A particle travels along a straight line with a velocity of v(t)=3e^(-1/2)sin(2t) meters per second. What is the total distance in meters, traveled by the particle during the time interval 0
1 answer:
Solve for v(t)=0 over the interval [0,2] <span>sin(pi)<0, try t=pi/2, </span> <span>3e^(-pi/4)sin(pi)= 0, so the interval 0 to pi/2 the particle travels forward [0,pi/2), then it goes negative for the rest of the interval (pi/2,2) and travels backward. </span> <span>total distance = |integral 0 to pi/2 v(t) dt| + |integral pi/2 to 2 v(t) dt| </span>∫[0 to π/2] v(t) dt = ∫[0 to π/2] (3 e^(−t/2) sin(2t)) dt <span>. . . . . . . . . . . . . = ∫[0 to π/2] (3 e^(−t/2) sin(2t)) dt </span> <span>. . . . . . . . . . . . . = −6/17 e^(−t/2) (sin(2t) + 4cos(2t)) |[0 to π/2] </span> <span>. . . . . . . . . . . . . = −6/17 (e^(−π/4) (sin(π) + 4cos(π)) − e^(0) (sin(0) + 4cos(0))) </span> <span>. . . . . . . . . . . . . = −6/17 (e^(−π/4) (0 − 4) − (0 + 4)) </span> <span>. . . . . . . . . . . . . = −6/17 (−4e^(−π/4) − 4) </span> <span>. . . . . . . . . . . . . = 24/17 (e^(−π/4) + 1) </span> <span>. . . . . . . . . . . . . = 2.05544 </span> ∫[π/2 to 2] v(t) dt = ∫[π/2 to 2] (3 e^(−t/2) sin(2t)) dt <span>. . . . . . . . . . . . . = ∫[π/2 to 2] (3 e^(−t/2) sin(2t)) dt </span> <span>. . . . . . . . . . . . . = −6/17 e^(−t/2) (sin(2t) + 4cos(2t)) |[π/2 to 2] </span> <span>. . . . . . . . . . . . . = −6/17 (e^(−1) (sin(4) + 4cos(4)) − e^(−π/4) (sin(π) + 4cos(π))) </span> <span>. . . . . . . . . . . . . = −6/17 ( (sin(4)+4cos(4))/e − e^(−π/4) (0 − 4)) </span> <span>. . . . . . . . . . . . . = −6/17 ( (sin(4)+4cos(4))/e + 4e^(−π/4)) </span> <span>. . . . . . . . . . . . . = −0.205938 </span><span> </span> <span>when you add absolute values of area you get actual distance traveled: </span> <span>∫[0 to π/2] v(t) dt − ∫[π/2 to 2] v(t) dt </span> <span>= 2.05544 − (−0.205938) </span> <span>= 2.05544 + 0.205938 </span> <span>= 2.261378 </span>
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