The First Law of Thermodynamics states that the change in internal energy of a system equals the sum of heat transferred to the system and work done on the system:
This is conservation of energy for thermodynamic processes. Energy of the universe is constant—if a system gains energy, surroundings lose it. The system can gain energy two ways:
Heat flowing in (q > 0): molecules collide with hotter surroundings, speed up
Work done on it (w > 0): compression makes molecules crowd and move faster
Physicist convention (don't use in chemistry): ΔU = q − w (work done BY system is positive). We avoid this because chemists care about the system's perspective: what happens to the system.
Starting point: Conservation of energy for an isolated system (system + surroundings).
Euniverse=Esystem+Esurroundings=constant
Taking differentials:
dEsystem+dEsurroundings=0
So:
dEsystem=−dEsurroundings
For the system, internal energy can change via:
Heat transfer (δq): energy transfer due to temperature difference
Work transfer (δw): energy transfer due to organized force × displacement
WHY these two only? These are the ONLY ways energy crosses boundaries at the molecular level. Heat = random molecular collisions. Work = coordinated force (like a piston pushing).
For an infinitesimal process:
dU=δq+δw
Integrating over a finite process:
ΔU=∫δq+∫δw=q+w
WHY is ΔU a state function but q and w are not?
ΔU depends only on initial and final states (like elevation change hiking: only depends on start/end altitude, not path).
q and w depend on the PATH taken (like distance walked: depends if you zigzag or go straight).
This is why we write dU (exact differential) but δq and δw (inexact differentials).
Enthalpy definition: At constant P, we define H = U + PV so that ΔH = q_p (heat at constant pressure). This only makes sense BECAUSEΔU = q + w.
Hess's Law: ΔU is path-independent, so we can add reaction steps algebraically.
Calorimetry: We measure heat (q) under controlled conditions (constant V or P) to find ΔU orΔH.
Carnot cycle: Efficiency limits arise from first law applied to cyclic processes (ΔU_cycle = 0).
Philosophical point: This law says energy is conserved but transferable. The universe's total energy is fixed since the Big Bang. Every chemical reaction, every engine, every living cell operates under this constraint. We can't create energy; we can only move it around and change its form.
Recall Explain to a 12-year-old
Imagine you have a pigy bank (the system). The money inside is the "internal energy." You can change how much money is in there two ways:
Someone gives you money (heat q): You get $5 from grandma → q = +5. The pigy bank has more money now.
You do chores and earn money (work w): You help wash the car and earn $3 → w = +3. Again, more money in the bank.
Or the reverse:
You buy candy (release heat): You take out $2 for candy → q = −2
You lend your friend money (do work on surroundings): You loan $4 → w = −4
The First Law just says: The change in your piggy bank (ΔU) = money given to you (q) + money you earned (w).
If grandma gave you 5butyouloaned5 to a friend, your piggy bank didn't change (ΔU = 0), even though money moved around. That's like isothermal expansion: heat comes in, work goes out, internal energy stays same!
What is the First Law of Thermodynamics in chemist sign convention? :: ΔU = q + w, where ΔU is change in internal energy, q is heat absorbed by system, w is work done on system.
In chemist sign convention, what is the sign of q when heat is absorbed by the system? :: Positive (+). Heat flowing INTO the system is positive.
In chemist sign convention, what is the sign of w when work is done BY the system (expansion)?
Negative (−). Work done BY the system means energy leaves, so w < 0.
Why is internal energy U a state function but heat q and work w are path functions?
U depends only on initial and final states (like altitude). q and w depend on the process path taken between states (like distance traveled).
For an ideal gas undergoing isothermal expansion, what is ΔU and why?
ΔU = 0 because internal energy of ideal gas depends only on temperature. Isothermal means ΔT = 0, so ΔU = 0.
A gas absorbs 600 J of heat and does 200 J of work on its surroundings. What is ΔU?
ΔU = q + w = (+600) + (−200) = +400 J. Heat in is +600 J, work by system is −200 J.
Why does a bomb calorimeter measure ΔU directly?
Because it operates at constant volume (rigid container), so w = 0. Then ΔU = q +0 = q. The heat measured equalsΔU.
In adiabatic compression, 500 J of work is done on a gas. What is q andΔU?
q = 0 (adiabatic means no heat transfer). ΔU = 0 + 500 = +500 J. All compression work becomes internal energy.
What happens to the energy of a system during one complete cycle in a cyclic process?
ΔU = 0 for a complete cycle because U is a state function. The system returns to initial state, so U_final = U_initial.
Why does isothermal expansion of an ideal gas require heat input even though temperature doesn't change?
The gas does work (w < 0) during expansion. To keepΔU = 0 (since ΔT = 0), heat must flow in (q > 0) to balance: ΔU = q + w = 0.
Thermodynamics ka sabse important rule hai First Law: ΔU = q + w. Iska matlab hai ki system ki internal energy (U) sirf do tarike se badal sakti hai—ya toh heat flow hoke (q) ya phir work karke (w).
Chemist sign convention mein hum system ki taraf se sochte hain: agar heat system mein aye toh q positive (+), agar system se bahar jaye toh q negative (−). Similarly, agar koi system par work kare (compression) toh w positive, aur agar system khud work kare (expansion) toh w negative. Ye "bank account" jaisa hai—jo andar aye woh plus, jo bahar jaaye woh minus.
Example lo: ek gas 500 J heat absorb kare aur 200 J work kare apne surroundings par (expansion). Toh ΔU = (+500) + (−200) = +300 J. Iska matlab internal energy 300 J badh gayi because heatzyada aaya, work kam kiya.
Ye law pure universe mein lagta hai—energy na ban sakti hai, na mit sakti hai, sirf transfer hoti hai. Isliye jab bhi reaction karo, combustion engine chalao, ya kuch bhi—is First Law ki boundary ke andar hi rehna padta hai. Chemistry mein hum isse use karke enthalpy (ΔH), calorimetry calculations, aur Hess's Law ko samajhte hain. Bilkul fundamental hai!