Question #196810

In a four bar chain ABCD, link AD is fixed and the crank AB rotates at 10 rad/sec clockwise. Length of the links are AB=60

mm; BC=CD=70 mm; DA= 120 mm. When the angle DAB = 60o and both B and C lie on the same side of AD, find 1.angular

velocities (magnitude and direction) of BC and CD; and 2.angular acceleration of BC and CD.


1
Expert's answer
2021-05-24T19:10:02-0400

By measurement , we find that-

VCD== Vector dc == 4.6×scale=4.6×0.1=0.46m/sec4.6 \times scale=4.6\times0.1=0.46m/sec

VCB== VBC== Vector C== 4.4×scale=4.4×0.1=0.44m/sec\times scale=4.4\times 0.1=0.44m/sec


Angular velocity if link BC-

VBC=Vectorbc=0.44m/secVBC= Vector bc =0.44m/sec

wBC=VBCBC=0.440.07=6.28rad/sec= \frac{VBC}{BC}= \frac{0.44}{0.07}=6.28rad/sec

wBC =6.28rad/sec=6.28rad/sec


Angular velocity of link CD

VCD=vector dc=0.46m/secVCD=vector \space dc=0.46m/sec

wCD=VCDCD=0.460.07=6.57rad/sec=\frac{VCD}{CD}=\frac{0.46}{0.07}=6.57rad/sec

wCD=6.57rad/sec=6.57rad/sec



Angular Acceleration of links BC &CD

-since the angular acceleration of the crank AB is not given, therefore there will be no tangential component of the acceleration of B with respect to A.

-we know that the radial component of the acceleration of B with respect to A ( on the acceleration of B)

aBAr=aBA=aB=vBA2AB=(0.6)20.06=6m/s2a^r_{BA}=a_{BA}=a_B=\frac{v^2_{BA}}{AB}=\frac{(0.6)^2}{0.06}=6m/s^2

-Radial component of the acceleration of C with respect to B1B_1

aCBr=V2CBBC=(0.44)20.07=2.76m/s2a^r_{CB}=\frac{V^2CB}{BC}=\frac{(0.44)^2}{0.07}=2.76m/s^2

and,

-radial component of the acceleration of C with respect to D (or the acceleration of C)

aCDr=aCD=ac=v2CDDC=(0.46)20.07=3.02m/s2a^r_{CD}=a_{CD}=a_c=\frac{v^2CD}{DC}=\frac{(0.46)^2}{0.07}=3.02m/s^2


(i) since A and D are fixed points ,therefore these points lie at one place in the acceleration diagram. Draw vector a'b' parallel to AB ,to some suitable scale , to represent the radial component of acceleration of B with it aBAra^r_{BA} or aBa_B such that,

vector a'b' =aBAr=aB=6M/S2=a ^r_{BA}=a_B=6M/S^2

(ii) from point b' , draw vector b' parallel to BC to represent the radial component of acceleration of C with respect to B i.e aCBra^r_{CB} such that


vectorbx=aCBr=2.76m/svector b'x=a^r_{CB}= 2.76m/s

(iii) from point x , draw vector xc' perpendicular to BC to respect the tangential component of acceleration of C with respect to B i.e aCBta_{CB}^t while magnitude is not yet known.

(iv) now from point d' draw vector d'y parallel to DC represent the radial component of the acceleration of C with respect to D

Vectordy=aCDr=3.02m/s2Vector d'y=a^r_{CD}=3.02m/s^2

(v) from point y, draw vector yc' perpendicular ti DC to represent the tangetial acceleration of C with respect to D i.e

aCDta^t_{CD}

(vi) the vector xc' and yc' intersect at join a'c' and b'c' . By measurement we find that-

aCBr=vectorxc=0.7×1=0.7m/s2a_{CB}^r= vector xc'= 0.7\times 1=0.7m/s^2

ACDt=vectoryc=7.2m/s2A_{CD}^t= vector yc' =7.2m/s^2

now ,angular acceleration of link BC,

αBC=aCBtBC=0.70.07=10rad/s2\alpha BC =\frac{a_{CB}^t}{BC}=\frac {0.7}{0.07}=10 rad/s^2

αCD=aCDtDC=7.20.07=102.85rad/s2\alpha CD = \frac{a_{CD}^t}{DC}=\frac {7.2}{0.07}=102.85 rad/s^2




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