THE IMPLICIT FUNCTION THEOREM. g ( x 0 2,x 0 3,..., x 0 n)
|
|
- Φίλητος Ζαχαρίου
- 8 χρόνια πριν
- Προβολές:
Transcript
1 THE IMPLICIT FUNCTION THEOREM 11 Statement of the theorem 1 A SIMPLE VERSION OF THE IMPLICIT FUNCTION THEOREM Theorem 1 (Simple Implicit Function Theorem) Suppose that φ is a real-valued functions defined on a domain D and continuously differentiable on an open set D 1 D R n, ( x 1,x 2,, x n) D 1, and Further suppose that φ ( x 1,x 2,, x n) (1) φ ( x 1,x 2,, x n) (2) Then there exists a neighborhood V δ (x 2,x 3,, x n) D 1, an open set W R 1 containing x 1 and a real valued function ψ 1 : V W, continuously differentiable on V, such that ( ) x 1 ψ 1 x 2,x 3,, x n φ ( ) (3) ψ 1 (x 2,x 3,, x n),x 2,x 3,, x n Furthermore for k 2,, n, ψ 1 (x 2,x 3,, x n) φ(ψ 1(x 2,x 3,, x n ),x 2,x 3,, x n ) x k φ(ψ 1(x 2,x 3,, x n ),x 2,x 3,, x n ) φ(x ) φ(x ) (4) We can prove this last statement as follows Define g:v R n as g ( x 2,x 3,, x n) ψ 1 (x 2,, x n) x 2 x 3 x n (5) Then (φ g)(x 2,, x n ) for all (x 2,, x n ) V Thus by the chain rule Date: October 1, 25 1
2 2 THE IMPLICIT FUNCTION THEOREM D (φ g)(x 2,, x n) Dφ ( g(x 2,, x n) ) Dg(x 2, x n) For any k 2, 3,, n, we then have Dφ ( x 1,x 2,, xn) Dg(x 2, x n) x 1 ψ 1 (x x 2,, x n) 2 x Dφ x 2 3 D x 3 x n x n ψ 1 ψ 1 ψ x 3 1 x n [ ] 1 φ, φ,, φ x n 1 [ ] 1 (6) φ(x 1,x 2,,x n ) ψ 1 (x 2,,x n ) + φ(x 1,x 2,,x n ) ψ 1(x 2,,x n) φ(x 1,x 2,,x n ) φ(x 1,x 2,,x n ) We can, of course, solve for any other x k ψ k ( x 1,x 2,,x k 1,x k+1,,x n), as a function of the other x s rather than x 1 as a function of ( x 2,x 3,x n) 12 Examples 121 Production function Consider a production function given by (7) Write this equation implicitly as y f(x 1,x 2, x n ) (8) φ(x 1,x 2,, x n,y) f(x 1,x 2, x n ) y (9) where φ is now a function of n+1 variables instead of n variables Assume that φ is continuously differentiable and the Jacobian matrix has rank 1 ie, φ f, j 1, 2,,n (1) Given that the implicit function theorem holds, we can solve equation 9 for x k as a function of y and the other x s ie Thus it will be true that or that x k ψ k (x 1,x 2,, x k 1,x k+1,, y) (11) φ(y, x 1,x 2,, x k 1,x k,x k+1,, x n ) (12)
3 THE IMPLICIT FUNCTION THEOREM 3 y f(x 1,x 2,, x k 1,x k,x k+1,, x n ) (13) Differentiating the identity in equation 13 with respect to x j will give or Or we can obtain this directly as f + f f (14) RT S MRS (15) f φ(y, x 1,x 2,, x k 1,ψ k,x k+1,, x n ) ψ k φ(y, x 1,x 2,, x k 1,ψ k,x k+1,, x n ) Consider the specific example φ φ f f MRS (16) y f (x 1,x 2 ) x 2 1 2x 1 x 2 + x 1 x 3 2 To find the partial derivative of x 2 with respect to x 1 we find the two partials of f as follows f f 2 x 1 2 x 2 + x x 1 x x 1 2 x 2 2 x 1 x x 1 x x Utility function u u (x 1,x 2 ) To find the partial derivative of x 2 with respect to x 1 we find the two partials of U as follows u u 123 Another utility function Consider a utility function given by This can be written implicitly as u x x x f (u, x 1,x 2,x 3 ) u x x x 1 6 3
4 4 THE IMPLICIT FUNCTION THEOREM Now consider some of the partial derivatives arising from this implicit function First consider the marginal rate of substitution of x 1 for x 2 f f ( 1 3 ) x x 3 2 x ( 1 4 ) 3 x 4 1 x x x 1 3 x 2 Now consider the marginal rate of substitution of x 2 for x 3 Now consider the marginal utility of x 2 x 3 u f x 3 f ( 1 6 ) x x x ( 1 3 ) x x x x 2 2 x 3 f f u ( 1 3 ) x x 3 2 x x x x THE GENERAL IMPLICIT FUNCTION THEOREM WITH P INDEPENDENT VARIABLES AND M IMPLICIT EQUATIONS 21 Motivation for implicit function theorem We are often interested in solving implicit systems of equations for m variables, say x 1,x 2,,x m in terms of m+p variables where there are a minimum of m equations in the system We typically label the variables x m+1,x m+2,,x m+p,y 1,y 2,,y p We are frequently interested in the derivatives xi where it is implicit that all other x k and all y l are held constant The conditions guaranteeing that we can solve for m of the variables in terms of p variables along with a formula for computing derivatives are given by the implicit function theorem One motivation for the implicit function theorem is that we can eliminate m variables from a constrained optimization problem using the constraint equations In this way the constrained problem is converted to an unconstrained problem and we can use the results on unconstrained problems to determine a solution 22 Description of a system of equations Suppose that we have m equations depending on m + p variables (parameters) written in implicit form as follows
5 THE IMPLICIT FUNCTION THEOREM 5 φ 1 (x 1,x 2,,x m,y 1,y 2,,y p ) φ 2 (x 1,x 2,,x m,y 1,y 2,,y p ) φ m (x 1,x 2,,x m,y 1,y 2,,y p ) (17) For example with m 2 and p 3, we might have φ 1 (x 1,x 2,p,w 1,w 2 ) (4) px1 6 x2 2 w 1 φ 2 (x 1,x 2,p,w 1,w 2 ) (2) px1 4 x2 8 w 2 where p, w 1 and w 2 are the independent variables y 1,y 2,andy 3 (18) 23 Jacobian matrix of the system The Jacobian matrix of the system in 17 is defined as matrix of first partials as follows J φ m φ m This matrix will be of rank m if its determinant is not zero x m x m φ m x m (19) 24 Statement of implicit function theorem Theorem 2 (Implicit Function Theorem) Suppose that φ i are real-valued functions defined on a domain D and continuously differentiable on an open set D 1 D R m+p, where p > and φ 1 (x 1,x 2,, x m,y 1,y 2,, y p) φ 2 (x 1,x 2,, x m,y 1,y 2,, y p) (2) We often write equation 2 as follows φ m (x 1,x 2,, x m,y 1,y 2,, y p) (x,y ) D 1 φ i (x,y ), i 1, 2,, m, and (x,y ) D 1 (21) [ ] φi(x Assume the Jacobian matrix,y ) has rank m Then there exists a neighborhood N δ (x,y ) D 1, an open set D 2 R p containing y and real valued functions ψ k, k 1, 2,, m, continuously differentiable on D 2, such that the following conditions are satisfied:
6 6 THE IMPLICIT FUNCTION THEOREM x 1 ψ 1 (y ) x 2 ψ 2 (y ) (22) For every y D 2, we have x m ψ m (y ) φ i (ψ 1 (y), ψ 2 (y),, ψ m (y), y 1,y 2,, y p ), i 1, 2,, m or (23) φ i (ψ(y),y), i 1, 2,, m We also have that for all (x,y) N δ (x,y ), the Jacobian matrix [ ] φi(x, y) the partial derivatives of ψ(y) are the solutions of the set of linear equations has rank m Furthermore for y D 2, m k1 m k1 m k1 (ψ(y),y) (ψ(y),y) φ m (ψ(y),y) ψ k (y) ψ k (y) ψ k (y) We can write equation 24 in the following alternative manner (ψ(y),y) (ψ(y),y) φ m(ψ(y),y) (24) m k1 φ i (ψ(y),y) φ m ψ k (y) or perhaps most usefully as the following matrix equation φ 1 x m φ 2 x m φ m This of course implies ψ 1(y) ψ 2(y) ψ m(y) φ m x m φ m φ i(ψ(y),y) i 1, 2,, m (25) ψ 1(y) ψ 2(y) ψ m(y) φ m x m x m φ m x m 1 (ψ(y),y) (ψ(y),y) φ m(ψ(y),y) (ψ(y),y) (ψ(y),y) φ m(ψ(y),y) (26) (27)
7 THE IMPLICIT FUNCTION THEOREM 7 We can expand equation 27 to cover the derivatives with respect to the other y l by expanding the matrix equation ψ 1 (y) 1 ψ 2 (y) 1 ψ m(y) 1 ψ 1 (y) 2 ψ 2 (y) 2 ψ m(y) 2 ψ 1 (y) p ψ 2 (y) p ψ m(y) p φ m φ m 1 (ψ(y),y) x m 1 (ψ(y),y) x m 1 φ m φ m (ψ(y),y) x m 1 (ψ(y),y) 2 (ψ(y),y) 2 φ m(ψ(y),y) 2 (ψ(y),y) p (ψ(y),y) p φ m(ψ(y),y) p (28) 25 Some intuition for derivatives computed using the implicit function theorem To see the intuition of equation 24, take the total derivative of φ i in equation 23 with respect to y j as follows φ i ψ 1 ψ 1 φ i (ψ 1 (y), ψ 2 (y),,ψ m (y),y) + φ i ψ 2 ψ φ i ψ m and then move φi equations to obtain m equations in the m partial derivatives, xi ψ m + φ i to the right hand side of the equation Then perform a similar task for the other For the case of only one implicit equation 24 reduces to m k1 φ(ψ(y), y) ψi (29) ψ k (y) φ(ψ(y), y) (3) If there is only one equation, we can solve for only one of the x variables in terms of the other x variables and the p y variables and obtain only one implicit derivative which can be rewritten as φ(ψ(y), y) ψ k (y) φ(ψ(y), y) (31) ψ k (y) This is more or less the same as equation 4 φ(ψ(y), y) φ(ψ(y), y) (32) If there are only two variables, x 1 and x 2 where x 2 is now like y 1, we obtain φ(ψ 1 (x 2 ),x 2 ) ψ 1 (x 2 ) φ(ψ 1(x 2 ),x 2 ) ψ 1(x 2 ) φ(ψ 1(x 2),x 2) φ(ψ 1(x 2),x 2) which is like the example in section 121 where φ takes the place of f (33) 26 Examples
8 8 THE IMPLICIT FUNCTION THEOREM 261 One implicit equation with three variables φ(x 1,x 2,y ) (34) The implicit function theorem says that we can solve equation 34 for x 1 as a function of x 2 and y, ie, and that The theorem then says that x 1 ψ 1 (x 2,y ) (35) φ(ψ 1 (x 2,y), x 2,y) (36) 262 Production function example φ(ψ 1 (x 2,y), x 2,y) ψ 1 φ(ψ 1(x 2,y), x 2,y) (x 2,y) (x 2,y) φ(x 1,x 2,y ) y f(x 1,x 2) The theorem says that we can solve the equation for x 1 φ(ψ 1(x 2,y), x 2,y) φ(ψ 1(x 2,y), x 2,y) φ(ψ1(x2,y),x2,y) φ(ψ 1(x 2,y),x 2,y) (37) (38) It is also true that x 1 ψ 1 (x 2,y ) (39) φ(ψ 1 (x 2,y), x 2,y) y f(ψ 1 (x 2,y),x 2 ) Now compute the relevant derivatives (4) The theorem then says that φ(ψ 1 (x 2,y), x 2,y) f(ψ 1(x 2,y),x 2 ) φ(ψ 1 (x 2,y), x 2,y) f(ψ 1(x 2,y),x 2 ) (x 2,y) [ φ(ψ1(x 2,y),x 2,y) φ(ψ 1(x 2,y),x 2,y) [ f(ψ 1(x 2,y),x 2) f(ψ1(x2,y),x2) f(ψ 1(x 2,y),x 2) f(ψ 1(x 2,y),x 2) ] ] (41) (42)
9 THE IMPLICIT FUNCTION THEOREM 9 27 General example with two equations and three variables Consider the following system of equations The Jacobian is given by φ 1 (x 1,x 2,y) 3x 1 +2x 2 +4y φ 2 (x 1,x 2,y) 4x 1 + x 2 + y φ [ φ1 1 ] [ ] We can solve system 43 for x 1 and x 2 as functions of y Move y to the right hand side in each equation (43) (44) 3x 1 +2x 2 4y (45a) 4x 1 + x 2 y (45b) Now solve equation 45b for x 2 x 2 y 4x 1 (46) Substitute the solution to equation 46 into equation 45a and simplify 3x 1 +2( y 4x 1 ) 4y 3x 1 2y 8x 1 5x 1 4y 2y (47) x y ψ 1(y) Substitute the solution to equation 47 into equation 46 and simplify x 2 y 4 [ ] 2 5 y x y 8 5 y (48) 13 5 y ψ 2(y) If we substitute these expressions for x 1 and x 2 into equation 43 we obtain and ( ) [ ] φ 1 y, 5 5 y, y ) 3 5 y +2 [ 135 ] y 6 5 y 26 5 y y 2 5 y y +4y (49)
10 1 THE IMPLICIT FUNCTION THEOREM ( ) [ ] φ 2 y, 5 5 y, y ) 4 5 y + [ 13 ] 5 y + y Furthermore 8 5 y 13 5 y y 13 5 y 13 5 y (5) ψ 1 ψ We can solve for these partial derivatives using equation 24 as follows (51) ψ 1 + ψ 2 ψ 1 + ψ 2 (52a) (52b) Now substitute in the derivatives of φ 1 and φ 2 with respect to x 1,x 2, and y 3 ψ 1 +2 ψ 2 4 ψ 1 +1 ψ 2 4 (53a) 1 (53b) Solve equation 53b for ψ2 ψ ψ 1 Now substitute the answer from equation 54 into equation 53a (54) 3 ψ ( ψ ) ψ ψ 1 5 ψ 1 If we substitute equation 55 into equation 54 we obtain ψ (55)
11 THE IMPLICIT FUNCTION THEOREM 11 ψ 2 ψ ψ 1 ( ) We could also do this by inverting the matrix (56) 271 Profit maximization example 1 Consider the system in equation 18 We can solve this system of m implicit equations for all m of the x variables as functions of the p independent (y) variables Specifically, we can solve the two equations for x 1 and x 2 as functions ( of ) p, w 1, and w 2, ie, x 1 ψ 1 (p, w 1,w 2 ) and x 2 ψ 2 (p, w 1,w 2 ) We can also find x1 x2 and, that is ψi, from the following two equations derived from equation 18 which is repeated here φ 1 (x 1,x 2,p,w 1,w 2 ) (4) px1 6 x2 2 w 1 φ 2 (x 1,x 2,p,w 1,w 2 ) (2) px1 4 x2 8 w 2 [ ] ( 24) px 16 1 x [ (8) px1 6 x 2 8 ] [ (8) px 6 1 x2 8 ] + [ ( 16) px1 4 x 2 18 ] We can write this in matrix form as [ ( 24) px 16 1 x2 2 (8) px1 6 x2 8 (8) px1 6 x2 8 ( 16) px1 4 x 2 18 ][ ] x1 (4) x 6 1 x 2 2 (2) x4 1 x2 8 [ ] (4) x 6 1 x 2 2 (2) x 4 1 x 2 8 (57) (58) 272 Profit maximization example 2 Let the production function for a firm by given by Profit for the firm is given by y 14x 1 +11x 2 x 2 1 x 2 2 (59) π py w 1 x 1 w 2 x 2 p (14x 1 +11x 2 x 2 1 x 2 (6) 2) w 1 x 1 w 2 x 2 The first order conditions for profit maximization imply that π 14px 1 +11px 2 px 2 1 px 2 2 w 1 x 1 w 2 x 2 π φ 1 14p 2 px 1 w 1 π φ 1 11p 2 px 2 w 2 We can solve the first equation for x 1 as follows (61)
12 12 THE IMPLICIT FUNCTION THEOREM π 14p 2 px 1 w 1 2 px 1 14p w 1 x 1 14 p w 1 2 p 7 w 1 2 p In a similar manner we can find x 2 from the second equation π 11p 2 px 2 w 2 2 px 2 11p w 2 x 2 11 p w 2 2 p 55 w 2 2 p We can find the derivatives of x 1 and x 2 with respect to p, w 1 and w 2 directly as follows: (62) (63) x 1 x w 1 p w 2 p w 1 p 2 w p 1 w 2 (64) 1 2 w 2 p 2 w p 1 w 2 We can also find these derivatives using the implicit function theorem The two implicit equations are φ 1 (x 1,x 2,p,w 1,w 2 ) 14p 2 px 1 w 1 φ 2 (x 1,x 2 p, w 1,w 2 ) 11p 2 px 2 w 2 (65) First we check the Jacobian of the system It is obtained by differentiating φ 1 and φ 2 with respect to x 1 and x 2 as follows [ ] φ1 [ ] x J 1 2 p (66) 2p The determinant is 4p 2 which is positive Now we have two equations we can solve using the implicit function theorem The theorem says
13 THE IMPLICIT FUNCTION THEOREM 13 m k1 φ i (g (y), y) For the case of two equations we obtain g k (y) φ i(ψ(y), y),i 1, 2, (67) + + We can write this in matrix form as follows Solving for x1 [ φ1 x2 and we obtain [ ] x1 [ φ1 ][ x1 ] [ ] φ2 ] 1 [ ] φ2 We can compute the various partial derivatives of φ as follows (68) (69) (7) φ 1 (x 1,x 2,p,w 1,w 2 ) 14p 2 px 1 w 1 2 p 14 2 x 1 φ 2 (x 1,x 2 p, w 1,w 2 ) 11p 2 px 2 w 2 2 p 11 2 x 2 Now writing out the system we obtain for the case at hand we obtain [ x1 ] [ φ1 Now substitute in the elements of the inverse matrix [ x1 If we then invert the matrix we obtain ] ] 1 [ ] φ2 [ 2p ] 1 [ ] 2 x1 14 2p 2 x 2 11 (71) (72) (73)
14 14 THE IMPLICIT FUNCTION THEOREM Given that we obtain [ x1 ] x 1 [ 1 2p 1 2p ][ ] 2 x x 2 11 [ ] (74) 7 x1 p 55 x 2 p w 1 p 1 x w 2 p 1 (75) 7 x 1 p 7 (7 1 2 w 1 p 1 ) p 1 2 w 1 p 2 55 x 2 p 55 ( w 2 p 1 ) p (76) which is the same as before 1 2 w 2 p Profit maximization example 3 Verify the implicit function theorem derivatives x1 for the profit maximization example 2 w 1, w 2, w 1, x2 w Profit maximization example 4 A firm sells its output into a perfectly competitive market and faces a fixed price p It hires labor in a competitive labor market at a wage w, and rents capital in a competitive capital market at rental rate r The production is f(l, K) The production function is strictly concave The firm seeks to maximize its profits which are π pf(l, K) wl rk (77) The first-order conditions for profit maximization are π L pf L (L,K ) w π K pf K (L,K ) r This gives two implicit equations for K and L The second order conditions are (78) 2 π L 2 (L,K ) <, We can compute these derivatives as 2 π L 2 2 π K 2 [ 2 ] 2 π > at (L,K ) (79) L K
15 THE IMPLICIT FUNCTION THEOREM 15 2 π (pf L (L,K ) w ) L 2 L pf LL 2 π K (pf K (L,K ) r ) 2 L pf KK (8) 2 π L K (pf L (L,K ) w ) K pf KL The first of the second order conditions is satisfied by concavity of f We then write the second condition as D pf LL pf LK pf KL pf KK > p 2 f LL f LK > (81) f KL f KK p 2 (f LL f KK f KL f LK ) > The expression is positive or at least non-negative because f is assumed to be strictly concave Now we wish to determine the effects on input demands, L and K, of changes in the input prices Using the implicit function theorem in finding the partial derivatives with respect to w, we obtain for the first equation L π LL w + π K LK w + π Lw L pf LL w + pf K KL w 1 For the second equation we obtain (82) L π KL w + π K KK w + π Kw L pf KL w + pf K (83) KK w We can write this in matrix form as [ ][ ] [ ] pfll pf LK L / w 1 pf KL pf KK K (84) / w Using Cramer s rule, we then have the comparative-statics results L w 1 pf LK pf KK pf KK D D K w pf (85) LL 1 pf KL pf KL D D The sign of the first is negative because f KK < and D > from the second-order conditions Thus, the demand curve for labor has a negative slope However, in order to sign the effect of a change in the wage rate on the demand for capital, we need to know the sign of f KL, the effect of a change in the labor input
16 16 THE IMPLICIT FUNCTION THEOREM on the marginal product of capital We can derive the effects of a change in the rental rate of capital in a similar way 275 Profit maximization example 5 Let the production function be Cobb-Douglas of the form y L α K β Find the comparative-static effects L / w and K / w Profits are given by π pf(l, K) wl rk pl α K β wl rk The first-order conditions are for profit maximization are π L αpl α 1 K β w π K βpl α K β 1 r This gives two implicit equations for K and L The second order conditions are (86) (87) 2 π L 2 (L,K ) <, We can compute these derivatives as 2 π L 2 2 π K 2 [ 2 ] 2 π > at (L,K ) (88) L K 2 π L 2 α (α 1) pl α 2 K β 2 π K 2 β (β 1) plα K β 2 (89) 2 π L K αβplα 1 K β 1 The first of the second order conditions is satisfied as long as α, β<1 We can write the second condition as D α (α 1) plα 2 K β αβpl α 1 K β 1 αβpl α 1 K β 1 β (β 1) pl α K β 2 > (9) We can simplify D as follows D α (α 1) plα 2 K β αβpl α 1 K β 1 αβpl α 1 K β 1 β (β 1) pl α K β 2 The condition is then that p 2 α (α 1) L α 2 K β αβ L α 1 K β 1 αβ L α 1 K β 1 β (β 1) L α K β 2 p [ 2 αβ(α 1) (β 1) L α 2 K β L α K β 2 α 2 β 2 L 2α 2 2β K 2] p [ 2 αβl α 2 K β L α K β 2 ((α 1) (β 1) αβ ) ] p [ 2 αβl α 2 K β L α K β 2 ( αβ β α +1 αβ ) ] p [ 2 αβl α 2 K β L α K β 2 (1 α β ) ] (91) D p 2 αβl 2α 2 K 2β 2 (1 α β) > (92) This will be true if α+β <1
17 THE IMPLICIT FUNCTION THEOREM 17 Now we wish to determine the effects on input demands, L and K, of changes in the input prices Using the implicit function theorem in finding the partial derivatives with respect to w, we obtain for the first equation α (α 1) pl α 2 K β L w For the second equation we obtain π LL L w + π LK K w + π Lw + αβplα 1 K β 1 K w 1 (93) L π KL w αβpl α 1 K β 1 L + π KK We can write this in matrix form as [ α (α 1) pl α 2 K β αβpl α 1 K β 1 K w + π Kw w + β (β 1) plα K β 2 αβpl α 1 K β 1 β (β 1) pl α K β 2 Using Cramer s rule, we then have the comparative-statics results L 1 αβplα 1 K β 1 w β (β 1) pl α K β 2 D ][ L / w K / w ] β (β 1) plα K β 2 D (96) K α (α 1) plα 2 K β 1 w αβpl α 1 K β 1 αβplα 1 K β 1 D D The sign of the first of is negative because pβ(β 1) L α K β 2 < (β <1), and D > by the second order conditions The cross partial derivative K w is also less than zero because pαβlα 1 K β 1 > and D > So, for the case of a two-input Cobb-Douglas production function, an increase in the wage unambiguously reduces the demand for capital 3 TANGENTS TO φ(x 1, x 2,,)c AND PROPERTIES OF THE GRADIENT 31 Direction numbers A direction in R 2 is determined by an ordered pair of two numbers (a,b), not both zero, called direction numbers The direction corresponds to all lines parallel to the line through the origin (,) and the point (a,b) The direction numbers (a,b) and the direction numbers (ra,rb) determine the same direction, for any nonzero r A direction in R n is determined by an ordered n-tuple of numbers ( x 1,x 2,,xn), not all zero, called direction numbers The direction corresponds to all lines parallel to the line through the origin (,,,) and the point ( ( ( ) x 1,x 2,,xn) The direction numbers x 1,x 2,,xn) and the direction numbers rx 1,rx 2,,rx n determine the same direction, for any nonzero r If pick an r in the following way [ 1 ] (94) (95) then r 1 (x 1 ) 2 +(x 2 )2 + +(x n) 2 1 x (97)
18 18 THE IMPLICIT FUNCTION THEOREM cos γ 1 x 1 (x 1 ) 2 +(x 2 )2 + +(x n) 2 cos γ 2 x 2 (x 1 ) 2 +(x 2 )2 + +(x n) 2 (98) cos γ n x n (x 1 ) 2 +(x 2 )2 + +(x n )2 where γ j is the angle of the vector running through the origin and the point ( x 1,x 2,,x n) with the xj axis With this choice of r, the direction numbers (ra,rb) are just the cosines of the angles that the line makes with the positive x 1,x 2, and x n axes These angles γ 1, γ 2, are called the direction angles, and their cosines (cos[γ 1 ], cos[γ 2 ],) are called the direction cosines of that direction See figure 1 They satisfy cos 2 [γ 1 ] + cos 2 [γ 2 ]+ + cos 2 [γ n ] 1 FIGURE 1 Direction numbers as cosines of vector angles with the respective axes x x 1 1 x 1 x 3 x 2 x 3 5,, x 1 From equation 98, we can also write x ( x 1,x 2,,x ) ( n x cos[γ 1 ], x cos[γ 2 ],, x ) cos[γ n x (cos[γ 1 ], cos[γ 2 ],,cos[γ n ]) Therefore (99)
19 THE IMPLICIT FUNCTION THEOREM 19 1 x x (cos[γ 1 ], cos[γ 2 ],,cos[γ n ]) (1) which says that the direction cosines of x are the components of the unit vector in the direction of x Theorem 3 Ifθ is the angle between the vectors a abd b, then a b a b cos θ (11) 32 Planes in R n 321 Planes through the origin A plane through the origin in R n is given implicitly by the equation p x p 1 x 1 + p 2 x p n x n (12) 322 More general planes in R n A plane in R n through the point ( x 1,x 2,,x n) is given implicitly by the equation p (x x ) (13) p 1 (x 1 x 1 )+p 2(x 2 x 2 )+ + p n(x n x n ) We say that the vector p is orthogonal to the vector ( x x ) or x 1 x 1 [ ] x 2 x 2 p1 p 2 p n (14) x n x n The coefficients [p 1,p 2,,p n ] are the direction numbers of a line L passing through the point x or alternatively they are the coordinates of a point on a line through the origin that is parallel to L If p 1 is equal to -1, we can write equation 14 as follows x 1 x 1 p 2(x 2 x 2 )+p 3(x 2 x 3 )+ + p n(x n x n ) (15) 33 The general equation for a tangent hyperplane Theorem 4 Suppose D 1 R n is open, ( x 1,x 2,,x n) D 1, φ : D 1 R 1 is continuously differentiable, and Dφ ( x 1,x 2,,x n) Suppose φ ( x 1,x 2,,x n) c Then consider the level surface of the function φ (x 1,x 2,,x n ) φ ( x 1,x 2,,x n) c Denote this level service by M φ 1 ({c}) which consists all all values of (x 1,x 2,,x n ) such that φ(x 1,x 2,,x n ) c Then the tangent hyperplane at ( x 1,x 2,,x n) of M is given by T x M {x R n : Dφ(x )(x x )} (16) that is φ(x ) is nomal to the tangent hyperplane
20 2 THE IMPLICIT FUNCTION THEOREM Proof Because Dφ(x ), we may assume without loss of generality that φ (x ) Apply the implicit function theorem (Theorem 1) to the function φ c We then know that the level set can be expressed as a graph of the function x 1 ψ 1 (x 2,x 3,,x n ) for some continuous function ψ 1 Now the tangent plane to the graph x 1 ψ 1 (x 2,x 3,,x n ) at the point x [ψ 1 (x 2,x 3,,x n ),x 2,x 3,x n ] is the graph of the gradient ( ) Dψ 1 (x 2,x 3,,x n) translated so that it passes through x Using equation 15 where ψ1 x 2,x 3,,x n are the direction numbers we obtain n x 1 x ψ 1 ( ) 1 x,x 3,,x n (xk x k) (17) k k2 Now make the substitution from equation 4 in equation 17 to obtain x 1 x 1 Rearrange equation 18 to obtain n k2 34 Example Consider a function n k2 n k2 φ(ψ 1(x 2,x 3,, x n ),x 2,x 3,, x n ) φ(ψ 1(x 2,x 3,, x n ),x 2,x 3,, x n ) φ(x ) φ(x ) (x k x k) (18) (x k x k ) φ(x ) (x k x k)+ φ(x ) (x 1 x 1) Dφ(x )(x x ) (19) y f (x 1,x 2,,x n ) (11) evaluated at the point ( x 1,x 2,,x n ) y f (x 1,x 2,,x n) (111) The equation of the hyperplane tangent to the surface at this point is given by (y y ) f (x 1 x x 1)+ f (x 2 x 2 )+ + f (x n x 1 x n) n f (x 1 x x 1)+ f (x 2 x 2 )+ + f (x n x 1 x n) ( y y ) n f(x 1,x 2,,x n ) f(x 1,x 2,,x n)+ f (x 1 x x 1)+ f (x 2 x 1 x 2)+ + f (x n x 2 x n) n where the partial derivatives f x i are evaluated at ( x 1,x 2,,x n ) We can also write this as (112) f (x) f (x ) f (x )(x x ) (113) Compare this to the tangent equation with one variable y f (x ) f (x )(x x ) y f (x )+f (x )(x x ) and the tangent plane with two variables (114)
21 THE IMPLICIT FUNCTION THEOREM 21 y f(x 1,x 2) f (x 1 x 1)+ f (x 2 x 2) y f(x 1,x 2)+ f (x 1 x 1)+ f (x 2 x 2) 35 Vector functions of a real variable Let x 1,x 2,,x n be functions of a variable t defined on an interval I and write x(t) (x 1 (t),x 2 (t),,x n (t)) (116) The function t x(t) is a transformation from R to R n and is called a vector function of a real variable As x runs through I, x(t) traces out a set of points in n-space called a curve In particular, if we put x 1 (t) x 1 + ta 1,x 2 (t) x 2 + ta 2,,x n (t) x n + ta n (117) the resulting curve is a straight line in n-space It passes through the point x (x 1,x 2,,x n ) at t, and it is in the direction of the vector a (a 1,a 2,,a n ) We can define the derivative of x(t) as dx dt ẋ (t) ( dx1 (t) dt, dx 2(t) dt,, dx n(t) dt If K is a curve in n-space traced out by x(t), then ẋ (t) can be interpreted as a vector tangent to K at the point t 36 Tangent vectors Consider the function r(t) (x 1 (t), x 2 (t),,x n (t))and its derivative ṙ (t) (ẋ 1 (t), ẋ 2 (t),,ẋ n (t)) This function traces out a curve in R n We can call the curve K For fixed t, r (t + h) r (t) ṙ (t) lim (119) h h If ṙ (t), then for t + h close enough to t, the vector r(t+h) - r(t) will not be zero As h tends to, the quantity r(t+h) - r(t) will come closer and closer to serving as a direction vector for the tangent to the curve at the point P This can be seen in figure 2 It may be tempting to take this difference as approximation of the direction of the tangent and then take the limit lim [ r (t + h) r (t)] (12) h and call the limit the direction vector for the tangent But the limit is zero and the zero vector has no direction Instead we use the a vector that for small h has a greater length, that is we use ) (115) (118) r (t + h) r (t) h For any real number h, this vector is parallel to r(t+h) - r(t) Therefore its limit r (t + h) r (t) ṙ (t) lim h h can be taken as a direction vector for the tangent line (121) (122)
22 22 THE IMPLICIT FUNCTION THEOREM FIGURE 2 Tangent to a Curve 37 Tangent lines, level curves and gradients Consider the equation f (x) f (x 1,x 2,,x n ) c (123) which defines a level curve for the function f Let x (x 1,x 2,,x n ) be a point on the surface and let x (t) (x 1 (t), x 2 (t),,x n (t)) represent a differentiable curve K lying on the surface and passing through x attt Because K lies on the surface, f [x(t)] f [x 1 (t), x 2 (t),,,, x n (t)] c for all t Now differentiate equation 123 with respect to t f(x) t + f(x) t + + f(x) t f (x ) ẋ (t ) Because the vector ẋ (t) (ẋ 1 (t), ẋ 2 (t),, ẋ n (t))has the same direction as the tangent to the curve Katx, the gradient of f is orthogonal to the curve K at the point x Theorem 5 Suppose f(x 1,x 2,,x n ) is continuous and differentiable in a domain A and suppose that x(x 1,x 2,,x n ) A The gradient (124)
23 THE IMPLICIT FUNCTION THEOREM 23 ( f f, f,, f ) x n has the following properties at points x where f(x) (i) f(x) is orthogonal to the level surfaces f(x 1,x 2,,x n )c (ii) f(x) points in the direction of the steepest increase on f (iii) f(x) is the value of the directional derivative in the direction of steepest increase
24 24 THE IMPLICIT FUNCTION THEOREM REFERENCES [1] Hadley, G Linear Algebra Reading, MA: Addison-Wesley, 1961 [2] Sydsaeter, Knut Topics in Mathematical Analysis for Economists New York: Academic Press, 1981
THE IMPLICIT FUNCTION THEOREM = 0 (1) φ ( x 0 1, x0 2,..., x0 n) x 1 = 0 (2)
THE IMPLICIT FUNCTION THEOREM Statement of the theorem A SIMPLE VERSION OF THE IMPLICIT FUNCTION THEOREM Theorem (Simple Implicit Function Theorem) Suppose that φ is a real-valued functions defined on
Homework 8 Model Solution Section
MATH 004 Homework Solution Homework 8 Model Solution Section 14.5 14.6. 14.5. Use the Chain Rule to find dz where z cosx + 4y), x 5t 4, y 1 t. dz dx + dy y sinx + 4y)0t + 4) sinx + 4y) 1t ) 0t + 4t ) sinx
Chapter 6: Systems of Linear Differential. be continuous functions on the interval
Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations
Parametrized Surfaces
Parametrized Surfaces Recall from our unit on vector-valued functions at the beginning of the semester that an R 3 -valued function c(t) in one parameter is a mapping of the form c : I R 3 where I is some
2 Composition. Invertible Mappings
Arkansas Tech University MATH 4033: Elementary Modern Algebra Dr. Marcel B. Finan Composition. Invertible Mappings In this section we discuss two procedures for creating new mappings from old ones, namely,
Second Order Partial Differential Equations
Chapter 7 Second Order Partial Differential Equations 7.1 Introduction A second order linear PDE in two independent variables (x, y Ω can be written as A(x, y u x + B(x, y u xy + C(x, y u u u + D(x, y
Areas and Lengths in Polar Coordinates
Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the
Section 8.3 Trigonometric Equations
99 Section 8. Trigonometric Equations Objective 1: Solve Equations Involving One Trigonometric Function. In this section and the next, we will exple how to solving equations involving trigonometric functions.
3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β
3.4 SUM AND DIFFERENCE FORMULAS Page Theorem cos(αβ cos α cos β -sin α cos(α-β cos α cos β sin α NOTE: cos(αβ cos α cos β cos(α-β cos α -cos β Proof of cos(α-β cos α cos β sin α Let s use a unit circle
derivation of the Laplacian from rectangular to spherical coordinates
derivation of the Laplacian from rectangular to spherical coordinates swapnizzle 03-03- :5:43 We begin by recognizing the familiar conversion from rectangular to spherical coordinates (note that φ is used
Areas and Lengths in Polar Coordinates
Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the
HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:
HOMEWORK 4 Problem a For the fast loading case, we want to derive the relationship between P zz and λ z. We know that the nominal stress is expressed as: P zz = ψ λ z where λ z = λ λ z. Therefore, applying
Chapter 6: Systems of Linear Differential. be continuous functions on the interval
Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations
CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS
CHAPTER 5 SOLVING EQUATIONS BY ITERATIVE METHODS EXERCISE 104 Page 8 1. Find the positive root of the equation x + 3x 5 = 0, correct to 3 significant figures, using the method of bisection. Let f(x) =
Example Sheet 3 Solutions
Example Sheet 3 Solutions. i Regular Sturm-Liouville. ii Singular Sturm-Liouville mixed boundary conditions. iii Not Sturm-Liouville ODE is not in Sturm-Liouville form. iv Regular Sturm-Liouville note
Math221: HW# 1 solutions
Math: HW# solutions Andy Royston October, 5 7.5.7, 3 rd Ed. We have a n = b n = a = fxdx = xdx =, x cos nxdx = x sin nx n sin nxdx n = cos nx n = n n, x sin nxdx = x cos nx n + cos nxdx n cos n = + sin
If we restrict the domain of y = sin x to [ π, π ], the restrict function. y = sin x, π 2 x π 2
Chapter 3. Analytic Trigonometry 3.1 The inverse sine, cosine, and tangent functions 1. Review: Inverse function (1) f 1 (f(x)) = x for every x in the domain of f and f(f 1 (x)) = x for every x in the
SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions
SCHOOL OF MATHEMATICAL SCIENCES GLMA Linear Mathematics 00- Examination Solutions. (a) i. ( + 5i)( i) = (6 + 5) + (5 )i = + i. Real part is, imaginary part is. (b) ii. + 5i i ( + 5i)( + i) = ( i)( + i)
Partial Differential Equations in Biology The boundary element method. March 26, 2013
The boundary element method March 26, 203 Introduction and notation The problem: u = f in D R d u = ϕ in Γ D u n = g on Γ N, where D = Γ D Γ N, Γ D Γ N = (possibly, Γ D = [Neumann problem] or Γ N = [Dirichlet
If we restrict the domain of y = sin x to [ π 2, π 2
Chapter 3. Analytic Trigonometry 3.1 The inverse sine, cosine, and tangent functions 1. Review: Inverse function (1) f 1 (f(x)) = x for every x in the domain of f and f(f 1 (x)) = x for every x in the
Reminders: linear functions
Reminders: linear functions Let U and V be vector spaces over the same field F. Definition A function f : U V is linear if for every u 1, u 2 U, f (u 1 + u 2 ) = f (u 1 ) + f (u 2 ), and for every u U
Homework 3 Solutions
Homework 3 Solutions Igor Yanovsky (Math 151A TA) Problem 1: Compute the absolute error and relative error in approximations of p by p. (Use calculator!) a) p π, p 22/7; b) p π, p 3.141. Solution: For
D Alembert s Solution to the Wave Equation
D Alembert s Solution to the Wave Equation MATH 467 Partial Differential Equations J. Robert Buchanan Department of Mathematics Fall 2018 Objectives In this lesson we will learn: a change of variable technique
Section 7.6 Double and Half Angle Formulas
09 Section 7. Double and Half Angle Fmulas To derive the double-angles fmulas, we will use the sum of two angles fmulas that we developed in the last section. We will let α θ and β θ: cos(θ) cos(θ + θ)
Matrices and Determinants
Matrices and Determinants SUBJECTIVE PROBLEMS: Q 1. For what value of k do the following system of equations possess a non-trivial (i.e., not all zero) solution over the set of rationals Q? x + ky + 3z
Problem Set 3: Solutions
CMPSCI 69GG Applied Information Theory Fall 006 Problem Set 3: Solutions. [Cover and Thomas 7.] a Define the following notation, C I p xx; Y max X; Y C I p xx; Ỹ max I X; Ỹ We would like to show that C
Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)
Phys460.nb 81 ψ n (t) is still the (same) eigenstate of H But for tdependent H. The answer is NO. 5.5.5. Solution for the tdependent Schrodinger s equation If we assume that at time t 0, the electron starts
Section 9.2 Polar Equations and Graphs
180 Section 9. Polar Equations and Graphs In this section, we will be graphing polar equations on a polar grid. In the first few examples, we will write the polar equation in rectangular form to help identify
forms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with
Week 03: C lassification of S econd- Order L inear Equations In last week s lectures we have illustrated how to obtain the general solutions of first order PDEs using the method of characteristics. We
EE512: Error Control Coding
EE512: Error Control Coding Solution for Assignment on Finite Fields February 16, 2007 1. (a) Addition and Multiplication tables for GF (5) and GF (7) are shown in Tables 1 and 2. + 0 1 2 3 4 0 0 1 2 3
4.6 Autoregressive Moving Average Model ARMA(1,1)
84 CHAPTER 4. STATIONARY TS MODELS 4.6 Autoregressive Moving Average Model ARMA(,) This section is an introduction to a wide class of models ARMA(p,q) which we will consider in more detail later in this
CRASH COURSE IN PRECALCULUS
CRASH COURSE IN PRECALCULUS Shiah-Sen Wang The graphs are prepared by Chien-Lun Lai Based on : Precalculus: Mathematics for Calculus by J. Stuwart, L. Redin & S. Watson, 6th edition, 01, Brooks/Cole Chapter
ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?
Teko Classes IITJEE/AIEEE Maths by SUHAAG SIR, Bhopal, Ph (0755) 3 00 000 www.tekoclasses.com ANSWERSHEET (TOPIC DIFFERENTIAL CALCULUS) COLLECTION # Question Type A.Single Correct Type Q. (A) Sol least
The Simply Typed Lambda Calculus
Type Inference Instead of writing type annotations, can we use an algorithm to infer what the type annotations should be? That depends on the type system. For simple type systems the answer is yes, and
Concrete Mathematics Exercises from 30 September 2016
Concrete Mathematics Exercises from 30 September 2016 Silvio Capobianco Exercise 1.7 Let H(n) = J(n + 1) J(n). Equation (1.8) tells us that H(2n) = 2, and H(2n+1) = J(2n+2) J(2n+1) = (2J(n+1) 1) (2J(n)+1)
Every set of first-order formulas is equivalent to an independent set
Every set of first-order formulas is equivalent to an independent set May 6, 2008 Abstract A set of first-order formulas, whatever the cardinality of the set of symbols, is equivalent to an independent
PARTIAL NOTES for 6.1 Trigonometric Identities
PARTIAL NOTES for 6.1 Trigonometric Identities tanθ = sinθ cosθ cotθ = cosθ sinθ BASIC IDENTITIES cscθ = 1 sinθ secθ = 1 cosθ cotθ = 1 tanθ PYTHAGOREAN IDENTITIES sin θ + cos θ =1 tan θ +1= sec θ 1 + cot
ΕΛΛΗΝΙΚΗ ΔΗΜΟΚΡΑΤΙΑ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΡΗΤΗΣ. Ψηφιακή Οικονομία. Διάλεξη 7η: Consumer Behavior Mαρίνα Μπιτσάκη Τμήμα Επιστήμης Υπολογιστών
ΕΛΛΗΝΙΚΗ ΔΗΜΟΚΡΑΤΙΑ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΡΗΤΗΣ Ψηφιακή Οικονομία Διάλεξη 7η: Consumer Behavior Mαρίνα Μπιτσάκη Τμήμα Επιστήμης Υπολογιστών Τέλος Ενότητας Χρηματοδότηση Το παρόν εκπαιδευτικό υλικό έχει αναπτυχθεί
Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit
Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit Ting Zhang Stanford May 11, 2001 Stanford, 5/11/2001 1 Outline Ordinal Classification Ordinal Addition Ordinal Multiplication Ordinal
( ) 2 and compare to M.
Problems and Solutions for Section 4.2 4.9 through 4.33) 4.9 Calculate the square root of the matrix 3!0 M!0 8 Hint: Let M / 2 a!b ; calculate M / 2!b c ) 2 and compare to M. Solution: Given: 3!0 M!0 8
Numerical Analysis FMN011
Numerical Analysis FMN011 Carmen Arévalo Lund University carmen@maths.lth.se Lecture 12 Periodic data A function g has period P if g(x + P ) = g(x) Model: Trigonometric polynomial of order M T M (x) =
Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3
Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3 1 State vector space and the dual space Space of wavefunctions The space of wavefunctions is the set of all
Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.
Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο The time integral of a force is referred to as impulse, is determined by and is obtained from: Newton s 2 nd Law of motion states that the action
Other Test Constructions: Likelihood Ratio & Bayes Tests
Other Test Constructions: Likelihood Ratio & Bayes Tests Side-Note: So far we have seen a few approaches for creating tests such as Neyman-Pearson Lemma ( most powerful tests of H 0 : θ = θ 0 vs H 1 :
Srednicki Chapter 55
Srednicki Chapter 55 QFT Problems & Solutions A. George August 3, 03 Srednicki 55.. Use equations 55.3-55.0 and A i, A j ] = Π i, Π j ] = 0 (at equal times) to verify equations 55.-55.3. This is our third
Notes on the Open Economy
Notes on the Open Econom Ben J. Heijdra Universit of Groningen April 24 Introduction In this note we stud the two-countr model of Table.4 in more detail. restated here for convenience. The model is Table.4.
Inverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------
Inverse trigonometric functions & General Solution of Trigonometric Equations. 1. Sin ( ) = a) b) c) d) Ans b. Solution : Method 1. Ans a: 17 > 1 a) is rejected. w.k.t Sin ( sin ) = d is rejected. If sin
6.3 Forecasting ARMA processes
122 CHAPTER 6. ARMA MODELS 6.3 Forecasting ARMA processes The purpose of forecasting is to predict future values of a TS based on the data collected to the present. In this section we will discuss a linear
Tridiagonal matrices. Gérard MEURANT. October, 2008
Tridiagonal matrices Gérard MEURANT October, 2008 1 Similarity 2 Cholesy factorizations 3 Eigenvalues 4 Inverse Similarity Let α 1 ω 1 β 1 α 2 ω 2 T =......... β 2 α 1 ω 1 β 1 α and β i ω i, i = 1,...,
b. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds!
MTH U341 urface Integrals, tokes theorem, the divergence theorem To be turned in Wed., Dec. 1. 1. Let be the sphere of radius a, x 2 + y 2 + z 2 a 2. a. Use spherical coordinates (with ρ a) to parametrize.
C.S. 430 Assignment 6, Sample Solutions
C.S. 430 Assignment 6, Sample Solutions Paul Liu November 15, 2007 Note that these are sample solutions only; in many cases there were many acceptable answers. 1 Reynolds Problem 10.1 1.1 Normal-order
Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in
Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in : tail in X, head in A nowhere-zero Γ-flow is a Γ-circulation such that
1 String with massive end-points
1 String with massive end-points Πρόβλημα 5.11:Θεωρείστε μια χορδή μήκους, τάσης T, με δύο σημειακά σωματίδια στα άκρα της, το ένα μάζας m, και το άλλο μάζας m. α) Μελετώντας την κίνηση των άκρων βρείτε
( y) Partial Differential Equations
Partial Dierential Equations Linear P.D.Es. contains no owers roducts o the deendent variables / an o its derivatives can occasionall be solved. Consider eamle ( ) a (sometimes written as a ) we can integrate
Exercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.
Exercises 0 More exercises are available in Elementary Differential Equations. If you have a problem to solve any of them, feel free to come to office hour. Problem Find a fundamental matrix of the given
k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +
Chapter 3. Fuzzy Arithmetic 3- Fuzzy arithmetic: ~Addition(+) and subtraction (-): Let A = [a and B = [b, b in R If x [a and y [b, b than x+y [a +b +b Symbolically,we write A(+)B = [a (+)[b, b = [a +b
ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007
Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Αν κάπου κάνετε κάποιες υποθέσεις να αναφερθούν στη σχετική ερώτηση. Όλα τα αρχεία που αναφέρονται στα προβλήματα βρίσκονται στον ίδιο φάκελο με το εκτελέσιμο
Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1
Conceptual Questions. State a Basic identity and then verify it. a) Identity: Solution: One identity is cscθ) = sinθ) Practice Exam b) Verification: Solution: Given the point of intersection x, y) of the
6.1. Dirac Equation. Hamiltonian. Dirac Eq.
6.1. Dirac Equation Ref: M.Kaku, Quantum Field Theory, Oxford Univ Press (1993) η μν = η μν = diag(1, -1, -1, -1) p 0 = p 0 p = p i = -p i p μ p μ = p 0 p 0 + p i p i = E c 2 - p 2 = (m c) 2 H = c p 2
Lecture 15 - Root System Axiomatics
Lecture 15 - Root System Axiomatics Nov 1, 01 In this lecture we examine root systems from an axiomatic point of view. 1 Reflections If v R n, then it determines a hyperplane, denoted P v, through the
Trigonometric Formula Sheet
Trigonometric Formula Sheet Definition of the Trig Functions Right Triangle Definition Assume that: 0 < θ < or 0 < θ < 90 Unit Circle Definition Assume θ can be any angle. y x, y hypotenuse opposite θ
TMA4115 Matematikk 3
TMA4115 Matematikk 3 Andrew Stacey Norges Teknisk-Naturvitenskapelige Universitet Trondheim Spring 2010 Lecture 12: Mathematics Marvellous Matrices Andrew Stacey Norges Teknisk-Naturvitenskapelige Universitet
Pg The perimeter is P = 3x The area of a triangle is. where b is the base, h is the height. In our case b = x, then the area is
Pg. 9. The perimeter is P = The area of a triangle is A = bh where b is the base, h is the height 0 h= btan 60 = b = b In our case b =, then the area is A = = 0. By Pythagorean theorem a + a = d a a =
Uniform Convergence of Fourier Series Michael Taylor
Uniform Convergence of Fourier Series Michael Taylor Given f L 1 T 1 ), we consider the partial sums of the Fourier series of f: N 1) S N fθ) = ˆfk)e ikθ. k= N A calculation gives the Dirichlet formula
Quadratic Expressions
Quadratic Expressions. The standard form of a quadratic equation is ax + bx + c = 0 where a, b, c R and a 0. The roots of ax + bx + c = 0 are b ± b a 4ac. 3. For the equation ax +bx+c = 0, sum of the roots
Problem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.
Chemistry 362 Dr Jean M Standard Problem Set 9 Solutions The ˆ L 2 operator is defined as Verify that the angular wavefunction Y θ,φ) Also verify that the eigenvalue is given by 2! 2 & L ˆ 2! 2 2 θ 2 +
Section 8.2 Graphs of Polar Equations
Section 8. Graphs of Polar Equations Graphing Polar Equations The graph of a polar equation r = f(θ), or more generally F(r,θ) = 0, consists of all points P that have at least one polar representation
Statistical Inference I Locally most powerful tests
Statistical Inference I Locally most powerful tests Shirsendu Mukherjee Department of Statistics, Asutosh College, Kolkata, India. shirsendu st@yahoo.co.in So far we have treated the testing of one-sided
2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits.
EAMCET-. THEORY OF EQUATIONS PREVIOUS EAMCET Bits. Each of the roots of the equation x 6x + 6x 5= are increased by k so that the new transformed equation does not contain term. Then k =... - 4. - Sol.
Approximation of distance between locations on earth given by latitude and longitude
Approximation of distance between locations on earth given by latitude and longitude Jan Behrens 2012-12-31 In this paper we shall provide a method to approximate distances between two points on earth
Ενότητα 3: Ακρότατα συναρτήσεων μίας ή πολλών μεταβλητών. Νίκος Καραμπετάκης Τμήμα Μαθηματικών
ΑΡΙΣΤΟΤΕΛΕΙΟ ΠΑΝΕΠΙΣΤΗΜΙΟ ΘΕΣΣΑΛΟΝΙΚΗΣ ΑΝΟΙΧΤΑ ΑΚΑΔΗΜΑΙΚΑ ΜΑΘΗΜΑΤΑ Ενότητα 3: Ακρότατα συναρτήσεων μίας ή πολλών μεταβλητών Νίκος Καραμπετάκης Το παρόν εκπαιδευτικό υλικό υπόκειται σε άδειες χρήσης Creative
1. (a) (5 points) Find the unit tangent and unit normal vectors T and N to the curve. r(t) = 3cost, 4t, 3sint
1. a) 5 points) Find the unit tangent and unit normal vectors T and N to the curve at the point P, π, rt) cost, t, sint ). b) 5 points) Find curvature of the curve at the point P. Solution: a) r t) sint,,
Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013
Notes on Average Scattering imes and Hall Factors Jesse Maassen and Mar Lundstrom Purdue University November 5, 13 I. Introduction 1 II. Solution of the BE 1 III. Exercises: Woring out average scattering
Second Order RLC Filters
ECEN 60 Circuits/Electronics Spring 007-0-07 P. Mathys Second Order RLC Filters RLC Lowpass Filter A passive RLC lowpass filter (LPF) circuit is shown in the following schematic. R L C v O (t) Using phasor
Solutions to Exercise Sheet 5
Solutions to Eercise Sheet 5 jacques@ucsd.edu. Let X and Y be random variables with joint pdf f(, y) = 3y( + y) where and y. Determine each of the following probabilities. Solutions. a. P (X ). b. P (X
Appendix S1 1. ( z) α βc. dβ β δ β
Appendix S1 1 Proof of Lemma 1. Taking first and second partial derivatives of the expected profit function, as expressed in Eq. (7), with respect to l: Π Π ( z, λ, l) l θ + s ( s + h ) g ( t) dt λ Ω(
The challenges of non-stable predicates
The challenges of non-stable predicates Consider a non-stable predicate Φ encoding, say, a safety property. We want to determine whether Φ holds for our program. The challenges of non-stable predicates
Lecture 13 - Root Space Decomposition II
Lecture 13 - Root Space Decomposition II October 18, 2012 1 Review First let us recall the situation. Let g be a simple algebra, with maximal toral subalgebra h (which we are calling a CSA, or Cartan Subalgebra).
Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8 questions or comments to Dan Fetter 1
Eon : Fall 8 Suggested Solutions to Problem Set 8 Email questions or omments to Dan Fetter Problem. Let X be a salar with density f(x, θ) (θx + θ) [ x ] with θ. (a) Find the most powerful level α test
Finite Field Problems: Solutions
Finite Field Problems: Solutions 1. Let f = x 2 +1 Z 11 [x] and let F = Z 11 [x]/(f), a field. Let Solution: F =11 2 = 121, so F = 121 1 = 120. The possible orders are the divisors of 120. Solution: The
Differential equations
Differential equations Differential equations: An equation inoling one dependent ariable and its deriaties w. r. t one or more independent ariables is called a differential equation. Order of differential
Tutorial problem set 6,
GENERAL RELATIVITY Tutorial problem set 6, 01.11.2013. SOLUTIONS PROBLEM 1 Killing vectors. a Show that the commutator of two Killing vectors is a Killing vector. Show that a linear combination with constant
Congruence Classes of Invertible Matrices of Order 3 over F 2
International Journal of Algebra, Vol. 8, 24, no. 5, 239-246 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/.2988/ija.24.422 Congruence Classes of Invertible Matrices of Order 3 over F 2 Ligong An and
SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM
SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM Solutions to Question 1 a) The cumulative distribution function of T conditional on N n is Pr T t N n) Pr max X 1,..., X N ) t N n) Pr max
Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics
Fourier Series MATH 211, Calculus II J. Robert Buchanan Department of Mathematics Spring 2018 Introduction Not all functions can be represented by Taylor series. f (k) (c) A Taylor series f (x) = (x c)
Derivations of Useful Trigonometric Identities
Derivations of Useful Trigonometric Identities Pythagorean Identity This is a basic and very useful relationship which comes directly from the definition of the trigonometric ratios of sine and cosine
Spherical Coordinates
Spherical Coordinates MATH 311, Calculus III J. Robert Buchanan Department of Mathematics Fall 2011 Spherical Coordinates Another means of locating points in three-dimensional space is known as the spherical
ECE Spring Prof. David R. Jackson ECE Dept. Notes 2
ECE 634 Spring 6 Prof. David R. Jackson ECE Dept. Notes Fields in a Source-Free Region Example: Radiation from an aperture y PEC E t x Aperture Assume the following choice of vector potentials: A F = =
Review Test 3. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.
Review Test MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. Find the exact value of the expression. 1) sin - 11π 1 1) + - + - - ) sin 11π 1 ) ( -
CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS
CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS EXERCISE 01 Page 545 1. Use matrices to solve: 3x + 4y x + 5y + 7 3x + 4y x + 5y 7 Hence, 3 4 x 0 5 y 7 The inverse of 3 4 5 is: 1 5 4 1 5 4 15 8 3
Parallel transport and geodesics
Parallel transport and geodesics February 4, 3 Parallel transport Before defining a general notion of curvature for an arbitrary space, we need to know how to compare vectors at different positions on
10.7 Performance of Second-Order System (Unit Step Response)
Lecture Notes on Control Systems/D. Ghose/0 57 0.7 Performance of Second-Order System (Unit Step Response) Consider the second order system a ÿ + a ẏ + a 0 y = b 0 r So, Y (s) R(s) = b 0 a s + a s + a
Solution Series 9. i=1 x i and i=1 x i.
Lecturer: Prof. Dr. Mete SONER Coordinator: Yilin WANG Solution Series 9 Q1. Let α, β >, the p.d.f. of a beta distribution with parameters α and β is { Γ(α+β) Γ(α)Γ(β) f(x α, β) xα 1 (1 x) β 1 for < x
9.09. # 1. Area inside the oval limaçon r = cos θ. To graph, start with θ = 0 so r = 6. Compute dr
9.9 #. Area inside the oval limaçon r = + cos. To graph, start with = so r =. Compute d = sin. Interesting points are where d vanishes, or at =,,, etc. For these values of we compute r:,,, and the values
10/3/ revolution = 360 = 2 π radians = = x. 2π = x = 360 = : Measures of Angles and Rotations
//.: Measures of Angles and Rotations I. Vocabulary A A. Angle the union of two rays with a common endpoint B. BA and BC C. B is the vertex. B C D. You can think of BA as the rotation of (clockwise) with
Lecture 10 - Representation Theory III: Theory of Weights
Lecture 10 - Representation Theory III: Theory of Weights February 18, 2012 1 Terminology One assumes a base = {α i } i has been chosen. Then a weight Λ with non-negative integral Dynkin coefficients Λ
ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 24/3/2007
Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Όλοι οι αριθμοί που αναφέρονται σε όλα τα ερωτήματα μικρότεροι του 10000 εκτός αν ορίζεται διαφορετικά στη διατύπωση του προβλήματος. Αν κάπου κάνετε κάποιες υποθέσεις
ST5224: Advanced Statistical Theory II
ST5224: Advanced Statistical Theory II 2014/2015: Semester II Tutorial 7 1. Let X be a sample from a population P and consider testing hypotheses H 0 : P = P 0 versus H 1 : P = P 1, where P j is a known
Variational Wavefunction for the Helium Atom
Technische Universität Graz Institut für Festkörperphysik Student project Variational Wavefunction for the Helium Atom Molecular and Solid State Physics 53. submitted on: 3. November 9 by: Markus Krammer
Appendix to On the stability of a compressible axisymmetric rotating flow in a pipe. By Z. Rusak & J. H. Lee
Appendi to On the stability of a compressible aisymmetric rotating flow in a pipe By Z. Rusak & J. H. Lee Journal of Fluid Mechanics, vol. 5 4, pp. 5 4 This material has not been copy-edited or typeset