Derivative of a Vector Function : vector Calculus #Derivative #of #a #Vector #Function : #vector Calculus

                                                                                                  
Contents :                                                                      
 
         1. Vector function of a scalar variable

         2. Limit of a vector function

         3. Continuity of a vector function

         4. Derivative of a vector function

         5. Higher order derivatives

         6. Properties of derivatives

1.  Vector function of a scalar variable :
                                                                 Let S ⊂ R. Corresponding to each scalar t 𝞊 S, there is associated a unique vector r, then r  is said to be a vector ( vector valued ) function . S is called domain of R. We express it as r= f(t), where f denotes the law of correspondence.
                                                               let i,j,k be the three mutually perpendicuclar unit vectors in three dimensional space. Then the vector function f(t) may be expressed in the form 
               r= f(t)= f1(t) I + f2(t) j + f3(t) k.
 here f1(t),f2(t),f3(t) are the real valued functions and are called the components of r.

2. Limit of a Vector Function
                                                              let f(t) be a vector function over the domain S and a 𝞊 S. If ther exists a vector L such that for each 𝞊 >0, it is possible to find s>0 , where  0 < | t-a | <s  => | f(t) - L | < 𝞊
 then the vector L  is called the limit of f(t) as t tends to a.
                  This is denoted by Lt f(t) = L as t tends to a.

Note :
 Let  Lt A(t) =L and Lt B(t) = M and 𝛌  being any constant then 
   i) Lt ( A(t) + B(t) = L+M   ii) Lt [  𝛌 A(t)] = 𝛌L  iii) Lt  [( A(t) . B(t) ] = L. M  
   iv) L [(A(t) x B(t) ] = L x M , where . and x represents dot and cross product of vectors.

 3. Continuity of a Vector Function
                                                              
                                Let f be a vector function on an interval I and a 𝞊 I. Then f is said          to  be  continuous at a if Lt f(t) = f(a) as t tends to a.

  The function f is said to be continuous on I if f is continuous at every point of I.          

Note :  
    If f and g are continuous  then f ± g, f.g and fxg are also continuous.


 4. Derivative of a Vector Function :
                                                           
               Let f be a vector function on an interval I and a 𝞊 I . Then
    Lt (f(t) -f (a)) / (t-a) if is exist , it called  the derivative of f at 'a' and is denoted by                 f '(a) or [df/dt]   at      t=a.
         Also it is said that f is differentiable at t=a.      

 
Note :
 *  If f is differentiable at t=a , then it is continuous at t=a.
 *  If  f is continuous at t=a then it need not be differentiable at that point.
 *  If f is differentiable on an intervel I and t 𝞊 I then the derivative of f at t is denoted             by df/dt.
 *  As in calculus of real variables, if the changes in r, f are denoted by 𝝳t  and  𝝳f                  respectively then we have  
             df/dt = Lt  (𝝳f/𝝳t) = Lt ( f(t+𝝳t ) - f(t) )/ 𝝳t 

 5. Higher Order Derivatives :
                                              
                       Let f be differentiable on an interval I and f ' = df/dt of f.

      If Lt ( f’(t) – f ’(a) )/ t-a exists for each t 𝞊 I1 I, then f ‘ is said to be differentiable        on I1.  Also f is said to possess second derivative on I1 and is denoted by f ‘’ (t)  or            d2f/ dt2 .

       By induction if f(n-1) is differentiable on In-1 In-2 ⊂ … ⊂ I2 ⊂I1 ⊂ I  then f is           said to be possess nth derivative on In-1 and is denoted by f(n)  or dn f / dtn.

Derivative of a Constant Function :

 Let f be constant vector function on an interval I and a 𝞊 I. Then f ‘ (a) =0.

Proof :

 Let f be a constant vector function on an interval .

        Suppose f(t) =c ∀ t 𝞊 I , where c is a constant.

Let a 𝞊 I.

 For t tends to a,

         f ‘ (a) = Lt [ (f(t) -f(a)) / (t -a) ]

                    = Lt [ ( c-c) / (t-a) ]                       ( since f(t) = f(a) = c )

                    = Lt [0 / (t-a) ]

      f ‘ (a)    =0.

Properties of derivatives :

      Let A , B and C be two differentiable vector functions of scalar variable t over the domain S then

·          d/dt ( A ± B ) = dA/dt  ± dB/dt

·         d/dt ( A.B ) = dA/dt . B + A. dB/dt

·         d/dt ( AxB ) = dA/dt x B + A x dB/dt

·           d/dt ( ABC ) = [ dA/dt BC ] +[ A dB/dt C ] + [ AB dC/dt ]

·         d/dt ( AxBxC ) = dA/dt x( BxC ) + Ax (dB/dt xC )

·         d/dt ( f ) = ∅ (df/dt) + (d∅/dt) f , here ∅ is a scalar differentiable function

·          If f = f1 (t)i + f2 ( t)j + f3(t)k , where f1(t), f2(t), f3(t) are the cartesian components of the vector  f

                       then  df/dt = (df1/dt) i + (df2/dt) j + (df3/dt) k.

·          If A is a differentiable vector function of a scalar t over a domain S then d/dt (A2)= 2A (dA/dt)

·          The necessary and sufficient condition that f(t) is a vector of constant magnitude is

                       f . (df/dt) = 0.


























































#Derivative #of #a #Vector #Function  :  #Integral Calculus

         

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