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Lagrange’s Mean Value Theorem

Here you will learn lagrange’s mean value theorem statement, its geometrical and physical interpretation with examples.

Let’s begin – 

Lagrange’s Mean Value Theorem (LMVT)

Statement : Let f be a function that satisfies the following conditions :

(i) f is continuous in [a, b]

(ii) f is differentiable in (a, b)

Then there is a number c in (a, b) such that f'(c) = f(b)f(a)ba

Geometrical Interpretation :

Geometrically, the lagrange’s mean value theorem says that somewhere between A and B the curve has atleast on tangent parallel to chord AB.

Physical Interpretation :

If we think  of the number (f(b) – f(a))/(b – a) as the average change in f over [a, b] and f'(c) as an instantaneous change, then the mean value theorem says that at some interior point the instantaneous change must equal the average change over the entire interval.

Example : find c of the Lagranges mean value theorem for the function f(x) = 3x2 + 5x + 7 in the interval [1, 3].

Solution : Given f(x) = 3x2 + 5x + 7

f(1) = 3 + 5 + 7 = 15 and f(3) = 27 + 15 + 7 = 49

Now, Differentiating f(x) with respect to x,

f'(x) = 6x + 5

Here a = 1, b = 3

Now from lagrange’s mean value theorem 

f'(c) = f(b)f(a)ba 6c + 5 = 49152 = 17

c = 2

Example : If f(x) is continuous and differentiable over [-2, 5] and -4 < f'(x) < 3 for all x in (-2, 5), then the greatest possible value of f(5) – f(-2) is –

Solution : Applying Lagranges mean value theorem (LMVT),

f'(x) = f(5)f(2)5(2) for some x in (-2, 5) 

Now, -4 f(5)f(2)7 3

-28 f(5) – f(-2) 21

  Greatest possible value of f(5) – f(-2) is 21.

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