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The function f:""R""~""{0}vec given by...

The function `f:""R""~""{0}vec` given by `f(x)=1/x-2/(e^(2x)-1)` can be made continuous at x = 0 by defining f(0) as

A

0

B

1

C

2

D

`-1`

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To determine the value of \( f(0) \) that makes the function \( f(x) = \frac{1}{x} - \frac{2}{e^{2x} - 1} \) continuous at \( x = 0 \), we need to find the limit of \( f(x) \) as \( x \) approaches 0. ### Step 1: Set up the limit We need to compute: \[ \lim_{x \to 0} f(x) = \lim_{x \to 0} \left( \frac{1}{x} - \frac{2}{e^{2x} - 1} \right) \] ### Step 2: Rewrite the limit To combine the two fractions, we find a common denominator: \[ f(x) = \frac{(e^{2x} - 1) - 2x}{x(e^{2x} - 1)} \] Thus, we rewrite the limit as: \[ \lim_{x \to 0} \frac{(e^{2x} - 1) - 2x}{x(e^{2x} - 1)} \] ### Step 3: Evaluate the limit As \( x \) approaches 0, both the numerator and denominator approach 0, which gives us a \( \frac{0}{0} \) indeterminate form. We can apply L'Hôpital's Rule. First, we differentiate the numerator and the denominator: - The derivative of the numerator \( (e^{2x} - 1) - 2x \) is \( 2e^{2x} - 2 \). - The derivative of the denominator \( x(e^{2x} - 1) \) is \( (e^{2x} - 1) + 2xe^{2x} \). Now we apply L'Hôpital's Rule: \[ \lim_{x \to 0} \frac{2e^{2x} - 2}{(e^{2x} - 1) + 2xe^{2x}} \] ### Step 4: Substitute \( x = 0 \) Now we substitute \( x = 0 \): - The numerator becomes \( 2e^{0} - 2 = 2 - 2 = 0 \). - The denominator becomes \( (e^{0} - 1) + 2 \cdot 0 \cdot e^{0} = 0 + 0 = 0 \). Since we still have a \( \frac{0}{0} \) form, we apply L'Hôpital's Rule again. ### Step 5: Differentiate again Differentiate the numerator and denominator again: - The second derivative of the numerator \( 2e^{2x} \) is \( 4e^{2x} \). - The second derivative of the denominator \( (e^{2x} - 1) + 2xe^{2x} \) is \( 2e^{2x} + 2e^{2x} + 4xe^{2x} = 4e^{2x} + 4xe^{2x} \). Now we apply L'Hôpital's Rule again: \[ \lim_{x \to 0} \frac{4e^{2x}}{4e^{2x} + 4xe^{2x}} \] ### Step 6: Substitute \( x = 0 \) again Substituting \( x = 0 \): - The numerator becomes \( 4e^{0} = 4 \). - The denominator becomes \( 4e^{0} + 0 = 4 + 0 = 4 \). Thus, the limit is: \[ \lim_{x \to 0} \frac{4}{4} = 1 \] ### Conclusion To make the function continuous at \( x = 0 \), we define: \[ f(0) = 1 \]

To determine the value of \( f(0) \) that makes the function \( f(x) = \frac{1}{x} - \frac{2}{e^{2x} - 1} \) continuous at \( x = 0 \), we need to find the limit of \( f(x) \) as \( x \) approaches 0. ### Step 1: Set up the limit We need to compute: \[ \lim_{x \to 0} f(x) = \lim_{x \to 0} \left( \frac{1}{x} - \frac{2}{e^{2x} - 1} \right) \] ...
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OBJECTIVE RD SHARMA ENGLISH-CONTINUITY AND DIFFERENTIABILITY-Exercise
  1. The function f:""R""~""{0}vec given by f(x)=1/x-2/(e^(2x)-1) can b...

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  2. The function f(x) = (4-x^(2))/(4x-x^(3)) is discontinuous at

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  3. Let f(x)=|x| and g(x)=|x^3| , then (a).f(x) and g(x) both are continuo...

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  4. The function f(x)=sin^(-1)(cosx) is discontinuous at x=0 (b) continuou...

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  5. The set of points where the function f(x)=x|x| is differentiable is...

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  6. On the interval I = [-2, 2], if the function f(x) = {{:((x+1)e^(-((1)/...

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  7. If f(x)={{:(,(|x+2|)/(tan^(-1)(x+2)),x ne -2),(,2, x=-2):}, then f(x) ...

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  8. Let f(x)=(x+|x|)|x| . Then, for all x f is continuous

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  9. The set of all points where the function f(x)=sqrt(1-e^(-x^2)) is di...

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  10. The function f(x)=e^(-|x|) is continuous everywhere but not differe...

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  11. The function f(x)=[cos x] is

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  12. If f(x)=sqrt(1-sqrt(1-x^2)) , then f(x) is (a) continuous on [-1, 1] ...

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  13. If f(x) = sin ^(-1)((2x)/(1 + x^(2))) then f (x) is differentiable in ...

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  14. about to only mathematics

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  15. If f(x)=|x-a|varphi(x), where varphi(x) is continuous function, then f...

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  16. If f(x)=x^2+(x^2)/(1+x^2)+(x^2)/((1+x^2)^2)+. . . . +(x^2)/((1+x^2)^n)...

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  17. If f(x)= | log10x| then at x=1.

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  18. If f(x)=|log(e) x|,then

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  19. If f(x)=|log(e)|x||," then "f'(x) equals

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  20. Let f(x)={1/(|x|)\ \ \ \ \ for\ |x|geq1a x^2+b\ \ \ \ \ \ \ \ for\ |x|...

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  21. Let h(x)="min "{x,x^(2)} for every real number of x. Then, which one o...

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