A particle A moves along a circle of radius R=50 cm so that its radius vector r relative to the point O (figure) rotates with the constant angular velocity ω=0.4 rad/s. Then modulus of the velocity of the particle, and the modulus of its total acceleration will be:
We fix the coordinate system as shown so that ∠BOA=θ
The particles rotates clockwise thus w=−dθ/dt
From triangle OAB
Rsinθ=rsin(π−2θ)⇒r=2Rcosθ
Since
→r=rcosθ^i+rsinθ^j=2Rcos2θ^i=Rsin2θ^jd→rdt=→v=2R2cos(−sinθ)dθdt^i+2Rcos2θdθdt^j=2Rw(sin2θ^i−cos2θ^j)∣∣→v∣∣=2wR=0.4m/s
Since w is constant dvdt=0
∴ centripetal acceleration:
ac=v2R=4w2R=0.32m/s2