapter 9 Uniform Circular Motion

Chapter 9 Uniform Circular Motion 9.1 Introduction Chapter 9 Uniform Circular Motion Special cases often dominate our study of physics, and circular motion is certainly no exception. We see circular motion in many instances in the world;

More information

AE301 Aerodynamics I UNIT B: Theory of Aerodynamics

AE301 Aerodynamics I UNIT B: Theory of Aerodynamics AE301 Aerodynamics I UNIT B: Theory of Aerodynamics ROAD MAP... B-1: Mathematics for Aerodynamics B-: Flow Field Representations B-3: Potential Flow Analysis B-4: Applications of Potential Flow Analysis

More information

Fundamentals of Applied Electromagnetics. Chapter 2 - Vector Analysis

Fundamentals of Applied Electromagnetics. Chapter 2 - Vector Analysis Fundamentals of pplied Electromagnetics Chapter - Vector nalsis Chapter Objectives Operations of vector algebra Dot product of two vectors Differential functions in vector calculus Divergence of a vector

More information

TECHNO INDIA BATANAGAR

TECHNO INDIA BATANAGAR TECHNO INDIA BATANAGAR ( DEPARTMENT OF ELECTRONICS & COMMUNICATION ENGINEERING) QUESTION BANK- 2018 1.Vector Calculus Assistant Professor 9432183958.mukherjee@tib.edu.in 1. When the operator operates on

More information

Vector Calculus handout

Vector Calculus handout Vector Calculus handout The Fundamental Theorem of Line Integrals Theorem 1 (The Fundamental Theorem of Line Integrals). Let C be a smooth curve given by a vector function r(t), where a t b, and let f

More information

Chapter 2. Vector Analysis

Chapter 2. Vector Analysis Chapter 2. Vector nalysis Cheng; 3/4/2007; 2-2. verview t a given position and time a scalar function a magnitude, a vector function a magnitude and a direction Function conversion between different coordinates

More information

ENGI Surface Integrals Page 2.01

ENGI Surface Integrals Page 2.01 ENGI 543. urface Integrals Page.1. urface Integrals This chapter introduces the theorems of Green, Gauss and tokes. Two different methods of integrating a function of two variables over a curved surface

More information

1 + f 2 x + f 2 y dy dx, where f(x, y) = 2 + 3x + 4y, is

1 + f 2 x + f 2 y dy dx, where f(x, y) = 2 + 3x + 4y, is 1. The value of the double integral (a) 15 26 (b) 15 8 (c) 75 (d) 105 26 5 4 0 1 1 + f 2 x + f 2 y dy dx, where f(x, y) = 2 + 3x + 4y, is 2. What is the value of the double integral interchange the order

More information

Math Review 1: Vectors

Math Review 1: Vectors Math Review 1: Vectors Coordinate System Coordinate system: used to describe the position of a point in space and consists of 1. An origin as the reference point 2. A set of coordinate axes with scales

More information

xˆ z ˆ. A second vector is given by B 2xˆ yˆ 2z ˆ.

xˆ z ˆ. A second vector is given by B 2xˆ yˆ 2z ˆ. Directions for all homework submissions Submit your work on plain-white or engineering paper (not lined notebook paper). Write each problem statement above each solution. Report answers using decimals

More information

One side of each sheet is blank and may be used as scratch paper.

One side of each sheet is blank and may be used as scratch paper. Math 244 Spring 2017 (Practice) Final 5/11/2017 Time Limit: 2 hours Name: No calculators or notes are allowed. One side of each sheet is blank and may be used as scratch paper. heck your answers whenever

More information

2.20 Fall 2018 Math Review

2.20 Fall 2018 Math Review 2.20 Fall 2018 Math Review September 10, 2018 These notes are to help you through the math used in this class. This is just a refresher, so if you never learned one of these topics you should look more

More information

EE2007: Engineering Mathematics II Vector Calculus

EE2007: Engineering Mathematics II Vector Calculus EE2007: Engineering Mathematics II Vector Calculus Ling KV School of EEE, NTU ekvling@ntu.edu.sg Rm: S2-B2a-22 Ver: August 28, 2010 Ver 1.6: Martin Adams, Sep 2009 Ver 1.5: Martin Adams, August 2008 Ver

More information

Maxwell s Equations in Differential Form, and Uniform Plane Waves in Free Space

Maxwell s Equations in Differential Form, and Uniform Plane Waves in Free Space C H A P T E R 3 Maxwell s Equations in Differential Form, and Uniform Plane Waves in Free Space In Chapter 2, we introduced Maxwell s equations in integral form. We learned that the quantities involved

More information

PRACTICE PROBLEMS. Please let me know if you find any mistakes in the text so that i can fix them. 1. Mixed partial derivatives.

PRACTICE PROBLEMS. Please let me know if you find any mistakes in the text so that i can fix them. 1. Mixed partial derivatives. PRACTICE PROBLEMS Please let me know if you find any mistakes in the text so that i can fix them. 1.1. Let Show that f is C 1 and yet How is that possible? 1. Mixed partial derivatives f(x, y) = {xy x

More information

Math Review Night: Work and the Dot Product

Math Review Night: Work and the Dot Product Math Review Night: Work and the Dot Product Dot Product A scalar quantity Magnitude: A B = A B cosθ The dot product can be positive, zero, or negative Two types of projections: the dot product is the parallel

More information

Vectors and Fields. Vectors versus scalars

Vectors and Fields. Vectors versus scalars C H A P T E R 1 Vectors and Fields Electromagnetics deals with the study of electric and magnetic fields. It is at once apparent that we need to familiarize ourselves with the concept of a field, and in

More information

University of Alabama Department of Physics and Astronomy. PH 125 / LeClair Spring A Short Math Guide. Cartesian (x, y) Polar (r, θ)

University of Alabama Department of Physics and Astronomy. PH 125 / LeClair Spring A Short Math Guide. Cartesian (x, y) Polar (r, θ) University of Alabama Department of Physics and Astronomy PH 125 / LeClair Spring 2009 A Short Math Guide 1 Definition of coordinates Relationship between 2D cartesian (, y) and polar (r, θ) coordinates.

More information

Math 11 Fall 2016 Final Practice Problem Solutions

Math 11 Fall 2016 Final Practice Problem Solutions Math 11 Fall 216 Final Practice Problem olutions Here are some problems on the material we covered since the second midterm. This collection of problems is not intended to mimic the final in length, content,

More information

S12.1 SOLUTIONS TO PROBLEMS 12 (ODD NUMBERS)

S12.1 SOLUTIONS TO PROBLEMS 12 (ODD NUMBERS) OLUTION TO PROBLEM 2 (ODD NUMBER) 2. The electric field is E = φ = 2xi + 2y j and at (2, ) E = 4i + 2j. Thus E = 2 5 and its direction is 2i + j. At ( 3, 2), φ = 6i + 4 j. Thus the direction of most rapid

More information

Math review. Math review

Math review. Math review Math review 1 Math review 3 1 series approximations 3 Taylor s Theorem 3 Binomial approximation 3 sin(x), for x in radians and x close to zero 4 cos(x), for x in radians and x close to zero 5 2 some geometry

More information

7a3 2. (c) πa 3 (d) πa 3 (e) πa3

7a3 2. (c) πa 3 (d) πa 3 (e) πa3 1.(6pts) Find the integral x, y, z d S where H is the part of the upper hemisphere of H x 2 + y 2 + z 2 = a 2 above the plane z = a and the normal points up. ( 2 π ) Useful Facts: cos = 1 and ds = ±a sin

More information

UNIVERSITY of LIMERICK OLLSCOIL LUIMNIGH

UNIVERSITY of LIMERICK OLLSCOIL LUIMNIGH UNIVERSITY of LIMERICK OLLSCOIL LUIMNIGH College of Informatics and Electronics END OF SEMESTER ASSESSMENT PAPER MODULE CODE: MS4613 SEMESTER: Autumn 2002/03 MODULE TITLE: Vector Analysis DURATION OF EXAMINATION:

More information

Lecture 10 Divergence, Gauss Law in Differential Form

Lecture 10 Divergence, Gauss Law in Differential Form Lecture 10 Divergence, Gauss Law in Differential Form ections: 3.4, 3.5, 3.6 Homework: ee homework file Properties of the Flux Integral: Recap flux is the net normal flow of the vector field F through

More information

5. Suggestions for the Formula Sheets

5. Suggestions for the Formula Sheets 5. uggestions for the Formula heets Below are some suggestions for many more formulae than can be placed easily on both sides of the two standard 8½" " sheets of paper for the final examination. It is

More information

The Calculus of Vec- tors

The Calculus of Vec- tors Physics 2460 Electricity and Magnetism I, Fall 2007, Lecture 3 1 The Calculus of Vec- Summary: tors 1. Calculus of Vectors: Limits and Derivatives 2. Parametric representation of Curves r(t) = [x(t), y(t),

More information

Vector Analysis. Electromagnetic Theory PHYS 401. Fall 2017

Vector Analysis. Electromagnetic Theory PHYS 401. Fall 2017 Vector Analysis Electromagnetic Theory PHYS 401 Fall 2017 1 Vector Analysis Vector analysis is a mathematical formalism with which EM concepts are most conveniently expressed and best comprehended. Many

More information

MATH 280 Multivariate Calculus Fall Integrating a vector field over a surface

MATH 280 Multivariate Calculus Fall Integrating a vector field over a surface MATH 280 Multivariate Calculus Fall 2011 Definition Integrating a vector field over a surface We are given a vector field F in space and an oriented surface in the domain of F as shown in the figure below

More information

ENGI 4430 Parametric Vector Functions Page dt dt dt

ENGI 4430 Parametric Vector Functions Page dt dt dt ENGI 4430 Parametric Vector Functions Page 2-01 2. Parametric Vector Functions (continued) Any non-zero vector r can be decomposed into its magnitude r and its direction: r rrˆ, where r r 0 Tangent Vector:

More information

Introduction and Vectors Lecture 1

Introduction and Vectors Lecture 1 1 Introduction Introduction and Vectors Lecture 1 This is a course on classical Electromagnetism. It is the foundation for more advanced courses in modern physics. All physics of the modern era, from quantum

More information

ENERGY IN ELECTROSTATICS

ENERGY IN ELECTROSTATICS ENERGY IN ELECTROSTATICS We now turn to the question of energy in electrostatics. The first question to consider is whether or not the force is conservative. You will recall from last semester that a conservative

More information

The Divergence Theorem

The Divergence Theorem The Divergence Theorem 5-3-8 The Divergence Theorem relates flux of a vector field through the boundary of a region to a triple integral over the region. In particular, let F be a vector field, and let

More information

VECTORS. Vectors OPTIONAL - I Vectors and three dimensional Geometry

VECTORS. Vectors OPTIONAL - I Vectors and three dimensional Geometry Vectors OPTIONAL - I 32 VECTORS In day to day life situations, we deal with physical quantities such as distance, speed, temperature, volume etc. These quantities are sufficient to describe change of position,

More information

Tutorial 3 - Solutions Electromagnetic Waves

Tutorial 3 - Solutions Electromagnetic Waves Tutorial 3 - Solutions Electromagnetic Waves You can find formulas you require for vector calculus at the end of this tutorial. 1. Find the Divergence and Curl of the following functions - (a) k r ˆr f

More information

Ma 1c Practical - Solutions to Homework Set 7

Ma 1c Practical - Solutions to Homework Set 7 Ma 1c Practical - olutions to omework et 7 All exercises are from the Vector Calculus text, Marsden and Tromba (Fifth Edition) Exercise 7.4.. Find the area of the portion of the unit sphere that is cut

More information

EE2007: Engineering Mathematics II Vector Calculus

EE2007: Engineering Mathematics II Vector Calculus EE2007: Engineering Mathematics II Vector Calculus Ling KV School of EEE, NTU ekvling@ntu.edu.sg Rm: S2-B2b-22 Ver 1.1: Ling KV, October 22, 2006 Ver 1.0: Ling KV, Jul 2005 EE2007/Ling KV/Aug 2006 My part:

More information

Idz[3a y a x ] H b = c. Find H if both filaments are present:this will be just the sum of the results of parts a and

Idz[3a y a x ] H b = c. Find H if both filaments are present:this will be just the sum of the results of parts a and Chapter 8 Odd-Numbered 8.1a. Find H in cartesian components at P (, 3, 4) if there is a current filament on the z axis carrying 8mAinthea z direction: Applying the Biot-Savart Law, we obtain H a = IdL

More information

Announcements. From now on, the problem sets from each week s homework assignments will be the following Wednesday.

Announcements. From now on, the problem sets from each week s homework assignments will be the following Wednesday. Announcements From now on, the problem sets from each week s homework assignments will be the following Wednesday. Late assignments will not be accepted. I will post the solutions on line after class on

More information

Keble College - Hilary 2015 CP3&4: Mathematical methods I&II Tutorial 4 - Vector calculus and multiple integrals II

Keble College - Hilary 2015 CP3&4: Mathematical methods I&II Tutorial 4 - Vector calculus and multiple integrals II Keble ollege - Hilary 2015 P3&4: Mathematical methods I&II Tutorial 4 - Vector calculus and multiple integrals II Tomi Johnson 1 Prepare full solutions to the problems with a self assessment of your progress

More information

Multivariable Calculus

Multivariable Calculus Multivariable alculus Jaron Kent-Dobias May 17, 2011 1 Lines in Space By space, we mean R 3. First, conventions. Always draw right-handed axes. You can define a L line precisely in 3-space with 2 points,

More information

Integral Theorems. September 14, We begin by recalling the Fundamental Theorem of Calculus, that the integral is the inverse of the derivative,

Integral Theorems. September 14, We begin by recalling the Fundamental Theorem of Calculus, that the integral is the inverse of the derivative, Integral Theorems eptember 14, 215 1 Integral of the gradient We begin by recalling the Fundamental Theorem of Calculus, that the integral is the inverse of the derivative, F (b F (a f (x provided f (x

More information

Disclaimer: This Final Exam Study Guide is meant to help you start studying. It is not necessarily a complete list of everything you need to know.

Disclaimer: This Final Exam Study Guide is meant to help you start studying. It is not necessarily a complete list of everything you need to know. Disclaimer: This is meant to help you start studying. It is not necessarily a complete list of everything you need to know. The MTH 234 final exam mainly consists of standard response questions where students

More information

Divergence Theorem December 2013

Divergence Theorem December 2013 Divergence Theorem 17.3 11 December 2013 Fundamental Theorem, Four Ways. b F (x) dx = F (b) F (a) a [a, b] F (x) on boundary of If C path from P to Q, ( φ) ds = φ(q) φ(p) C φ on boundary of C Green s Theorem:

More information

Stokes s Theorem 17.2

Stokes s Theorem 17.2 Stokes s Theorem 17.2 6 December 213 Stokes s Theorem is the generalization of Green s Theorem to surfaces not just flat surfaces (regions in R 2 ). Relate a double integral over a surface with a line

More information

Calculus III. Math 233 Spring Final exam May 3rd. Suggested solutions

Calculus III. Math 233 Spring Final exam May 3rd. Suggested solutions alculus III Math 33 pring 7 Final exam May 3rd. uggested solutions This exam contains twenty problems numbered 1 through. All problems are multiple choice problems, and each counts 5% of your total score.

More information

Math 11 Fall 2018 Practice Final Exam

Math 11 Fall 2018 Practice Final Exam Math 11 Fall 218 Practice Final Exam Disclaimer: This practice exam should give you an idea of the sort of questions we may ask on the actual exam. Since the practice exam (like the real exam) is not long

More information

Code No. : Sub. Code : GMMA 21/ GMMC 21

Code No. : Sub. Code : GMMA 21/ GMMC 21 Reg. No. :... ode No. : 08 Sub. ode : GMMA 1/ GMM 1 B.Sc. (BS) DEGREE EXAMINATION, NOVEMBER 016. Second Semester Mathematics Main VETOR ALULUS (Also common to Maths with omputer Applications) (For those

More information

Divergence Theorem Fundamental Theorem, Four Ways. 3D Fundamental Theorem. Divergence Theorem

Divergence Theorem Fundamental Theorem, Four Ways. 3D Fundamental Theorem. Divergence Theorem Divergence Theorem 17.3 11 December 213 Fundamental Theorem, Four Ways. b F (x) dx = F (b) F (a) a [a, b] F (x) on boundary of If C path from P to Q, ( φ) ds = φ(q) φ(p) C φ on boundary of C Green s Theorem:

More information