Finally, a paragraph will be dedicated to the measurement techniques available for achieving these quantities. The instantaneous lifting velocity of the external resistance and the instantaneous force applied to the external resistance during a resistance training exercise can be estimated in two different ways. This can be achieved by measuring the instantaneous displacement of the external resistance or by estimating its instantaneous acceleration. These two approaches imply the use of two different measurement techniques/technologies: a draw wire encoder (i.e. linear position transducer or simply linear encoder) in the first case and a linear accelerometer in the second case. While accelerometers are completely wireless, draw-wire encoders still need cables for power supply and communication, although draw wire encoders with Bluetooth data transmission have recently become commercially available. From the instantaneous vertical displacement of the external resistance that is measured by a draw wire encoder, the lifting velocity and the acceleration can be estimated by the first and the double numerical differentiation of the vertical displacements, respectively. The force that is applied to the external resistance can then be obtained by multiplying the acceleration of the external resistance, added with the gravitational acceleration, multiplied by the mass of the external resistance (
11,
36). The force applied to the external resistance can be directly measured using accelerometers fixed on the barbell or on the weightstack (
8,
27,
37,
38), while instantaneous vertical velocity of the external resistance can be computed by numerical integration of the vertical acceleration. In dynamic conditions, an accelerometer sensor measures the sum of the gravitational acceleration and the acceleration due to the force impressed to the sensor along its sensitive axis. Prior to compute linear velocity through numerical integration, the acceleration due to gravity has to be removed from the sensor’s readings. This means that the use of a uniaxial accelerometer fixed on the external resistance implies an accurate manual alignment of the sensor’s sensitive axis along the vertical line in order to both easily subtract the contribution due to gravity (i.e., 9.81 m/s
2) and to fully sense the vertical acceleration produced by the force applied to the external resistance. The use of a triaxial accelerometer allows to overcome such limitations as the vertical acceleration can be computed through simple trigonometry as long as the orientation of the accelerometer remains constant during the movement of the external resistance (
37). This condition is, for instance, satisfied when the accelerometer is fixed on a weightstack. Conversely, when this condition cannot be ensured (e.g. when using barbells), the orientation in space of the accelerometer has to be known so that the 3D acceleration vector can be rotated from the sensor-embedded to a global fixed system of reference. In turn, when the sensor’s orientation is known, the accelerometer can be fixed with an arbitrarily orientation on the barbell or on the weightstack and no manual alignment is required. For this reason, accelerometers are typically used in a combination with gyroscopes becoming Inertial Measurements Units (IMU). IMU’s orientation is computed through so called “sensor fusion” algorithms (
39). Commercially available IMU’s generally come with an on-board algorithm that returns the absolute vertical acceleration. Finally, both approaches present errors due to numerical calculus. The force and the velocity that are estimated by using encoders are affected by high frequency errors related to the numerical differentiation (
40), while the velocity that is estimated by using accelerometers is affected by a low drift that is introduced by the numerical integration (
41). Errors due to numerical integration affect the accuracy of the computed linear velocity more than those related to the numerical differentiation. In fact, linear encoders have been found to be more accurate that IMUs in estimating the barbell’s vertical velocity during a squat exercise performed at a Smith machine (
42). In this same study, velocity has been proved to be more reliable than power. As power is the algebraic product of the linear velocity of the external resistance and the force applied to the external resistance, this mechanical quantity carries errors related to the computation of force when using linear encoders and errors related to the estimate of velocity when using IMUs. For this reason, a combination of a draw-wire encoder and an accelerometer, as adopted by Jidovtseff and colleagues (
9), may be the suitable measurement solution to solve the previously mentioned computational issues and obtaining a reliable determination of force, velocity and power data. It can be concluded that draw-wire encoders should be preferred to accelerometry when the force-velocity profile assessment has to be pushed towards very high loads as it has been shown how the reliability of accelerometers decreases approaching 90% of the 1RM (
43). This is because the acceleration of the external resistance would be close to the gravitation acceleration in case of very slow movements and the accelerometer would not be able to sense any variation of velocity.