By M. J. Iremonger
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Extra resources for Basic Stress Analysis
1 270 PRINT 280 NEXT El 290 GO TO 30 READY RUN E X 3 P 01N T 4 GRAVITIONAL 3 - J U N ···· 81 13 : 4 5 Î 4 6 IMPACT LOADING STRESSES AND STRAINS INPUTÎ MASS OF FALLING WEIGHT (KG) - 0 TO STOP? 80 DROP HEIGHT (M)? 1. :l. (Ï1 1. * '. '"V. G2'1! ♦ flAl'ilVÎÏ ♦ 'M1I 1 ♦ I <4AHV 200 200 200 1. 1. ill M \ ,'Vfl ίΠ . 'Τ. Ιί'. 'M 2V ■ i ♦ 12 '245 0Λ(»1"ίΙ(1 Λ -}Λ ,'<0""> (KG) - 0 TO STOP? e. xhPh where P is the maximum force induced in the member). 14) hence Solving this quadratic equation in P for the positive root gives the required expression for P.
15) This is calculated and printed as a percentage in line 230. (3) The calculations are performed using units of newtons and millimetres. The input data is immediately converted to these units and is converted back to the original units if required for output (line 230). (4) The range of values for E, L and diameter D are generated automatically by DO loops. Note the indirect way in which the values of E and L are determined (lines 170 and 190). 5 Materials comparison A range of materials with typical properties for short-term loading at 20°C is tabulated below.
Write a program to calculate the other two constants if any two of them are specified. 7 for the torsion of circular shafts is not restricted to situations in which the torque is applied statically. Rotating shafts are used for transmitting power. e. Nm/s), equals torque multiplied by the angle through which the shaft rotates per unit of time. The rotational speed is usually measured in revolutions per minute (rev/min). 5 so that the value of torque used in the analyses (Γ, N mm) are determined from 'run-time' input of power to be transmitted (in kW) and rotational speed (in rev/ min).
Basic Stress Analysis by M. J. Iremonger