This application is based upon and claims the benefit of priority of the prior Japanese Patent Application No. 2014-208041, filed on Oct. 9, 2014, the entire contents of which are incorporated herein by reference.
The embodiments discussed herein are related to a valve structure.
As a valve structure provided to an exhaust pipe, Japanese Utility Model Laid-Open (JP-U) No. H03-51124, for example, describes a structure provided to an outer shell of a muffler in which, when high pressure exhaust gas acts on a valve body being biased against an opening by a spring, the valve body rotates about a shaft, and opens the opening.
For example, there is a description in Japanese Patent Application Laid-Open (JP-A) No. H09-303143 of a structure in which a butterfly valve is fixed to a valve shaft provided so as to be rotatable to a casing. In JP-A No. H09-303143, the butterfly valve is constantly biased in the closing direction by the recovery force of a return spring wound around the outer periphery of the valve shaft. The structure of JP-A No. H09-303143 is such that the spring force of a compression spring acts on a link fixed to the valve shaft. When the butterfly valve is open, spring force of the compression spring acts in the butterfly valve closing direction up to the point that a coupling pin of the link reaches a turnover position. When the coupling pin passes the turnover position, the spring force of the compression spring acts in the butterfly valve opening direction.
JP-U No. H03-51124
JP-A No. H09-303143
As a valve structure for opening and closing the inside of an exhaust pipe by rotating (swinging) a valve member, there is a structure in which a valve member is biased to a closed position by employing a spring or the like. When a portion of spring force acts as a large load on a shaft of a valve member, the friction against a shaft bearing portion becomes large, and the valve member becomes difficult to close. If the spring force in the closing direction is set large in order to reliably close the valve member (maintain the closed position), it becomes difficult to secure a large opening angle.
Moreover, although a structure is conceivable in which a link is attached to a rotation shaft, and spring force acts on this link, in a structure in which a torsion spring is wound around a rotation shaft, it is difficult to secure an effective length for the link.
In consideration of the above circumstances, the present invention addresses obtaining a valve structure that secures a large opening angle of the valve member by reducing the friction between rotation shaft and shaft bearing by reducing the biasing force of a biasing member that biases a valve member in the closing direction.
In a first aspect, a valve member is provided at an exhaust pipe and rotates from a closed position closing off the exhaust pipe to an open position opening the exhaust pipe upon being contacted by exhaust gas, a rotation shaft is fixed to the valve member at a position, when viewing the valve member along an exhaust gas flow direction, inside a tangent to an outer periphery of the valve member and avoiding a center point of the valve member, and is attached to the exhaust pipe so as to be capable of rotating, a link member is fixed to the rotation shaft and includes an action point at a position distanced from the rotation shaft in the flow direction, and a tension spring is provided at the exhaust pipe and causes tension force to constantly act on the action point to generate a rotation force toward a closing direction of the valve member.
In this valve structure, the valve member rotates with the rotation shaft as the center of rotation, and opens and closes the inside of the exhaust pipe.
Tension force of the tension spring acts on the action point of the link member fixed to the rotation shaft. A portion of this tension force acts on the rotation shaft as rotation force toward the valve member closing direction. Namely, the valve member receives rotation force toward the closing direction from the tension force of the tension spring. When the force from the exhaust gas acting on the valve member toward the opening direction becomes large, the valve member is rotated in the opening direction against the rotation force from the tension force of the tension spring in the closing direction.
The rotation shaft (center of rotation) is at a position that is inside a tangent to the outer periphery of the valve member and avoids the center point of the valve member. Namely, forces from the exhaust gas acting on the valve member act as rotation forces in opposite directions to each other on a large area portion (a face including the center point, a pressure bearing face) and on a small area portion (a face not including the center point) that have the rotation shaft as the boundary therebetween. A portion of the force from the exhaust gas acting on the large area portion of the valve member is canceled out by the force acting on the small area portion. The effective force from the exhaust gas acting on the valve member in the opening direction is accordingly smaller than in structures in which the rotation shaft is provided at a position of the tangent to the outer periphery of the valve member.
In this manner, the force from the exhaust gas acting on the valve member in the opening direction is smaller, and therefore even if a small tension force is set for the tension spring, the valve member can still be reliably returned to the closed position, or the closed position can be maintained, in a state in which there is a weak flow of exhaust gas.
By making the tension force of the tension spring weaker, the component of the tension force from the tension spring on the rotation shaft in the direction toward the center of rotation also becomes smaller. Frictional force acts between the rotation shaft and shaft bearings, however this frictional force is also smaller. The frictional force being smaller enables a large rotation angle to be set for the open position of the valve member.
In addition, in the first aspect, it is the tension spring that is the member that causes tension force, generating rotation force toward the valve member closing direction to constantly act on the action point. This member, accordingly, gives a high degree of freedom in the shape of a link member in comparison to structures in which this member is configured by a torsion spring wound around a rotation shaft, for example. Setting the position of the action point of the link member a sufficient distance away from the rotation shaft enables the rotation moment acting on the rotation shaft to be made larger. This thereby enables the tension force of the tension spring to be set smaller, enabling the component of the tension force on the rotation shaft from the tension spring in the direction toward the center of rotation to be made smaller.
A second aspect is the first aspect in which a pressure bearing face including the center point of the valve member has a shape bulging toward a downstream side in the flow direction.
Thus, when the valve member is oriented in the open position, the surface pressure acting due to the flow of exhaust gas is higher, and the force that rotates the valve member toward the open position is also larger, on progression away from the rotation shaft.
A third aspect is the second aspect in which a curvature of the pressure bearing face, as viewed in cross-section taken along the flow direction, increases as a distance from the rotation shaft increases, or is constant.
If the curvature of the pressure bearing face, as viewed in cross-section taken along the flow direction, is shaped so as to decrease as the distance from the center of rotation increases, there is a concern that negative pressure might be generated when exhaust gas hits the pressure bearing face and flows along the pressure bearing face. As in the third aspect, by making the curvature of the pressure bearing face increase as the distance from the center of rotation increases, or constant, negative pressure can be suppressed from occurring, and so there is a large force rotating the valve member toward the open position.
Explanation follows regarding a valve structure of a first exemplary embodiment of the present invention, with reference to the drawings.
As illustrated in
The direction of exhaust gas flow is illustrated by the arrow F1 in the drawings. Reference simply to “upstream” and “downstream” respectively indicates “upstream” and “downstream” in the direction of exhaust gas flow. In the present exemplary embodiment, the outer tube 34 has a substantially cylindrical shape overall. The flow direction of exhaust gas matches the axial direction of the outer tube 34.
As illustrated in
The valve structure 32 includes a valve member 38 disposed inside the outer tube 34. As illustrated in
The shape of the valve member 38 as viewed face-on (as viewed along the arrow F1 direction) is, in the first exemplary embodiment, a substantially circular shape matching the internal shape of the outer tube 34, as can be seen from
The center point CP of the valve member 38 illustrated in
A rotation shaft 40 is fixed to the valve member 38. Both end portions of the rotation shaft 40 are supported by shaft bearings 42 attached to the outer tube 34, so as to be capable of rotating with respect to the outer tube 34. In the present exemplary embodiment, the shaft bearings 42 are provided at the recesses 36, and portions on both sides of the rotation shaft 40 pierce through the outer tube 34 at the recesses 36. Packing 44 is disposed between the pierced portions (through holes) in the outer tube 34, and the rotation shaft 40, maintaining an airtight seal between the inside and the outside of the outer tube 34.
The position of the rotation shaft 40 is to the inside of a tangent to the outer periphery of the valve member 38, and is a position avoiding the center point CP of the valve member 38. Thus, as can be seen from
A bracket 48 is fixed to the outer periphery of the outer tube 34. An anchor portion 50 is formed to a leading end of the bracket 48. One end of a return spring 52 (anchor point KP) is anchored to the anchor portion 50. In the first exemplary embodiment, the bracket 48 is provided at a position of one of the recesses 36.
A link arm 54, serving as an example of a link member, is fixed to a portion where the rotation shaft 40 projects out from the outer tube 34 and the shaft bearing 42 (on the same side as the bracket 48). An anchor portion 56 is formed to the link arm 54. The other end of the return spring 52 is anchored to the anchor portion 56.
The return spring 52 is a tension coil spring that causes a tension force to act on the link arm 54. The tension force of the return spring 52 acts on the rotation shaft 40 through the link arm 54. Part of the tension force (tangential direction component SF-T, described below) acts constantly in a direction to swing the valve member 38 in the closing direction (an arrow T1 direction).
As is apparent from
A stopper tab 58 is attached to the outer periphery of the outer tube 34 at the upstream side of the rotation shaft 40. A closing direction stopper projection 60 and an opening direction stopper projection 62 are formed to the link arm 54. The closing direction stopper projection 60 and the opening direction stopper projection 62 respectively project out to the radial direction outside as viewed along the rotation shaft 40.
The closing direction stopper projection 60 is formed at a position so as to abut the stopper tab 58 when the valve member 38 attempts to rotate further in the closing direction (the arrow T1 direction) from a closed position TP (see
The opening direction stopper projection 62 is formed at a position so as to abut the stopper tab 58 when the valve member 38 attempts to rotate further in the opening direction (the arrow H1 direction) from an open position HP (see
Explanation next follows regarding operation of the present exemplary embodiment.
In a state in which exhaust gas is not flowing inside the outer tube 34, and in a state in which there is a low flow velocity of exhaust gas, the valve member 38 receives part of the tension force acting from the return spring 52 as a rotation force in the closing direction, and is in the closed position TP, as illustrated in
When the flow velocity of the exhaust gas inside the outer tube 34 rises, a force from the exhaust gas acts on the valve member 38, acting in the opening direction (the arrow H1 direction) on the large area portion 38A, and acting in the closing direction (the arrow T1 direction) on the small area portion 38B. Due to the surface area of the large area portion 38A being greater than the surface area of the small area portion 38B, the force received from the exhaust gas is also greater, with these forces acting in opposite rotation directions to each other. Part of the rotation force in the opening direction acting on the large area portion 38A is accordingly canceled out by the rotation force in the closing direction acting on the small area portion 38B. As a result a rotation force acts on the valve member 38 in the opening direction. When this rotation force becomes larger than the rotation force from the return spring 52 acting in the closing direction, the valve member 38 rotates in the opening direction.
As illustrated in
When the rotation force from the exhaust gas acting in the opening direction becomes less than the rotation force from the return spring 52 acting in the closing direction, the valve member 38 rotates in the closing direction.
Explanation follows regarding the position of the rotation shaft 40, namely, the center of rotation of the valve member 38, with reference to
In
In contrast thereto, in
In
As is apparent from
As is apparent from
As is apparent from the graph, in the first exemplary embodiment, the rotation force acting on the valve member 38 from the exhaust gas in the opening direction is smaller than in the first comparative example. Thus the rotation force acting on the rotation shaft 40 from the return spring 52 in the closing direction is also set smaller in the first exemplary embodiment than in the first comparative example. The “shaft friction resistance force”, namely the frictional force between the rotation shaft 40 and the shaft bearings 42, is also smaller in the exemplary embodiment than in the first comparative example. In order to actually rotate the valve member 38 in the closing direction, the rotation force in the closing direction needs to be larger than the shaft friction resistance force, and the opening angle of the valve member 38 at the intersection of the curves indicating this point is the “maximum degree of opening”. It is apparent that in the first exemplary embodiment, the maximum degree of opening is larger than that of the first comparative example.
Moreover, in the first exemplary embodiment, the return spring 52, as an example of a tension coil spring, is employed as the member to cause rotation force to act on the rotation shaft 40 in the closing direction. In contrast thereto, instead of a tension coil spring, for example, a type of spring that is wound around the rotation shaft 40 (a torsion coil spring) might also be considered. However, if a torsion coil spring is mounted to the rotation shaft 40 with an action point AP (see
In the first exemplary embodiment, the tension coil spring is employed as a member to cause rotation force to act on the valve member 38 in the closing direction, and so there is a large degree of freedom for setting the position of the action point AP. It is accordingly possible to position the action point AP at a position a distance away from the rotation shaft 40. Distancing the action point AP from the rotation shaft 40 enables a large rotation force (rotation moment) to act on the rotation shaft 40 in the closing direction, even when the tension force of the return spring 52 is weak. Making the tension force of the return spring 52 weak makes the “maximum degree of opening” of the valve member 38 larger.
As described above, the position of the rotation shaft 40 (the center of rotation) is preferably near to the center point CP from the perspective of making the rotation force in the opening direction from the exhaust acting on the valve member 38 gas smaller. However, if, as illustrated in
Explanation follows regarding a second exemplary embodiment. In the second exemplary embodiment, elements, members, etc. that are the same as those of the first exemplary embodiment are allocated the same reference numerals, and detailed explanation will be omitted thereof.
In a valve structure 112 of the second exemplary embodiment, the structure of the valve member differs from that of the first exemplary embodiment. Namely, as illustrated in
In the example illustrated in
In the valve structure 112 of the second exemplary embodiment, in a state in which exhaust gas is not flowing inside the outer tube 34 and a state in which the flow velocity of exhaust gas is low, the valve member 118 does not rotate in the opening direction or the closing direction, and is maintained in the closed position TP.
In the second exemplary embodiment, the large area portion 118A (pressure bearing face) has a bulging shape toward the downstream side in the flow direction of the exhaust gas. Thus, as illustrated in
Specifically, in the second exemplary embodiment, the curvature of the large area portion 118A of the valve member 118 is constant irrespective of the distance from the rotation shaft 40 (the center of rotation). In other words, in the second exemplary embodiment, as illustrated in
In the second exemplary embodiment, as illustrated in
A valve member 120 of a first modified example of the second exemplary embodiment may be employed as a valve member, as illustrated in
In the structure illustrated in
Consider, as a second modified example of the second exemplary embodiment, as illustrated in
In the second modified example, when the imaginary circle KC is envisaged at a freely selected point AA of the large area portion 128A, then the large area portion 128A is positioned further to the downstream side than the imaginary circle KC at positions further from the rotation shaft 40 than point AA. In such a structure, as illustrated in
Although the structure of the second modified example is also included in the present invention, generation of negative pressure that acts as a rotation force on the valve member 118, 120 in the closing direction can be particularly suppressed from being generated in the second exemplary embodiment and the first modified example when the valve member 118, 120 is in the open position HP. This thereby makes the opening angle of the valve member 118, 120 large.
Explanation next follows regarding a third exemplary embodiment. The same reference numerals are appended in the third exemplary embodiment to elements and members the same as those of the first exemplary embodiment and the second exemplary embodiment, and detailed explanation thereof will be omitted.
A valve structure 212 of the third exemplary embodiment includes, as illustrated in
The bracket 214 includes an anchor portion 216. The position of the anchor portion 216 (an anchor point KP2) has point symmetry centered on the rotation shaft 40 to the position of the anchor portion 50 (an anchor point KP1) in a side view of the outer tube 34, as illustrated in
A link arm 218 of the third exemplary embodiment includes two anchor portions 220, 222. The anchor portion 220 (an action point AP1) and the anchor portion 222 (an action point AP2) are positioned with point symmetry to each other, centered on the rotation shaft 40.
The third exemplary embodiment includes a return spring 224 in addition to the return spring 52. One end of the return spring 52 is anchored to the anchor portion 50, and the other end thereof is anchored to the anchor portion 220. One end of the return spring 224 is anchored to the anchor portion 216, and the other end thereof is anchored to the anchor portion 222. The two return springs 52, 224 accordingly cause tension forces SF, TF to act in directions with point symmetry with respect to the link arm 218, at positions with point symmetry centered on the rotation shaft 40.
However, a normal direction component SF-N of the tension force SF acting from the return spring 52 and of a normal direction component TF-N of the tension force TF acting from the return spring 224 have the same magnitude as each other, and act in opposing directions so as to cancel each other out. Thus there is no effective force from the return springs 52, 224 acting at the contact portions between the rotation shaft 40 and the shaft bearings 42 (or only a small force even if one acts), and frictional force between the rotation shaft 40 and the shaft bearings 42 is also small.
In the third exemplary embodiment, as described above, since there is no effective force from the return springs 52, 224 acting at the contact portions between the rotation shaft 40 and the shaft bearings 42, the frictional force between the rotation shaft 40 and the shaft bearings 42 is small, and is constant irrespective of the opening angle. The maximum degree of opening of the third exemplary embodiment is accordingly a larger maximum degree of opening than the maximum degree of opening of the first exemplary embodiment and the maximum degree of opening of the second exemplary embodiment.
In the third exemplary embodiment, in the above example, the two return springs 52, 224 can be said to have a rotational symmetry relationship that is two-fold rotational symmetry about the rotation shaft 40. In the third exemplary embodiment N return springs may be provided at positions so as to give N-fold rotational symmetry, wherein N is an integer of two or more. For example, if N=3, then this would be a configuration in which three return springs are provided at rotation symmetrical positions, at positions having center angles of 120°.
In the first exemplary embodiment to the third exemplary embodiment, the pair of recess 36 are formed to the outer tube 34, and the shaft bearings 42 are provided in the recesses 36. Namely, the recesses 36 act as the seating faces of the shaft bearings 42. This thereby enables a structure to be implemented with high surface rigidity of the seating face portions of the shaft bearings 42. The high surface rigidity of the seating face portions of the shaft bearings 42 suppresses flexing from occurring in the outer tube 34 due to force acting on the outer tube 34 from the shaft bearings 42. Misalignment between the center lines of the shaft bearings 42 and the rotation shaft 40 is thereby suppressed, suppressing the frictional force between the shaft bearings 42 and the rotation shaft 40 from increasing, and enabling a larger maximum degree of opening of the valve member 38, 118.
As explained above, a large opening of the valve member 38, 118 is possible in the valve structures of the first exemplary embodiment to the third exemplary embodiment, enabling a wide cross-sectional area to be secured for exhaust gas to pass through. Therefore, for example, even when an engine is operating at high revolutions, the pressure loss in the valve member 38 is small, enabling implementation of the valve structure 32 with a high back pressure reduction effect.
As an example,
As can be seen from
In the valve structures of the first exemplary embodiment to the third exemplary embodiment, the large opening of the valve member 38 enables noise arising from exhaust gas hitting the valve member 38 to be reduced.
As an example,
Moreover, in the valve structure of the first exemplary embodiment to the third exemplary embodiment, the large opening of the valve member 38 enables resonation noise arising from the return spring 52 (or the return springs 52, 224) and exhaust gas acting on the valve member 38, 118 to be suppressed.
In a system that vibrates with one degree of freedom, generally a vibration frequency f is given by the following equation, wherein the spring constant of a spring causing the tension force in the system is k, and the inertial moment of the system is I.
I is related by the following equation to the mass m of the system, and a distance L from the center of rotation (the rotation shaft 40) to the center of mass.
For example, it is apparent from Equation (2) that as the mass m increases, the inertial moment I of the system also gets larger. It is apparent from Equation (1) that when the inertial moment I increases, the vibration frequency f decreases. However, a larger mass m also leads to an increase in mass of the valve structure.
In contrast, in the first exemplary embodiment to the third exemplary embodiment, the springs with small tension force can be employed as the return springs 52, 224, with this leading to a small spring constant k in Equation (1). The mass m of the valve members 38, 118 is not large in the first exemplary embodiment to the third exemplary embodiment, so this does not lead to an increase in mass of the valve structures 32, 112, 212.
In the present application, biasing force of a biasing member biasing the valve member in closing direction is lowered, reducing friction between the rotation shaft and the shaft bearings, and enabling a large opening angle of the valve member to be secured.
The entire content of the disclosure of Japanese Patent Application No. 2014-208041 filed on 9 Oct. 2014 is incorporated by reference in the present application.
All cited documents, patent applications and technical standards mentioned in the present specification are incorporated by reference in the present specification to the same extent as if the individual cited documents, patent applications and technical standards were specifically and individually incorporated by reference in the present specification.
Number | Date | Country | Kind |
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2014-208041 | Oct 2014 | JP | national |