Page 1
Pelton-Wheel
There are three basic hydraulic machines: Pelton, Francis and Kaplan.
The fluid density is constant but the complication is that cavitation may
occur in the machine. Cavitation is effectively the boiling of the liquid as
it is exposed to extrem ely low pressures in certain parts of the turbine.
The Pelton wheel or Pelton turbine is a tangential flow impulse turbine.
The water strikes the bucket along the tangent of the runner. The energy
available at the inlet of the turbine is only kinetic energy. The pressure
at the inlet and outlet of the turbine is atmospheric. The turbine is used
for high heads and is named after L.A Pelton, an American Engineer.
The Pelton wheel is composed of a nozzle which converts the whole
available head to kinetic energy and a rotor made up of a series of
double hemispherical buckets fastened on the periphery of the rotor. The
rotor is not enclosed, and the water leaving the buckets goes
immediately to the tailrace.
The Pelton wheel falls in a large class of these machines known as the
axial-flow type where the nozzle angle relative to the runner is zero.
However, the bucket cannot have a 180° camber angle, since the water
must have a finite radial velocity component away from the wheel in
order to avoid interference.
The main parts of the pelton turbine are: -
• Nozzle and flow regulating arrangement.
• Runner and buckets.
• Casing.
• Breaking Jet.
Page 2
Pelton-Wheel
There are three basic hydraulic machines: Pelton, Francis and Kaplan.
The fluid density is constant but the complication is that cavitation may
occur in the machine. Cavitation is effectively the boiling of the liquid as
it is exposed to extrem ely low pressures in certain parts of the turbine.
The Pelton wheel or Pelton turbine is a tangential flow impulse turbine.
The water strikes the bucket along the tangent of the runner. The energy
available at the inlet of the turbine is only kinetic energy. The pressure
at the inlet and outlet of the turbine is atmospheric. The turbine is used
for high heads and is named after L.A Pelton, an American Engineer.
The Pelton wheel is composed of a nozzle which converts the whole
available head to kinetic energy and a rotor made up of a series of
double hemispherical buckets fastened on the periphery of the rotor. The
rotor is not enclosed, and the water leaving the buckets goes
immediately to the tailrace.
The Pelton wheel falls in a large class of these machines known as the
axial-flow type where the nozzle angle relative to the runner is zero.
However, the bucket cannot have a 180° camber angle, since the water
must have a finite radial velocity component away from the wheel in
order to avoid interference.
The main parts of the pelton turbine are: -
• Nozzle and flow regulating arrangement.
• Runner and buckets.
• Casing.
• Breaking Jet.
1. Nozzle and flow regulating arrangement: The amount of water
striking the buckets of the runner is controlled by providing a spear
in the nozzle. The spear is a conical needle which is operated either
by a hand wheel or automatically in an axial direction depending
upon the size of the unit. When the spear is pushed forward into the
nozzle the amount of water striking the runner is reduced. On the
other hand if the spear is pushed back, the amount of water striking
the runner increases.
2. Runner with buckets: It consists of a circular disc on the periphery of
which a number of buckets evenly spaced are fixed. The shape of
the buckets is of a double hemispherical cup or bowl. Each bucket is
divided into two hemispherical parts by a dividing wall which is
known as splitter.
3. Casing: The function of the casing is to prevent the splashing of the
water and to discharge water to tail race. It also acts as a safeguard
against accidents. It is made of cast iron or fabricated steel plates.
As pelton wheel is an impulse turbine, the casing of the pelton wheel
does not perform any hydraulic function.
4. Breaking Jet: When the nozzle is completely closed by moving the
spear in the forward direction the amount of water striking the
runner reduces to zero. But the runner due to inertia goes on
revolving for a long time. To stop the runner in a short tim e, a small
nozzle is provided which directs the Jet of water on the back of the
buckets. This Jet of water is called breaking Jet.
Working of Pelton wheel Turbine:
The water from the reservoir flows through the penstocks at the outlet of
which a nozzle is fitted. The nozzle increases the kinetic energy of the
water flowing through the penstock by converting pressure energy into
kinetic energy. At the outlet of the nozzle, the water comes out in the
form of a Jet and strikes on the splitter, which splits up the jet into two
parts. These parts of the Jet, glides over the inner surfaces and comes
out at the outer edge. The buckets are shaped in such a way that
buckets rotates, runner of the turbine rotates and thus hydraulic energy
of water gets converted into mechanical energy on the runner of turbine
which is further converted into electrical energy in a
generator/alternator.
The Pelton wheel shown in the following figure is a pure impulse (R = 0)
turbine. It is used in very high head installations and develops efficiencies very
close to the Francis and Kaplan reaction turbines.
Page 3
Pelton-Wheel
There are three basic hydraulic machines: Pelton, Francis and Kaplan.
The fluid density is constant but the complication is that cavitation may
occur in the machine. Cavitation is effectively the boiling of the liquid as
it is exposed to extrem ely low pressures in certain parts of the turbine.
The Pelton wheel or Pelton turbine is a tangential flow impulse turbine.
The water strikes the bucket along the tangent of the runner. The energy
available at the inlet of the turbine is only kinetic energy. The pressure
at the inlet and outlet of the turbine is atmospheric. The turbine is used
for high heads and is named after L.A Pelton, an American Engineer.
The Pelton wheel is composed of a nozzle which converts the whole
available head to kinetic energy and a rotor made up of a series of
double hemispherical buckets fastened on the periphery of the rotor. The
rotor is not enclosed, and the water leaving the buckets goes
immediately to the tailrace.
The Pelton wheel falls in a large class of these machines known as the
axial-flow type where the nozzle angle relative to the runner is zero.
However, the bucket cannot have a 180° camber angle, since the water
must have a finite radial velocity component away from the wheel in
order to avoid interference.
The main parts of the pelton turbine are: -
• Nozzle and flow regulating arrangement.
• Runner and buckets.
• Casing.
• Breaking Jet.
1. Nozzle and flow regulating arrangement: The amount of water
striking the buckets of the runner is controlled by providing a spear
in the nozzle. The spear is a conical needle which is operated either
by a hand wheel or automatically in an axial direction depending
upon the size of the unit. When the spear is pushed forward into the
nozzle the amount of water striking the runner is reduced. On the
other hand if the spear is pushed back, the amount of water striking
the runner increases.
2. Runner with buckets: It consists of a circular disc on the periphery of
which a number of buckets evenly spaced are fixed. The shape of
the buckets is of a double hemispherical cup or bowl. Each bucket is
divided into two hemispherical parts by a dividing wall which is
known as splitter.
3. Casing: The function of the casing is to prevent the splashing of the
water and to discharge water to tail race. It also acts as a safeguard
against accidents. It is made of cast iron or fabricated steel plates.
As pelton wheel is an impulse turbine, the casing of the pelton wheel
does not perform any hydraulic function.
4. Breaking Jet: When the nozzle is completely closed by moving the
spear in the forward direction the amount of water striking the
runner reduces to zero. But the runner due to inertia goes on
revolving for a long time. To stop the runner in a short tim e, a small
nozzle is provided which directs the Jet of water on the back of the
buckets. This Jet of water is called breaking Jet.
Working of Pelton wheel Turbine:
The water from the reservoir flows through the penstocks at the outlet of
which a nozzle is fitted. The nozzle increases the kinetic energy of the
water flowing through the penstock by converting pressure energy into
kinetic energy. At the outlet of the nozzle, the water comes out in the
form of a Jet and strikes on the splitter, which splits up the jet into two
parts. These parts of the Jet, glides over the inner surfaces and comes
out at the outer edge. The buckets are shaped in such a way that
buckets rotates, runner of the turbine rotates and thus hydraulic energy
of water gets converted into mechanical energy on the runner of turbine
which is further converted into electrical energy in a
generator/alternator.
The Pelton wheel shown in the following figure is a pure impulse (R = 0)
turbine. It is used in very high head installations and develops efficiencies very
close to the Francis and Kaplan reaction turbines.
The utilization factor described in Equation 3 can be further simplified as
follows: For these machines there is no change of rotor radius, so U- 1 =
U2. Further, since the energy transfer is entirely at atmospheric pressure,
the absolute flow velocity remains unchanged; i.e., an impulse machine of
the axial-flow type has
. Thus the energy transfer is wholly derived from a change in the
velocity's direction. This resulting change in momentum (im pulse) causes
a force on the turbine buckets. The denominator of Equation 3
representing energy available then becomes sim p ly ^ 2.
The ideal utilization factor, e, is the ratio of Eutil to Eavail, i.e.,
- f u , v - u ^ g
g. * ‘ '
^ + ( u f - u
( u ^ - u A g
The Vu terms in the numerator of above equation can be simplified by
referring to the above vector diagram.
VU [ = Vj = U + VI ;
= U — V, cos a.
where a2 is described in the above given figure.
Thus the utilization factor for a Pelton wheel turbine becomes
2U ((u + V ,) - (u - v f; C O S Q , ) ) 2UV, (l+ c o sa 2)
v r
V.-
2U | V — U i(l-i- c o s a ,)
= ------^ 4 -------------—= 2 il-c c o s a
Vf
ij
u u
:
,vf.
The theoretical maximum value of utilization factor should occur when
Page 4
Pelton-Wheel
There are three basic hydraulic machines: Pelton, Francis and Kaplan.
The fluid density is constant but the complication is that cavitation may
occur in the machine. Cavitation is effectively the boiling of the liquid as
it is exposed to extrem ely low pressures in certain parts of the turbine.
The Pelton wheel or Pelton turbine is a tangential flow impulse turbine.
The water strikes the bucket along the tangent of the runner. The energy
available at the inlet of the turbine is only kinetic energy. The pressure
at the inlet and outlet of the turbine is atmospheric. The turbine is used
for high heads and is named after L.A Pelton, an American Engineer.
The Pelton wheel is composed of a nozzle which converts the whole
available head to kinetic energy and a rotor made up of a series of
double hemispherical buckets fastened on the periphery of the rotor. The
rotor is not enclosed, and the water leaving the buckets goes
immediately to the tailrace.
The Pelton wheel falls in a large class of these machines known as the
axial-flow type where the nozzle angle relative to the runner is zero.
However, the bucket cannot have a 180° camber angle, since the water
must have a finite radial velocity component away from the wheel in
order to avoid interference.
The main parts of the pelton turbine are: -
• Nozzle and flow regulating arrangement.
• Runner and buckets.
• Casing.
• Breaking Jet.
1. Nozzle and flow regulating arrangement: The amount of water
striking the buckets of the runner is controlled by providing a spear
in the nozzle. The spear is a conical needle which is operated either
by a hand wheel or automatically in an axial direction depending
upon the size of the unit. When the spear is pushed forward into the
nozzle the amount of water striking the runner is reduced. On the
other hand if the spear is pushed back, the amount of water striking
the runner increases.
2. Runner with buckets: It consists of a circular disc on the periphery of
which a number of buckets evenly spaced are fixed. The shape of
the buckets is of a double hemispherical cup or bowl. Each bucket is
divided into two hemispherical parts by a dividing wall which is
known as splitter.
3. Casing: The function of the casing is to prevent the splashing of the
water and to discharge water to tail race. It also acts as a safeguard
against accidents. It is made of cast iron or fabricated steel plates.
As pelton wheel is an impulse turbine, the casing of the pelton wheel
does not perform any hydraulic function.
4. Breaking Jet: When the nozzle is completely closed by moving the
spear in the forward direction the amount of water striking the
runner reduces to zero. But the runner due to inertia goes on
revolving for a long time. To stop the runner in a short tim e, a small
nozzle is provided which directs the Jet of water on the back of the
buckets. This Jet of water is called breaking Jet.
Working of Pelton wheel Turbine:
The water from the reservoir flows through the penstocks at the outlet of
which a nozzle is fitted. The nozzle increases the kinetic energy of the
water flowing through the penstock by converting pressure energy into
kinetic energy. At the outlet of the nozzle, the water comes out in the
form of a Jet and strikes on the splitter, which splits up the jet into two
parts. These parts of the Jet, glides over the inner surfaces and comes
out at the outer edge. The buckets are shaped in such a way that
buckets rotates, runner of the turbine rotates and thus hydraulic energy
of water gets converted into mechanical energy on the runner of turbine
which is further converted into electrical energy in a
generator/alternator.
The Pelton wheel shown in the following figure is a pure impulse (R = 0)
turbine. It is used in very high head installations and develops efficiencies very
close to the Francis and Kaplan reaction turbines.
The utilization factor described in Equation 3 can be further simplified as
follows: For these machines there is no change of rotor radius, so U- 1 =
U2. Further, since the energy transfer is entirely at atmospheric pressure,
the absolute flow velocity remains unchanged; i.e., an impulse machine of
the axial-flow type has
. Thus the energy transfer is wholly derived from a change in the
velocity's direction. This resulting change in momentum (im pulse) causes
a force on the turbine buckets. The denominator of Equation 3
representing energy available then becomes sim p ly ^ 2.
The ideal utilization factor, e, is the ratio of Eutil to Eavail, i.e.,
- f u , v - u ^ g
g. * ‘ '
^ + ( u f - u
( u ^ - u A g
The Vu terms in the numerator of above equation can be simplified by
referring to the above vector diagram.
VU [ = Vj = U + VI ;
= U — V, cos a.
where a2 is described in the above given figure.
Thus the utilization factor for a Pelton wheel turbine becomes
2U ((u + V ,) - (u - v f; C O S Q , ) ) 2UV, (l+ c o sa 2)
v r
V.-
2U | V — U i(l-i- c o s a ,)
= ------^ 4 -------------—= 2 il-c c o s a
Vf
ij
u u
:
,vf.
The theoretical maximum value of utilization factor should occur when
A-
_U
Vj
d?
U
= 0 = 2|1 — cos a . 1 - 2 —
v , .
u
= 0 = 2 11 — c o s q , l 1 - 2 —
v ,
v,
IJ
U 1
or — = —
Vt 2
U 1
or — = —
Vi 2
i.e ., when the linear velocity of the bucket is half that of the absolute
velocity of the impinging jet.
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