Technical Field
[0001] The present invention relates to an elevator rope used for suspending a car in an
elevator, and an elevator apparatus.
Background Art
[0002] In general, an elevator apparatus has the following structure. That is, a rope is
looped around a sheave that is fixed to a motor of a hoisting machine, and a car is
suspended at one end of the rope while a weight for keeping balance with the car is
suspended at the other end of the rope. Conventionally, in an elevator apparatus having
the structure as described above, in order to prevent early abrasion and breakage
of the rope, there has been used a sheave having a diameter that is at least 40 times
as large as the diameter of the rope (hereinafter, referred to as "rope diameter").
The diameter of the sheave (hereinafter, referred to as "sheave diameter") has a direct
relationship with drive torque of the motor that is necessary to raise and lower the
car. Therefore, various components of the elevator apparatus as typified by the motor
can be reduced in size and weight by reducing the sheave diameter. In particular,
in order to reduce the sheave diameter, the rope diameter also needs to be reduced
for the reason described above.
[0003] However, when the rope diameter is reduced without changing the number of ropes,
the strength of the rope decreases, and as a result, the maximum rated load of the
elevator decreases. On the other hand, when the number of ropes is increased, the
structure of the elevator apparatus becomes complicated. Further, when the sheave
diameter is reduced, the bending fatigue life of the rope is shortened, which raises
a need to replace the rope frequently.
[0004] As a measure to solve the problems, there is proposed an elevator rope, which is
obtained by twisting together a plurality of strands formed by twisting a plurality
of steel wires together, and covering it with a resin material on its outermost periphery
(see, for example, Patent Document 1). An elevator apparatus using such an elevator
rope is driven by a frictional force between the sheave and the resin material that
covers the outermost periphery of the rope. Therefore, there is a demand for improvement
and stabilization of the friction characteristics of the resin material.
In order to improve the friction characteristics of the sheave and the rope, there
is proposed an elevator rope covered with a polyurethane covering material containing
no wax (see, for example, Patent Document 2).
[0005] In general, a friction coefficient of a resin material is known to heavily depend
on sliding velocity and temperature. It is also known that viscoelastic characteristics
such as dynamic viscoelasticity of the resin material correlate with the sliding velocity
and temperature (Williams-Landel-Ferry equation (WLF equation)). In particular, it
is described that, even in the case of rubber, the viscoelastic characteristics correlate
similarly with the sliding velocity and temperature, and hence viscoelastic characteristics
of rubber are related to friction characteristics of rubber (see, for example, Non
Patent Document 1).
Citation List
Patent Documents
Non Patent Document
Disclosure of the Invention
Problems to be Solved by the Invention
[0008] As described above, in a resin material containing rubber, the friction coefficient
changes depending on changes in sliding velocity and temperature, and the friction
coefficient varies depending on an increase in sliding velocity or an increase in
temperature. Therefore, even in the polyurethane covering material containing no wax
described in Patent Document 2, the friction coefficient changes depending on changes
in sliding velocity and temperature, and hence there is a problem in that it is impossible
to brake a car stably. Further, in order to stop the car for a long period of time,
it is necessary to maintain the static condition of the car by the frictional force
between the rope and the sheave. However, even when a rope is covered with the polyurethane
covering material containing no wax as described in Patent Document 2, there is a
problem in that a friction coefficient at a small sliding velocity cannot be maintained
stably because the polyurethane covering material has a large variation in friction
coefficient, with the result that the stop position of the car shifts with time.
[0009] Therefore, the present invention has been made to solve the above problems, and an
object of the present invention is to provide an elevator rope and an elevator apparatus
which can brake a car stably in a wide range of sliding velocities from a range of
small sliding velocities required for maintaining a static condition of the car to
sliding velocities during normal operation by covering a rope with a resin material
having a stable friction coefficient independent of temperature and sliding velocity.
Means for Solving the Problems
[0010] The inventors of the preset invention have made intensive studies on friction characteristics
of a variety of resin materials to solve the problems, and as a result, have obtained
the following findings.
FIG. 1 is an example of a graph showing relationships between frequencies and loss
moduli E" in resin materials different in sliding velocity dependency of a friction
coefficient (i.e., resin materials having different variations in friction coefficient
with respect to a sliding velocity). As clear from FIG. 1, a resin material having
small sliding velocity dependency of the friction coefficient has small frequency
dependency of the loss modulus E" (i.e., variation in loss modulus E" is small in
the case where frequency varies), while a resin material having large sliding velocity
dependency of the friction coefficient has large frequency dependency of the loss
modulus E" (i.e., variation in loss modulus E" is large in the case where frequency
varies). That is, the inventors have found that the sliding velocity dependency of
the friction coefficient correlates with the frequency dependency of the loss modulus
E", and the sliding velocity dependency of the friction coefficient can be decreased
by decreasing the frequency dependency of the loss modulus E".
[0011] Based on such findings, the inventors have made further studies on compositions of
resin materials, and as a result, have found that, both the frequency dependency of
the loss modulus and the sliding velocity dependency of the friction coefficient can
be decreased by a molded product obtained from a resin composition including two kinds
of resin components having a difference in glass transition temperature of 20°C or
more at a mass ratio within a predetermined range.
[0012] That is, the present invention is an elevator rope comprising a rope main body and
a covering resin layer that covers a periphery of the rope main body, in which the
covering resin layer is formed from a molded product of a resin composition comprising
a first resin component and a second resin component at a mass ratio of 90:10 to 70:30,
the first resin component and the second resin component having a difference in glass
transition temperature of 20°C or more.
Further, the present invention is an elevator apparatus comprising the elevator rope.
Effects of the Invention
[0013] According to the present invention, it is possible to provide an elevator rope and
an elevator apparatus which can brake a car stably in a wide range of sliding velocities
from the range of small sliding velocities required for maintaining a static condition
of the car to sliding velocities during normal operation by covering a rope with a
resin material having a stable friction coefficient independent of temperature and
sliding velocity.
Brief Description of the Drawings
[0014]
[FIG. 1] FIG. 1 is a graph showing relationships between frequencies and loss moduli
in resin materials different in sliding velocity dependency of a friction coefficient.
[FIG. 2] FIG. 2 is a cross-sectional view of an elevator rope of the present invention.
[FIG. 3] FIG. 3 is viscoelastic spectra of a general resin material.
[FIG. 4] FIG. 4 is a configuration diagram of a system for evaluating a friction coefficient.
Modes for Carrying Out the Invention
Embodiment 1.
[0015] An elevator rope of the present invention comprises a rope main body and a covering
resin layer that covers a periphery of the rope main body.
Hereinafter, preferred embodiments of the elevator rope of the present invention are
described with reference to the drawings.
FIG. 2 is a cross-sectional view of the elevator rope. In FIG. 2, the elevator rope
comprises a rope main body 1 and a covering resin layer 2 that covers a periphery
of the rope main body 1.
[0016] The elevator rope is characterized by the covering resin layer 2 that covers the
periphery of the rope main body 1, and hence the rope main body 1 on which the covering
resin layer 2 is formed is not particularly limited and may be any known one. Examples
of the rope main body 1 include a strand formed by twisting a plurality of steel wires
together and a load-supporting member such as a cord. In addition, the load-supporting
member may have not only a rope shape but also a belt shape. It should be noted that
load-supporting members are described in detail in Patent Documents 1 and 2,
WO 2003/050348 A1,
WO 2004/002868 A1, and the like, which are incorporated herein by reference.
[0017] The covering resin layer 2 is formed from a molded product of a resin composition
comprising two kinds of resin components (a first resin component and a second resin
component) having a difference in glass transition temperature of 20°C or more.
Here, FIG. 3 shows an example of viscoelastic spectra (storage modulus E', loss modulus
E", and loss tangent tanδ) of a general resin material (thermoplastic polyurethane
elastomer). The viscoelastic spectra were determined under the following conditions:
measurement mode: bending mode; measurement frequency: 10 Hz; and temperature increase
rate: 5°C/min. As clear from FIG. 3, the spectrum of the loss modulus E" has a peak
at about -40°C, and the temperature corresponds to a glass transition temperature
of the thermoplastic polyurethane elastomer.
In the present invention, a resin composition comprising two kinds of resin components
having a difference in glass transition temperature of 20°C or more is used, and hence
in the spectrum of the loss modulus E" of the covering resin layer 2 formed from a
molded product of the resin composition, the peak of the loss modulus E" becomes broad
or is divided into two small peaks. As a result, the frequency dependency of the loss
modulus of the covering resin layer 2 formed from the molded product of the resin
composition is decreased.
[0018] The first resin component in the resin composition for forming the covering resin
layer 2 is not particularly limited as long as the first resin component and the second
resin component have a difference in glass transition temperature of 20°C or more,
but is preferably a thermoplastic polyurethane elastomer. In general, thermoplastic
polyurethane elastomer refers to one which includes a hard segment having a urethane
structure and a soft segment derived from a polyol raw material and which exhibits
rubber elasticity at room temperature. The thermoplastic polyurethane elastomer is
classified into polyether-based, polyester-based, polycarbonate-based, silicone-based,
and olefin-based thermoplastic polyurethane elastomers depending on the type of the
polyol raw material used.
[0019] Such thermoplastic polyurethane elastomers may be produced by generally known methods.
For example, the elastomers may be produced by copolymerization of an isocyanate,
a polyol, and a chain extender as raw materials. The polymerization reaction is generally
known, and the blending ratio of the raw materials and synthetic conditions may be
appropriately adjusted depending on the raw materials used, and are not particularly
limited.
Further, any commercially available thermoplastic polyurethane elastomer may be used.
[0020] When the thermoplastic polyurethane elastomer is obtained by synthesis, examples
of the isocyanate include tolylene diisocyanate, 4,4'-diphenylmethane diisocyanate,
1,5-naphthylene diisocyanate, tolidine diisocyanate, 1,6-hexamethylene diisocyanate,
isophorone diisocyanate, xylene diisocyanate, hydrogenated xylene diisocyanate, triisocyanate,
tetramethylxylene diisocyanate, 1,6,11-undecane triisocyanate, 1,8-diisocyanate methyloctane,
a lysine ester triisocyanate, 1,3,6-hexamethylene triisocyanate, and bicycloheptane
triisocyanate. These may be used alone or in combination of two or more kinds thereof.
[0021] Examples of the polyol include a polyester polyol, a polycarbonate polyol, a polyester
ether polyol, a polyether polyol, a silicone polyol, and a polyolefin polyol. These
may be used alone or in combination of two or more kinds thereof.
[0022] Examples of the polyester polyol include: a polyester polyol obtained through a condensation
reaction between a dicarboxylic acid or an esterified compound or acid anhydride thereof
and a diol; and a polylactonediol obtained through ring-opening polymerization of
a lactone monomer such as ε-caprolactone. Here, as the dicarboxylic acid, there may
be used: aliphatic dicarboxylic acids such as succinic acid, adipic acid, sebacic
acid, and azelaic acid; aromatic dicarboxylic acids such as phthalic acid, terephthalic
acid, isophthalic acid, and naphthalenedicarboxylic acid; and alicyclic dicarboxylic
acids such as hexahydroterephthalic acid, hexahydrophthalic acid, and hexahydroisophthalic
acid. As the diol, there may be used, for example, ethylene glycol, 1,3-propylene
glycol, 1,2-propylene glycol, 1,3-butanediol, 1,4-buanediol, 1,5-pentanediol, 1,6-hexanediol,
3-methyl-1,5-pentanediol, neopentyl glycol, 1,3-octanediol, and 1,9-nonanediol. These
may be used alone or in combination of two or more kinds thereof.
[0023] Examples of the polycarbonate polyol include a polycarbonate polyol obtained by allowing
diethylene carbonate, diethyl carbonate, or the like to react with one or more kinds
of polyhydric alcohols such as ethylene glycol, 1,3-propylene glycol, 1,2-propylene
glycol, 1,3-butanediol, 1,4-butanediol, 1,5-pentanediol, 1,6-hexanediol, 3-methyl-1,5-pentanediol,
neopentyl glycol, 1,8-octanediol, 1,9-nonanediol, and diethylene glycol. Specific
examples thereof include polyhexamethylene carbonate diol, polytrimethylene carbonate
diol, poly-3-methyl(pentamethylene) carbonate diol, and copolymers thereof. These
may be used alone or in combination of two or more kinds thereof.
[0024] Examples of the polyester ether polyol include condensation reaction products of
the aliphatic dicarboxylic acids, aromatic dicarboxylic acids, alicyclic dicarboxylic
acids, or esters or acid anhydrides thereof with glycols such as diethylene glycol
and a propylene oxide adduct. These may be used alone or in combination of two or
more kinds thereof.
[0025] Examples of the polyether polyol include polyethylene glycol, polypropylene glycol,
polytetramethylene glycol, and the like obtained by polymerizing cyclic ethers such
as ethylene oxide, propylene oxide, and tetrahydrofuran, respectively, and copolyethers
thereof. These may be used alone or in combination of two or more kinds thereof.
[0026] Examples of the silicone polyol include dimethylpolysiloxanediol, methylphenylpolysiloxanediol,
an amino-modified silicone oil, a both-end diamine-modified silicone oil, a polyether-modified
silicone oil, an alcohol-modified silicone oil, a carboxyl group-modified silicone
oil, and a phenyl-modified silicone oil each having two active hydrogens at both ends.
These may be used alone or in combination of two or more kinds thereof.
[0027] Examples of the polyolefin polyol include polyisoprene polyol, polybutadiene polyol,
or copolymers thereof with styrene and acrylonitrile and hydrogenated products thereof.
These may be used alone or in combination of two or more kinds thereof.
[0028] As the chain extender, a low molecular weight polyol may be used, and examples thereof
include: aliphatic polyols such as ethylene glycol, 1,3-propylene glycol, 1,2-propylene
glycol, 1,3-butanediol, 1,4-butanediol, 1,5-pentanediol, 1,6-hexanediol, 3-methyl-1,5-pentanediol,
neopentyl glycol, 1,8-octanediol, 1,9-nonanediol, diethylene glycol, 1,4-cyclohexanedimethanol,
and glycerin; and aromatic glycols such as 1,4-dimethylolbenzene, bisphenol A, and
an ethylene oxide adduct and propylene oxide adduct of bisphenol A. These may be used
alone or in combination of two or more kinds thereof.
[0029] Of the thermoplastic polyurethane elastomers of various kinds, the first resin component
is preferably a thermoplastic polyurethane elastomer other than a polyester-based
thermoplastic polyurethane elastomer from the viewpoint of prevention of hydrolysis
which occurs under a usage environment. In consideration of the variety of characteristics
(such as flexibility, durability, and cold resistance) required for an elevator rope,
the first resin component is more preferably a polyether-based thermoplastic polyurethane
elastomer having a JIS A hardness (hardness specified by JIS K7215 and determined
using a type A durometer) of 85 to 95.
[0030] The second resin component in the resin composition for forming the covering resin
layer 2 is a resin component which has a glass transition temperature higher or lower
by 20°C or more than that of the first resin component.
The second resin component having such characteristics is not particularly limited
as long as it satisfies the above-mentioned conditions. However, from the viewpoints
of durability and abrasion resistance, the second resin component is preferably a
thermoplastic polyurethane elastomer obtained using, as a raw material, a polyol different
from the thermoplastic polyurethane elastomer as the first resin component, or a polyamide
resin. Further, among the thermoplastic polyurethane elastomers of various kinds,
the second resin component is preferably a polycarbonate-based thermoplastic polyurethane
elastomer or a silicone-based thermoplastic polyurethane elastomer having a JIS A
hardness (hardness specified by JIS K7215 and determined using a type A durometer)
of 85 to 95 in consideration of a variety of characteristics (such as flexibility,
durability, and cold resistance) required for an elevator rope.
[0031] Examples of the polyamide resin include a polyamide-based thermoplastic elastomer
and a polyamide-based thermoplastic resin.
In general, polyamide-based thermoplastic elastomer refers to one which includes a
hard segment of a polyamide and a soft segment of a polyether or a polyester and which
exhibits rubber elasticity at room temperature. Of these, the elastomer is preferably
a polyamide-based thermoplastic elastomer which includes a hard segment of a polyamide
and a soft segment of a polyether from the viewpoint of hydrolysis resistance.
In general, polyamide-based thermoplastic resin refers to a thermoplastic resin having
a polyamide bond in its molecular chain, and examples thereof include nylon 6, nylon
66, nylon 11, and nylon 12. These may be used alone or in combination of two or more
kinds thereof.
[0032] The mass ratio of the first resin component to the second resin component is 90:10
to 70:30. When the mass ratio of the second resin component is too low, an effect
obtained by blending the second resin component (in particular, a stable friction
coefficient in the covering resin layer 2) cannot be obtained. On the other hand,
when the mass ratio of the second resin component is too high, the characteristics
of the second resin component become dominant. In consequence, the covering resin
layer 2 formed from a molded product of a resin composition becomes too hard, and
flexibility of the rope may be impaired or durability of the covering resin layer
2 may be lowered. As a result, when an elevator apparatus using such rope is driven,
problems such as increased power consumption and impaired durability when the rope
is bent repeatedly may be caused.
[0033] The resin composition for forming the covering resin layer 2 can be prepared by mixing
the above-mentioned components using known means. The covering resin layer 2 can be
formed by molding the resin composition so that the composition covers the periphery
of the rope main body 1 by known molding means such as extrusion molding or injection
molding. Further, in order to stabilize physical properties of the molded product
of the resin composition, a heat treatment may be carried out. Conditions for the
heat treatment may be appropriately adjusted depending on the resin composition used,
and are not particularly limited.
[0034] As the glass transition temperature of the covering resin layer 2 increases, the
sliding velocity dependency of the friction coefficient tends to decrease, while the
elastic modulus of the covering resin layer 2 tends to increase. Therefore, in the
case where a rope having formed thereon the covering resin layer 2 having a higher
glass transition temperature is employed for an elevator apparatus, the flexibility
of the rope is liable to be impaired or fatigue failure such as cracking of the covering
resin layer 2 is liable to occur owing to stress when the rope is bent repeatedly
in an environment having a temperature higher than the glass transition temperature
of the covering resin layer 2. Accordingly, the glass transition temperature of the
covering resin layer 2, specified by the peak temperature of the loss modulus E" in
the viscoelastic spectra, is desirably set to -20°C or less, more preferably -25°C
or less in the case where there is only one peak. Meanwhile, in the case where there
are two peak temperatures, the glass transition temperature of the first resin component
in the covering resin layer 2 is desirably set to -20°C or less, more preferably -25°C
or less.
[0035] In addition, when the JIS A hardness (hardness specified by JIS K7215 and determined
using a type A durometer) of the covering resin layer 2 is more than 98, the flexibility
of the rope is liable to be impaired, resulting in increased power consumption in
the case where an elevator apparatus using the rope is driven. On the other hand,
when the JIS A hardness of the covering resin layer 2 is less than 85, the durability
is liable to be impaired when the layer is bent repeatedly as an elevator rope. Therefore,
the JIS A hardness of the covering resin layer 2 is desirably set to 85 to 98.
[0036] From the viewpoint of improvement of adhesion between the rope main body 1 and the
covering resin layer 2 in the elevator rope, the covering resin layer 2 may be formed
after an adhesive is applied in advance to the rope main body 1. The adhesive is not
particularly limited as long as it is an adhesive for metal and polyurethane, and
examples thereof include Chemlok (registered trademark) 218 (manufactured by LORD
Far East, Inc.).
[0037] In an elevator rope having the above-mentioned characteristics, a rope is covered
with a resin material having a stable friction coefficient independent of a temperature
and a sliding velocity. Therefore, in the case where the rope is used for an elevator
apparatus, a car can be braked stably in a wide range of sliding velocities from a
range of small sliding velocities required for maintaining a static condition of the
car to sliding velocities during normal operation.
Examples
[0038] Hereinafter, the present invention is described in detail by way of examples, but
is not limited by the following examples.
(Example 1)
[0039] Pellets of a polyether-based thermoplastic polyurethane elastomer (JIS A hardness:
95, glass transition temperature: -30°C) obtained by reacting polytetramethylene glycol,
4,4'-diphenylmethane diisocyanate, and 1,4-butanediol were mixed with pellets of a
polycarbonate-based thermoplastic polyurethane elastomer (JIS A hardness: 95, glass
transition temperature: 5°C) obtained by reacting polyhexamethylene carbonate diol,
4,4'-diphenylmethane diisocyanate, and 1,4-butanediol at a mass ratio of 90:10 to
prepare a resin composition.
[0040] Next, the resin composition was supplied to an extrusion molding machine, and extrusion
molding was carried out so that the composition covered the periphery of a rope main
body, to thereby mold a covering resin layer on the periphery of the rope main body.
Here, a strand formed by twisting a plurality of steel wires together, as described
in
WO 2003/050348 A1, was used as the rope main body, and Chemlok (registered trademark) 218 (manufactured
by LORD Far East, Inc.) was applied in advance to the rope main body and dried before
the formation of the covering resin layer.
Subsequently, in order to stabilize the physical properties of the covering resin
layer, the rope was heated at 100°C for 2 hours, to thereby obtain an elevator rope
having a diameter of 12 mm. The viscoelastic spectra of the covering resin layer of
the elevator rope were measured. (The measurement was carried out under the following
conditions: measurement mode: bending mode; measurement frequency: 10 Hz; and temperature
increase rate: 5°C/min. In the Examples and Comparative Examples below, the measurement
was carried out under the same conditions.) As a result, the loss modulus E" in the
viscoelastic spectra was found to have one peak, and the peak temperature corresponding
to the glass transition temperature was found to be -30°C. Further, the JIS A hardness
of the covering resin layer of the elevator rope was measured, and as a result, the
JIS A hardness was found to be 95.
(Example 2)
[0041] An elevator rope was obtained in the same manner as in Example 1 except that the
mass ratio of the pellets of the polyether-based thermoplastic polyurethane elastomer
to the pellets of the polycarbonate-based thermoplastic polyurethane elastomer was
changed to 80:20. The viscoelastic spectra and JIS A hardness of the covering resin
layer of the elevator rope were measured. As a result, the loss modulus E" in the
viscoelastic spectra was found to have one peak, and the peak temperature corresponding
to the glass transition temperature was found to be -28°C. Further, the JIS A hardness
of the covering resin layer was found to be 95.
(Example 3)
[0042] An elevator rope was obtained as in the same manner as in Example 1 except that the
mass ratio of the pellets of the polyether-based thermoplastic polyurethane elastomer
to the pellets of the polycarbonate-based thermoplastic polyurethane elastomer was
changed to 70:30. The viscoelastic spectra and JIS A hardness of the covering resin
layer of the elevator rope were measured. As a result, the loss modulus E" in the
viscoelastic spectra was found to have one peak, and the peak temperature corresponding
to the glass transition temperature was found to be -25°C. Further, the JIS A hardness
of the covering resin layer was found to be 95.
(Example 4)
[0043] An elevator rope was obtained in the same manner as in Example 1 except for using
a resin composition obtained by mixing the pellets of the polyether-based thermoplastic
polyurethane elastomer used in Example 1 with pellets of a silicone-based thermoplastic
polyurethane elastomer (JIS A hardness: 95, glass transition temperature: -50°C) obtained
by reacting both-end carbinyl-modified siloxane, polytetramethylene glycol, 4,4'-diphenylmethane
diisocyanate, and 1,4-butanediol at a mass ratio of 80:20. The viscoelastic spectra
and JIS A hardness of the covering resin layer of the elevator rope were measured.
As a result, the loss modulus E" in viscoelastic spectra was found to have one peak,
and the peak temperature corresponding to the glass transition temperature was found
to be -32°C. Further, the JIS A hardness of the covering resin layer was found to
be 95.
(Example 5)
[0044] An elevator rope was obtained in the same manner as in Example 1 except for using
a resin composition obtained by mixing the pellets of the polyether-based thermoplastic
polyurethane elastomer used in Example 1 with pellets of nylon 6 (glass transition
temperature: 50°C) at a mass ratio of 80:20. The viscoelastic spectra and JIS A hardness
of the covering resin layer of the elevator rope were measured. As a result, the loss
modulus E" in the viscoelastic spectra was found to have two peaks, and the peak temperature
corresponding to the glass transition temperature of the polyether-based thermoplastic
polyurethane elastomer as the first resin component was found to be -28°C. Further,
the JIS A hardness of the covering resin layer was found to be 97.
(Example 6)
[0045] An elevator rope was obtained in the same manner as in Example 1 except for using
a resin composition obtained by mixing the pellets of the polyether-based thermoplastic
polyurethane elastomer used in Example 1 with pellets of nylon 66 (glass transition
temperature: 55°C) at a mass ratio of 80:20. The viscoelastic spectra and JIS A hardness
of the covering resin layer of the elevator rope were measured. As a result, the loss
modulus E" in the viscoelastic spectra was found to have two peaks, and the peak temperature
corresponding to the glass transition temperature of the polyether-based thermoplastic
polyurethane elastomer as the first resin component was found to be -30°C. Further,
the JIS A hardness of the covering resin layer was found to be 98.
(Example 7)
[0046] An elevator rope was obtained in the same manner as in Example 1 except for using
a resin composition obtained by mixing the pellets of the polyether-based thermoplastic
polyurethane elastomer used in Example 1 with pellets of nylon 12 (glass transition
temperature: 40°C) at a mass ratio of 80:20. The viscoelastic spectra and JIS A hardness
of the covering resin layer of the elevator rope were measured. As a result, the loss
modulus E" in the viscoelastic spectra was found to have two peaks, and the peak temperature
corresponding to the glass transition temperature of the polyether-based thermoplastic
polyurethane elastomer as the first resin component was found to be -30°C. Further,
the JIS A hardness of the covering resin layer was found to be 97.
(Comparative Example 1)
[0047] An elevator rope was obtained in the same manner as in Example 1 except that a covering
resin layer was formed by using only the polyether-based thermoplastic polyurethane
elastomer used in Example 1. The viscoelastic spectra and JIS A hardness of the covering
resin layer of the elevator rope were measured. As a result, the loss modulus E" in
the viscoelastic spectra was found to have one peak, and the peak temperature corresponding
to the glass transition temperature was found to be -30°C. Further, the JIS A hardness
of the covering resin layer was found to be 95.
(Comparative Example 2)
[0048] An elevator rope was obtained in the same manner as in Example 1 except that a covering
resin layer was formed by using only the polycarbonate-based thermoplastic polyurethane
elastomer used in Example 1. The viscoelastic spectra and JIS A hardness of the covering
resin layer of the elevator rope were measured. As a result, the loss modulus E" in
the viscoelastic spectra was found to have one peak, and the peak temperature corresponding
to the glass transition temperature was found to be 5°C. Further, the JIS A hardness
of the covering resin layer was found to be 95.
(Comparative Example 3)
[0049] An elevator rope was obtained in the same manner as in Example 1 except that a covering
resin layer was formed by using only the silicone-based thermoplastic polyurethane
elastomer used in Example 4. The viscoelastic spectra and JIS A hardness of the covering
resin layer of the elevator rope were measured. As a result, the loss modulus E" in
the viscoelastic spectra was found to have one peak, and the peak temperature corresponding
to the glass transition temperature was found to be -50°C. Further, the JIS A hardness
of the covering resin layer was found to be 95.
(Comparative Example 4)
[0050] An elevator rope was obtained in the same manner as in Example 1 except that a covering
resin layer was formed by using only the nylon 12 used in Example 7. The viscoelastic
spectra and JIS A hardness of the covering resin layer of the elevator rope were measured.
As a result, the loss modulus E" in the viscoelastic spectra was found to have one
peak, and the peak temperature corresponding to the glass transition temperature was
found to be 40°C. Further, the JIS A hardness of the covering resin layer was found
to be 100.
(Comparative Example 5)
[0051] An elevator rope was obtained in the same manner as in Example 1 except that the
mass ratio of the pellets of the polyether-based thermoplastic polyurethane elastomer
to the pellets of the polycarbonate-based thermoplastic polyurethane elastomer was
changed to 60:40. The viscoelastic spectra and JIS A hardness of the covering resin
layer of the elevator rope were measured. As a result, the loss modulus E" in the
viscoelastic spectra was found to have one peak, and the peak temperature corresponding
to the glass transition temperature was found to be -15°C. Further, the JIS A hardness
of the covering resin layer was found to be 95.
(Comparative Example 6)
[0052] An elevator rope was obtained in the same manner as in Example 1 except for using
a resin composition obtained by mixing the polyether-based thermoplastic polyurethane
elastomer used in Example 1 with pellets of a polyester-based thermoplastic polyurethane
elastomer (JIS D hardness: 60, glass transition temperature: -20°C) obtained by reacting
polycaprolactone diol, 4,4'-diphenylmethane diisocyanate, and 1,4-butanediol at a
mass ratio of 80:20. The viscoelastic spectra and JIS A hardness of the covering resin
layer of the elevator rope were measured. As a result, the loss modulus E" in the
viscoelastic spectra was found to have one peak, and the peak temperature corresponding
to the glass transition temperature was found to be -28°C. Further, the JIS A hardness
of the covering resin layer was found to be 97.
[0053] The friction coefficient of the elevator rope obtained in each of Examples and Comparative
Examples above was evaluated. It should be noted that the elevator rope of each of
Comparative Examples 4 and 5 was not evaluated here because the covering resin layer
was hard, and as a result, it was impossible to produce a rope having such flexibility
that the rope was capable of being bent repeatedly.
The friction coefficient was evaluated for both small sliding velocity and sliding
velocity during normal operation. FIG. 4 illustrates a configuration diagram of a
system for this evaluation. As illustrated in FIG. 4, an elevator rope 10 obtained
in each of Examples and Comparative Examples was wound around a sheave 11 at an angle
of 180 degrees, and one end thereof was connected to a weight 12. The other end was
fixed to the ground 13. Further, in order to measure a rope tension (T
1) on the weight 12 side, a load cell 14 was provided in the vicinity of a connection
part between the elevator rope 10 and the weight 12. Similarly, in order to measure
a rope tension (T
2) on the ground 13 side, the load cell 14 was provided in the vicinity of a connection
part between the elevator rope 10 and the ground 13.
[0054] In this system, when the sheave 11 is rotated in a clockwise direction at a predetermined
rate, a rope tension (T
2) on the ground 13 side is decreased by a value corresponding to a friction force
between the elevator rope 10 and the sheave 11, resulting in a tension difference
from a rope tension (T
1) on the weight 12 side. At that time, the rope tensions (T
1 and T
2) were measured using the load cell 14, and the results were substituted into the
following equation, to thereby determine a friction coefficient between the elevator
rope 10 and the sheave 11. It should be noted that measurement of the rope tensions
(T
1 and T
2) was carried out by rotating the sheave 11 in a clockwise direction at a small sliding
velocity defined as 1×10
-5 mm/sec or sliding velocities during normal operation defined as 0.01 mm/sec and 1
mm/sec. In addition, the measurement was carried out at a temperature of 25°C.
[0055] 
[0056] In the equation, θ represents a rope winding angle (i.e., 180 degrees), and K
2 represents a coefficient dependent on the shape of a sheave groove (i.e., 1.19).
For the results of friction coefficients obtained by the equation, the friction coefficients
at sliding velocities of 0.01 mm/sec and 1×10
-5 mm/sec were expressed as relative values to the friction coefficient at a sliding
velocity of 1 mm/sec, which was defined as 100. Table 1 shows the results.
[0057]
[Table 1]
| |
Sliding velocity (mm/sec) |
| 0.01 |
1×10-5 |
| Example 1 |
85 |
75 |
| Example 2 |
90 |
85 |
| Example 3 |
100 |
90 |
| Example 4 |
90 |
85 |
| Example 5 |
95 |
85 |
| Example 6 |
100 |
85 |
| Example 7 |
100 |
90 |
| Comparative Example 1 |
80 |
20 |
| Comparative Example 2 |
80 |
40 |
| Comparative Example 3 |
85 |
45 |
| Comparative Example 4 |
- |
- |
| Comparative Example 5 |
- |
- |
| Comparative Example 6 |
80 |
25 |
[0058] As is clear from the results shown in Table 1, the friction coefficients of the elevator
ropes obtained in Examples and Comparative Examples displayed a tendency to decrease
as the sliding velocity decreased. However, in the elevator rope obtained in each
of the Examples, the friction coefficient at a sliding velocity of 1×10
-5 mm/sec was able to be maintained to 75% or more of the friction coefficient at a
sliding velocity of 1 mm/sec, and the variation in friction coefficient was small.
On the other hand, in the elevator rope obtained in each of the Comparative Examples,
the friction coefficient at a sliding velocity of 1×10
-5 mm/sec decreased to 45% or less of the friction coefficient at a sliding velocity
of 1 mm/sec, and the variation in friction coefficient was large.
Further, as is clear from the results of Examples 1 to 3 and Comparative Example 5,
as the ratio of the polycarbonate-based thermoplastic polyurethane elastomer becomes
larger, the variation in friction coefficient becomes smaller. However, when the mass
ratio of the polycarbonate-based thermoplastic polyurethane elastomer to the polyether-based
thermoplastic polyurethane elastomer was too high, the covering resin layer of the
elevator rope became too hard. As a result, it was impossible to produce a rope having
such flexibility that the rope was capable of being bent repeatedly.
[0059] As is clear from the above-mentioned results, according to the present invention,
it is possible to provide an elevator rope and elevator apparatus which can stably
brake a car in a wide range of sliding velocities from a range of small sliding velocities
required for maintaining a static condition of the car to sliding velocities during
normal operation by covering a rope with a resin material having a stable friction
coefficient independent of temperature and sliding velocity.