Full energy of spring-mass system is W = W p + W k W = Wp + Wk W = W p + Wk ;
W p = k x 2 2 − Wp = \frac{kx^2}{2} - W p = 2 k x 2 − Potential energy
W k = m V 2 2 Wk = \frac{mV^2}{2} Wk = 2 m V 2 - kinetic energy
x - displacement of mass;
K - constant factor characteristic of the spring, its stiffness.
m-mass;
V-velocity of mass;
If equation of oscillation is x = A cos ( w t ± φ ) x = A\cos (wt \pm \varphi) x = A cos ( wt ± φ ) or x = A sin ( w t ± φ ) x = A\sin (wt \pm \varphi) x = A sin ( wt ± φ ) , we have
W p = k ( ( A cos ( w t ± φ ) ) 2 2 = k 2 A 2 cos 2 ( w t ± φ ) Wp = \frac{k\left(\left(A\cos(wt\pm\varphi)\right)^{2} \right.}{2} = \frac{k}{2} A^{2}\cos^{2}(wt\pm\varphi) W p = 2 k ( ( A c o s ( wt ± φ ) ) 2 = 2 k A 2 cos 2 ( wt ± φ )
V = x ′ ( t ) V = x^{\prime}(t) V = x ′ ( t ) - derivative from x ( t ) \mathbf{x}(t) x ( t )
x ′ ( t ) = ( A s i n ( w t ± φ ) ) ′ = A ⋅ w ⋅ cos ( w t ± φ ) x^{\prime}(t) = \left(Asin(wt\pm \varphi)\right)^{\prime} = A\cdot w\cdot \cos (wt\pm \varphi) x ′ ( t ) = ( A s in ( wt ± φ ) ) ′ = A ⋅ w ⋅ cos ( wt ± φ )
W k = m V 2 2 = m 2 ⋅ A 2 ⋅ w 2 ⋅ s i n 2 ( w t ± φ ) Wk = \frac{mV^2}{2} = \frac{m}{2}\cdot A^2\cdot w^2\cdot sin^2 (wt\pm \varphi) Wk = 2 m V 2 = 2 m ⋅ A 2 ⋅ w 2 ⋅ s i n 2 ( wt ± φ )
W = m 2 ⋅ A 2 ⋅ w 2 ⋅ sin 2 ( w t ± φ ) + k 2 A 2 cos 2 ( w t ± φ ) W = \frac{m}{2} \cdot A^2 \cdot w^2 \cdot \sin^2(wt \pm \varphi) + \frac{k}{2} A^2 \cos^2(wt \pm \varphi) W = 2 m ⋅ A 2 ⋅ w 2 ⋅ sin 2 ( wt ± φ ) + 2 k A 2 cos 2 ( wt ± φ )
Where w = k / m w = \sqrt{k / m} w = k / m