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HAL Id: hal-02496089

https://hal.archives-ouvertes.fr/hal-02496089

Preprint submitted on 2 Mar 2020

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Sharp inequalities for ratio of trigonometric and hyperbolic functions

Abd Chouikha

To cite this version:

Abd Chouikha. Sharp inequalities for ratio of trigonometric and hyperbolic functions. 2020. �hal-

02496089�

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Sharp inequalities for ratio of trigonometric and hyperbolic functions

Abd Raouf Chouikha

Abstract

In this paper we establish a new variant of the Bernoulli inequal- ity in special cases. This result allows us to improve exponential and polynomial bounds for cosh x/ cos x as well as bounds for sinh x/ sin x . Key Words and phrases: Circular function, hyperbolic function, Innite product, Bernoulli inequality.

1

The classical Bernoulli inequality is known (1 + x)

s

1 + sx

It is dened for x > 1 and 0 s 1 , for s > 1 , the inequality reverses.

This one has been generalized in a number of ways. See Mitrinovic and Pecaric [1] for a survey.

This inequality played a historical role in improving the bounds of certain trigonometric and hyperbolic inequalities. Any renancing of this inequality has a denite impact on these improvements. One can refer to [1] and [2].

Recently the authors [3] and [4] have highlighted renements of the Bernoulli inequality, i.e. for u, v (0, 1) :

(1 v)

u

1 uv.

[email protected]. 4, Cour des Quesblais 35430 Saint-Pere

1

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

(3)

This allowed them to produce inequalities with better bounds. These relate to both trigonometric and hyperbolic functions as well as their ratio or prod- uct. In [3] the authors introduced a function f (u, v) which permits to sharp the Bernoulli inequality. We shall propose an other function g(u, v) . This func- tion is nest than f (u, v) in the sense that the following inequalities are satised

(1 v)

u

f (u, v)(1 v)

u

g(u, v)(1 v)

u

1 uv.

In this paper we deduce from this variant of Bernoulli inequality new bounds to the ratio functions cosh x/ cos x as well as bounds for sinh x/ sin x , im- proving some of those established in the literature.

1 New variant of Bernoulli inequality

In [3] the authors proved the following which gives a renement of the stan- dard Bernoulli inequality

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

1 uv f (u, v)(1 v)

u

where f(u, v) denotes the function

f (u, v) = 1 + uv (1 + v)

u

1

This proposition may be improved thanks to the following which allows us to derive a function g(u, v) nest than f(u, v).

Proposition 1-1 For u, v (0, 1) the following inequalities hold log

( 1 + uv )

2uv(1 u

2

) + u

3

log

( 1 + v )

u log

( 1 + v )

.

(4)

Proof We will use the logarithmic series expansion. For u, v (0, 1) we may write

log

( 1 + uv 1 uv

)

= 2

k≥1

(uv)

2k1

2k 1 = 2uv + 2[ (uv )

3

3 + (uv)

5

5 + ...]

For u, v (0, 1) and k 2 , we have u

2k1

u

3

. Therefore

2

k≥1

(uv)

2k1

2k 1 2uv + 2u

3

[ v

3

3 + v

5

5 + ...]

= 2uv + 2u

3

[ v + v + v

3

3 + v

5

5 + ...] = 2uv + u

3

[ 2v + 2

k≥1

v

2k1

2k 1 ]

= 2uv + u

3

[ 2v + log

( 1 + v 1 v

)

].

We thus obtain the left inequality log

( 1 + uv 1 uv

)

2uv(1 u

2

) + u

3

log

( 1 + v 1 v

)

.

To prove the right inequality it suces to remark that for v (0, 1) the well known inequality

2v log

( 1 + v 1 v

)

implies in multiplying by u u

3

0

2v(u u

3

) (u u

3

) log

( 1 + v 1 v

)

which also implies

2v(u u

3

) (u u

3

) log

( 1 + v 1 v

)

0.

Therefore

2v(u u

3

) + u

3

log

( 1 + v 1 v

)

u log

( 1 + v 1 v

)

.

(5)

As a corollary we deduce the following which improves the above Propo- sition 1

Corollary 1-2 For u, v (0, 1) the function f(u, v) dened above veries the following inequalities

1 f(u, v) = 1 + uv

(1 + v)

u

g (u, v) 1 uv (1 v )

u

where

g(u, v) = e

[2uv(1u2)]

1 uv (1 v)

u

[ 1 + v 1 v

]

[u3−u]

=

[

e

2v

( 1 v 1 + v )

]

(u−u3)

1 uv (1 v)

u

. Proof From Proposition 1-1 composing by the exponential function we then obtain

1 + uv

(1 uv ) e

[2uv(1u2)]

( 1 + v 1 v

)

u3

( 1 + v 1 v

)

u

which implies

( 1 + uv 1 uv

) ( 1 v 1 + v

)

u

e

[2uv(1u2)]

( 1 + v 1 v

)

[u3−u]

1.

Thus

f(u, v) = 1 + uv

(1 + v)

u

e

[2uv(1−u2)]

1 uv (1 v)

u

[ 1 + v 1 v

]

[u3−u]

1 uv (1 v)

u

. We then have for u, v (0, 1) the inequalities

(1 v)

u

f (u, v)(1 v)

u

g(u, v)(1 v)

u

1 uv.

2 Some new bounds for ratio functions

In this section we will apply result of Corollary 1-2 in order to determine

bounds for ratios of functions sine and cosine. We will show that these

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bounds are sharp. We think it is possible to apply it in other similar situa- tions.

The following result proposes an exponential upper bound for the ratio func- tion cosh(x)/ cos(x) better than the one proposed by [3, Proposition 2].

Proposition 2-1 For x, α (0, π/2) the following inequalities holds cosh(x)

cos(x) e

α2

[ cos(α) cosh(α)

]

(x2

α2xα66)

[ cosh(α) cos(α)

]

x2

α2

Proof We will use innite products for expressions of cosh(x) and cos(x) . For x IR one has

cos(x) =

k≥1

[1 ( 2x

π(2k 1) )

2

], cosh(x) =

k≥1

[1 + ( 2x

π(2k 1) )

2

].

Then the ratio can be expressed cosh(x)

cos(x) =

k≥1

[1 + (

π(2k2x1)

)

2

] [1 (

π(2k2x1)

)

2

] . which may also be written for α (0, π/2)

cosh(x) cos(x) =

k≥1

[1 + (

π(2k1)

)

2

]

αx22

[1 (

π(2k1)

)

2

]

αx22

.

Moreover, it follows from Corollary 1-2 for u, v (0, 1) 1 + uv

1 uv = f (u, v) (1 + v)

u

1 uv g(u, v) (1 + v)

u

1 uv =

[

e

2v

( 1 v 1 + v )

]

(u−u3)

( 1 + v 1 v

)

u

.

Thus, for u =

xα22

and v = (

π(2k1)

)

2

one obtains cosh(x)

cos(x) =

k≥1

[

1 + (

π(2k1)

)

2

]

αx22

[

1 (

π(2k1)

)

2

]

αx22

k≥1

[

e

2v

( 1 v 1 + v )

]

(u−u3)

cosh(x) cos(x)

k≥1

e

2(2k−1 )2

 1 (

π(2k1)

)

2

1 + (

π(2k1)

)

2

(x2

α2(x2

α2)3)

(7)

Therefore since

k≥1 1

(2k−1)2

=

π82

one gets cosh(x)

cos(x) e

2

k1(π(2k−1) )2

k≥1

 1 (

π(2k1)

)

2

1 + (

π(2k1)

)

2

(x2

α2(x2

α2)3)

cosh(x) cos(x) e

α2

[ cos(α) cosh(α)

]

(x2

α2αx66)

[ cosh(α) cos(α)

]

x2

α2

.

This proves the inequality.

Moreover, the right inequality is derived from Corollaries 1-3.

Turn now to the bounds for ratio of sine and hyperbolic sine functions.

The following result proposes an exponential upper bound for the ratio func- tion sinh(x)/ sin(x) better than the one proposed by [3, Proposition 4].

Proposition 2-2 For x, α (0, π/2) the following inequalities hold sinh(x)

sin(x)

[

e

α

2

3

sin(α) sinh(α)

]

(x2

α2(x2

α2)3)

[ sinh(α) sin(α)

]

(x2

α2)

.

Proof We will use innite products for expressions of sinh(x)/x and sin(x)/x . For x IR one has

sin(x)

x =

k≥1

(1 x

2

π

2

k

2

), sinh(x)

x =

k≥1

(1 + x

2

π

2

k

2

).

Then the ratio can be expressed in the simple following form sinh(x)

sin(x) =

k≥1

[1 + (

πkx

)

2

] [1 (

πkx

)

2

] . which may also be written for α (0, π/2)

sinh(x)

= [1 + (

πkα

)

2

(

αx

)

2

]

.

(8)

Then it follows from Corollary 1-2 for u, v (0, 1) 1 + uv

1 uv = f (u, v) (1 + v)

u

1 uv g(u, v) (1 + v)

u

1 uv =

[

e

2v

( 1 v 1 + v )

]

(u−u3)

( 1 + v 1 v

)

u

.

Thus, for u =

xα22

and v = (

πkα

)

2

we have sinh(x)

sin(x) =

k≥1

[1 + (

πkα

)

2

(

xα

)

2

] [1 (

πkα

)

2

(

xα

)

2

]

k≥1

[

e

2v

( 1 v 1 + v )

]

(u−u3)

sinh(x) sin(x)

k≥1

[

e

2(πkα)2

( 1 (

πkα

)

2

1 + (

πkα

)

2

)]

(x2

α2(x2

α2)3)

Since

k≥1 1

k2

=

π42

then we have sinh(x)

sin(x)

[

e

α

2

3

sin(α) sinh(α)

]

(x2

α2(x2

α2)3)

. This proves the inequality.

Moreover, the right inequality is derived from Corollaries 1-3.

Using these corollaries it is possible to prove other similar results as it will be done by the following.

Proposition 2-3 For x (0, π/2) the following inequalities hold cosh(x)

cos(x)

[

e

(8x

2 π2 )

( π

2

4x

2

π

2

+ 4x

2

)]

π2

8 (1120π4)

( π

2

+ 4x

2

π

2

4x

2

)

π2

8

Proof We will use again innite products for expressions of cosh(x) and cos(x) . For x IR one has the ratio

cosh(x) cos(x) =

k≥1

[1 + (

π(2k2x1)

)

2

] [1 (

π(2k2x1)

)

2

] .

Thus, for u =

(2k11)2

and v = (

2xπ

)

2

we have by Corollary 1-2 1 + uv

1 uv [ e

2v

( 1 v 1 + v )

]

(u−u3)

( 1 + v 1 v

)

u

.

(9)

cosh(x) cos(x) =

k≥1

1 + uv 1 uv

[

e

2(2xπ)2

( 1 (

2xπ

)

2

1 + (

2xπ

)

2

)]

( 1

(2k1)2( 1

(2k1)2)3)

k≥1

( 1 + (

2xπ

)

2

1 (

2xπ

)

2

)

1

(2k1)2

.

cosh(x) cos(x)

[

e

2(2xπ)2

( π

2

4x

2

π

2

+ 4x

2

)]∑

k1( 1

(2k1)2( 1

(2k1)2)3)

( π + 4x

2

π 4x

2

)∑

k1 1 (2k1)2

.

We then deduce the left inequality since

k≥1

 1 (2k 1)

2

( 1 (2k 1)

2

)

3

 = π

2

8 π

6

960 = π

2

8 (1 π

4

120 ).

We may prove by the same way the analog for the ratio

sinh(x)sin(x)

Proposition 2-4 For x (0, π/2) the following inequalities hold sinh(x)

sin(x)

[

e

(2x

2

π2)

π

2

x

2

π

2

+ x

2

]

(π2

6 945π6)

( π

2

+ x

2

π

2

x

2

)

π2

6

Proof We use again innite products for expressions of sinh(x) and sin(x) . For x IR one has the ratio

sinh(x) sin(x) =

k≥1

[1 + (

πkx

)

2

] [1 (

πkx

)

2

] .

Thus, for u =

k12

and v = (

xπ

)

2

we have by Corollary 1-2 1 + uv

1 uv [ e

2v

( 1 v 1 + v )

]

(u−u3)

( 1 + v 1 v

)

u

.

sinh(x)

= 1 + uv

[

e

2(xπ)2

( 1 (

πx

)

2

)]

(k12(k12)3)

( 1 + (

πx

)

2

)

k12

.

(10)

sinh(x) sin(x)

[

e

2(2xπ)2

( π

2

x

2

π

2

+ x

2

)]∑

k1

(

k12(1

k2)3

)

( π + x

2

π x

2

)∑

k1 1 (2k1)2

We then deduce the left inequality since

k≥1

( 1

k

2

( 1 k

2

)

3

)

= π

2

6 π

6

945 .

REFERENCES

[1] D. S. Mitrinovic, J. E. Pecaric, On Bernoulli's inequality, Facta. Univ.

Nis. Ser. Math. Infor., 5, 55-56, 1990.

[2] D. S. Mitrinovic, J. E. Pecaric, A. M. Fink, Bernoulli's Inequality.

In: Classical and New Inequalities in Analysis, Mathematics and Its Appli- cations(East European Series), 61, Springer, Dordrecht, pp. 65-81,1993.

[3] Christophe Chesneau, Yogesh J. Bagul. Some new bounds for ratio functions of trigonometric and hyperbolic functions. 2019. hal-01940170v2.

[4] L. Zhu and J. Sun, Six new Redheer-type inequalities for circular

and hyperbolic functions, Comput. Math. Appl., 56, 522-529, 2008.

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