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7.1 Physics for Engineers

Key Takeaways

  • Newtonian mechanics governs physical kinetics via F=maF = ma, impulse-momentum (Δp=FΔt\Delta p = F \Delta t), work-energy relations, and rotational torque τ=Iα\tau = I \alpha.

  • The First Law of Thermodynamics specifies energy conservation (ΔU=Q−W\Delta U = Q - W), while the Second Law establishes entropy bounds and the Carnot efficiency limit ηCarnot=1−TCTH\eta_{\text{Carnot}} = 1 - \frac{T_C}{T_H}.

  • Electromagnetism relies on Coulomb's law, Gauss's law (∮E⋅dA=Qencε0\oint \mathbf{E} \cdot d\mathbf{A} = \frac{Q_{\text{enc}}}{\varepsilon_0}), Ampere's law, and Faraday's law of induction (e=−NdΦdte = -N \frac{d\Phi}{dt}) with Lenz's law establishing opposing polarity.

  • Heat transfer occurs through conduction (q=−kAdTdxq = -k A \frac{dT}{dx}), convection (q=hAΔTq = h A \Delta T), and radiation (q=εσAT4q = \varepsilon \sigma A T^4), which dictate equipment thermal rating and cooling.

  • Waves and optics govern simple harmonic motion (T=2πmkT = 2\pi\sqrt{\frac{m}{k}}), wave propagation (v=fλv = f \lambda), Snell's law of refraction (n1sin⁡θ1=n2sin⁡θ2n_1 \sin\theta_1 = n_2 \sin\theta_2), and total internal reflection.

Last updated: August 2026

7.1 Physics for Engineers

Engineering Physics serves as a core foundation for the Engineering Sciences and Allied Subjects (ESAS) portion of the PRC Registered Electrical Engineer (REE) Licensure Examination. A rigorous understanding of mechanics, thermodynamics, heat transfer, electromagnetism, and wave optics is vital for solving board exam problems and analyzing physical systems.


1. Classical Mechanics & Rotational Dynamics

Kinematics & Linear Kinetics

Linear motion under constant acceleration aa is described by the fundamental kinematic equations:

v=v0+atv = v_0 + at s=v0t+12at2s = v_0 t + \frac{1}{2} a t^2 v2=v02+2asv^2 = v_0^2 + 2as

According to Newton's Second Law of Motion, the net external force acting on a body equals the time rate of change of its linear momentum:

F=dpdt=maF = \frac{dp}{dt} = m a
  • Work (WW): W=∫F⋅ds=Fscos⁡θW = \int \mathbf{F} \cdot d\mathbf{s} = F s \cos\theta
  • Kinetic Energy (KK): K=12mv2K = \frac{1}{2} m v^2
  • Work-Energy Theorem: Wnet=ΔK=Kf−KiW_{\text{net}} = \Delta K = K_f - K_i
  • Impulse-Momentum Principle: J=∫Fdt=Δp=m(vf−vi)J = \int F dt = \Delta p = m(v_f - v_i)
  • Mechanical Power (PP): Rate of doing work: P=dWdt=F⋅vP = \frac{dW}{dt} = \mathbf{F} \cdot \mathbf{v}

Rotational Dynamics

For rigid bodies rotating about a fixed axis with angular velocity ω\omega and angular acceleration α\alpha:

Linear QuantityRotational AnalogGoverning Relationship
Position ssAngle θ\thetas=rθs = r \theta
Velocity vvAngular Velocity ω\omegav=rωv = r \omega
Acceleration aaAngular Acceleration α\alphaat=rαa_t = r \alpha
Mass mmMoment of Inertia III=∫r2dmI = \int r^2 dm
Force FFTorque τ\tauτ=Iα=rFsin⁡θ\tau = I \alpha = r F \sin\theta
Momentum p=mvp = mvAngular Momentum LLL=IωL = I \omega
Kinetic Energy KL=12mv2K_L = \frac{1}{2}mv^2Rotational KE KRK_RKR=12Iω2K_R = \frac{1}{2} I \omega^2
Power P=FvP = FvRotational Power PPP=τωP = \tau \omega

2. Thermodynamics & Heat Transfer

Laws of Thermodynamics

  1. First Law (Energy Conservation): The change in internal energy ΔU\Delta U of a closed system is equal to net heat added QQ minus net work done by the system WW: ΔU=Q−W\Delta U = Q - W
  2. Second Law (Entropy & Efficiency): Heat cannot spontaneously flow from a colder body to a hotter body. The thermal efficiency of any heat engine operating between a hot reservoir at absolute temperature THT_H and a cold reservoir at TCT_C is strictly bounded by the Carnot Efficiency: ηCarnot=1−TCTH=TH−TCTH\eta_{\text{Carnot}} = 1 - \frac{T_C}{T_H} = \frac{T_H - T_C}{T_H} (Note: Temperatures THT_H and TCT_C must always be converted to absolute units in Kelvin: K=∘C+273.15K = ^\circ\text{C} + 273.15)

Heat Transfer Modes

  • Conduction (Fourier's Law): Heat transfer through a solid medium via molecular vibration:

    q=−kAdTdx  ⟹  Q=kA(T1−T2)tLq = -k A \frac{dT}{dx} \implies Q = \frac{k A (T_1 - T_2) t}{L}

    where kk is thermal conductivity (W/(m⋅K)\text{W}/(\text{m}\cdot\text{K})), AA is cross-sectional area, LL is thickness, and tt is time.

  • Convection (Newton's Law of Cooling): Heat transfer between a surface and a flowing fluid:

    q=hA(Ts−Tf)q = h A (T_s - T_f)

    where hh is the convection heat transfer coefficient (W/(m2⋅K)\text{W}/(\text{m}^2\cdot\text{K})).

  • Radiation (Stefan-Boltzmann Law): Thermal radiation emitted by a body at absolute temperature TT:

    q=εσAT4q = \varepsilon \sigma A T^4

    where σ=5.670×10−8 W/(m2⋅K4)\sigma = 5.670 \times 10^{-8}\ \text{W}/(\text{m}^2\cdot\text{K}^4) is the Stefan-Boltzmann constant, and ε\varepsilon is surface emissivity (0≤ε≤10 \le \varepsilon \le 1).


3. Electromagnetism & Field Fundamentals

Electrostatics & Coulomb's Law

The electrostatic force between two point charges q1q_1 and q2q_2 separated by distance rr in vacuum is:

F=14πε0q1q2r2F = \frac{1}{4\pi \varepsilon_0} \frac{q_1 q_2}{r^2}

where ε0≈8.854×10−12 F/m\varepsilon_0 \approx 8.854 \times 10^{-12}\ \text{F/m} is the permittivity of free space.

Gauss's Law

The net electric flux through any closed surface equals the enclosed charge divided by ε0\varepsilon_0:

∮E⋅dA=Qencε0\oint \mathbf{E} \cdot d\mathbf{A} = \frac{Q_{\text{enc}}}{\varepsilon_0}

Electromagnetic Induction & Faraday's Law

An induced electromotive force (emf) ee is produced in a closed circuit whenever the magnetic flux Φ=∫B⋅dA\Phi = \int \mathbf{B} \cdot d\mathbf{A} linking the circuit changes over time:

≠=−NdΦdt\ne = -N \frac{d\Phi}{dt}

According to Lenz's Law (represented by the negative sign), the direction of the induced current creates a magnetic field that opposes the change in magnetic flux that produced it.

Lorentz Force Law

A charge qq moving with velocity v\mathbf{v} through electric field E\mathbf{E} and magnetic field B\mathbf{B} experiences force:

F=q(E+v×B)\mathbf{F} = q (\mathbf{E} + \mathbf{v} \times \mathbf{B})

4. Waves, Sound & Optics

Simple Harmonic Motion (SHM) & Wave Motion

For a mass-spring system in SHM, the period of oscillation TT and frequency ff are:

T=2πmk,f=12πkmT = 2\pi \sqrt{\frac{m}{k}}, \quad f = \frac{1}{2\pi} \sqrt{\frac{k}{m}}

For wave propagation with velocity vv, frequency ff, and wavelength λ\lambda:

v=fλv = f \lambda

Geometrical Optics & Refraction

  • Snell's Law of Refraction: n1sin⁡θ1=n2sin⁡θ2n_1 \sin\theta_1 = n_2 \sin\theta_2 where n=c/vn = c/v is the refractive index of the medium.
  • Critical Angle & Total Internal Reflection: Occurs when light travels from a dense medium (n1n_1) into a less dense medium (n2<n1n_2 < n_1) at an angle exceeding θc\theta_c: sin⁡θc=n2n1\sin\theta_c = \frac{n_2}{n_1}
  • Thin Lens Formula: 1f=1do+1di\frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i} where ff is focal length, dod_o is object distance, and did_i is image distance.

Solved Practice Examples

Example 1: Rotational Power & Torque Calculation

Problem: An electric motor generates a constant shaft torque of 180 N⋅m180\ \text{N}\cdot\text{m} while rotating at 1,750 rpm1,750\ \text{rpm}. Calculate the mechanical output power in kilowatts (kW) and horsepower (hp).

Solution:

  1. Convert rotational speed rpm\text{rpm} to angular velocity ω\omega in rad/s\text{rad/s}: ω=1,750×2π60=3,500π60≈183.26 rad/s\omega = 1,750 \times \frac{2\pi}{60} = \frac{3,500 \pi}{60} \approx 183.26\ \text{rad/s}
  2. Calculate mechanical power P=τωP = \tau \omega: P=180×183.26=32,986.7 W≈32.99 kWP = 180 \times 183.26 = 32,986.7\ \text{W} \approx 32.99\ \text{kW}
  3. Convert kW to mechanical horsepower (1 hp=746 W1\ \text{hp} = 746\ \text{W}): Php=32,986.7746≈44.22 hpP_{\text{hp}} = \frac{32,986.7}{746} \approx 44.22\ \text{hp}

Example 2: Carnot Engine Thermal Efficiency

Problem: A thermal power plant operates between a steam turbine inlet temperature of 520∘C520^\circ\text{C} and a condenser cooling water outlet temperature of 35∘C35^\circ\text{C}. Determine the maximum theoretical Carnot thermal efficiency of this power plant.

Solution:

  1. Convert inlet (THT_H) and outlet (TCT_C) temperatures to absolute Kelvin: TH=520+273.15=793.15 KT_H = 520 + 273.15 = 793.15\ \text{K} TC=35+273.15=308.15 KT_C = 35 + 273.15 = 308.15\ \text{K}
  2. Compute Carnot efficiency ηCarnot\eta_{\text{Carnot}}: ηCarnot=1−TCTH=1−308.15793.15=1−0.3885=0.6115(61.15%)\eta_{\text{Carnot}} = 1 - \frac{T_C}{T_H} = 1 - \frac{308.15}{793.15} = 1 - 0.3885 = 0.6115 \quad (61.15\%)
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Thermodynamic Heat Engine Cycle & Carnot Efficiency
Theoretical Carnot Thermal Efficiency (%) vs Hot Reservoir Temperature TH (with TC = 300 K)
Test Your Knowledge

A rotating generator shaft delivers a torque of 250 N⋅m250\ \text{N}\cdot\text{m} at a constant speed of 1,200 rpm1,200\ \text{rpm}. What is the mechanical power output of the shaft?

A

31.42 kW

B

300.00 kW

C

15.71 kW

D

62.83 kW

Test Your Knowledge

A heat engine operates between a heat source at 450∘C450^\circ\text{C} and a heat sink at 50∘C50^\circ\text{C}. What is the maximum possible thermal efficiency of this engine?

A

88.89%

B

55.31%

C

45.00%

D

62.15%

Test Your Knowledge

A coil with 200 turns is placed in a magnetic field. If the magnetic flux through the coil decreases uniformly from 0.05 Wb0.05\ \text{Wb} to 0.01 Wb0.01\ \text{Wb} in a time interval of 0.1 seconds0.1\ \text{seconds}, what is the magnitude of the induced electromotive force (emf)?

A

8 Volts

B

40 Volts

C

80 Volts

D

800 Volts

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