Force Voltage Analogy

In this Article, We will be going to Know what is Force Voltage Analogy, We will go through the Mathematical Model of the Mechanical System Which is Classified into Two types Translational and Rotational Systems. Then we go through the Mathematical Model of the Electrical System, Then we go through the Force Voltage Analogy, At last, we will Conclude our Article With its Applications and Some FAQs.

What is the Force Voltage Analogy?

Two systems are said to be analogous to each other when they respond to inputs and disturbances in a mathematically equivalent way, even though the underlying physical processes or components are completely different. The systems can be modeled by the same differential equations and exhibit similar transient responses, steady-state behavior, and stability characteristics. For example, both systems might show exponential decay, sinusoidal behavior, or other recognizable responses. The core idea of the Force-Voltage analogy in control systems engineering is to relate mechanical systems with their electrical counterparts, by assuming Force in a mechanical system to be analogous to the Voltage in an electrical system.

Mathematical Model of Mechanical Systems

Mechanical Systems can be classified into two types based on their type of motion:

• Translational Systems – Linear motion
• Rotational Systems – Circular motion

Translational Systems

Translational Systems are characterized by movement in straight lines and primarily consist of three basic elements – masses, springs and dampers. Consider the following translational mechanical system.

Translation Mechanical System

A mass ‘M’ is tethered to a fixed rigid support via a spring (with spring constant ‘K’), and the friction between the mass ‘M’ and the fixed surface is indicated by a damper with viscous damping coefficient ‘B’. An external force F(t) is being applied to this mass, causing a displacement x(t) in the direction of the applied force. Thus, the free body diagram of the Mass block can be drawn as follows.

Mass Block Free Body Diagram

Now, according to Newtons second law, the sum of all external forces applied on a body is directly related to the acceleration it undergoes in the same direction, and inversely proportional to its mass.

∑ External Forces = Mass ✖ Acceleration

bringing the right hand side to the left,

∑ F – ma = 0

and then considering the ‘ma’ term to be a force itself, we are left with D’Alembert’s Law

∑ F = 0

essentially implying that the algebraic sum of all the forces acting on a mechanical system is zero. In other words, the sum of all applied forces is equal to the sum of all opposing forces.

Going back to the considered system, and applying this law,

Externally applied force = Inertial force + Frictional force + Restoring force of Spring

[Tex]F(t) [/Tex] = [Tex]F_m [/Tex] + [Tex]F_{\text{friction}} [/Tex] + [Tex]F{\text{spring}} [/Tex]

F(t) = Ma(t) + Bv(t) + Kx(t)

[Tex]F(t) = M \frac{d^2x(t)}{dt^2} + B \frac{dx(t)}{dt} + kx(t) [/Tex]

Taking the Laplace Transform of this equation (assuming initial conditions to be zero), we get the s-domain equation modeling a translational mechanical system

[Tex]F(s) = Ms^2X(s) + BsX(s) + KX(s) [/Tex] ⇒ Eq. 1

Mathematical Model of Electrical Systems

Next, an electrical RLC network is considered

RLC network (Electrical System)

An input voltage v(t) is applied generating a current i(t) flowing through the Resistor ‘R’, Inductor ‘L’ and Capacitor ‘C’. According to Kirchhoff’s Voltage Law, the algebraic sum of potential differences in a loop must be equal to zero. Employing this law, the equation for this RLC network is given by

[Tex]V(t) – V_R – V_L – V_c = 0 [/Tex]

Writing this equation in terms of the currents flowing through the RLC elements,

[Tex]V(t) = R i(t) + L\frac{di(t)}{dt} + \frac{1}{c} \int i(t) \, dt [/Tex]

Taking the Laplace Transform of this equation leaves us with,

[Tex]LsI(s) + RI(s) + \frac{1}{c} \frac{I(s)}{s} [/Tex]

Although this equation describes a differential model of an electrical network, it isn’t comparable to Eq. 1 derived for a mechanical system just yet since the powers of ‘s’ are one order higher in every term of the mechanical systems equation.

Since current is nothing but the rate of flow of electric charge

[Tex]i(t) [/Tex] = [Tex]\frac{dq(t)}{dt} [/Tex]

taking the Laplace Transform of this equation gives

[Tex]I(s) = sQ(s) [/Tex]

Hence, modeling the electrical networks equation with replace [Tex]I(s) [/Tex] with [Tex]sQ(s) [/Tex] instead, we get a more comparable s-domain equation modeling an electrical RLC system

[Tex]Ls^2Q(s)+RsQ(s)+\frac{Q(s)}{c} [/Tex] ⇒ Eq. 2

Force-Voltage Analogy

• Assuming Force (F) in a mechanical system to be analogous to Voltage (V) in an electrical system
• On comparing the coefficients of the [Tex]s^2 [/Tex] terms of the differential equations modeling a mechanical and electrical system in Eq.1 and Eq.2 respectively, it can be inferred that the Mass (M) in a mechanical system is analogous to Inductance (L) in an electrical system
• Comparing the coefficients of the [Tex]s^1 [/Tex] terms of Eq.1 and Eq.2, it can be inferred that the Viscous Damping Coefficient (B) in a mechanical system is analogous to Resistance (R) in an electrical system
• Comparing the coefficients of the [Tex]s^0 [/Tex] terms of Eq.1 and Eq.2, it can be inferred that the Spring Constant (K) in a mechanical system is analogous to the Reciprocal of Capacitance (1/C) in an electrical system
• Analogies can also be drawn from the variables modeling the differential equations for the two systems. Hence, the displacement x(t) in a mechanical system is analogous to charge q(t) in an electrical system
• It can also be inferred that velocity v(t) in a mechanical system is analogous to current i(t) in an electrical system from the previous statement

Rotational Systems

This analogy can also be extended to rotational systems where a Torque balanced equation is used to model the differential equation representing the system.

Rotational Mechanical System

Applied Torque = Inertial Torque + Frictional Torque + Restoring Torque of Spring

[Tex]\tau(t) = \tau_m + \tau_{friction}+\tau_{sping} [/Tex]

[Tex]\tau = J \frac{d^2\theta(t)}{dt^2} + B \frac{d\theta(t)}{dt} + K\theta(t) [/Tex]

Correlating this equation to the differential equations representing the translational and electrical systems, the following table of analogous quantities can be drawn

TRANSLATIONAL SYSTEM	ROTATIONAL SYSTEM	ELECTRICAL SYSTEM
Force (F)	Torque (T)	Voltage (V)
Mass (M)	Moment of Inertia( J)	Inductance (L)
Viscous Damping Coefficient (B)	Torsional Frictional Constant (B)	Resistance (R)
Spring Constant (K)	Torsional Spring Constant (K)	Reciprocal of Capacitance (1/C)
Displacement (x)	Angular Displacement (θ)	Charge (q)
Velocity (v)	Angular Velocity (ω)	Current (I)

Translational Mechanical to Electrical System Conversion Example

Now that correlations between mechanical and electrical systems have been made, converting systems with a single set of translational, rotational or RLC elements is pretty straight forward. However, when systems have multiple sets of elements a few additional analogies have to be taken into consideration:

• Similar to how elements in series in electrical systems have the same current flowing through them, in mechanical systems, elements with the same velocity are considered to be in series
• Each Mass block (Node) in mechanical systems correspond to a closed loop in an electrical system
• Elements connected between two masses in mechanical systems correspond to elements common between two meshes in electrical systems

Let us consider the following two-mass-block translational system

Two-mass-block Translational System

The two mass blocks imply the electrical system must have two closed loops in the electrical system, and the spring [Tex]K_{12} [/Tex] is converted to a common capacitor [Tex]C_{12} [/Tex] between the two loops.

Two-loop Electrical System

Applications of Force Voltage Analogy

• Transducers are devices that take energy from one domain as input and convert it to another energy domain as output. With respect to electromechanical systems they are typically sensors or actuators. Designing and understanding the dynamics of such systems becomes significantly easier by treating them as electrical circuits with corresponding components representing their mechanical equivalents
• By drawing parallels between mechanical and electrical parameters, existing electrical filter theory can be applied to mitigate unwanted vibrations in mechanical systems
• Roboticists also take advantage of the Force-Voltage analogy when selecting actuators, analyzing sensor data and designing control algorithms
• Investigation of mechanical properties of materials under different stress and strain conditions can be done using specialized transducers and electrical analysis
• The mechanical parts of acoustic systems like record player pickups and tonearms can be analyzed using electrical analogies

Conclusion

In conclusion, the Force-Voltage analogy proves to be a powerful tool in designing and analyzing control systems that utilize both mechanical and electrical components. By establishing parallels between Force and Voltage, Mass and Inductance, Displacement and Charge, Friction and Resistance and Springs and Capacitance, existing knowledge and techniques in electrical systems can be used to address problems in the mechanical world and vice-versa. It is crucial, however, to acknowledge that the accuracy of the Force-Voltage Analogy is particularly limited to linear and/or low-frequency ideal systems. Despite these limitations, the analogies present a swift practical path to designing and optimizing control systems.

FAQs on Force Voltage Analogy

Can the force-voltage analogy be extended to rotational systems? If so, how?

Yes, using torque instead of force, and moment of inertia instead of mass

What additional analogies need to be considered when converting systems with multiple mechanical or electrical elements?

Similar elements in series have the same velocity, mass blocks correspond to closed loops, elements between masses correspond to elements between meshes

How do transducers benefit from the force-voltage analogy?

Simpler design process of electromechanical systems by treating them as electrical circuits.

What are some limitations of the force-voltage analogy?

Accuracy is limited to linear and low-frequency ideal systems.