• Aucun résultat trouvé

Sharp inequalities on circular and hyperbolic functions using a Bernoulli inequality type

N/A
N/A
Protected

Academic year: 2021

Partager "Sharp inequalities on circular and hyperbolic functions using a Bernoulli inequality type"

Copied!
10
0
0

Texte intégral

(1)

HAL Id: hal-02496097

https://hal.archives-ouvertes.fr/hal-02496097

Preprint submitted on 2 Mar 2020

HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires

Sharp inequalities on circular and hyperbolic functions using a Bernoulli inequality type

Abd Chouikha

To cite this version:

Abd Chouikha. Sharp inequalities on circular and hyperbolic functions using a Bernoulli inequality

type. 2020. �hal-02496097�

(2)

Sharp inequalities on circular and hyperbolic functions using a Bernoulli inequality type

Abd Raouf Chouikha

Abstract

In this paper, new sharp bounds for circular and hyperbolic func- tions are proved. We provide some improvements of previous results by using innite products, power series expansions and a variant of the so-called Bernoulli inequality. New proofs, renements as well as new results are oered.

Key Words and phrases: Circular function, Innite product, Bernoulli inequality.

1

During the past several years, sharp inequalities involving circular and hyperbolic functions have received a lot of attention. Thanks to their useful- ness in all areas of mathematics. Old and new such inequalities, as well as renements of the so-called Jordan's, Cusa-Huygens and Wilker inequalities, can be found in [5], and the references therein.

In this paper we present a new variant of the standard Bernoulli inequality.

This is more general than the one proved in [1]. It permits us to deduce some bounds for circular and hyperbolic functions. These bounds appear to be sharper than those proved previously.

In this paper we provide new lower bounds for the function cos(x) and

sin(x)x

as well as bounds for the products

sinh(x) sin(x)

x2

and cosh(x) cos(x), improving some of those established in the literature.

chouikha@math.univ-paris13.fr. 4, Cour des Quesblais 35430 Saint-Pere

1

2010 Mathematics Subject Classication : 26D07; 33B10; 33B20.

(3)

1 A variant of the Bernoulli inequality

The following two results concerning circular functions, they have been proved by C. Chesneau and Y. Bagul [1]. They improve theorems 1,2 of [2].

The rst result concerns bounds for cos(x) .

Proposition 2 For α (0, π/2) and x (0, α) , we have e

βx2

cos(x) e

x2/2

,

with β =

log(cos(xα)) α2

.

The second concerns bounds for

sin(x)x

.

Proposition 3 For α (0, π/2) and x (0, α) , we have e

γx2

cos(x) e

x2/2

,

with γ =

log(sin(xα)) α2

.

Their proofs are based on innite products of circular functions as well as the following standard Bernoulli inequality

Proposition 1 For u, v (0, 1) , we have 1 uv (1 v)

u

.

In this paper we propose at rst the following main result which improves the preceding

Theorem 1-1 For u, v (0, 1) , we have

1 uv (1 v)

u2

e

uv(u1)

(1 v)

u

.

Proof of Theorem 1-1 For u, v (0, 1) and k 1 , one has u

k

u

(4)

The logarithm series expansion gives log(1 uv) =

k≥1

u

k

v

k

k = uv

k≥2

u

k

v

k

k

≥ − uv + u

2

(

k≥2

v

k

k ) = uv + u

2

(v + log(1 v).

Composing by the exponential function, we obtain the left inequality. To prove the right inequality it suces to note that the function

f(v) = (1 v)e

v

is bounded by 1 for v (0, 1) . Then powering by u u

2

0 one gets f (v)

uu2

= (1 v)

uu2

e

v(uu2)

1

Implying

(1 v)

u2u

e

v(u2u)

1 or equivalently

(1 v )

u2

e

uv(u1)

(1 v )

u

since u

2

u .

Theorem 1-1 is a sort of a renement of the classical Bernoulli inequality.

It allows us in particular to improve the lower bounds of preceding Proposi- tions 1 and 2. It also allows to bring many other inequalities as well as with sharp bounds.

Proposition 1-2 For α (0, π/2) and x (0, α) , we have the following inequalities

(cos(α))

x2

(cos(α))

x4

e

(x

4α2x2

2 )

cos(x) e

x2/2

Proof of Proposition 1-2 We will use the innite product of the cosine function. For x IR we have

cos(x) = (1 4x

2

)

(5)

The upper bound has been proved (Proposition 2 of [1]). The lower bound follows from Theorem 1. We have to prove the middle bound. With respect that x (0, α) using the innite product and Theorem 1 we may write following [1]

cos(x) =

k≥1

(1

2

x

2

α

2

π

2

(2k 1)

2

) =

k≥1

(1

2

π

2

(2k 1)

2

x

2

α

2

)

k≥1

(1

2

x

2

π

2

(2k 1)

2

)

x

4 α4

e

2 π2(2k1)2(x4

α4xα22)

= (cos(α))

x

4 α4

e

k1(π2(2k2

1)2(x4

α4xα22))

. On the other hand the sum may be written

k≥1

2

π

2

(2k 1)

2

( x

4

α

4

x

2

α

2

) = ( x

4

α

4

x

2

α

2

) 4α

2

π

2

k≥1

1 (2k 1)

2

= ( x

4

α

4

x

2

α

2

) 4α

2

π

2

π

2

π

2

8 = ( x

4

α

4

x

2

α

2

) α

2

2 since

k≥1 1

(2k1)2

=

π82

.

Finally, we obtain the inequality

cos(x) (cos(α))

x4

e

(x

4 α4xα22)α22

.

The result below gives a generalization of [1, Proposition 3 ]. It improves the lower bound

Proposition 1-3 For α (0, π/2) and x (0, α) , we have the following inequalities

( sin(α) α )

x

2

α2

( sin(α) α )

x

4 α4

e

(x

4α2x2

2 )

sin(x)

x e

x2/6

(6)

Proof of Proposition 1-3 We will use the innite product of the sine function the so-called Euler expansion. For x IR we have

sin(x)

x =

k≥1

(1 x

2

π

2

k

2

)

The upper bound has been proved (Proposition 2 of [1]). The lower bound follows from Theorem 1. We have to prove the middle bound. With respect that x (0, α) using the innite product and Theorem 1 we may write following [1]

sin(x)

x =

k≥1

(1 α

2

x

2

α

2

π

2

k

2

) =

k≥1

(1 α

2

π

2

k

2

x

2

α

2

)

k≥1

(1 α

2

x

2

π

2

k

2

)

x

4 α4

e

α

2 π2k2(x4

α4αx22)

= ( sin(α) α )

x

4 α4

e

k≥1( α2

π2k2(x4

α4xα22))

. On the other hand the sum may be written

k≥1

α

2

π

2

k

2

( x

4

α

4

x

2

α

2

) = ( x

4

α

4

x

2

α

2

) α

2

π

2

k≥1

1 k

2

= ( x

4

α

4

x

2

α

2

) α

2

π

2

π

2

6 = ( x

4

α

4

x

2

α

2

) α

2

6 since

k≥1 1

k2

=

π62

.

Finally, we obtain the inequality sin(x)

x ( sin(α) α )

x

4 α4

e

(x

4 α4αx22)α62

.

(7)

2 Others applications on the lower bounds

In [3, Theorem 1.26] the authors proved for x (0, π) the following inequality sin(x)

x (1 x

2

π

2

)

π

2 6

.

The following improves this lower bound

Proposition 2-4 For x (0, π) we have the inequalities sin(x)

x (1 x

2

π

2

)

π

4 90

e

x2(π

2

9016)

(1 x

2

π

2

)

π

2 6

.

Proof of Proposition 2-4 By Theorem 1 and the innite product we get sin(x)

x =

k≥1

(1 x

2

π

2

k

2

)

k≥1

(1 x

2

π

2

)

k14

e

x

2 π2k2(1

k21)

= (1 x

2

π

2

)

k1

1 k

4

e

x

2 π2(

k1 1 k4

k1 1 k2)

= (1 x

2

π

2

)

π

4 90

e

x

2

π2(π904π62)

.

On the other hand, the well known inequality of the product

sin(x) sinh(x) x

2

has been improved in [4, Propositions 2.1 and 2.2] in using innite product and Bernoulli inequality. We propose the following which is a renement than the previous.

Proposition 2-5 For x (0, π) we have the inequalities ( sin(α) sinh(α)

α

2

)

x

4

α4

( sin(α) sinh(α) α

2

)

x

8 α8

e

[x

4 90(x4

α41)]

sin(x) sinh(x)

x

2

e

x

4 90

x

2

(1 x

4

π

4

)

π

4

90

x

2

(1 x

4

π

4

)

π

8 9450

e

[x

4 90(x4

π4−1)]

sin(x) sinh(x)

x

2

(8)

Proof of Proposition 2-5 The upper bound has been proved (Proposition 2.1 of [4]). The lower bound follows from Theorem 1. We have to prove the middle bound. With respect that x (0, α) using the innite products

sin(x)

x =

k≥1

(1 x

2

π

2

k

2

), sinh(x)

x =

k≥1

(1 + x

2

π

2

k

2

).

Therefore

sin(x) sinh(x) = x

2

k≥1

(1 x

4

π

4

k

4

).

For this bound we will use Theorem 1. It follows sin(x) sinh(x) = x

2

k≥1

(1 α

4

x

4

π

4

α

4

k

4

)

k≥1

(1 α

4

π

4

k

4

)

x

8 α8

e

[ x

4 π4k4(x4

α4−1)]

= x

2

( sin(α) sinh(α) α

2

)

x

8 α8

e

[x

4 π4(x4

α41)

k1 1 k4]

. It implies the inequality since

k≥1 1

k4

=

π904

.

For the second inequality which is sharp than the preceding we use again the innite products

sin(x) sinh(x) = x

2

k≥1

(1 x

4

π

4

k

4

).

By Theorem 1 we may write

sin(x) sinh(x) = x

2

k≥1

(1 x

4

π

4

1

k

4

) x

2

k≥1

(1 x

4

π

4

)

k18

e

[ x

4 π4k4(x4

π41)]

= x

2

(1 x

4

π

4

)

ζ(8)

e

x

4 π4(x4

π41)ζ(4)

. Thus

sin(x) sinh(x) x

2

(1 x

4

π

4

)

π

8 9450

e

[x

4 π4(x4

π41)π904]

.

Similarly, for the cosine product cos(x) cosh(x) we have the following result

(9)

Proposition 2-6 For x (0, π) we have the inequalities [cos(α) cosh(α)]

x

4

α4

[cos(α) cosh(α)]

x

8 α8

e

[16x

4 96 (x4

α41)]

cos(x) cosh(x) e

x

4 6

(1 16x

4

π

4

)

π

4

90

(1 16x

4

π

4

)

17π

8 161280

e

[16x

4 96 (x4

π41)]

cos(x) cosh(x).

Proof of Proposition 2-6 The upper bound has been proved (Proposition 2.3 of [4]). The lower bound follows from Theorem 1. We have to prove the middle bound. With respect that x (0, α) using the innite products For x IR we have

cos(x) =

k≥1

(1 4x

2

π

2

(2k 1)

2

), cosh(x)

x =

k≥1

(1 + 4x

2

π

2

(2k 1)

2

).

Therefore

cos(x) cosh(x) =

k≥1

(1 16x

4

π

4

(2k 1)

4

).

For this bound we will use Theorem 1. It follows cos(x) cosh(x) =

k≥1

(1 16α

4

x

4

π

4

α

4

(2k 1)

4

)

k≥1

[1 α

4

π

4

(2k 1)

4

]

x

8 α8

e

[

16x4 π4(2k−1)4(x4

α41)]

= [cos(α) cosh(α)]

x

8 α8

e

[

16x4 π4 (x4

α41)

k1 1 (2k1)4]

. It implies the inequality since

k≥1 1

(2k1)4

=

π964

.

For the second inequality which is sharp than the preceding we use again the innite products

cos(x) cosh(x) =

k≥1

(1 16x

4

π

4

(2k 1)

4

).

By Theorem 1 we may write cos(x) cosh(x) =

k≥1

(1 16x

4

π

4

1

(2k 1)

4

) x

2

k≥1

[1 16x

4

π

4

]

1 (2k1)8

e

[

16x4 π4(2k1)4(x4

π41)]

(10)

= [1 16x

4

π

4

]

17π

8 161280

e

[16x

4 π4 (x4

π4−1)π964]

since

k≥1 1

(2k1)8

=

16128017π8

. Thus

cos(x) cosh(x) [1 16x

4

π

4

]

17π

8 161280

e

[x

4 96(x4

π41)]

.

REFERENCES

[1] C. Chesneau and Y. Bagul, A note on some new bounds for trigono- metric functions using innite products, 2018. hal-01934571v2.

[2] Y. Bagul, Inequalities involving circular, hyperbolic and exponential functions, J. of Math. Ineq, vol 11, n 3, pp 695-699, 2017.

[3] B. Bhayo and J. Sandor, On Jordan's, Redheer's and Wilker's in- equality, J. of Math. Ineq, vol 19, n 3, pp 823-839, 2016.

[4] C. Chesneau and Y. Bagul, New renements of two well-known in- equalities, https://www.researchgate.net/publication/332849515.

[5] L. Zhu, A source of inequalities for circular functions, Comp. and

Math. with Appl., 58, pp 1998-2004, 2009.

Références

Documents relatifs

The main aim of this note is to prove a sharp Poincaré-type inequality for vector- valued functions on S 2 , that naturally emerges in the context of micromagnetics of spherical

For other interesting applications of the main results, sharp bounds of the truncated Gaussian sine integral and error functions are established.. They can be useful in

Bagul, New inequalities involving circular, inverse circu- lar, hyperbolic, inverse hyperbolic and exponential functions, Ad- vances in Inequalities and Applications, Volume

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des

Estimates of the norms of derivatives for polynomials and rational functions (in different functional spaces) is a classical topic of complex analysis (see surveys by A.A.

By using inequalities involving several means, Neuman [4] presented the fol- lowing inequality chain generalizing the Adamovic-Mitrinovic inequality... (5) Proof Indeed, Let us

Key Words and phrases: Circular function, hyperbolic function, Innite product, Bernoulli inequality.. See Mitrinovic and Pecaric [1] for

The aim of this paper is to give the sharp form of the Bernstein and Markov in- equalities for rational functions on smooth Jordan curves and arcs. We shall be primarily interested