Site pages

Current course

Participants

General

Module 1. Introduction to Theory of Machine

Module 2. Planar Mechanism

Module 3. Velocity and Acceleration Analysis

15 March - 21 March

22 March - 28 March

29 March - 4 April

5 April - 11 April

12 April - 18 April

19 April - 25 April

26 April - 2 May

## Lesson 24.

**24.1** Consider a pulley 1 driving the pulley 2. The pulley 1 is called driver and pulley 2 is called driven. So velocity ratio may be defined as the ratio of speed of driven to that of driver or ratio of diameter of driver to that of driven.

Mathematically** **the equation is:

\[\frac{{{{\text{N}}_{\text{2}}}{\text{ }}}}{{{{\text{N}}_{\text{1}}}}} = \frac{{{{\text{D}}_{\text{1}}}}}{{{\text{ }}{{\text{D}}_{\text{2}}}}}\]

N_{1 }= Speed of driver pulley in rpm

_{} N_{2 }= Speed of driven pulley in rpm

_{}D_{1 }= Diameter of driver pulley in mm

_{} D_{2 }= Diameter of driven pulley in mm

When the thickness of the belt (t) is considered, then velocity ratio is given by

\[\frac{{{{\text{N}}_{\text{2}}}}}{{{{\text{N}}_{\text{1}}}}} = {\text{ }}\frac{{\left( {{{\text{D}}_{\text{1}}} + {\text{ t}}} \right){\text{ }}}}{{\left( {{{\text{D}}_{\text{2}}} + {\text{t}}} \right)}}\]

**24.2 SLIP OF BELT DRIVES**

The forward motion of the driver without carrying the belt with it is called slip of the belt and is generally expressed in percentage. For slippage velocity ratio is given by

\[\frac{{{{\text{N}}_{\text{2}}}}}{{{{\text{N}}_{\text{1}}}}}={\text{}}\frac{{\left({{{\text{D}}_{\text{1}}}+{\text{t}}}\right){\text{}}}}{{\left({{{\text{D}}_{\text{2}}} + {\text{t}}} \right)}}\times {\text{ }}\left( {{\text{1}} - \frac{{\text{S}}}{{100}}} \right)\]

Where S= S_{1}+S_{2 }(total percentage of slip)

S_{1 }= Percentage slip between driver and the belt and

S_{2}= Percentage slip between belt and the follower

**24.3 Length of open belt drive**

Consider an open belt drive; both the pulleys rotate in the same direction as shown in the figure 5.7

Let r_{1 }and r_{2} be radii of larger and smaller pulley

X= distance between the centres of two pulleys i.e. (C_{1}, C_{2})

L= Total length of the belt

Fig. 5.7 Length of open belt drive

Let the belt leaves the larger pulley at A and C and smaller pulley at B and D. Through C_{2} draw C_{2}G parallel to AB.

From the figure, C_{2}G will be perpendicular to C_{1}A.

Let the angle GC_{2}C_{1}=α radians

We know that length of belt is given by

L= Arc CEA+AB+Arc BFD+DC

=2(Arc AE+AB+Arc BF)

From the figure,

AB= GC_{2}= [(C_{1}C_{2})^{2} – (C_{1}G)^{ 2}]^{1/2}= [x^{2}-(r_{1}-r_{2})^{2}]^{1/2}

Expanding by binomial theorem

Substituting the values of arc AE from equation, arc BF and AB from equations we get

**24.4 Ratio between belt tensions**

A driven pulley rotating in clockwise direction is shown in figure 5.8

Let T_{1} = Tension on tight side of the belt

T_{2} = Tension on slack side of the belt

θ = Angle of contact of belt with pulley in radians

µ = Coefficient of friction between the belt and pulley.

Considering a small portion of belt XY in contact with the pulley. X makes angle δθ at the centre of the pulley. Let T be the tension in the belt at X and (T + δT) be the tensions in the belt at Y.

Fig 5.8 Ratio of driving tensions

The belt portion XY is in equilibrium under the action of following forces:

1. Tension T in belt at X.

2. Tension T + δT in belt at Y.

3. Frictional reaction R at U.

4. Frictional force µR between belt and pulley.

Now again solving the forces expression in horizontal direction

µR = (T + δT) cos (δθ / 2) - T cos (δθ / 2)

Since δθ is very small

cos (δθ / 2) = 1

µR + T = (T + δT)

µR = δT …(1)

and resolving the force is vertical reaction.

R = T sin (δθ / 2) + (T + δT) sin (δθ/2)

Since, δθ is very small, so

R = T δθ/2 + (T + δT) δθ/2 = T δθ …(2)

From equations (1) and (2)

µ(T δθ) = δT (neglecting δT. δθ / 2 )

δT / T = µ δθ

On integration, we get

^{T2}∫_{T1} δT/T = ∫_{o}^{θ} µdθ

loge T_{1} / T_{2} = µθ

T_{1} / T_{2} = (e)^{µθ}

**24.5 Power transmitted by belt drive**

Power transmitted, P = (T_{1} - T_{2}) V (Watt)

V is the velocity of the belt = \[ = \frac{{{\text{ }}{{\text{D}}_{\text{1}}}{{\text{N}}_{\text{1}}}}}{{60}}\] (m/sec)

**24.6 Tension in the belts**

The initial tension (T_{0}) ensures that the belt would not slip under designed load. Belts are mounted on the pulleys with a certain amount of tension T_{0}. At rest, the forces acting on the two sides of belts are equal. As the power is transmitted, the tension on the tight side increases and tension on the slack side decreases.

Fig 5.8 (b) Pulleys Working

Mathematically Initial tension is given by

Where T_{1} and T_{2} are tensions on tight side and slack side and T_{c }is the centrifugal tension given by

Tc=mv^{2}

Where m= mass of belt per unit length and V=Velocity of belt in m/s

**24.7 Condition for the transmission of Maximum power**

Power transmitted by belt drive is given by

P= (T_{1}-T_{2}) V…………………………….(1)

Where T_{1}= Tension in the belt on tight side

T_{2}= tension in the belt on slack side

V= velocity of belts

Also \[\frac{{{{\text{T}}_{\text{1}}}}}{{{{\text{T}}_{\text{2}}}}} = {{\text{e}}^\mu }^\theta \]

Substituting the value of T_{2}, we get

\[= ({{\text{T}}_{\text{1}}}--{\text{ }}\frac{{{{\text{T}}_{\text{1}}}{\text{ }}}}{{{{\text{e}}^{\mu \theta }}}}){\text{V}} = {\text{ }}{{\text{T}}_{\text{1}}}({\text{1}} - \frac{{\text{1}}}{{{{\text{e}}^{\mu \theta }}}}){\text{V}} = {{\text{T}}_{\text{1}}}.{\text{V}}.{\text{Z}}\] ……………… (2)

Where

\[{\text{Z}} = {\text{1}} - \frac{{{\text{1 }}}}{{{{\text{e}}^{\mu \theta }}}}\]

Also maximum tension (T) in the belt considering centrifugal tension (Tc) is given by

T=T_{1}+T_{c}

Substituting the value T_{1} in equation (2)

P= (T-T_{c}) V.Z= (T.V-mV^{3}) Z

Differentiating with respect to V for maximum power and equate to zero