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Turbo Pascal Chain module | 1987-10-26 | 36.7 KB | 285 lines |
- DATA AREA FOR BUILDEXE FOLLOWS
- GBIGTURBO - Large Code Model. Copyright (c) 1985 by TurboPower Software.
- "All Rights Reserved. Version 1.08D
- 0123456789ABCDEFLL
- module:
- procedure:
- called from
- module: 0
- 1Out of BIGTURBO stack space or no modules loaded.
- 3Attempting to call routine in uninitialized module.
- 3Invalid FarIncoming pointer or corrupt module code.
- Program error - code
- in FarOutgoing.
- Error while calling module:
- , procedure:
- from module
- F(AB)
- F(AB)
- F(KL)
- F(KL)
- F(KL)
- F(KL)
- F(AB)
- F(AB)
- F(KL)
- F(KL)
- F(KL)
- F(KL)
- F(AB)
- F(KL)
- F(KL)
- =The frame shown consists of two vertical members AKC and BLD
- <supported by pins and brackets at C and D and pin-connected
- >to the links AB and KL. Two horizontal loads (~P and ~Q) are
- applied at A and K as shown.
- >\We propose to find the reactions at the supports C and D and
- 4the forces exerted on member BLD by links AB and KL.
- iSelect the magnitude and sense of each load (from 5 to 100 kN), specifying its sense, and the dimensions
- (b (from 1 to 6 m) and c (from 0 to 6 m).
- D\For the value of c you have chosen, member BLD becomes a two-force
- Imember. While the method of analysis that we shall follow is still valid
- $it is not the most efficient to use.
- :For later reference, we shall determine the angle ~
- that
- $member KL forms with the horizontal:
- ~ ~[======] m `
- tan (~
- ~ ~[======] m
- VALUES
- \ ~
- Member/Frame/
- ?Shall we draw the free-body diagram of the entire frame (F) or
- 'of an individual member (M)? ~[======]
- YOUR ANSWER [M or F]
- 6\Do we know the direction of the reaction at C? ~[===]
- 6This means the reaction at C should be represented by
- ~[===] unknowns.
- YOUR ANSWER
- DThese 2 unknowns represent the components Cx and Cy of the reaction
- 7at C. We shall show them both on the free-body diagram.
- 6Do we know the direction of the reaction at D? ~[===]
- FThis means the reaction at D should be represented by ~[===] unknowns.
- YOUR ANSWER
- ;These 2 unknowns represent the components Dx and Dy of the
- Greaction at D. We shall show them both on the figure and thus complete
- #the free-body diagram of the frame.
- J&We are now ready to write the equilibrium equations for the entire frame.
- BHow many _independent_ equilibrium equations can we write? ~[===]
- YOUR ANSWER
- $How many unknowns do we have? ~[===]
- YOUR ANSWER
- D\This means that we cannot determine _all_ of the unknowns from the
- >equilibrium conditions for the entire frame. We may, however,
- determine _some_ of them.
- DIn order to write an equation involving only one unknown, should we
- Kconsider the components or the moments of the various forces? ~[==========]
- ;About what point do you wish to compute the moments of the
- forces? ~[=]
- YOUR ANSWER [C or D]
- We write the equation\
- ~MC = 0: ~[=] Dy (~[===] m) ~[=] (
- kN) (~[===] m) ~[=] (
- kN) (~[===] m) = 0
- ~MD = 0: ~[=] Cy (~[===] m) ~[=] (
- kN) (~[===] m) ~[=] (
- kN) (~[===] m) = 0
- SIGNS AND VALUES
- Solving this equation for
- , we obtain
- kN.
- <Does the sign obtained indicate that this force is directed
- upward or downward? ~[========]
- Upward/Downward/
- YOUR ANSWER [U or D]
- CCan we write _another_ equation involving only one unknown? ~[===]
- 6Will it involve moments or components? ~[===========]
- Moments about what point? ~[=]
- A/B/C/D/
- YOUR ANSWER [A,B, or D]
- YOUR ANSWER [A,B, or C]
- #Components in what direction? ~[=]
- YOUR ANSWER [X or Y]
- We write the equation
- ~Fy = 0:
- ~[=] ~[======] kN = 0
- SIGN AND VALUE
- Solving this equation for
- , we obtain
- =\Does the sign obtained indicate that this force is directed
- upward or downward? ~[========]
- Upward/Downward/
- YOUR ANSWER [U or D]
- CWe have used 2 equilibrium equations associated with the free-body
- Dof the entire frame and found 2 of the unknown reaction components,
- namely Cy and Dy.
- ;\How many more unknown reaction components are left? ~[===]
- YOUR ANSWER
- These components are Cx and Dx.
- J\Can you write an equation involving only _one_ of these unknowns? ~[====]
- ECan you write an equation involving _both_ of these unknowns? ~[====]
- <Let us write the most obvious equation involving Cx and Dx :
- ~
- ~Fx = 0: Cx + Dx +
- kN +
- kN = 0
- \We therefore have
- Cx + Dx =
- Cx+Dx
- kN
- A\Can we write another equation involving Cx and Dx, so that both
- Eequations can be solved simultaneously for these two unknowns? ~[===]
- Actually
- :, we could write an equation involving moments about some
- <appropriate point, but this equation _would not contain any
- @information we do not already have_, since only 3 _independent_
- 5equations can be obtained from any 2-dimensional FBD.
- So, we must try something else.
- >In order to proceed with the solution of the problem, we must
- @dismember the frame and sketch the free-body diagram of each of
- )its members, namely AKC, BLD, AB, and KL.
- 3\Is any of these members a two-force member? ~[===]
- 1/2/3/4/
- A\Please list all two-force members in order by number. ~[=] ~[=]`
- $ 1. AKC 2. BLD 3. AB 4. KL
- YOUR ANSWERS [1, 2, 3, or 4]
- :Let us first consider the two-force members AB and KL and
- the forces exerted on them.
- 0Do we know the direction of these forces? ~[===]
- #Do we know their magnitude? ~[====]
- Do we know their sense? ~[====]
- =While we know neither the magnitude nor the sense of the two
- Gforces acting on AB, we know they must be equal and opposite. We shall
- Marbitrarily assume that they _pull_ on AB, that is, the member is in tension.
- @Since the forces exerted on each other by two members are equal
- Band opposite (see Sec. 6.10 of _Vector Mechanics for Engineers_),
- =we may represent as shown the forces exerted by AB and KL on
- #the two vertical multiforce members
- VSince we have no further use for the two-force members AB and KL, we shall erase them.
- BWe now may use either member AKC or BLD as a free body. Since the
- Dproblem calls for the determination of the forces exerted on member
- EBLD (in addition to the reactions at both supports), we shall choose
- BLD as a free body.
- EWriting that the sum of the y components of the forces must be zero,
- Gwe conclude that Dy = 0. But we found earlier a different value for Dy.
- R\This inconsistency is due to the fact that the frame is _improperly constrained_
- *and will collapse under the given loading.
- HWe recall that we found Dy = 0 from the free-body diagram of the entire
- Lframe. We check that the equilibrium equation (~
- Fy = 0) written for _this_
- free body is satisfied.
- 6But this leaves only _two_ more independent equations
- D(out of three) to solve for the three unknowns Dx, F(AB), and F(KL).
- KThe frame is statically indeterminate. It is also _improperly constrained_
- -and would collapse under a different loading.
- GLet us remember that we have already determined the reaction component
- JDy from the free-body diagram of the entire frame. How many of the forces
- 3shown on this free-body diagram are unknown? ~[===]
- VALUE
- ,The unknown forces are Dx, F(AB), and F(KL).
- BHow many independent equilibrium equations are available from the
- 'free-body diagram of member BLD? ~[===]
- VALUE
- ?This means we can write as many equations as we have unknowns.
- 4So, we should be able to determine all the unknowns.
- ~LLet us try to write an equation with only one unknown. Should this equation
- W~;involve the components or the moments of the forces acting
- ~ on the free body? ~[===========]
- }"Components in what direction? ~[=]
- YOUR ANSWER [X or Y]
- We write the equation\
- ~Fy = 0: ~[=] F(KL) sin
- ~[=] ~[======] kN = 0\
- SIGNS AND VALUES
- z1Solving this equation for F(KL), we find F(KL) =
- <zRDoes the sign indicate that F(KL) is directed toward or away from L? ~[==========]
- Toward/Away from/
- YOUR ANSWER [T or A]
- 2x2The force exerted by KL on member BLD is therefore
- F(KL) =
- kN ~
- F(KL)
- 33333
- vIThe relatively large value obtained for F(KL) indicates a poor design of
- vJthe frame. Point L should not have been selected so close to the midpoint
- of member BD.
- uCLet us try to write another equation with only one unknown. Should
- uCthis equation involve the components or the moments of the various
- gu/forces acting on the free body? ~[===========]
- \Moments about what point? ~[=]
- YOUR ANSWER [B or D]
- (t9Referring to the free-body diagram, we write the equation
- cos/sin/
- /+/-/
- ~MB = 0: ~[=] Dx (~[======] m) ~[=] F(KL) (~[===] ~
- ) (~[======] m) = 0\
- /+/-/
- ~MD = 0: ~[=] (F(AB) ~[======] m) ~[=] F(KL) (~[===] ~
- ) (~[======] m) = 0\
- Oq-SIGNS, VALUES, AND S for SINE OR C for COSINE
- p:Substituting the numerical values of ~
- and F(KL), we have
- p6 + F(AB) (6 m) - (~[======] kN) (cos ~[======] ) (
- m) = 0
- o6 + F(AB) (6 m) + (~[======] kN) (cos ~[======] ) (
- m) = 0
- n3 + Dx (6 m) + (~[======] kN) (cos ~[======] ) (
- m) = 0
- n3 + Dx (6 m) - (~[======] kN) (cos ~[======] ) (
- m) = 0
- NUMERICAL VALUES
- Solving for Dx, we find Dx =
- l#Solving for F(AB), we find F(AB) =
- l@\Does the sign obtained indicate that this force is directed to
- ?l"the right or to the left? ~[=====]
- Left/Right/
- YOUR ANSWER [L or R]
- YOUR ANSWER [L or R]
- F(AB)
- dj5The horizontal component of the reaction at D is thus
- Dx =
- Yi,The force exerted at B on member BLD is thus
- F(AB) =
- e,force F(AB) exerted on member BLD at point B
- e!component Dx of the reaction at D
- We still have to determine the
- . Equating to zero
- eAthe sum of the x components of the forces shown on the free-body
- diagram, we write
- cos/sin/
- F(AB) ~[=] Dx
- Dx ~[=] F(AB)
- ~Fx = 0: ~[=]
- ~[=] F(KL) ~[===] ~
- b$SIGNS AND S for SINE or C for COSINE
- - F(AB)
- + Dx
- F(AB)
- ~Fx = 0:
- F(KL) cos ~
- a<\Substituting the numerical values obtained earlier we have
- - F(AB)
- ~[======]
- + Dx
- ~[======]
- ~[======] cos ~[======] = 0
- SIGNS AND VALUES
- _DWe still have to determine the horizontal component of the reaction
- ^Gat the support C of the frame. Recalling the equation obtained earlier
- ^8from the free-body diagram of the entire frame, we write
- Cx + Dx =
- ]FSubstituting the value found for Dx with the appropriate sign, we have
- Cx ~[=] ~[======] =
- VALUE
- Solving for Cx, we find Cx =
- [8\Does the sign obtained indicate that Cx is directed to
- O["the right or to the left? ~[=====]
- Left/Right/
- YOUR ANSWER [L or R]
- kN ~
- Y5The horizontal component of the reaction at C is thus
- Cx =
- X?\We have now determined all the forces and reactions requested.
- SETUPJUMPTABLE FOLLOWS
- FARCALLHANDLER FOLLOWS
-