koopas
Aerospace
- Aug 24, 2002
- 106
Good morning all,
I was reading the FAA paper by T. Swift entitled "Repairs to Damage Tolerant Aircraft"
I've got a few questions regarding the highest rivet loads at the first row (end row) of fasteners (pages 3, 4, figs. 1, 3, & 5 of the paper).
I can grasp the rationale behind how load is being incidentally transferred from the skin into the external doubler starting at the first row. Let me paraphrase: the load sigma_hoop is being partially reacted by the first fastener with the force F. The load that's not reacted is being bypassed to the next fastener in the basic skin as shown by sigma_bp. Now, the force F at the first skin fastener is being reacted in the doubler hole by and
opposite load F.
First question: Is force F acting on the skin and doubler holes opposite and equal in magnitude?
Second question: Refer to Fig. 1c, regarding the reacted force F in the DOUBLER skin hole, shouldn't force F's direction be in the same direction as force F of the skin hole? Isn't the doubler "helping out" with countering the hoop stress sigma_hoop? I am not physically seeing it. Perhaps someone could slowly walk me through what's happening in Fig. 1c.
Third question: Ref. fig 1c, is sigma_d acting on the doubler related to force F on the doubler hole in the following way: F = sigma_d*(0.05*width of doubler) ?
Fourth question: On page 4, the first row rivets are calculated to experience 187.2 lbs each. Is that value equal to force F? I.e. is the force F equal to the fastener load?
Fifth question: The bearing stress in the basic skin is then computed at 187.2/(0.04 x .19) ~ 24 ksi, where 0.04 is the basic skin thickness and .19 is the rivet diameter. Would the bearing stress in the doubler be computed as 187.3/(0.05 x .19) ~ 20 ksi, where 0.05 is the doubler thickness. Does this explain why cracks in external doubler repairs occur at the outer row, on the thinner basic skin?
Last question: I don't understand why the end fastener load is a function of doubler thickess. I would think the end fastener load would be constant, only being dependent upon the basic skin's characteristics. As previously discussed, the skin hole reacts some of the hoop stress with force F, and that load is reacted into the doubler. The doubler simply seems to passively receive the load. How can increasing the doubler thickness increase the fastener load? In fact, due to the larger doubler cross sectional area, the stress in the doubler should be reduced. I am confused.
Thanks for shedding some light,
Alex
I was reading the FAA paper by T. Swift entitled "Repairs to Damage Tolerant Aircraft"
I've got a few questions regarding the highest rivet loads at the first row (end row) of fasteners (pages 3, 4, figs. 1, 3, & 5 of the paper).
I can grasp the rationale behind how load is being incidentally transferred from the skin into the external doubler starting at the first row. Let me paraphrase: the load sigma_hoop is being partially reacted by the first fastener with the force F. The load that's not reacted is being bypassed to the next fastener in the basic skin as shown by sigma_bp. Now, the force F at the first skin fastener is being reacted in the doubler hole by and
opposite load F.
First question: Is force F acting on the skin and doubler holes opposite and equal in magnitude?
Second question: Refer to Fig. 1c, regarding the reacted force F in the DOUBLER skin hole, shouldn't force F's direction be in the same direction as force F of the skin hole? Isn't the doubler "helping out" with countering the hoop stress sigma_hoop? I am not physically seeing it. Perhaps someone could slowly walk me through what's happening in Fig. 1c.
Third question: Ref. fig 1c, is sigma_d acting on the doubler related to force F on the doubler hole in the following way: F = sigma_d*(0.05*width of doubler) ?
Fourth question: On page 4, the first row rivets are calculated to experience 187.2 lbs each. Is that value equal to force F? I.e. is the force F equal to the fastener load?
Fifth question: The bearing stress in the basic skin is then computed at 187.2/(0.04 x .19) ~ 24 ksi, where 0.04 is the basic skin thickness and .19 is the rivet diameter. Would the bearing stress in the doubler be computed as 187.3/(0.05 x .19) ~ 20 ksi, where 0.05 is the doubler thickness. Does this explain why cracks in external doubler repairs occur at the outer row, on the thinner basic skin?
Last question: I don't understand why the end fastener load is a function of doubler thickess. I would think the end fastener load would be constant, only being dependent upon the basic skin's characteristics. As previously discussed, the skin hole reacts some of the hoop stress with force F, and that load is reacted into the doubler. The doubler simply seems to passively receive the load. How can increasing the doubler thickness increase the fastener load? In fact, due to the larger doubler cross sectional area, the stress in the doubler should be reduced. I am confused.
Thanks for shedding some light,
Alex