Newton's 2nd Law applied to Rigid Bodies
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Rf=W2+Wg(hl)a;Rr=W2−Wg(hl)a
Rf=Rr=W2+Wg(hl)a
Rf=Rr=W2−Wg(hl)a
Rf=W2−Wg(hl)a;Rr=W2+Wg(hl)a
- 3.48 m/s2
- 1.78 m/s2
- 3.78 m/s2
- 3.56 m/s2
- 55.2 N
- 62.5 N
- 74.3 N
- 86.2 N
- 5 N
- 7 N
- 3.5 N
- 10 N
AB and CD are two uniform and identical bars of mass 10 kg each, as shown. The hinges at A and B are frictionless. The assembly is released from rest and motion occurs in the vertical plane. At the instant that the hinge B passes the point B', the angle between the two bars will be
60 degrees
37.4 degrees
30 degrees
45 degrees
Given in addition that the eccentric mass = 2 grams, eccentricity = 2.19 mm, mass of the mobile = 90 grams, g=9.81 ms2. Uniform speed of the motor in RPM for which the mobile will get just lifted off the ground at the end Q is approximately.
- 3000
- 3500
- 4000
- 4500
- F1≠F2;τ1=I1¨θ;F2=I2r1r22¨θ1
- F1=F2;τ1=I1[I1+I2(r1r2)2]¨θ;F2=I2r1r22¨θ1
- F1=F2;τ1=I1¨θ1;F2=I21r2¨θ2
- F1≠F2;τ1=I1[I1+I2(r1r2)2]¨θ1;F2=I21r2¨θ2
A stone of mass m at the end of a string of length I is whirled in a vertical circle at a constant speed. The tension is the string will be maximum when the stone is
At the top of the circle
Half way down from the top
Quarter way down from the top
At the bottom of the circle
A car moving with uniform acceleration covers 450 m in a 5 second interval, and covers 700 m in the next 5 second interval. The acceleration of the car is
7ms2
50ms2
25ms2
10ms2