The equation of motion of a one-dimensional forced harmonic oscillator in the presence of a dissipative...
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The equation of motion of a one-dimensional forced harmonic oscillator in the presence of a dissipative force is described by +16x=6te +4t²e". The general form of the d²x dt² dx dt particular solution, in terms of constants A, B etc., is (a) t(At² + Bt+C)e²²¹ +(Dt +E) e¨¯³¹ (c) 1 (At² + Bt+C)e²²¹ +1(Dt+E) e¯³ +10. -8r (b) (At² + Bt+C)e²¹ +(Dt + E)e-³¹ (d) (At² + Bt+C)e²²¹ +t(Dt+E)e¯* The equation of motion of a one-dimensional forced harmonic oscillator in the presence of a dissipative force is described by +16x=6te +4t²e". The general form of the d²x dt² dx dt particular solution, in terms of constants A, B etc., is (a) t(At² + Bt+C)e²²¹ +(Dt +E) e¨¯³¹ (c) 1 (At² + Bt+C)e²²¹ +1(Dt+E) e¯³ +10. -8r (b) (At² + Bt+C)e²¹ +(Dt + E)e-³¹ (d) (At² + Bt+C)e²²¹ +t(Dt+E)e¯*
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